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<Worksheet><Version major="6" minor="1"/><View-Properties><Zoom percentage="100"/></View-Properties><Styles><Layout alignment="left" firstindent="0.0" leftmargin="0.0" linebreak="space" linespacing="0.0" name="Heading 3" rightmargin="0.0" spaceabove="0.0" spacebelow="0.0"/><Layout alignment="centred" firstindent="0.0" leftmargin="0.0" linebreak="space" linespacing="0.0" name="Author" rightmargin="0.0" spaceabove="8.0" spacebelow="8.0"/><Layout alignment="left" firstindent="0.0" leftmargin="0.0" linebreak="space" linespacing="0.0" name="Heading 2" rightmargin="0.0" spaceabove="8.0" spacebelow="2.0"/><Layout alignment="left" firstindent="0.0" leftmargin="0.0" linebreak="space" linespacing="0.0" name="Heading 1" rightmargin="0.0" spaceabove="8.0" spacebelow="4.0"/><Layout alignment="left" firstindent="0.0" leftmargin="0.0" linebreak="space" linespacing="0.0" name="Normal" rightmargin="0.0" spaceabove="0.0" spacebelow="0.0"/><Layout alignment="centred" bullet="none" name="Maple 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executable="false" family="Times New Roman" foreground="[0,0,0]" italic="false" name="Normal260" readonly="false" size="12" underline="false"/><Font background="[0,0,0]" family="Times New Roman" name="Page Number" underline="false"/><Font background="[0,0,0]" italic="true" name="_cstyle263"/><Font background="[0,0,0]" italic="true" name="_cstyle262"/><Font background="[0,0,0]" italic="true" name="_cstyle261"/><Font background="[0,0,0]" italic="true" name="_cstyle260"/></Styles><Page-Numbers enabled="false" first-number="1" first-numbered-page="1" horizontal-location="right" style="Page Number" vertical-location="bottom"/><Group><Input><Text-field layout="Title" style="Title">Description of Mechanical Systems by the Use of Quadripole Parameters</Text-field><Text-field layout="Author" style="Author">Harald Kammerer</Text-field><Text-field layout="Normal263" style="Normal263">The author expects that this worksheet will only be used for teaching and educational purposes and not for commercial profit without contacting the author for a licensed agreement. </Text-field><Text-field layout="Normal" style="Normal">The following numerical values are only academic examples and have no reference to real structures.</Text-field></Input></Group><Group><Input><Text-field layout="Heading 1" style="Heading 1">Motivation</Text-field><Text-field layout="Normal" style="Normal">Let's consider a mechanical device defined with an input gate and an output gate. At the input gate there are two values of the force <Equation input-equation="F[1]" style="2D Comment">NiMmJSJGRzYjIiIi</Equation> and the velocity <Equation input-equation="v[1]" style="2D Comment">NiMmJSJ2RzYjIiIi</Equation>.  At the output gate there are the two values of the force <Equation input-equation="F[2];" style="2D Comment">NiMmJSJGRzYjIiIj</Equation> and the velocity <Equation input-equation="v[2];" style="2D Comment">NiMmJSJ2RzYjIiIj</Equation>. So we have all in all two gates and four items. This system can be described in the equivalent manner as an electrical quadripole. So we call this system a mechanical quadripole. Such a quadripole is shown in Figure 1.</Text-field><Text-field alignment="centred"><Image height="104" 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style="Normal">

For example in [2] there is some more detailed description of this method. Here we will give a first introduction in this theory.</Font></Text-field><Text-field layout="Normal" style="Normal">We can consider it as a black box. It is not important of what the device consists. It is only important how it works. In this worksheet we will see how we can use this method to work with some special dynamical systems. But first we have to give some conditions for the  mechanical systems. Perhaps not all of the following conditions are necessary, but they will help to understand this idea.</Text-field></Input></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">restart:</Font></Text-field></Input></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">with(linalg):with(plots):</Font></Text-field></Input></Group><Group><Input><Text-field layout="Normal" style="Normal">We define a helpful procedure first. This procedure is used in the following to convert complex values into the standard form <Equation input-equation="z=a+I*b" style="2D Comment">NiMvJSJ6RywmJSJhRyIiIiomJSJJR0YnJSJiR0YnRic=</Equation>. </Text-field></Input></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">complexextension:=proc(a)</Font></Text-field><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">local z,n,zr,nr,zi,ni,zbr,zbi,nb,b;</Font></Text-field><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">z:=numer(a);</Font></Text-field><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">n:=denom(a);</Font></Text-field><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">zi:=coeff(z,I);</Font></Text-field><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">zr:=simplify(z-zi*I);</Font></Text-field><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">ni:=coeff(n,I);</Font></Text-field><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">nr:=simplify(n-ni*I);</Font></Text-field><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">zbr:=(zr*nr+zi*ni);</Font></Text-field><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">zbi:=(zi*nr-zr*ni);</Font></Text-field><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">nb:=(nr**2+ni**2);</Font></Text-field><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">b:=simplify(zbr/nb)+simplify(zbi/nb)*I;</Font></Text-field><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">end:</Font></Text-field></Input></Group><Group><Input><Text-field layout="Heading 1" style="Heading 1">Conditions</Text-field><Text-field layout="Normal" style="Normal">At first we assume that all  motions are harmonic vibrations. All other kind of motions must be analyzed by use of a Fourier transformation. Further, the devices should be a straight line. There is only one input gate and one output gate. That means for example that no rocking of the foundation is possible. We consider devices with linearly dependantence between the force and the displacement, velocity or the acceleration is possible. For example no Duffing device is considered.</Text-field></Input></Group><Group><Input><Text-field layout="Normal" style="Normal">All the following relations are defined by use of the angular frequency <Equation input-equation="Omega" style="2D Comment">NiMlJk9tZWdhRw==</Equation>. For practical use it is usual to consider the frequency <Equation input-equation="f" style="2D Comment">NiMlImZH</Equation>. The relation between <Equation input-equation="Omega" style="2D Comment">NiMlJk9tZWdhRw==</Equation> and <Equation input-equation="f " style="2D Comment">NiMlImZH</Equation> is</Text-field></Input></Group><Group><Input><Text-field layout="Normal256" prompt="&gt; " style="2D Input"><Equation executable="true" input-equation="sub1:=Omega=2*Pi*f;" style="2D Input">NiM+JSVzdWIxRy8lJk9tZWdhRyooIiIjIiIiJSNQaUdGKSUiZkdGKQ==</Equation></Text-field></Input><Output><Text-field layout="Maple Output" style="2D Output"><Equation>NiM+SSVzdWIxRzYiL0kmT21lZ2FHRiUsJComSSNQaUdJKnByb3RlY3RlZEdGKyIiIkkiZkdGJUYsIiIj</Equation></Text-field></Output></Group><Group><Input><Text-field layout="Heading 1" style="Heading 1">Description of the motion</Text-field><Text-field layout="Normal" style="Normal">Every motion, especially every harmonic vibration, can be described by the displacement, the velocity or the acceleration. Of course there are some constants of integration, but in our consideration they are not important.
We describe here the motion by the velocity, as shown in Figure 1. The velocity should be given as a harmonic vibration in complex notation.</Text-field></Input></Group><Group><Input><Text-field layout="Normal256" prompt="&gt; " style="2D Input"><Equation executable="true" input-equation="v(t):=v0*exp(I*Omega*t):" style="2D Input">NiM+LSUidkc2IyUidEcqJiUjdjBHIiIiLSUkZXhwRzYjKiglIklHRiolJk9tZWdhR0YqRidGKkYq</Equation></Text-field></Input></Group><Group><Input><Text-field layout="Normal" style="Normal">The displacement is can be integrated from the velocity</Text-field></Input></Group><Group><Input><Text-field layout="Normal256" prompt="&gt; " style="2D Input"><Equation executable="true" input-equation="x(t):=int(v(t),t);" style="2D Input">NiM+LSUieEc2IyUidEctJSRpbnRHNiQtJSJ2R0YmRic=</Equation></Text-field></Input><Output><Text-field layout="Maple Output" style="2D Output"><Equation>NiM+LUkieEc2IjYjSSJ0R0YmKipeIyEiIiIiIkkmT21lZ2FHRiZGK0kjdjBHRiZGLC1JJGV4cEc2JEkqcHJvdGVjdGVkR0YySShfc3lzbGliR0YmNiMqKF4jRixGLEYtRixGKEYsRiw=</Equation></Text-field></Output></Group><Group><Input><Text-field layout="Normal" style="Normal">And the acceleration is derived from the velocity</Text-field></Input></Group><Group><Input><Text-field layout="Normal256" prompt="&gt; " style="2D Input"><Equation executable="true" input-equation="a(t):=diff(v(t),t);" style="2D Input">NiM+LSUiYUc2IyUidEctJSVkaWZmRzYkLSUidkdGJkYn</Equation></Text-field></Input><Output><Text-field layout="Maple Output" style="2D Output"><Equation>NiM+LUkiYUc2IjYjSSJ0R0YmKipeIyIiIkYrSSN2MEdGJkYrSSZPbWVnYUdGJkYrLUkkZXhwRzYkSSpwcm90ZWN0ZWRHRjFJKF9zeXNsaWJHRiY2IyooRipGK0YtRitGKEYrRis=</Equation></Text-field></Output></Group><Group><Input><Text-field layout="Normal" style="Normal">Here we express the displacement and the acceleration by the velocity. This allows us to generate a formalism to describe any device. For example the displacement <Equation input-equation="x[1](t)" style="2D Comment">NiMtJiUieEc2IyIiIjYjJSJ0Rw==</Equation> and acceleration <Equation input-equation="a[1](t)" style="2D Comment">NiMtJiUiYUc2IyIiIjYjJSJ0Rw==</Equation> are expressed by the velocity <Equation input-equation="v[1](t)" style="2D Comment">NiMtJiUidkc2IyIiIjYjJSJ0Rw==</Equation></Text-field></Input></Group><Group><Input><Text-field layout="Normal256" prompt="&gt; " style="2D Input"><Equation executable="true" input-equation="x[1](t):=x(t)/v(t)*v[1](t);" style="2D Input">NiM+LSYlInhHNiMiIiI2IyUidEcqKC1GJkYpRigtJSJ2R0YpISIiLSZGLkYnRilGKA==</Equation></Text-field></Input><Output><Text-field layout="Maple Output" style="2D Output"><Equation>NiM+LSZJInhHNiI2IyIiIjYjSSJ0R0YnKiheIyEiIkYpSSZPbWVnYUdGJ0YuLSZJInZHRidGKEYqRik=</Equation></Text-field></Output></Group><Group><Input><Text-field layout="Normal256" prompt="&gt; " style="2D Input"><Equation executable="true" input-equation="a[1](t):=a(t)/v(t)*v[1](t);" style="2D Input">NiM+LSYlImFHNiMiIiI2IyUidEcqKC1GJkYpRigtJSJ2R0YpISIiLSZGLkYnRilGKA==</Equation></Text-field></Input><Output><Text-field layout="Maple Output" style="2D Output"><Equation>NiM+LSZJImFHNiI2IyIiIjYjSSJ0R0YnKiheI0YpRilJJk9tZWdhR0YnRiktJkkidkdGJ0YoRipGKQ==</Equation></Text-field></Output></Group><Group><Input><Text-field layout="Heading 1" style="Heading 1">Impedance</Text-field><Text-field layout="Normal" style="Normal">We have assumed that the forces are linearly dependant on the displacement, velocity or the acceleration. Additionally we assumed that only harmonic vibrations are considered. This means that we can write for the relation between force and velocity</Text-field><Text-field layout="Normal256" style="2D Comment"><Equation input-equation="F(t) = R*v(t);" style="2D Comment">NiMvLSUiRkc2IyUidEcqJiUiUkciIiItJSJ2R0YmRio=</Equation></Text-field><Text-field layout="Normal" style="Normal">or</Text-field><Text-field layout="Normal256" style="2D Comment"><Equation input-equation="R = F(t)/v(t);" style="2D Comment">NiMvJSJSRyomLSUiRkc2IyUidEciIiItJSJ2R0YoISIi</Equation></Text-field><Text-field layout="Normal" style="Normal">R is called the impedance of a device or a structure.</Text-field><Text-field layout="Heading 2" style="Heading 2">Impedances of Standard Devices</Text-field><Text-field layout="Normal" style="Normal">Let's consider some typical devices and their impedances. </Text-field><Text-field layout="Heading 3" style="Heading 3"/><Text-field layout="Heading 3" style="Heading 3">Spring</Text-field><Text-field layout="Normal" style="Normal">First consider the spring in Figure 2.</Text-field><Text-field alignment="centred"><Image height="135" 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layout="Normal256" style="Normal256">Figure 2</Text-field><Text-field layout="Normal" style="Normal">The displacement at the upper end of the spring should be given by <Equation input-equation="x[1](t);" style="2D Comment">NiMtJiUieEc2IyIiIjYjJSJ0Rw==</Equation>, the velocity is <Equation input-equation="v[1](t);" style="2D Comment">NiMtJiUidkc2IyIiIjYjJSJ0Rw==</Equation>.</Text-field><Text-field layout="Normal" style="Normal">The force which is neededed to produce this displacement is</Text-field></Input></Group><Group><Input><Text-field layout="Normal256" prompt="&gt; " style="2D Input"><Equation executable="true" input-equation="F1[spring](t) := k*x[1](t):" style="2D Input">NiM+LSYlI0YxRzYjJSdzcHJpbmdHNiMlInRHKiYlImtHIiIiLSYlInhHNiNGLUYpRi0=</Equation></Text-field></Input></Group><Group><Input><Text-field layout="Normal" style="Normal">For the impedance of the spring we get</Text-field></Input></Group><Group><Input><Text-field layout="Normal256" prompt="&gt; " style="2D Input"><Equation executable="true" input-equation="R[spring]:=F1[spring](t)/v[1](t);" style="2D Input">NiM+JiUiUkc2IyUnc3ByaW5nRyomLSYlI0YxR0YmNiMlInRHIiIiLSYlInZHNiNGLkYsISIi</Equation></Text-field></Input><Output><Text-field layout="Maple Output" style="2D Output"><Equation>NiM+JkkiUkc2IjYjSSdzcHJpbmdHRiYqKF4jISIiIiIiSSJrR0YmRixJJk9tZWdhR0YmRis=</Equation></Text-field></Output></Group><Group><Input><Text-field layout="Heading 3" style="Heading 3">Damper</Text-field><Text-field layout="Normal" style="Normal">We repeat the same consideration for a viscous damper.</Text-field></Input></Group><Group><Input><Text-field alignment="centred"><Image height="144" 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layout="Normal256" style="Normal256">Figure 3</Text-field></Input></Group><Group><Input><Text-field layout="Normal" style="Normal">The displacement and the velocity are again given by <Equation input-equation="x[1](t);" style="2D Comment">NiMtJiUieEc2IyIiIjYjJSJ0Rw==</Equation> and <Equation input-equation="v[1](t);" style="2D Comment">NiMtJiUidkc2IyIiIjYjJSJ0Rw==</Equation>.</Text-field><Text-field layout="Normal" style="Normal">The Force on the damper is now</Text-field></Input></Group><Group><Input><Text-field layout="Normal256" prompt="&gt; " style="2D Input"><Equation executable="true" input-equation="F1[damper](t):=d*v[1](t):" style="2D Input">NiM+LSYlI0YxRzYjJSdkYW1wZXJHNiMlInRHKiYlImRHIiIiLSYlInZHNiNGLUYpRi0=</Equation></Text-field></Input></Group><Group><Input><Text-field layout="Normal256" prompt="&gt; " style="2D Input"><Equation executable="true" input-equation="R[damper]:=F1[damper](t)/v[1](t);" style="2D Input">NiM+JiUiUkc2IyUnZGFtcGVyRyomLSYlI0YxR0YmNiMlInRHIiIiLSYlInZHNiNGLkYsISIi</Equation></Text-field></Input><Output><Text-field layout="Maple Output" style="2D Output"><Equation>NiM+JkkiUkc2IjYjSSdkYW1wZXJHRiZJImRHRiY=</Equation></Text-field></Output></Group><Group><Input><Text-field layout="Heading 3" style="Heading 3">Mass</Text-field><Text-field layout="Normal" style="Normal">The third standard device is a rigid body with mass m.</Text-field></Input></Group><Group><Input><Text-field alignment="centred"><Image height="144" width="144">MFNWtKUb<ob<R=MDLCdNB^>ZJ@[<Zb_^owW@ka`N\\@Nd\\QgqxHqQ`Pslik]yJ>]LK\\LDdRJdRGPtTUOLUx_mv\\eocMnpqjR]sTAUeMPUdtYdqfmt`eWPqtYdkPqTUXWehxAuyZamgeOd]TPqlGAmgeoFqlO`NRLV\\LjLMN>MxuAXxxQhhmK`MgyLWXxvtqhXwIxVIYwstswuYiYwoqqhYwCEMV\\MF`j>pYyiyqapn`pN`lNXKXlkZpqxpqCTL`<p_qmkUv@IuSHj;HJHAu[TQwiywIwcIw[Ew>`pB=Yb]yrIxfUmTPmxlyrYVtEYCQl_ToPeoTdw`atNat[pv?AnoXWQqopp`whqwxhVIhAipQqeeXxJVaaysYxtwq[RAmKwcIwcPodPfuWAuRAyVYhIIZ:gggggSGeSAgFIZt@rZ?fZ>cXqiuiwIvavA\\HV_dN_<>`j`y]ykynr?G[`g[E>fcHf;^_mV`M_]mYuiwq;plRp^x@_=V]gGbeOv>IkgiwgieWge:v[dQ\\^Pq;AiQIZUVtQfklCq;fr=wYISMoFWMViSxZKxMATSsE_?U[=E\\cGXkF:AvaKyWks:gGJ?VaqsWWImmvF[ilKuwArZcG_CtaWHfYrN_Ih;Cs[BH=HECDZEfKIVl?wNYsTQRSCESCXXCBjCWcCk:lr[<SmXVa=uKlVhXr@qm>qLbAPp`Xn]YHAL^LqS=M]DK_TJ;HULETt@Xntr:IJuYuLANTywRxKfEvO@yvDPRdnfawf]Rb@v;MLlatZAPSySkURR=ue\\fmOh:a]jv^A^sCIZm?rV`]jvnyo\\j^aUXhaqsSI^Xvk?pdi>cawsXhli^orHlwfvJ`e>I]WVoYNcCGc;y[?V`pOtMYtOvr=ydoHgaH\\nFgLa^pP[qXZU>yGgmtfhnXmWprX>pYwiwihlavCQkW^r\\@aT?\\;>ltQytAfc>hDwkL@uH?btfy]Q^KGvY>f:o`d>wAq`H?sAXcSGeS?n?v\\H@fuvn>?hRPncAk>gc[_]t^hbpohpw^IsMP[:nySp\\h^erAw]xkTawNwcIwssYxaynFGm\\Al^>[jpuXquF`kF`wfagWNZRqkWValOhl_gT_f>fv`qvpxpqxsTh`EGek>kM_jdXvK@a:agTvdlA\\[qdJ?djQtEw_O_dN_ejqinx\\rFrO?gl^nbvk]F^Wvk>IwjV\\w_xxN^KhwkXfAAp;Od@G^hyamovF^wOHmSHkxVtNa\\<Ht[FcVXvfnuLx__HqZ?dKasM>rbaap?njHk>Wxd_vtHu^@hlGmFQxu>up_hn_ajAr=vwvXxHp_cF_;WyY^ijIrWxhXIsRQwdQwLI]GWlpohpojF>`sOsl`xHx]yn_HHnkA_afvAnmxfiTXobg`;xrS^hX>`Yfat_\\``whqwHOxZicGgtrHZsneRFxjqwuxw\\w`cQ\\A``Jp^n^`n^\\Qv\\m^wJAtZ@[n`kvn[MV`TqrL>`tfeF^ZX>uNVhaqs?n]_f_c_vDA[^hsapcWPdxakLgtDPkDP^=IkfGca>d[_^;nZp_wQyeygy=y[y>kaa^jnqyqyuysyvyvGylivQhepG]gQZ?aqv`asHnn^^;FlTH`mNaRVgvhqCv`TqtVauvasmvsfquwX]=PZjnisivQ>x=xvbYkQwewglPQgZVhmy^Y`i<paUwqxgqx_^SOxJCPOG<KGoixoywywyxQh_Us:EdpEttwxXYYIsukEx\\irLetLodI]IkaBx[Svuim;X:GGd_Re_HRcFPIDQsgyoytKHJoRD;HRSgj?hjUt`gSnuBt;BjQUTMUhiiqquQwUxEUGwSP;V]KyToT:yx:Sheuth[dSkwASbCGtpWXaqsdOgd_yvaYTKrb[vFqhgUuxGy`YE_;wa;F]mWfcstMiU]S]?cNahcUtpwWYqYYiYqICR?uk_sOMuIIsiuiwqx?yDY]YpIuaETZ=feCxL_GLAeMqT`YWsEYsSBhuwXii:_rjWumwVIKxvqtUuW_ueP=V_]ipQueedOgdbeHJQhOiD[At[=f?Af]icc=Hr=FGIJ<puflRBdJhDq;imjMLV=ycynYPvYUPHEVu<tLtU`DtbAPoeNqPXKQn?UwPio=qT^]Q[hnZuooXWQqUqeuoMsLeWgeW?uSidUt`LIXPk<WGHXfDTPUJ]=lKyrxPPgEMdPr@XlQxUxEqnTPJLXBqy`isUHVoLMF@V>ls^LuWlpXLRHIkTLruYr:=oRyOx@y<<YTTMUTOdLObEWY]lDUSEEqDAq^=rcEWM=m\\dM`yrBaLNaXQ\\m^Tp\\lLCDsVTtS\\POHre<QM@sXmLcHp:\\pTLjhhVFiqsqvU`qaTvf`of`SdPm=EuG=K@dpkDPmURcXVBpLgmvOySV@Q;tKCqXBxu@drcilkeOalNxamaMTBpjvdxNYTGeSGUypiwUQp_UkvHLSMrnxle`kKeNuUOLqLT<rbYWCaJvEVjMl`<kiYSTxt<ATG<NNmPd@T]]PGTtcUv@ikT\\VTMT`_g^^j_VwApb^NgO?k?f\\kgkKh\\AqkWVkmAko>mhAfJPu\\oT_SpAv=wC\\IG\\uxDwbnORJgEHMH:EdJKWEMBLaxAAYter:SRsSFhiV_kUNAeXWHamcPMR@;Dg[vXkUQYRIcI^ofSsFceU?_Ya=UJUs^mGTGxY;nCdO;qN;uKTMsU<qbYpRmrn`mx@jAUjp@ML=SJQKUPTQaU>PN_@M`<K@<yIEueDKruyk`MH<v^EntePclQTmvr`SWPQOmpSO`S`e=WmqI\\=FgegbB>\\Opp\\H_nnbA>[;X\\BFfJYt@@yEgw\\gyXfcU?^X?tAFZVox=Pk<I^EisGivGfL=WsMd<scnOyv]drssOAH;kVtqDXEdvUi>uiAmKt@rLYK>DnV<UGIqbeUQhOmmL:qL=MpaPVGqSgloOPvKySCxwkdjriSEUm^Qt?eOWDQ^Mm[EP_dOgiry@P@ex\\EkCPj@lW>UOW=rF]V^hVfAj:hY_dmntVg@VD@L_xqZeJZ=RBHoqDqdTrOXb=HvDqk<nfTGhEhnhVvp^bca^;XZFOcXgugH_WopVHdYPrx@pBPvU?a=^m^Xq;FcPqp\\OpLg_V`vp>pQ_s?xe=h\\>Qjj_[yHsS`mV`]J_vXXck`k<NbcGZ>^[^N`mV`anbCX`gf_g>[kNyWp_`wvuxwxXZ^FmdgggggKHvtFZGisGypWqhUHiky^Iom>nchyZ]?XkrLaDTYuUYUUUUIcEt[BlMCGaDOcD?[Vtax\\Qga;eOMGbYW[gRAutPqtPytQYcgad@KVkIuRMrUMumwVIaisUx^ouJcYocHoKSDAhSMIcSEkWn^=L:?fS?rmGlrypFAg:HlTHr\\oujHf=nbT`rZnl^`cJ?m=otGHm]hv_ivmwvHivFnu?Ndh@nZ@nn`pNnu\\qZcIap_`[`oFR\\ODSAi_UsP?DOOwBKfKIVvCfZaF<ogtOiTQWb?WpUBuQRxYbHysTgHeOf\\ORwqg>uRbqyuywYeiteHq;Up;II?HN\\qnXNPyJbxTOeTseL;xyW@vC<VJ=QOTx;Ul^UkQtOPTS?mjeuRCqqQEOUlxcaxlPpl<YBXoBqRSMNBxrepotPKXXt=@NaEJIIsKMwfawf=Wb=KQMJe=LAmLWQW`Um`DsplWVAk>YlJTvL<j;hNj<jDTQr<XemtfHlctOUuU[yYReWuqhaySYxZ_f\\Oxq_VmMrHWSP_G;cG^aVBot_gb@]DvKxBYFmsVHabgavAGB@SQIlq;]x;PkVdPs`sLeUlPxqtWXaW;UUHAovPkF<lOUoPeUyeyoAw?ALgXC;Hf;C:Sdw?RiYFaCuDAe>QWj_wWSkJhNCiKbqPJEl^\\P_mjpQOf\\Ov]ykyr;hOkDqRtyt<rjhPXQYeiOrqRxtOWusPDoruxWyXi<Uj@NLTlq]OyUSdQKcEkWHO`TprMLU]pQeV_eNF@KuEkgaMjHP`LYpmrFHMqaumuKPyJfERQTJXLsC<P\\Tr[`VmPL_Lvf<v>pyuHw`Xm\\EQFTnyIwaxmPmW[]rE\\UxYL^`MRhpeut\\=t=HMfiRqUtcAN;<PnAqOLpn@qmPNZ<QTAK:]mslsEXxrhwCyNY`lItLthTOIV<\\KYPYwQyoipohpldvkUlK]W]\\r`LxJaUc]O:=x:Es;hKLXLxTTdXLPLKAPXZaLsxSFmjTyqE<PsaqnuPwqoDPYelTf@qeqou`O=UkU\\l=QKaDJ@<MBMRdMp@dSpPX_QSwaLfin>]kB]Xp<RHMRRMy[djkpj\\ptLOcPvcGPdJQx[SUKbMKFkAr;WBggggWhausxGx@YE]aTc\\N:Iov]VR`kAmKX\\QB`yvPvDXODMSD=Wf`SveOj\\KT`WNhKFYmm\\MKyuDHKNitOiKWUMkTx@un><X>Iw_dLxApMHxepKREqJlJYls:HkDO[fP^q?`eNllqvtWbEwb:vlIpatA_GQ^SAurPkH>`bQZRwrWoZ?PZFPsnqfAF`rNuuOc`?]qOgLgclVlYFkGOvIh[^yZA`^di^a^olYikGhkOmt@jQiohpoPXyS@p^ntyP]iPdxOov>`oYiV@lLP\\<^nLad@We_Ni^qocQlDpcbyhNvxD^\\ZOm:NfyilQoeKQbJqkHpk[hj[d[=yPatNaUwexOIbOmhB[X?uHbQY_Ud?yyDAbnYDb?ulWI_sEb]XTME^Odu[x_KbZmHVwHViiuuxcWTa_djYxYEdB[X`wCNuIb;WkATEsBUee]CHDAWL?rrwrHSVoEVfoWQwCQ[hpQxDMCPOHjocVCI<UHsUx[GE<UXxihbQemCbGEDN]sCxpEujc<yNtuPQT@yjPAMdDWAqTeQKa@u^]o:ElodSMDSTxVBUtdiUCQY>qkl`l\\aT[US\\AkEhwSen;MstAqZiybLWG]XwIuyDPMITyToOMT;USO@TXYNUEyxawJQn[HY\\dqk\\rk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layout="Normal256" style="Normal256">Figure 4</Text-field><Text-field layout="Normal" style="Normal"> Now we define the displacement and the velocity again with <Equation input-equation="x1(t)" style="2D Comment">NiMtJSN4MUc2IyUidEc=</Equation> and <Equation input-equation="v1(t)" style="2D Comment">NiMtJSN2MUc2IyUidEc=</Equation>. Additionally we use now the acceleration <Equation input-equation="a1(t)" style="2D Comment">NiMtJSNhMUc2IyUidEc=</Equation>.</Text-field><Text-field layout="Normal" style="Normal">The force which is needed to move the body is</Text-field></Input></Group><Group><Input><Text-field layout="Normal256" prompt="&gt; " style="2D Input"><Equation executable="true" input-equation="F1[mass](t):=m*a[1](t):" style="2D Input">NiM+LSYlI0YxRzYjJSVtYXNzRzYjJSJ0RyomJSJtRyIiIi0mJSJhRzYjRi1GKUYt</Equation></Text-field></Input></Group><Group><Input><Text-field layout="Normal256" prompt="&gt; " style="2D Input"><Equation executable="true" input-equation="R[mass]:=F1[mass](t)/v[1](t);" style="2D Input">NiM+JiUiUkc2IyUlbWFzc0cqJi0mJSNGMUdGJjYjJSJ0RyIiIi0mJSJ2RzYjRi5GLCEiIg==</Equation></Text-field></Input><Output><Text-field layout="Maple Output" style="2D Output"><Equation>NiM+JkkiUkc2IjYjSSVtYXNzR0YmKiheIyIiIkYrSSJtR0YmRitJJk9tZWdhR0YmRis=</Equation></Text-field></Output></Group><Group><Input><Text-field bookmark="elastichalfspace" layout="Heading 3" style="Heading 3">Elastic Half-Space</Text-field><Text-field layout="Normal" style="Normal">At last we give the Impedance for an elastic half-space as an example as shown in Figure 5. 
</Text-field><Text-field alignment="centred"><Image height="111" 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layout="Normal256" style="Normal256">Figure 5</Text-field><Text-field layout="Normal" style="Normal">Such an elastic half-space is used to describe the soil under a foundation. It is not so easy to deduce the impedance of this half-space. It is given for example in [1] by</Text-field></Input></Group><Group><Input><Text-field layout="Normal256" prompt="&gt; " style="2D Input"><Equation executable="true" input-equation="R[ELASTIC_HALF_SPACE]:=(19/100*(1-mu)*Omega**2/(G*sqrt(G/rho))+I*(1-mu)/Pi*Omega/G/a)**(-1):" style="2D Input">NiM+JiUiUkc2IyUzRUxBU1RJQ19IQUxGX1NQQUNFRyksJiosIiM+IiIiIiQrIiEiIiwmRixGLCUjbXVHRi5GLCUmT21lZ2FHIiIjKiYlIkdHRiwtJSVzcXJ0RzYjKiZGNEYsJSRyaG9HRi5GLEYuRiwqLiUiSUdGLEYvRiwlI1BpR0YuRjFGLEY0Ri4lImFHRi5GLCwkRixGLg==</Equation></Text-field></Input></Group><Group><Input><Text-field layout="Normal" style="Normal">In this relation <Equation input-equation="G" style="2D Comment">NiMlIkdH</Equation> is the shear modulus, <Equation input-equation="mu" style="2D Comment">NiMlI211Rw==</Equation> is the Poisson's ratio and <Equation input-equation="rho" style="2D Comment">NiMlJHJob0c=</Equation> is the specific mass of the soil. <Equation input-equation="Omega" style="2D Comment">NiMlJk9tZWdhRw==</Equation> is the angular frequency of the harmonic vibration. <Equation input-equation="a" style="2D Comment">NiMlImFH</Equation> is the radius of the area where the force is acting.</Text-field></Input></Group><Group><Input><Text-field layout="Heading 1" style="Heading 1">Quadripole Parameters</Text-field><Text-field layout="Normal" style="Normal">In practice two different ways to describe a quadripole as shown in Figure 1 are common. The first form is the <Font bold="false" executable="false" family="Times New Roman" foreground="[0,0,0]" size="12" style="_cstyle259" underline="false">chain form</Font>, the second is the <Font bold="false" executable="false" family="Times New Roman" foreground="[0,0,0]" size="12" style="_cstyle260" underline="false">impedance form.</Font></Text-field><Text-field layout="Heading 2" style="Heading 2">Chain Form</Text-field><Text-field layout="Normal" style="Normal">In this form we describe the values of the input gate dependent on the values of the output gate:</Text-field><Text-field layout="Normal256" style="2D Comment"><Equation input-equation="F[1]=f[1](F[2],v[2])" style="2D Comment">NiMvJiUiRkc2IyIiIi0mJSJmR0YmNiQmRiU2IyIiIyYlInZHRi0=</Equation></Text-field><Text-field layout="Normal256" style="2D Comment"><Equation input-equation="v[1] = f[2](F[2],v[2]);" style="2D Comment">NiMvJiUidkc2IyIiIi0mJSJmRzYjIiIjNiQmJSJGR0YrJkYlRis=</Equation></Text-field><Text-field layout="Normal" style="Normal">Due to the condition that all forces are linearly dependantent on the displacement, velocity or the acceleration and the condition that we only consider harmonic vibrations, it follows</Text-field><Text-field layout="Normal256" style="2D Comment"><Equation input-equation="F[1]=A[1,1]*F[2]+A[1,2]*v[2]" style="2D Comment">NiMvJiUiRkc2IyIiIiwmKiYmJSJBRzYkRidGJ0YnJkYlNiMiIiNGJ0YnKiYmRis2JEYnRi9GJyYlInZHRi5GJ0Yn</Equation></Text-field><Text-field layout="Normal256" style="2D Comment"><Equation input-equation="v[1]=A[2,1]*F[2]+A[2,2]*v[2]" style="2D Comment">NiMvJiUidkc2IyIiIiwmKiYmJSJBRzYkIiIjRidGJyYlIkZHNiNGLUYnRicqJiZGKzYkRi1GLUYnJkYlRjBGJ0Yn</Equation></Text-field><Text-field layout="Normal" style="Normal">The values <Equation input-equation="A[1,1]" style="2D Comment">NiMmJSJBRzYkIiIiRiY=</Equation>, <Equation input-equation="A[1,2]" style="2D Comment">NiMmJSJBRzYkIiIiIiIj</Equation>, <Equation input-equation="A[2,1]" style="2D Comment">NiMmJSJBRzYkIiIjIiIi</Equation> and <Equation input-equation="A[2,2]" style="2D Comment">NiMmJSJBRzYkIiIjRiY=</Equation> are called the <Font bold="false" executable="false" family="Times New Roman" foreground="[0,0,0]" size="12" style="_cstyle261" underline="false">quadripole parameter of the chain form</Font>.</Text-field><Text-field layout="Normal" style="Normal">In matrix form we can write </Text-field><Text-field layout="Normal256" style="2D Comment"><Equation input-equation="matrix([[F[1]], [v[1]]]) = matrix([[A[1,1], A[1,2]], [A[2,1], A[2,2]]])*matrix([[F[2]], [v[2]]]);" style="2D Comment">NiMvLSUnbWF0cml4RzYjNyQ3IyYlIkZHNiMiIiI3IyYlInZHRisqJi1GJTYjNyQ3JCYlIkFHNiRGLEYsJkY2NiRGLCIiIzckJkY2NiRGOkYsJkY2NiRGOkY6RiwtRiU2IzckNyMmRio2I0Y6NyMmRi9GRUYs</Equation></Text-field></Input></Group><Group><Input><Text-field layout="Heading 2" style="Heading 2">Impedance Form</Text-field><Text-field layout="Normal" style="Normal">In this form we describe all forces dependent on the velocities:</Text-field><Text-field layout="Normal256" style="2D Comment"><Equation input-equation="F[1] = g[1](v[1],v[2]);" style="2D Comment">NiMvJiUiRkc2IyIiIi0mJSJnR0YmNiQmJSJ2R0YmJkYtNiMiIiM=</Equation></Text-field><Text-field layout="Normal256" style="2D Comment"><Equation input-equation="F[2] = g[2](v[1],v[2]);" style="2D Comment">NiMvJiUiRkc2IyIiIy0mJSJnR0YmNiQmJSJ2RzYjIiIiJkYtRiY=</Equation></Text-field><Text-field layout="Normal" style="Normal">Same as in the chain form, this yields</Text-field><Text-field layout="Normal256" style="2D Comment"><Equation input-equation="F[1] = Z[1,1]*v[1]+Z[1,2]*v[2];" style="2D Comment">NiMvJiUiRkc2IyIiIiwmKiYmJSJaRzYkRidGJ0YnJiUidkdGJkYnRicqJiZGKzYkRiciIiNGJyZGLjYjRjJGJ0Yn</Equation></Text-field><Text-field layout="Normal256" style="2D Comment"><Equation input-equation="F[2] = Z[2,1]*v[1]+Z[2,2]*v[2];" style="2D Comment">NiMvJiUiRkc2IyIiIywmKiYmJSJaRzYkRiciIiJGLSYlInZHNiNGLUYtRi0qJiZGKzYkRidGJ0YtJkYvRiZGLUYt</Equation></Text-field><Text-field layout="Normal" style="Normal">The values <Equation input-equation="Z[1,1];" style="2D Comment">NiMmJSJaRzYkIiIiRiY=</Equation>, <Equation input-equation="Z[1,2];" style="2D Comment">NiMmJSJaRzYkIiIiIiIj</Equation>, <Equation input-equation="Z[2,1];" style="2D Comment">NiMmJSJaRzYkIiIjIiIi</Equation> and <Equation input-equation="Z[2,2];" style="2D Comment">NiMmJSJaRzYkIiIjRiY=</Equation> are called the <Font bold="false" executable="false" family="Times New Roman" foreground="[0,0,0]" size="12" style="_cstyle262" underline="false">quadripole parameter of the impedance form</Font>.</Text-field><Text-field layout="Normal" style="Normal">In matrix form we can write </Text-field><Text-field layout="Normal256" style="2D Comment"><Equation input-equation="matrix([[F[1]], [F[2]]]) = matrix([[Z[1,1], Z[1,2]], [Z[2,1], Z[2,2]]])*matrix([[v[1]], [v[2]]]);" style="2D Comment">NiMvLSUnbWF0cml4RzYjNyQ3IyYlIkZHNiMiIiI3IyZGKjYjIiIjKiYtRiU2IzckNyQmJSJaRzYkRixGLCZGNzYkRixGMDckJkY3NiRGMEYsJkY3NiRGMEYwRiwtRiU2IzckNyMmJSJ2R0YrNyMmRkVGL0Ys</Equation></Text-field><Text-field layout="Normal" style="Normal">In this worksheet we use the impedance form only as an aid. So when we say "quadripole parameter" we mean the quadripole parameter of the chain form.</Text-field></Input></Group><Group><Input><Text-field layout="Heading 2" style="Heading 2">Conversion</Text-field><Text-field layout="Normal" style="Normal">Of course both forms can be converted to the other. It is practical to make this by use of procedures.</Text-field></Input></Group><Group><Input><Text-field layout="Normal" style="Normal">Calculate the quadripole parameter of the impedance form from the quadripole parameter of the chain form (chain form -&gt; impedance form)</Text-field></Input></Group><Group><Input><Text-field bookmark="chain2impedance" layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">chain2impedance:=proc(A)</Font></Text-field><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">local Z,F1,v1,F2,v2,eq1,eq2;</Font></Text-field><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">Z:=matrix(2,2);</Font></Text-field><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">eq1:=F1=evalm(A&amp;*vector(2,[F2,v2]))[1];</Font></Text-field><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">eq2:=v1=evalm(A&amp;*vector(2,[F2,v2]))[2];</Font></Text-field><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">assign(solve({eq1,eq2},{F1,F2}));</Font></Text-field><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">Z[1,1]:=coeff(F1,v1);</Font></Text-field><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">Z[1,2]:=coeff(F1,v2);</Font></Text-field><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">Z[2,1]:=coeff(F2,v1);</Font></Text-field><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">Z[2,2]:=coeff(F2,v2);</Font></Text-field><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">evalm(Z);</Font></Text-field><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">end:</Font></Text-field></Input></Group><Group><Input><Text-field layout="Normal" style="Normal">Calculate the quadripole parameter of the chain form from the quadripole parameter of the impedance form (impedance form -&gt; chain form)</Text-field></Input></Group><Group><Input><Text-field bookmark="impedance2chain" layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">impedance2chain:=proc(Z)</Font></Text-field><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">local A,F1,v1,F2,v2,eq1,eq2;</Font></Text-field><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">A:=matrix(2,2);</Font></Text-field><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">eq1:=F1=evalm(Z&amp;*vector(2,[v1,v2]))[1];</Font></Text-field><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">eq2:=F2=evalm(Z&amp;*vector(2,[v1,v2]))[2];</Font></Text-field><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">assign(solve({eq1,eq2},{F1,v1}));</Font></Text-field><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">A[1,1]:=coeff(F1,F2);</Font></Text-field><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">A[1,2]:=coeff(F1,v2);</Font></Text-field><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">A[2,1]:=coeff(v1,F2);</Font></Text-field><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">A[2,2]:=coeff(v1,v2);</Font></Text-field><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">evalm(A);</Font></Text-field><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">end:</Font></Text-field></Input></Group><Group><Input><Text-field layout="Heading 2" style="Heading 2">Quadripole Parameter of Standard Devices</Text-field><Text-field layout="Normal" style="Normal">Now we will give the quadripole parameter for some typical devices.</Text-field><Text-field layout="Heading 3" style="Heading 3"/><Text-field layout="Heading 3" style="Heading 3">Spring</Text-field><Text-field layout="Normal" style="Normal">First we consider the spring shown in Figure 6</Text-field><Text-field alignment="centred"><Image height="192" 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layout="Normal256" style="Normal256">Figure 6</Text-field></Input></Group><Group><Input><Text-field layout="Normal" style="Normal">To get the quadripole parameter we first consider the forces <Equation input-equation="F[1];" style="2D Comment">NiMmJSJGRzYjIiIi</Equation> and <Equation input-equation="F[2];" style="2D Comment">NiMmJSJGRzYjIiIj</Equation>. To fulfill the condition for the equilibrium, the forces must be equal.</Text-field><Text-field layout="Normal256" style="2D Comment"><Equation input-equation="F[1] = F[2];" style="2D Comment">NiMvJiUiRkc2IyIiIiZGJTYjIiIj</Equation></Text-field><Text-field layout="Normal" style="Normal">Next we know that the spring will be stretched by</Text-field><Text-field layout="Normal256" style="2D Comment"><Equation input-equation="Delta*x = x[1]-x[2];" style="2D Comment">NiMvKiYlJkRlbHRhRyIiIiUieEdGJiwmJkYnNiNGJkYmJkYnNiMiIiMhIiI=</Equation></Text-field><Text-field layout="Normal" style="Normal">With the displacement on the input gate we get</Text-field><Text-field layout="Normal256" style="2D Comment"><Equation input-equation="x[1] = -I/Omega*v[1];" style="2D Comment">NiMvJiUieEc2IyIiIiwkKiglIklHRiclJk9tZWdhRyEiIiYlInZHRiZGJ0Ys</Equation></Text-field><Text-field layout="Normal" style="Normal">and on the output gate</Text-field><Text-field layout="Normal256" style="2D Comment"><Equation input-equation="x[2] = -I/Omega*v[2];" style="2D Comment">NiMvJiUieEc2IyIiIywkKiglIklHIiIiJSZPbWVnYUchIiImJSJ2R0YmRitGLQ==</Equation></Text-field><Text-field layout="Normal260" style="Normal260">For the relation between the stretching of the spring and the force we assume linearly dependence</Text-field><Text-field layout="Normal256" style="2D Comment"><Equation input-equation="(x[1]-x[2])*k = F[2];" style="2D Comment">NiMvKiYsJiYlInhHNiMiIiJGKSZGJzYjIiIjISIiRiklImtHRikmJSJGR0Yr</Equation></Text-field><Text-field layout="Normal" style="Normal">This yields for the relation between the force and the velocities at the input gate and the output gate</Text-field><Text-field layout="Normal256" style="2D Comment"><Equation input-equation="F[2]/k = -I*v[1]/Omega+I*v[2]/Omega;" style="2D Comment">NiMvKiYmJSJGRzYjIiIjIiIiJSJrRyEiIiwmKiglIklHRikmJSJ2RzYjRilGKSUmT21lZ2FHRitGKyooRi5GKSZGMEYnRilGMkYrRik=</Equation></Text-field><Text-field layout="Normal" style="Normal">or after rearrangement</Text-field><Text-field layout="Normal256" style="2D Comment"><Equation input-equation="v1 = I*Omega/k*F[2]+v[2];" style="2D Comment">NiMvJSN2MUcsJioqJSJJRyIiIiUmT21lZ2FHRiglImtHISIiJiUiRkc2IyIiI0YoRigmJSJ2R0YuRig=</Equation></Text-field><Text-field layout="Normal" style="Normal">Now we have the four quadripole parameter for the matrix <Equation input-equation="A[spring]" style="2D Comment">NiMmJSJBRzYjJSdzcHJpbmdH</Equation></Text-field></Input></Group><Group><Input><Text-field layout="Normal256" prompt="&gt; " style="2D Input"><Equation executable="true" input-equation="A11[spring]:=1:" style="2D Input">NiM+JiUkQTExRzYjJSdzcHJpbmdHIiIi</Equation></Text-field></Input></Group><Group><Input><Text-field layout="Normal256" prompt="&gt; " style="2D Input"><Equation executable="true" input-equation="A12[spring]:=0:" style="2D Input">NiM+JiUkQTEyRzYjJSdzcHJpbmdHIiIh</Equation></Text-field></Input></Group><Group><Input><Text-field layout="Normal256" prompt="&gt; " style="2D Input"><Equation executable="true" input-equation="A21[spring]:=I*Omega/k:" style="2D Input">NiM+JiUkQTIxRzYjJSdzcHJpbmdHKiglIklHIiIiJSZPbWVnYUdGKiUia0chIiI=</Equation></Text-field></Input></Group><Group><Input><Text-field layout="Normal256" prompt="&gt; " style="2D Input"><Equation executable="true" input-equation="A22[spring]:=1:" style="2D Input">NiM+JiUkQTIyRzYjJSdzcHJpbmdHIiIi</Equation></Text-field></Input></Group><Group><Input><Text-field layout="Normal" style="Normal">In matrix form we get</Text-field></Input></Group><Group><Input><Text-field layout="Normal256" prompt="&gt; " style="2D Input"><Equation executable="true" input-equation="A[spring]:=matrix(2,2,[A11[spring],A12[spring],A21[spring],A22[spring]]);" style="2D Input">NiM+JiUiQUc2IyUnc3ByaW5nRy0lJ21hdHJpeEc2JSIiI0YrNyYmJSRBMTFHRiYmJSRBMTJHRiYmJSRBMjFHRiYmJSRBMjJHRiY=</Equation></Text-field></Input><Output><Text-field layout="Maple Output" style="2D Output"><Equation>NiM+JkkiQUc2IjYjSSdzcHJpbmdHRiYtSSdtYXRyaXhHNiRJKnByb3RlY3RlZEdGLEkoX3N5c2xpYkdGJjYjNyQ3JCIiIiIiITckKiheI0YxRjFJJk9tZWdhR0YmRjFJImtHRiYhIiJGMQ==</Equation></Text-field></Output></Group><Group><Input><Text-field layout="Heading 3" style="Heading 3">Damper</Text-field><Text-field layout="Normal" style="Normal">Next consider the damper in Figure 7.</Text-field><Text-field alignment="centred"><Image height="204" 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layout="Normal256" style="Normal256">Figure 7</Text-field></Input></Group><Group><Input><Text-field layout="Normal" style="Normal">The situation is equivalent to that for the spring. To fulfill the equilibrium condition, <Equation input-equation="F[1];" style="2D Comment">NiMmJSJGRzYjIiIi</Equation> and <Equation input-equation="F[2];" style="2D Comment">NiMmJSJGRzYjIiIj</Equation> must be equal.</Text-field><Text-field layout="Normal256" style="2D Comment"><Equation input-equation="F[1] = F[2];" style="2D Comment">NiMvJiUiRkc2IyIiIiZGJTYjIiIj</Equation></Text-field><Text-field layout="Normal" style="Normal">The damper is stretched by</Text-field><Text-field layout="Normal256" style="2D Comment"><Equation input-equation="Delta*x = x[1]-x[2];" style="2D Comment">NiMvKiYlJkRlbHRhRyIiIiUieEdGJiwmJkYnNiNGJkYmJkYnNiMiIiMhIiI=</Equation></Text-field><Text-field layout="Normal" style="Normal">and the difference of the velocities on both sides is</Text-field><Text-field layout="Normal256" style="2D Comment"><Equation input-equation="Delta*v = v[1]-v[2];" style="2D Comment">NiMvKiYlJkRlbHRhRyIiIiUidkdGJiwmJkYnNiNGJkYmJkYnNiMiIiMhIiI=</Equation></Text-field><Text-field layout="Normal260" style="Normal260">For the relation between the relative velocity and the damping force we assume linearity</Text-field><Text-field layout="Normal256" style="2D Comment"><Equation input-equation="(v[1]-v[2])*d = F[2];" style="2D Comment">NiMvKiYsJiYlInZHNiMiIiJGKSZGJzYjIiIjISIiRiklImRHRikmJSJGR0Yr</Equation></Text-field><Text-field layout="Normal" style="Normal">After rearrangement we get</Text-field><Text-field layout="Normal256" style="2D Comment"><Equation input-equation="v1 = F[2]/d+v[2];" style="2D Comment">NiMvJSN2MUcsJiomJiUiRkc2IyIiIyIiIiUiZEchIiJGKyYlInZHRilGKw==</Equation></Text-field><Text-field layout="Normal" style="Normal">Now we have the four quadripole parameter for the matrix <Equation input-equation="A[damper];" style="2D Comment">NiMmJSJBRzYjJSdkYW1wZXJH</Equation></Text-field></Input></Group><Group><Input><Text-field layout="Normal256" prompt="&gt; " style="2D Input"><Equation executable="true" input-equation="A11[damper]:=1:" style="2D Input">NiM+JiUkQTExRzYjJSdkYW1wZXJHIiIi</Equation></Text-field></Input></Group><Group><Input><Text-field layout="Normal256" prompt="&gt; " style="2D Input"><Equation executable="true" input-equation="A12[damper]:=0:" style="2D Input">NiM+JiUkQTEyRzYjJSdkYW1wZXJHIiIh</Equation></Text-field></Input></Group><Group><Input><Text-field layout="Normal256" prompt="&gt; " style="2D Input"><Equation executable="true" input-equation="A21[damper]:=1/d:" style="2D Input">NiM+JiUkQTIxRzYjJSdkYW1wZXJHKiYiIiJGKSUiZEchIiI=</Equation></Text-field></Input></Group><Group><Input><Text-field layout="Normal256" prompt="&gt; " style="2D Input"><Equation executable="true" input-equation="A22[damper]:=1:" style="2D Input">NiM+JiUkQTIyRzYjJSdkYW1wZXJHIiIi</Equation></Text-field></Input></Group><Group><Input><Text-field layout="Normal" style="Normal">In matrix form we get</Text-field></Input></Group><Group><Input><Text-field layout="Normal256" prompt="&gt; " style="2D Input"><Equation executable="true" input-equation="A[damper]:=matrix(2,2,[A11[damper],A12[damper],A21[damper],A22[damper]]);" style="2D Input">NiM+JiUiQUc2IyUnZGFtcGVyRy0lJ21hdHJpeEc2JSIiI0YrNyYmJSRBMTFHRiYmJSRBMTJHRiYmJSRBMjFHRiYmJSRBMjJHRiY=</Equation></Text-field></Input><Output><Text-field layout="Maple Output" style="2D Output"><Equation>NiM+JkkiQUc2IjYjSSdkYW1wZXJHRiYtSSdtYXRyaXhHNiRJKnByb3RlY3RlZEdGLEkoX3N5c2xpYkdGJjYjNyQ3JCIiIiIiITckKiRJImRHRiYhIiJGMQ==</Equation></Text-field></Output></Group><Group><Input><Text-field layout="Heading 3" style="Heading 3">Mass</Text-field><Text-field layout="Normal" style="Normal">As the last standard device, we consider the rigid body in Figure 8.</Text-field><Text-field alignment="centred"><Image height="180" 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layout="Normal256" style="Normal256">Figure 8</Text-field></Input></Group><Group><Input><Text-field layout="Normal" style="Normal">for a rigid body, the displacement and the velocity at the input gate and at the output gate are the same.</Text-field><Text-field layout="Normal256" style="2D Comment"><Equation input-equation="v[1] = v[2];" style="2D Comment">NiMvJiUidkc2IyIiIiZGJTYjIiIj</Equation></Text-field><Text-field layout="Normal" style="Normal">In the equilibrium condition, we have to consider the inertia</Text-field><Text-field layout="Normal256" style="2D Comment"><Equation input-equation="F[1] = F[2]+m*a[2];" style="2D Comment">NiMvJiUiRkc2IyIiIiwmJkYlNiMiIiNGJyomJSJtR0YnJiUiYUdGKkYnRic=</Equation></Text-field><Text-field layout="Normal" style="Normal">We replace the acceleration by the velocity and get</Text-field><Text-field layout="Normal256" style="2D Comment"><Equation input-equation="F[1] = F[2]+m*I*Omega*v[2];" style="2D Comment">NiMvJiUiRkc2IyIiIiwmJkYlNiMiIiNGJyoqJSJtR0YnJSJJR0YnJSZPbWVnYUdGJyYlInZHRipGJ0Yn</Equation></Text-field><Text-field layout="Normal" style="Normal">Now we have the four quadripole parameters for the matrix <Equation input-equation="A[mass];" style="2D Comment">NiMmJSJBRzYjJSVtYXNzRw==</Equation></Text-field></Input></Group><Group><Input><Text-field layout="Normal256" prompt="&gt; " style="2D Input"><Equation executable="true" input-equation="A11[mass]:=1:" style="2D Input">NiM+JiUkQTExRzYjJSVtYXNzRyIiIg==</Equation></Text-field></Input></Group><Group><Input><Text-field layout="Normal256" prompt="&gt; " style="2D Input"><Equation executable="true" input-equation="A12[mass]:=m*a[1](t)/v[1](t):" style="2D Input">NiM+JiUkQTEyRzYjJSVtYXNzRyooJSJtRyIiIi0mJSJhRzYjRio2IyUidEdGKi0mJSJ2R0YuRi8hIiI=</Equation></Text-field></Input></Group><Group><Input><Text-field layout="Normal256" prompt="&gt; " style="2D Input"><Equation executable="true" input-equation="A21[mass]:=0:" style="2D Input">NiM+JiUkQTIxRzYjJSVtYXNzRyIiIQ==</Equation></Text-field></Input></Group><Group><Input><Text-field layout="Normal256" prompt="&gt; " style="2D Input"><Equation executable="true" input-equation="A22[mass]:=1:" style="2D Input">NiM+JiUkQTIyRzYjJSVtYXNzRyIiIg==</Equation></Text-field></Input></Group><Group><Input><Text-field layout="Normal" style="Normal">In matrix form we get</Text-field></Input></Group><Group><Input><Text-field layout="Normal256" prompt="&gt; " style="2D Input"><Equation executable="true" input-equation="A[mass]:=matrix(2,2,[A11[mass],A12[mass],A21[mass],A22[mass]]);" style="2D Input">NiM+JiUiQUc2IyUlbWFzc0ctJSdtYXRyaXhHNiUiIiNGKzcmJiUkQTExR0YmJiUkQTEyR0YmJiUkQTIxR0YmJiUkQTIyR0Ym</Equation></Text-field></Input><Output><Text-field layout="Maple Output" style="2D Output"><Equation>NiM+JkkiQUc2IjYjSSVtYXNzR0YmLUknbWF0cml4RzYkSSpwcm90ZWN0ZWRHRixJKF9zeXNsaWJHRiY2IzckNyQiIiIqKF4jRjFGMUkibUdGJkYxSSZPbWVnYUdGJkYxNyQiIiFGMQ==</Equation></Text-field></Output></Group><Group><Input><Text-field bookmark="source" layout="Heading 2" style="Heading 2">Quadripole Parameter of a Vibration Source</Text-field><Text-field layout="Normal" style="Normal">In some structures the vibration source is a very complex system that cannot easily be described analytically. But sometimes the impedance <Equation input-equation="R[s]" style="2D Comment">NiMmJSJSRzYjJSJzRw==</Equation> of the vibration source is known, for example from the constructer of the machine.</Text-field><Text-field alignment="centred"><Image height="192" 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layout="Normal256" style="Normal256">Figure 9</Text-field><Text-field layout="Normal" style="Normal">For such a structure, we assume that the force <Equation input-equation="F[1];" style="2D Comment">NiMmJSJGRzYjIiIi</Equation> which will be transmitted to the connected device at the output gate 1 can be measured. Additionally we assume that the structure is rigid. So we know that </Text-field><Text-field layout="Normal256" style="Normal256"><Equation input-equation="v[0]=v[1]" style="2D Comment">NiMvJiUidkc2IyIiISZGJTYjIiIi</Equation>.</Text-field><Text-field layout="Normal" style="Normal">The force that generates the vibration is then</Text-field></Input></Group><Group><Input><Text-field layout="Normal256" prompt="&gt; " style="2D Input"><Equation executable="true" input-equation="F[0]:=F[1]-R[s]*v[1]:" style="2D Input">NiM+JiUiRkc2IyIiISwmJkYlNiMiIiJGKyomJiUiUkc2IyUic0dGKyYlInZHRipGKyEiIg==</Equation></Text-field></Input></Group><Group><Input><Text-field layout="Normal" style="Normal">In matrix form this yields</Text-field><Text-field layout="Normal256" style="Normal256"> <Equation input-equation="matrix([[F[0]], [v[0]]]) = matrix([[A[s][1,1], A[s][1,2]], [A[s][2,1], A[s][2,2]]])*matrix([[F[1]], [v[1]]]);" style="2D Comment">NiMvLSUnbWF0cml4RzYjNyQ3IyYlIkZHNiMiIiE3IyYlInZHRisqJi1GJTYjNyQ3JCYmJSJBRzYjJSJzRzYkIiIiRjsmRjY2JEY7IiIjNyQmRjY2JEY+RjsmRjY2JEY+Rj5GOy1GJTYjNyQ3IyZGKjYjRjs3IyZGL0ZJRjs=</Equation></Text-field><Text-field layout="Normal" style="Normal">The matrix of the quadripole parameter is then</Text-field></Input></Group><Group><Input><Text-field layout="Normal256" prompt="&gt; " style="2D Input"><Equation executable="true" input-equation="A[s]:=matrix(2,2,[1,R[s],0,1]);" style="2D Input">NiM+JiUiQUc2IyUic0ctJSdtYXRyaXhHNiUiIiNGKzcmIiIiJiUiUkdGJiIiIUYt</Equation></Text-field></Input><Output><Text-field layout="Maple Output" style="2D Output"><Equation>NiM+JkkiQUc2IjYjSSJzR0YmLUknbWF0cml4RzYkSSpwcm90ZWN0ZWRHRixJKF9zeXNsaWJHRiY2IzckNyQiIiImSSJSR0YmRic3JCIiIUYx</Equation></Text-field></Output></Group><Group><Input><Text-field layout="Heading 1" style="Heading 1">Combination of Standard Devices</Text-field><Text-field layout="Normal" style="Normal">A lot of different devices can be described by combinations of the standard devices spring, damper and mass. There are two principal ways to combine two devices.</Text-field><Text-field layout="Heading 2" style="Heading 2">Serial Connection</Text-field><Text-field layout="Normal" style="Normal">First the devices can be combined as a chain one behind the other as shown in Figure 10.</Text-field><Text-field alignment="centred"><Image height="264" 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layout="Normal256" style="Normal256">Figure 10</Text-field><Text-field layout="Normal" style="Normal">This is called a serial connection.We have two devices.</Text-field><Text-field layout="Normal" style="Normal">The device 1 has the input gate <Equation input-equation="matrix([[F[1]], [v[1]]]);" style="2D Comment">NiMtJSdtYXRyaXhHNiM3JDcjJiUiRkc2IyIiIjcjJiUidkdGKg==</Equation> and the output gate <Equation input-equation="matrix([[F[2]], [v[2]]]);" style="2D Comment">NiMtJSdtYXRyaXhHNiM3JDcjJiUiRkc2IyIiIzcjJiUidkdGKg==</Equation>.</Text-field><Text-field layout="Normal" style="Normal">At the same time <Equation input-equation="matrix([[F[2]], [v[2]]])" style="2D Comment">NiMtJSdtYXRyaXhHNiM3JDcjJiUiRkc2IyIiIzcjJiUidkdGKg==</Equation> is the input gate of the device 2 and <Equation input-equation="matrix([[F[3]], [v[3]]]);" style="2D Comment">NiMtJSdtYXRyaXhHNiM3JDcjJiUiRkc2IyIiJDcjJiUidkdGKg==</Equation> is the output gate of device 2.</Text-field><Text-field layout="Normal" style="Normal">So we get the relations</Text-field><Text-field layout="Normal256" style="2D Comment"><Equation input-equation="matrix([[F[1]], [v[1]]]) = matrix([[A[1][1,1], A[1][1,2]], [A[1][2,1], A[1][2,2]]])*matrix([[F[2]], [v[2]]]);" style="2D Comment">NiMvLSUnbWF0cml4RzYjNyQ3IyYlIkZHNiMiIiI3IyYlInZHRisqJi1GJTYjNyQ3JCYmJSJBR0YrNiRGLEYsJkY2NiRGLCIiIzckJkY2NiRGO0YsJkY2NiRGO0Y7RiwtRiU2IzckNyMmRio2I0Y7NyMmRi9GRkYs</Equation></Text-field><Text-field layout="Normal256" style="2D Comment"><Equation input-equation="matrix([[F[2]], [v[2]]]) = matrix([[A[2][1,1], A[2][1,2]], [A[2][2,1], A[2][2,2]]])*matrix([[F[3]], [v[3]]]);" style="2D Comment">NiMvLSUnbWF0cml4RzYjNyQ3IyYlIkZHNiMiIiM3IyYlInZHRisqJi1GJTYjNyQ3JCYmJSJBR0YrNiQiIiJGOSZGNjYkRjlGLDckJkY2NiRGLEY5JkY2NiRGLEYsRjktRiU2IzckNyMmRio2IyIiJDcjJkYvRkZGOQ==</Equation></Text-field><Text-field layout="Normal" style="Normal">with the quadripole parameter <Equation input-equation="A[1][i,j] " style="2D Comment">NiMmJiUiQUc2IyIiIjYkJSJpRyUiakc=</Equation>of device 1 and <Equation input-equation="A[2][i,j] " style="2D Comment">NiMmJiUiQUc2IyIiIzYkJSJpRyUiakc=</Equation>of device 2. Joining both equations yields</Text-field><Text-field layout="Normal256" style="2D Comment"><Equation input-equation="matrix([[F[1]], [v[1]]]) = matrix([[A[1][1,1], A[1][1,2]], [A[1][2,1], A[1][2,2]]])*matrix([[A[2][1,1], A[2][1,2]], [A[2][2,1], A[2][2,2]]])*matrix([[F[3]], [v[3]]]);" style="2D Comment">NiMvLSUnbWF0cml4RzYjNyQ3IyYlIkZHNiMiIiI3IyYlInZHRisqKC1GJTYjNyQ3JCYmJSJBR0YrNiRGLEYsJkY2NiRGLCIiIzckJkY2NiRGO0YsJkY2NiRGO0Y7RiwtRiU2IzckNyQmJkY3NiNGO0Y4JkZGRjo3JCZGRkY+JkZGRkBGLC1GJTYjNyQ3IyZGKjYjIiIkNyMmRi9GUUYs</Equation></Text-field><Text-field layout="Normal" style="Normal">The matrix of the quadripole parameter of the serial connection of two devices is the product of the matrices of the quadripole parameter of both single devices.</Text-field><Text-field layout="Normal256" style="Normal256"><Equation input-equation="A=A[1]*A[2]" style="2D Comment">NiMvJSJBRyomJkYkNiMiIiJGKCZGJDYjIiIjRig=</Equation>.</Text-field><Text-field layout="Normal" style="Normal">This function is defined in the following procedure for several serial connected devices.</Text-field></Input></Group><Group><Input><Text-field bookmark="serialconnection" layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">serialconnection:=proc()</Font></Text-field><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">local AB,i;</Font></Text-field><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">AB:=matrix(2,2,[1,0,0,1]);</Font></Text-field><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">for i from 1 by 1 to nargs do</Font></Text-field><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">AB:=multiply(AB,args[i]);</Font></Text-field><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">od:</Font></Text-field><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">end:</Font></Text-field></Input></Group><Group><Input><Text-field layout="Heading 2" style="Heading 2">Parallel Connection</Text-field><Text-field layout="Normal" style="Normal">Now we consider the situation of two devices combined in parallel as shown in Figure 11.</Text-field><Text-field alignment="centred"><Image height="185" 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layout="Normal256" style="Normal256">Figure 11</Text-field><Text-field layout="Normal" style="Normal">This is called a parallel connection. Again we have two devices. But now the situation is a bit more complicated.</Text-field><Text-field layout="Normal" style="Normal">Device 1 has the input gate <Equation input-equation="matrix([[F[a1]], [v[a1]]]);" style="2D Comment">NiMtJSdtYXRyaXhHNiM3JDcjJiUiRkc2IyUjYTFHNyMmJSJ2R0Yq</Equation> and the output gate <Equation input-equation="matrix([[F[a2]], [v[a2]]]);" style="2D Comment">NiMtJSdtYXRyaXhHNiM3JDcjJiUiRkc2IyUjYTJHNyMmJSJ2R0Yq</Equation>.</Text-field><Text-field layout="Normal" style="Normal">Device 2 has the input gate <Equation input-equation="matrix([[F[b1]], [v[b1]]]);" style="2D Comment">NiMtJSdtYXRyaXhHNiM3JDcjJiUiRkc2IyUjYjFHNyMmJSJ2R0Yq</Equation> and the output gate <Equation input-equation="matrix([[F[b2]], [v[b2]]]);" style="2D Comment">NiMtJSdtYXRyaXhHNiM3JDcjJiUiRkc2IyUjYjJHNyMmJSJ2R0Yq</Equation>.</Text-field><Text-field layout="Normal" style="Normal">At last ,the input gate of the total device should be <Equation input-equation="matrix([[F[1]], [v[1]]]);" style="2D Comment">NiMtJSdtYXRyaXhHNiM3JDcjJiUiRkc2IyIiIjcjJiUidkdGKg==</Equation> and the output gate <Equation input-equation="matrix([[F[2]], [v[2]]]);" style="2D Comment">NiMtJSdtYXRyaXhHNiM3JDcjJiUiRkc2IyIiIzcjJiUidkdGKg==</Equation>.</Text-field><Text-field layout="Normal" style="Normal">The velocities at the input gate must all be equal. That means <Equation input-equation="v[a1] = v[1];" style="2D Comment">NiMvJiUidkc2IyUjYTFHJkYlNiMiIiI=</Equation> and <Equation input-equation="v[b1] = v[1];" style="2D Comment">NiMvJiUidkc2IyUjYjFHJkYlNiMiIiI=</Equation>. The same is valid for the output gate:  <Equation input-equation="v[a2] = v[2];" style="2D Comment">NiMvJiUidkc2IyUjYTJHJkYlNiMiIiM=</Equation> and <Equation input-equation="v[b2] = v[2];" style="2D Comment">NiMvJiUidkc2IyUjYjJHJkYlNiMiIiM=</Equation></Text-field><Text-field layout="Normal" style="Normal">The force on both gates of the parallel connection is the sum of the forces at all single devices. That means <Equation input-equation="F[1]=F[a1]+F[b1] " style="2D Comment">NiMvJiUiRkc2IyIiIiwmJkYlNiMlI2ExR0YnJkYlNiMlI2IxR0Yn</Equation> and <Equation input-equation="F[2]=F[a2]+F[b2]" style="2D Comment">NiMvJiUiRkc2IyIiIywmJkYlNiMlI2EyRyIiIiZGJTYjJSNiMkdGLA==</Equation>.</Text-field><Text-field layout="Normal" style="Normal">Now we use the impedance form of our quadripoles. We can use the above defined procedure <Hyperlink bold="false" executable="false" family="Times New Roman" hyperlink="true" linktarget="Wks:#chain2impedance" size="12" style="Hyperlink">chain2impedance</Hyperlink> to convert the quadripole parameter of the chain form <Equation input-equation="A[a]" style="2D Comment">NiMmJSJBRzYjJSJhRw==</Equation> and <Equation input-equation="A[b]" style="2D Comment">NiMmJSJBRzYjJSJiRw==</Equation> into the quadripole parameter of the impedance form <Equation input-equation="Z[a]" style="2D Comment">NiMmJSJaRzYjJSJhRw==</Equation> and <Equation input-equation="Z[b]" style="2D Comment">NiMmJSJaRzYjJSJiRw==</Equation>.</Text-field><Text-field layout="Normal256" style="2D Comment"><Equation input-equation="Z[a]=chain2impedance(A[a])" style="2D Comment">NiMvJiUiWkc2IyUiYUctJTBjaGFpbjJpbXBlZGFuY2VHNiMmJSJBR0Ym</Equation></Text-field><Text-field layout="Normal256" style="2D Comment"><Equation input-equation="Z[b]=chain2impedance(A[b])" style="2D Comment">NiMvJiUiWkc2IyUiYkctJTBjaGFpbjJpbXBlZGFuY2VHNiMmJSJBR0Ym</Equation></Text-field><Text-field layout="Normal" style="Normal">With this we can write</Text-field><Text-field layout="Normal256" style="Normal256"> <Equation input-equation="matrix([[F[a1]], [F[a2]]]) = matrix([[Z[a][1,1], Z[a][1,2]], [Z[a][2,1], Z[a][2,2]]])*matrix([[v[1]], [v[2]]]);" style="2D Comment">NiMvLSUnbWF0cml4RzYjNyQ3IyYlIkZHNiMlI2ExRzcjJkYqNiMlI2EyRyomLUYlNiM3JDckJiYlIlpHNiMlImFHNiQiIiJGPCZGNzYkRjwiIiM3JCZGNzYkRj9GPCZGNzYkRj9GP0Y8LUYlNiM3JDcjJiUidkc2I0Y8NyMmRko2I0Y/Rjw=</Equation></Text-field><Text-field layout="Normal256" style="2D Comment"><Equation input-equation="matrix([[F[b1]], [F[b2]]]) = matrix([[Z[b][1,1], Z[b][1,2]], [Z[b][2,1], Z[b][2,2]]])*matrix([[v[1]], [v[2]]]);" style="2D Comment">NiMvLSUnbWF0cml4RzYjNyQ3IyYlIkZHNiMlI2IxRzcjJkYqNiMlI2IyRyomLUYlNiM3JDckJiYlIlpHNiMlImJHNiQiIiJGPCZGNzYkRjwiIiM3JCZGNzYkRj9GPCZGNzYkRj9GP0Y8LUYlNiM3JDcjJiUidkc2I0Y8NyMmRko2I0Y/Rjw=</Equation></Text-field><Text-field layout="Normal" style="Normal">Remember that all velocities at the input gate are the same, and the same holds at the output gate. Combination of theses equations yields</Text-field><Text-field layout="Normal256" style="2D Comment"><Equation input-equation="matrix([[F[a1]], [F[a2]]])+matrix([[F[b1]], [F[b2]]]) = matrix([[Z[a][1,1], Z[a][1,2]], [Z[a][2,1], Z[a][2,2]]])*matrix([[v[1]], [v[2]]])+matrix([[Z[b][1,1], Z[b][1,2]], [Z[b][2,1], Z[b][2,2]]])*matrix([[v[1]], [v[2]]]);" style="2D Comment">NiMvLCYtJSdtYXRyaXhHNiM3JDcjJiUiRkc2IyUjYTFHNyMmRis2IyUjYTJHIiIiLUYmNiM3JDcjJkYrNiMlI2IxRzcjJkYrNiMlI2IyR0YyLCYqJi1GJjYjNyQ3JCYmJSJaRzYjJSJhRzYkRjJGMiZGRTYkRjIiIiM3JCZGRTYkRkxGMiZGRTYkRkxGTEYyLUYmNiM3JDcjJiUidkc2I0YyNyMmRlc2I0ZMRjJGMiomLUYmNiM3JDckJiZGRjYjJSJiR0ZJJkZcb0ZLNyQmRlxvRk8mRlxvRlFGMkZSRjJGMg==</Equation></Text-field><Text-field layout="Normal" style="Normal">or</Text-field><Text-field layout="Normal256" style="2D Comment"><Equation input-equation="matrix([[F[1]], [F[2]]]) = matrix([[Z[1,1], Z[1,2]], [Z[2,1], Z[2,2]]])*matrix([[v[1]], [v[2]]]);" style="2D Comment">NiMvLSUnbWF0cml4RzYjNyQ3IyYlIkZHNiMiIiI3IyZGKjYjIiIjKiYtRiU2IzckNyQmJSJaRzYkRixGLCZGNzYkRixGMDckJkY3NiRGMEYsJkY3NiRGMEYwRiwtRiU2IzckNyMmJSJ2R0YrNyMmRkVGL0Ys</Equation></Text-field><Text-field layout="Normal" style="Normal">with the matrix of the quadripole parameter of the impedance form of the total device as the sum of the matrices of the quadripole parameter of the impedance form of all the single devices</Text-field><Text-field layout="Normal256" style="Normal256"><Equation input-equation="matrix([[Z[1,1], Z[1,2]], [Z[2,1], Z[2,2]]]))=matrix([[Z[a][1,1], Z[a][1,2]], [Z[a][2,1], Z[a][2,2]]])+matrix([[Z[b][1,1], Z[b][1,2]], [Z[b][2,1], Z[b][2,2]]])" style="2D Comment">NiMvLSUnbWF0cml4RzYjNyQ3JCYlIlpHNiQiIiJGLCZGKjYkRiwiIiM3JCZGKjYkRi9GLCZGKjYkRi9GLywmLUYlNiM3JDckJiZGKjYjJSJhR0YrJkY7Ri43JCZGO0YyJkY7RjRGLC1GJTYjNyQ3JCYmRio2IyUiYkdGKyZGR0YuNyQmRkdGMiZGR0Y0Riw=</Equation>.</Text-field><Text-field layout="Normal260" style="Normal260">Finally we get the quadripole parameter of the chain form of the total device by convert ing the quadripole parameter of the impedance form by use of the procedure <Hyperlink bold="false" executable="false" family="Times New Roman" hyperlink="true" linktarget="Wks:#impedance2chain" size="12" style="Hyperlink">impedance2chain</Hyperlink>.</Text-field><Text-field layout="Normal256" style="2D Comment"><Equation input-equation="A = chain2impedance(Z);" style="2D Comment">NiMvJSJBRy0lMGNoYWluMmltcGVkYW5jZUc2IyUiWkc=</Equation></Text-field><Text-field layout="Normal" style="Normal">This process is also defined in the following procedure for several parallel connected devices.</Text-field></Input></Group><Group><Input><Text-field bookmark="parallelconnection" layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">parallelconnection:=proc()</Font></Text-field><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">local ZA,AB,i;</Font></Text-field><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">ZA:=matrix(2,2,[0,0,0,0]):</Font></Text-field><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">for i from 1 by 1 to nargs do</Font></Text-field><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">ZA:=matadd(ZA,chain2impedance(args[i]),1,1);</Font></Text-field><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">od:</Font></Text-field><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">AB:=impedance2chain(ZA);</Font></Text-field><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">end:</Font></Text-field></Input></Group><Group><Input><Text-field layout="Heading 2" style="Heading 2">Some typical combinations of standard devices</Text-field><Text-field layout="Normal" style="Normal">There are several combination of the above defined standard devices often used in practice. Some of them are shown here.</Text-field><Text-field layout="Heading 3" style="Heading 3">KELVIN-VOIGT Model</Text-field><Text-field layout="Normal" style="Normal">This model is used to describe visco-elastic devices as parallel connection of an ideal elastic spring with an ideal viscous damper as shown in Figure 12</Text-field><Text-field alignment="centred"><Image height="175" 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layout="Normal256" style="Normal256">Figure 12</Text-field><Text-field layout="Normal" style="Normal"/><Text-field layout="Normal" style="Normal">The quadripole parameters of this model are calculated by use of the procedure <Hyperlink bold="false" executable="false" family="Times New Roman" hyperlink="true" linktarget="Wks:#parallelconnection" size="12" style="Hyperlink">parallelconnection</Hyperlink>.</Text-field><Text-field layout="Normal" style="Normal">The input parameters for this procedure are the matrices of the quadripole parameter of the damper</Text-field></Input></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">evalm(A[damper]);</Font></Text-field></Input><Output><Text-field layout="Maple Output" style="2D Output"><Equation>NiMtSSdtYXRyaXhHNiRJKnByb3RlY3RlZEdGJkkoX3N5c2xpYkc2IjYjNyQ3JCIiIiIiITckKiRJImRHRighIiJGLA==</Equation></Text-field></Output></Group><Group><Input><Text-field layout="Normal" style="Normal">and the spring</Text-field></Input></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">evalm(A[spring]);</Font></Text-field></Input><Output><Text-field layout="Maple Output" style="2D Output"><Equation>NiMtSSdtYXRyaXhHNiRJKnByb3RlY3RlZEdGJkkoX3N5c2xpYkc2IjYjNyQ3JCIiIiIiITckKiheI0YsRixJJk9tZWdhR0YoRixJImtHRighIiJGLA==</Equation></Text-field></Output></Group><Group><Input><Text-field layout="Normal" style="Normal">The matrix of the quadripole parameter of the KELVIN-VOIGT model is consequently</Text-field></Input></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">A[KELVINVOIGT]:=parallelconnection(A[damper],A[spring]);</Font></Text-field></Input><Output><Text-field layout="Maple Output" style="2D Output"><Equation>NiM+JkkiQUc2IjYjSSxLRUxWSU5WT0lHVEdGJi1JJ21hdHJpeEc2JEkqcHJvdGVjdGVkR0YsSShfc3lzbGliR0YmNiM3JDckIiIiIiIhNyQsJComSSZPbWVnYUdGJkYxLCYqJkkiZEdGJkYxRjZGMSEiIiomXiNGMUYxSSJrR0YmRjFGMUY6RjpGMQ==</Equation></Text-field></Output></Group><Group><Input><Text-field layout="Normal" style="Normal">Additionally we will consider the impedance of such a device. This can be derived different ways. First we can consider the quadripole parameter for the case that the velocity at the output gate is <Equation input-equation="v[2]" style="2D Comment">NiMmJSJ2RzYjIiIj</Equation>=0.</Text-field><Text-field layout="Normal" style="Normal">We will not do this here but we consider the relation between the force and the velocity. The force which passes through the KELVIN-VOIGT model is given by</Text-field></Input></Group><Group><Input><Text-field layout="Normal256" prompt="&gt; " style="2D Input"><Equation executable="true" input-equation="F[KELVINVOIGT](t):=F1[spring](t)+F1[damper](t);" style="2D Input">NiM+LSYlIkZHNiMlLEtFTFZJTlZPSUdURzYjJSJ0RywmLSYlI0YxRzYjJSdzcHJpbmdHRikiIiItJkYuNiMlJ2RhbXBlckdGKUYx</Equation></Text-field></Input><Output><Text-field layout="Maple Output" style="2D Output"><Equation>NiM+LSZJIkZHNiI2I0ksS0VMVklOVk9JR1RHRic2I0kidEdGJywmKipeIyEiIiIiIkkia0dGJ0YwSSZPbWVnYUdGJ0YvLSZJInZHRic2I0YwRipGMEYwKiZJImRHRidGMEYzRjBGMA==</Equation></Text-field></Output></Group><Group><Input><Text-field layout="Normal" style="Normal">And the impedance is the quotient of the force and the velocity</Text-field></Input></Group><Group><Input><Text-field layout="Normal256" prompt="&gt; " style="2D Input"><Equation executable="true" input-equation="R[KELVINVOIGT] := expand(F[KELVINVOIGT](t)/v[1](t));" style="2D Input">NiM+JiUiUkc2IyUsS0VMVklOVk9JR1RHLSUnZXhwYW5kRzYjKiYtJiUiRkdGJjYjJSJ0RyIiIi0mJSJ2RzYjRjFGLyEiIg==</Equation></Text-field></Input><Output><Text-field layout="Maple Output" style="2D Output"><Equation>NiM+JkkiUkc2IjYjSSxLRUxWSU5WT0lHVEdGJiwmSSJkR0YmIiIiKiheIyEiIkYrSSJrR0YmRitJJk9tZWdhR0YmRi5GKw==</Equation></Text-field></Output></Group><Group><Input><Text-field layout="Normal" style="Normal">We see this is the sum of the impedances of the two single devices.</Text-field></Input></Group><Group><Input><Text-field layout="Heading 3" style="Heading 3">MAXWELL Model</Text-field><Text-field layout="Normal" style="Normal">This is another model which is used to describe viscous elastic devices. Here an ideal elastic spring and an ideal viscous damper are connected as a chain in series as shown in Figure 13</Text-field><Text-field alignment="centred"><Image height="240" 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eld><Text-field layout="Normal256" style="Normal256">Figure 13</Text-field><Text-field layout="Normal" style="Normal">Such a device is only able to transmit dynamic forces.</Text-field><Text-field layout="Normal" style="Normal">The quadripole parameter of this model are calculated by use of the procedure <Hyperlink bold="false" executable="false" family="Times New Roman" hyperlink="true" linktarget="Wks:#serialconnection" size="12" style="Hyperlink">serialconnection</Hyperlink>.</Text-field><Text-field layout="Normal" style="Normal">The input parameters for this procedure are again the matrices of the quadripole parameter of the damper</Text-field></Input></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">evalm(A[damper]);</Font></Text-field></Input><Output><Text-field layout="Maple Output" style="2D Output"><Equation>NiMtSSdtYXRyaXhHNiRJKnByb3RlY3RlZEdGJkkoX3N5c2xpYkc2IjYjNyQ3JCIiIiIiITckKiRJImRHRighIiJGLA==</Equation></Text-field></Output></Group><Group><Input><Text-field layout="Normal" style="Normal">and the spring</Text-field></Input></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">evalm(A[spring]);</Font></Text-field></Input><Output><Text-field layout="Maple Output" style="2D Output"><Equation>NiMtSSdtYXRyaXhHNiRJKnByb3RlY3RlZEdGJkkoX3N5c2xpYkc2IjYjNyQ3JCIiIiIiITckKiheI0YsRixJJk9tZWdhR0YoRixJImtHRighIiJGLA==</Equation></Text-field></Output></Group><Group><Input><Text-field layout="Normal" style="Normal">The matrix of the quadripole parameter of the MAXWELL model is consequently</Text-field></Input></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">A[MAXWELL]:=serialconnection(A[damper],A[spring]);</Font></Text-field></Input><Output><Text-field layout="Maple Output" style="2D Output"><Equation>NiM+JkkiQUc2IjYjSShNQVhXRUxMR0YmLUknbWF0cml4RzYkSSpwcm90ZWN0ZWRHRixJKF9zeXNsaWJHRiY2IzckNyQiIiIiIiE3JCwmKiRJImRHRiYhIiJGMSooXiNGMUYxSSZPbWVnYUdGJkYxSSJrR0YmRjdGMUYx</Equation></Text-field></Output></Group><Group><Input><Text-field layout="Normal" style="Normal">Again we will also consider the impedance of such a device. We assume for this that the velocity on the output gate of this device is <Equation input-equation="v[2]=0" style="2D Comment">NiMvJiUidkc2IyIiIyIiIQ==</Equation>. The force must go directly through the device. That means that the force on the spring and the force on the damper are eqaul: <Equation input-equation="F[damper]=F[1]" style="2D Comment">NiMvJiUiRkc2IyUnZGFtcGVyRyZGJTYjIiIi</Equation> and <Equation input-equation="F[spring]=F[1]" style="2D Comment">NiMvJiUiRkc2IyUnc3ByaW5nRyZGJTYjIiIi</Equation>. The velocity of the damper is then given by</Text-field></Input></Group><Group><Input><Text-field layout="Normal256" prompt="&gt; " style="2D Input"><Equation executable="true" input-equation="v[1][MAXWELL_damper](t):=F[1](t)/d:" style="2D Input">NiM+LSYmJSJ2RzYjIiIiNiMlL01BWFdFTExfZGFtcGVyRzYjJSJ0RyomLSYlIkZHRihGLEYpJSJkRyEiIg==</Equation></Text-field></Input></Group><Group><Input><Text-field layout="Normal" style="Normal">The displacement of the spring is</Text-field></Input></Group><Group><Input><Text-field layout="Normal256" prompt="&gt; " style="2D Input"><Equation executable="true" input-equation="x[1][MAXWELL_spring](t):=F[1](t)/k:" style="2D Input">NiM+LSYmJSJ4RzYjIiIiNiMlL01BWFdFTExfc3ByaW5nRzYjJSJ0RyomLSYlIkZHRihGLEYpJSJrRyEiIg==</Equation></Text-field></Input></Group><Group><Input><Text-field layout="Normal" style="Normal">Because we assume harmonic motion, we get for the velocity in the spring</Text-field></Input></Group><Group><Input><Text-field layout="Normal256" prompt="&gt; " style="2D Input"><Equation executable="true" input-equation="v[1][MAXWELL_spring](t):=x[1][MAXWELL_spring](t)*I*Omega;" style="2D Input">NiM+LSYmJSJ2RzYjIiIiNiMlL01BWFdFTExfc3ByaW5nRzYjJSJ0RyooLSYmJSJ4R0YoRipGLEYpJSJJR0YpJSZPbWVnYUdGKQ==</Equation></Text-field></Input><Output><Text-field layout="Maple Output" style="2D Output"><Equation>NiM+LSYmSSJ2RzYiNiMiIiI2I0kvTUFYV0VMTF9zcHJpbmdHRig2I0kidEdGKCoqXiNGKkYqLSZJIkZHRihGKUYtRipJImtHRighIiJJJk9tZWdhR0YoRio=</Equation></Text-field></Output></Group><Group><Input><Text-field layout="Normal" style="Normal">The velocity at the input gate of the total device is the sum of the single velocities</Text-field></Input></Group><Group><Input><Text-field layout="Normal256" prompt="&gt; " style="2D Input"><Equation executable="true" input-equation="v[1][MAXWELL](t):=v[1][MAXWELL_spring](t)+v[1][MAXWELL_damper](t);" style="2D Input">NiM+LSYmJSJ2RzYjIiIiNiMlKE1BWFdFTExHNiMlInRHLCYtJkYmNiMlL01BWFdFTExfc3ByaW5nR0YsRiktJkYmNiMlL01BWFdFTExfZGFtcGVyR0YsRik=</Equation></Text-field></Input><Output><Text-field layout="Maple Output" style="2D Output"><Equation>NiM+LSYmSSJ2RzYiNiMiIiI2I0koTUFYV0VMTEdGKDYjSSJ0R0YoLCYqKl4jRipGKi0mSSJGR0YoRilGLUYqSSJrR0YoISIiSSZPbWVnYUdGKEYqRioqJkYyRipJImRHRihGNkYq</Equation></Text-field></Output></Group><Group><Input><Text-field layout="Normal" style="Normal">And the impedance is the quotient of the force and the velocity</Text-field></Input></Group><Group><Input><Text-field layout="Normal256" prompt="&gt; " style="2D Input"><Equation executable="true" input-equation="R[MAXWELL]:=simplify(F[1](t)/v[1][MAXWELL](t));" style="2D Input">NiM+JiUiUkc2IyUoTUFYV0VMTEctJSlzaW1wbGlmeUc2IyomLSYlIkZHNiMiIiI2IyUidEdGMC0mJiUidkdGL0YmRjEhIiI=</Equation></Text-field></Input><Output><Text-field layout="Maple Output" style="2D Output"><Equation>NiM+JkkiUkc2IjYjSShNQVhXRUxMR0YmKihJImtHRiYiIiJJImRHRiZGKywmKiheI0YrRitJJk9tZWdhR0YmRitGLEYrRitGKkYrISIi</Equation></Text-field></Output></Group><Group><Input><Text-field layout="Heading 3" style="Heading 3">Spring-Damper-Mass-System</Text-field><Text-field layout="Normal" style="Normal">Next we consider how a simple spring-damper-mass-system is typically used to describe the simplest structural dynamic system as a single-degree-of-freedom system. This system is shown in Figure 14</Text-field><Text-field alignment="centred"><Image height="180" 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layout="Normal256" style="Normal256">Figure 14</Text-field><Text-field layout="Normal" style="Normal">This model is the parallel connection of a spring and a damper and these two devices together in series with the mass. The above formalism yields the following for the total device</Text-field></Input></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">A[spring_damper_mass]:=simplify(serialconnection(A[mass],parallelconnection(A[spring],A[damper])));</Font></Text-field></Input><Output><Text-field layout="Maple Output" style="2D Output"><Equation>NiM+JkkiQUc2IjYjSTNzcHJpbmdfZGFtcGVyX21hc3NHRiYtSSdtYXRyaXhHNiRJKnByb3RlY3RlZEdGLEkoX3N5c2xpYkdGJjYjNyQ3JComLCgqJkkiZEdGJiIiIkkmT21lZ2FHRiZGNSEiIiomXiNGNUY1SSJrR0YmRjVGNSooXiNGN0Y1SSJtR0YmRjVGNiIiI0Y1RjUsJkYzRjdGOEY1RjcqKEY5RjVGPUY1RjZGNTckLCQqJkY2RjVGP0Y3RjdGNQ==</Equation></Text-field></Output></Group><Group><Input><Text-field layout="Normal" style="Normal">The impedance of this device can be deduced when we assume that the velocity at gate 2 must be 0</Text-field></Input></Group><Group><Input><Text-field layout="Normal256" prompt="&gt; " style="2D Input"><Equation executable="true" input-equation="v[2][spring_damper_mass]:=0:" style="2D Input">NiM+JiYlInZHNiMiIiM2IyUzc3ByaW5nX2RhbXBlcl9tYXNzRyIiIQ==</Equation></Text-field></Input></Group><Group><Input><Text-field layout="Normal" style="Normal">From the definition of the quadripole parameter we know the relation</Text-field><Text-field layout="Normal256" style="2D Comment"><Equation input-equation="matrix([[F[1]], [v[1]]]) = matrix([[A[1,1], A[1,2]], [A[2,1], A[2,2]]])*matrix([[F[2]], [v[2]]]);" style="2D Comment">NiMvLSUnbWF0cml4RzYjNyQ3IyYlIkZHNiMiIiI3IyYlInZHRisqJi1GJTYjNyQ3JCYlIkFHNiRGLEYsJkY2NiRGLCIiIzckJkY2NiRGOkYsJkY2NiRGOkY6RiwtRiU2IzckNyMmRio2I0Y6NyMmRi9GRUYs</Equation></Text-field><Text-field layout="Normal" style="Normal">or written for this special case as two equations</Text-field></Input></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="2D Input"><Equation executable="true" input-equation="rel1:=F[1][spring_damper_mass] = A[spring_damper_mass][1,1]*F[2][spring_damper_mass]+A[spring_damper_mass][1,2]*v[2][spring_damper_mass];" style="2D Input">NiM+JSVyZWwxRy8mJiUiRkc2IyIiIjYjJTNzcHJpbmdfZGFtcGVyX21hc3NHLCYqJiYmJSJBR0YrNiRGKkYqRiomJkYoNiMiIiNGK0YqRioqJiZGMDYkRipGNkYqJiYlInZHRjVGK0YqRio=</Equation></Text-field></Input><Output><Text-field layout="Maple Output" style="2D Output"><Equation>NiM+SSVyZWwxRzYiLyYmSSJGR0YlNiMiIiI2I0kzc3ByaW5nX2RhbXBlcl9tYXNzR0YlKigsKComSSJkR0YlRitJJk9tZWdhR0YlRishIiIqJl4jRitGK0kia0dGJUYrRisqKF4jRjNGK0kibUdGJUYrRjIiIiNGK0YrLCZGMEYzRjRGK0YzJiZGKTYjRjpGLEYr</Equation></Text-field></Output></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="2D Input"><Equation executable="true" input-equation="rel2:= v[1][spring_damper_mass] = A[spring_damper_mass][2,1]*F[2][spring_damper_mass]+A[spring_damper_mass][2,2]*v[2][spring_damper_mass];" style="2D Input">NiM+JSVyZWwyRy8mJiUidkc2IyIiIjYjJTNzcHJpbmdfZGFtcGVyX21hc3NHLCYqJiYmJSJBR0YrNiQiIiNGKkYqJiYlIkZHNiNGM0YrRipGKiomJkYwNiRGM0YzRiomJkYoRjdGK0YqRio=</Equation></Text-field></Input><Output><Text-field layout="Maple Output" style="2D Output"><Equation>NiM+SSVyZWwyRzYiLyYmSSJ2R0YlNiMiIiI2I0kzc3ByaW5nX2RhbXBlcl9tYXNzR0YlLCQqKEkmT21lZ2FHRiVGKywmKiZJImRHRiVGK0YwRishIiIqJl4jRitGK0kia0dGJUYrRitGNCYmSSJGR0YlNiMiIiNGLEYrRjQ=</Equation></Text-field></Output></Group><Group><Input><Text-field layout="Normal" style="Normal">The solution of this two equations yields the force at the output gate <Equation input-equation="F[2][spring_damper_mass]" style="2D Comment">NiMmJiUiRkc2IyIiIzYjJTNzcHJpbmdfZGFtcGVyX21hc3NH</Equation> and the velocity at the input gate <Equation input-equation="v[1][spring_damper_mass]" style="2D Comment">NiMmJiUidkc2IyIiIjYjJTNzcHJpbmdfZGFtcGVyX21hc3NH</Equation>, both dependent on the force at the input gate <Equation input-equation="F[1][spring_damper_mass]" style="2D Comment">NiMmJiUiRkc2IyIiIjYjJTNzcHJpbmdfZGFtcGVyX21hc3NH</Equation>.</Text-field></Input></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">sols:=solve({rel1,rel2},{F[2][spring_damper_mass],v[1][spring_damper_mass]});</Font></Text-field></Input><Output><Text-field layout="Maple Output" style="2D Output"><Equation>NiM+SSVzb2xzRzYiPCQvJiZJInZHRiU2IyIiIjYjSTNzcHJpbmdfZGFtcGVyX21hc3NHRiUsJCooJiZJIkZHRiVGK0YtRixJJk9tZWdhR0YlRiwsKComSSJkR0YlRixGNEYsISIiKiZeI0YsRixJImtHRiVGLEYsKiheI0Y4RixJIm1HRiVGLEY0IiIjRixGOEY4LyYmRjM2I0Y/Ri0qKCwmRjZGOEY5RixGLEYxRixGNUY4</Equation></Text-field></Output></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">assign(sols);</Font></Text-field></Input></Group><Group><Input><Text-field layout="Normal" style="Normal">At last we calculate the relation between the force and the velocity at the input gate to get the impedance</Text-field></Input></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">R[spring_damper_mass] := simplify(F[1][spring_damper_mass]/v[1][spring_damper_mass]);</Font></Text-field></Input><Output><Text-field layout="Maple Output" style="2D Output"><Equation>NiM+JkkiUkc2IjYjSTNzcHJpbmdfZGFtcGVyX21hc3NHRiYsJComSSZPbWVnYUdGJiEiIiwoKiZJImRHRiYiIiJGK0YwRiwqJl4jRjBGMEkia0dGJkYwRjAqKF4jRixGMEkibUdGJkYwRisiIiNGMEYwRiw=</Equation></Text-field></Output></Group><Group><Input><Text-field layout="Heading 3" style="Heading 3">4-Parametrical MAXWELL Model</Text-field><Text-field layout="Normal" style="Normal">At last we consider a model which is composed by four single standard devices as shown in Figure 15</Text-field><Text-field alignment="centred"><Image height="240" 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layout="Normal256" style="Normal256">Figure 15</Text-field><Text-field layout="Normal" style="Normal">This model is the parallel connection of two MAXWELL models, which are themselves serial connections of a spring and a damper. The damper on the left line has damping resistance <Equation input-equation="d[a]" style="2D Comment">NiMmJSJkRzYjJSJhRw==</Equation>, the spring on the left line has stiffness <Equation input-equation="k[a]" style="2D Comment">NiMmJSJrRzYjJSJhRw==</Equation>. The damper and the spring on the right line have the damping resistance <Equation input-equation="d[b]" style="2D Comment">NiMmJSJkRzYjJSJiRw==</Equation> and the stiffness <Equation input-equation="k[b]" style="2D Comment">NiMmJSJrRzYjJSJiRw==</Equation>. We use the information about the MAXWELL model for the two partial devices on the left and on the right line to get the matrices of the quadripole parameter</Text-field></Input></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">A[a]:=subs({k=k[a],d=d[a]},evalm(A[MAXWELL]));</Font></Text-field></Input><Output><Text-field layout="Maple Output" style="2D Output"><Equation>NiM+JkkiQUc2IjYjSSJhR0YmLUknbWF0cml4RzYkSSpwcm90ZWN0ZWRHRixJKF9zeXNsaWJHRiY2IzckNyQiIiIiIiE3JCwmKiQmSSJkR0YmRichIiJGMSooXiNGMUYxSSZPbWVnYUdGJkYxJkkia0dGJkYnRjhGMUYx</Equation></Text-field></Output></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">A[b]:=subs({k=k[b],d=d[b]},evalm(A[MAXWELL]));</Font></Text-field></Input><Output><Text-field layout="Maple Output" style="2D Output"><Equation>NiM+JkkiQUc2IjYjSSJiR0YmLUknbWF0cml4RzYkSSpwcm90ZWN0ZWRHRixJKF9zeXNsaWJHRiY2IzckNyQiIiIiIiE3JCwmKiQmSSJkR0YmRichIiJGMSooXiNGMUYxSSZPbWVnYUdGJkYxJkkia0dGJkYnRjhGMUYx</Equation></Text-field></Output></Group><Group><Input><Text-field layout="Normal" style="Normal">The matrix of the quadripole parameter for the total device is now easy to calculate as a parallel connection of <Equation input-equation="A[a]" style="2D Comment">NiMmJSJBRzYjJSJhRw==</Equation> and <Equation input-equation="A[b]" style="2D Comment">NiMmJSJBRzYjJSJiRw==</Equation></Text-field></Input></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">A[MAXWELL2]:=simplify(parallelconnection(A[a],A[b]));</Font></Text-field></Input><Output><Text-field layout="Maple Output" style="2D Output"><Equation>NiM+JkkiQUc2IjYjSSlNQVhXRUxMMkdGJi1JJ21hdHJpeEc2JEkqcHJvdGVjdGVkR0YsSShfc3lzbGliR0YmNiM3JDckIiIiIiIhNyQqJiwqKigmSSJkR0YmNiNJImFHRiZGMSZJImtHRiZGOUYxJkY8NiNJImJHRiZGMUYxKixeI0YxRjFGN0YxRjtGMUkmT21lZ2FHRiZGMSZGOEY+RjFGMSooRkNGMUY9RjFGO0YxRjEqLEZBRjFGQ0YxRj1GMUZCRjFGN0YxRjEhIiIsKiomRjtGMUY9RjFGMSoqRkFGMUY7RjFGQkYxRkNGMUYxKipGQUYxRkJGMUY3RjFGPUYxRjEqKEZCIiIjRjdGMUZDRjFGRkYxRjE=</Equation></Text-field></Output></Group><Group><Input><Text-field layout="Normal" style="Normal">The impedance of this device is the sum of the impedance of the MAXWELL device on the left line and that on the right line, same as in the parallel connection of a damper with a spring</Text-field></Input></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">R[a]:=simplify(subs({k=k[a],d=d[a]},R[MAXWELL]));</Font></Text-field></Input><Output><Text-field layout="Maple Output" style="2D Output"><Equation>NiM+JkkiUkc2IjYjSSJhR0YmKigmSSJkR0YmRiciIiImSSJrR0YmRidGLCwmRi1GLCooXiNGLEYsSSZPbWVnYUdGJkYsRipGLEYsISIi</Equation></Text-field></Output></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">R[b]:=simplify(subs({k=k[b],d=d[b]},R[MAXWELL]));</Font></Text-field></Input><Output><Text-field layout="Maple Output" style="2D Output"><Equation>NiM+JkkiUkc2IjYjSSJiR0YmKigmSSJkR0YmRiciIiImSSJrR0YmRidGLCwmRi1GLCooXiNGLEYsSSZPbWVnYUdGJkYsRipGLEYsISIi</Equation></Text-field></Output></Group><Group><Input><Text-field layout="Normal256" prompt="&gt; " style="2D Input"><Equation executable="true" input-equation="R[MAXWELL2]:=simplify(R[a]+R[b]);" style="2D Input">NiM+JiUiUkc2IyUpTUFYV0VMTDJHLSUpc2ltcGxpZnlHNiMsJiZGJTYjJSJhRyIiIiZGJTYjJSJiR0Yv</Equation></Text-field></Input><Output><Text-field layout="Maple Output" style="2D Output"><Equation>NiM+JkkiUkc2IjYjSSlNQVhXRUxMMkdGJiooLCoqKCZJImRHRiY2I0kiYUdGJiIiIiZJImtHRiZGLkYwJkYyNiNJImJHRiZGMEYwKixeI0YwRjBGLEYwRjFGMEkmT21lZ2FHRiZGMCZGLUY0RjBGMCooRjlGMEYzRjBGMUYwRjAqLEY3RjBGOUYwRjNGMEY4RjBGLEYwRjBGMCwmRjFGMCooRjdGMEY4RjBGLEYwRjAhIiIsJkYzRjAqKEY3RjBGOEYwRjlGMEYwRj4=</Equation></Text-field></Output></Group><Group><Input><Text-field layout="Heading 1" style="Heading 1">Example</Text-field><Text-field layout="Normal" style="Normal">Now we will consider an example. As shown in Figure 16 we have a a special machine as the source of the vibration. All values here and in the following are given in N, m, kg and s. Consequently the impedances are given in Ns/m. Please note: These numerical values are academic examples only.</Text-field><Text-field alignment="centred"><Image height="300" 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layout="Normal256" style="Normal256">Figure 16</Text-field><Text-field layout="Normal" style="Normal">We have the input gate given by</Text-field></Input></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">input:=matrix([[F[0]],[v[0]]]);</Font></Text-field></Input><Output><Text-field layout="Maple Output" style="2D Output"><Equation>NiM+SSZpbnB1dEc2Ii1JJ21hdHJpeEc2JEkqcHJvdGVjdGVkR0YpSShfc3lzbGliR0YlNiM3JDcjJkkiRkdGJTYjIiIhNyMmSSJ2R0YlRjA=</Equation></Text-field></Output></Group><Group><Input><Text-field layout="Normal" style="Normal">and the output gate given by</Text-field><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">output:=matrix([[F[2]],[v[2]]]);</Font></Text-field></Input><Output><Text-field layout="Maple Output" style="2D Output"><Equation>NiM+SSdvdXRwdXRHNiItSSdtYXRyaXhHNiRJKnByb3RlY3RlZEdGKUkoX3N5c2xpYkdGJTYjNyQ3IyZJIkZHRiU2IyIiIzcjJkkidkdGJUYw</Equation></Text-field></Output></Group><Group><Input><Text-field layout="Normal" style="Normal">The impedance of the source shall be given by its real part</Text-field></Input></Group><Group><Input><Text-field layout="Normal256" prompt="&gt; " style="2D Input"><Equation executable="true" input-equation="real_R[s]:=250000*Pi**2*f**2/(6250000-4975*Pi**2*f**2+Pi**4*f**4):" style="2D Input">NiM+JiUncmVhbF9SRzYjJSJzRyoqIicrK0QiIiIqJCUjUGlHIiIjRiolImZHRi0sKCIoKytEJ0YqKigiJXZcRipGK0YqRi5GLSEiIiomRiwiIiVGLkY1RipGMw==</Equation></Text-field></Input></Group><Group><Input><Text-field layout="Normal" style="Normal">and its imaginary part</Text-field></Input></Group><Group><Input><Text-field layout="Normal256" prompt="&gt; " style="2D Input"><Equation executable="true" input-equation="imag_R[s]:=-50000*Pi*f*(-2500+Pi**2*f**2)/(6250000-4975*Pi**2*f**2+Pi**4*f**4):" style="2D Input">NiM+JiUnaW1hZ19SRzYjJSJzRywkKiwiJisrJiIiIiUjUGlHRislImZHRissJiIlK0QhIiIqJkYsIiIjRi1GMkYrRissKCIoKytEJ0YrKigiJXZcRisqJEYsRjJGK0YtRjJGMComRiwiIiVGLUY5RitGMEYw</Equation></Text-field></Input></Group><Group><Input><Text-field layout="Normal" style="Normal">So the impedance <Equation input-equation="R[s]" style="2D Comment">NiMmJSJSRzYjJSJzRw==</Equation> is</Text-field></Input></Group><Group><Input><Text-field layout="Normal256" prompt="&gt; " style="2D Input"><Equation executable="true" input-equation="R[s]:=real_R[s]+I*imag_R[s];" style="2D Input">NiM+JiUiUkc2IyUic0csJiYlJ3JlYWxfUkdGJiIiIiomJSJJR0YrJiUnaW1hZ19SR0YmRitGKw==</Equation></Text-field></Input><Output><Text-field layout="Maple Output" style="2D Output"><Equation>NiM+JkkiUkc2IjYjSSJzR0YmLCYqKEkjUGlHSSpwcm90ZWN0ZWRHRiwiIiNJImZHRiZGLSwoIigrK0QnIiIiKiZGK0YtRi5GLSEldlwqJkYrIiIlRi5GNUYxISIiIicrK0QqLF4jISYrKyZGMUYrRjFGLkYxLCYhJStERjFGMkYxRjFGL0Y2RjE=</Equation></Text-field></Output></Group><Group><Input><Text-field layout="Normal" style="Normal">Let's consider graphs of these functions.</Text-field></Input></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">PRsr:=plot(Re(R[s]),f=0..100,color=red,legend="real part"):</Font></Text-field></Input></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">PRsi:=plot(Im(R[s]),f=0..100,color=green,legend="imaginary part"):</Font></Text-field></Input></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">PRsa:=plot(abs(R[s]),f=0..100,color=blue,thickness=2,legend="absolute value"):</Font></Text-field></Input></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">PRsp:=plot(argument(R[s]),f=0..100,color=cyan,legend="argument"):</Font></Text-field></Input></Group><Group><Input><Text-field layout="Normal" style="Normal">Most of the time, the absolute value is the most interesting, so we draw it with a thick line.</Text-field></Input></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">display(PRsr,PRsi,PRsa,title="Impedance of the Vibration Source");</Font></Text-field><Text-field layout="Normal" style="Normal"/><Text-field layout="Normal" style="Normal"/></Input><Output><Text-field layout="Maple Plot"><Plot height="400" plot-scale="1.0" plot-xtrans="0.0" plot-ytrans="0.0" type="two-dimensional" width="400">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</Plot></Text-field></Output></Group><Group><Input><Text-field layout="Normal" style="Normal">The argument of this function is shown in the next picture</Text-field></Input></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">display(PRsp,title="Impedance of the Vibration Source");</Font></Text-field></Input><Output><Text-field layout="Maple Plot"><Plot height="400" plot-scale="1.0" plot-xtrans="0.0" plot-ytrans="0.0" type="two-dimensional" width="400">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</Plot></Text-field></Output></Group><Group><Input><Text-field layout="Normal" style="Normal">The matrix of the quadripole parameter of the vibration source follows from <Hyperlink bold="false" executable="false" family="Times New Roman" hyperlink="true" linktarget="Wks:#source" size="12" style="Hyperlink">above</Hyperlink> </Text-field></Input></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">A[s]:=matrix(2,2,[1,R[s],0,1]);</Font></Text-field></Input><Output><Text-field layout="Maple Output" style="2D Output"><Equation>NiM+JkkiQUc2IjYjSSJzR0YmLUknbWF0cml4RzYkSSpwcm90ZWN0ZWRHRixJKF9zeXNsaWJHRiY2IzckNyQiIiIsJiooSSNQaUdGLCIiI0kiZkdGJkY1LCgiKCsrRCdGMSomRjRGNUY2RjUhJXZcKiZGNCIiJUY2RjxGMSEiIiInKytEKixeIyEmKysmRjFGNEYxRjZGMSwmISUrREYxRjlGMUYxRjdGPUYxNyQiIiFGMQ==</Equation></Text-field></Output></Group><Group><Input><Text-field layout="Normal" style="Normal">Next we consider the foundation, the recipient. We assume the following numerical values and use the definition for the <Hyperlink bold="false" executable="false" family="Times New Roman" hyperlink="true" linktarget="Wks:#elastichalfspace" size="12" style="Hyperlink">elastic half-space</Hyperlink> defined above.</Text-field></Input></Group><Group><Input><Text-field layout="Normal256" prompt="&gt; " style="2D Input"><Equation executable="true" input-equation="soil:=G=200000000,mu=2/10,rho=2000,a=2:" style="2D Input">NiM+JSVzb2lsRzYmLyUiR0ciKisrKysjLyUjbXVHKiYiIiMiIiIiIzUhIiIvJSRyaG9HIiUrPy8lImFHRiw=</Equation></Text-field></Input></Group><Group><Input><Text-field layout="Normal" style="Normal">The impedance of the recipient is then</Text-field></Input></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">R[r]:=complexextension(subs({soil,sub1},R[ELASTIC_HALF_SPACE]));</Font></Text-field></Input><Output><Text-field layout="Maple Output" style="2D Output"><Equation>NiM+JkkiUkc2IjYjSSJyR0YmLCYqKEkjUGlHSSpwcm90ZWN0ZWRHRiwiIiMiIzUjIiIiRi0sJiomRisiIiVJImZHRiZGLSIkaCQiKSsrXWlGMCEiIiIvKysrK10oPSIqKF4jITIrKysrKytEYyJGMEY0RjdGMUY3RjA=</Equation></Text-field></Output></Group><Group><Input><Text-field layout="Normal" style="Normal">This result is best shown graphically. The first picture shows the real part, the imaginary part and the absolute value.</Text-field></Input></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">vw:=-2E7..2E7:</Font></Text-field></Input></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">PEr:=plot(Re(R[r]),f=0..100,vw,color=red,legend="real part"):</Font></Text-field></Input></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">PEi:=plot(Im(R[r]),f=0..100,vw,color=green,legend="imaginary part"):</Font></Text-field></Input></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">PEa:=plot(abs(R[r]),f=0..100,vw,color=blue,thickness=2,legend="absolute value"):</Font></Text-field></Input></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">PEp:=plot(argument(R[r]),f=0..100,-Pi..Pi,color=cyan,legend="argument"):</Font></Text-field></Input></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">display(PEr,PEi,PEa,title="Impedance of the Ground");</Font></Text-field></Input><Output><Text-field layout="Maple Plot"><Plot height="400" plot-scale="1.0" plot-xtrans="0.0" plot-ytrans="0.0" type="two-dimensional" width="400">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</Plot></Text-field></Output></Group><Group><Input><Text-field layout="Normal" style="Normal">The next picture shows the angle between the real part and the imaginary part of the impedance.</Text-field></Input></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">display(PEp,title="Impedance of the Ground");</Font></Text-field></Input><Output><Text-field layout="Maple Plot"><Plot height="400" plot-scale="1.0" plot-xtrans="0.0" plot-ytrans="0.0" type="two-dimensional" width="400">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</Plot></Text-field></Output></Group><Group><Input><Text-field layout="Normal" style="Normal">Now we consider some devices which are arranged between the machine and the soil for vibration control. Here we assume that the excitation force <Equation input-equation="F[0]" style="2D Comment">NiMmJSJGRzYjIiIh</Equation> for all the following examples is identical. That means that there is no feedback interaction from the structure to the source of the excitation. Otherwise this problem would be much more complicated and not so easily solved without more details about the excitation.</Text-field><Text-field layout="Heading 3" style="Heading 3"/><Text-field layout="Heading 3" style="Heading 3">Rigid Connection</Text-field><Text-field layout="Normal" style="Normal">Rigid connection means that the machine stands on the ground without any device. So we have the relation</Text-field><Text-field layout="Normal256" style="2D Comment"><Equation input-equation="matrix([[F[1]], [v[1]]]) = matrix([[1, 0], [0, 1]])*matrix([[F[2]], [v[2]]]);" style="2D Comment">NiMvLSUnbWF0cml4RzYjNyQ3IyYlIkZHNiMiIiI3IyYlInZHRisqJi1GJTYjNyQ3JEYsIiIhNyRGNUYsRiwtRiU2IzckNyMmRio2IyIiIzcjJkYvRjxGLA==</Equation></Text-field><Text-field layout="Normal" style="Normal">That means for the matrix of the quadripole parameter</Text-field></Input></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">A[rigid]:=matrix([[1,0],[0,1]]);</Font></Text-field></Input><Output><Text-field layout="Maple Output" style="2D Output"><Equation>NiM+JkkiQUc2IjYjSSZyaWdpZEdGJi1JJ21hdHJpeEc2JEkqcHJvdGVjdGVkR0YsSShfc3lzbGliR0YmNiM3JDckIiIiIiIhNyRGMkYx</Equation></Text-field></Output></Group><Group><Input><Text-field layout="Normal" style="Normal">The total structure is  a serial connection of the source with a rigid connection.</Text-field></Input></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">A[1]:=serialconnection(A[s],A[rigid]);</Font></Text-field></Input><Output><Text-field layout="Maple Output" style="2D Output"><Equation>NiM+JkkiQUc2IjYjIiIiLUknbWF0cml4RzYkSSpwcm90ZWN0ZWRHRixJKF9zeXNsaWJHRiY2IzckNyRGKCwmKihJI1BpR0YsIiIjSSJmR0YmRjQsKCIoKytEJ0YoKiZGM0Y0RjVGNCEldlwqJkYzIiIlRjVGO0YoISIiIicrK0QqLF4jISYrKyZGKEYzRihGNUYoLCYhJStERihGOEYoRihGNkY8Rig3JCIiIUYo</Equation></Text-field></Output></Group><Group><Input><Text-field layout="Normal" style="Normal">Of course this is the same as the matrix of the quadripole parameter of the source itself. The relation between the values of the input gate <Equation input-equation="F[0]" style="2D Comment">NiMmJSJGRzYjIiIh</Equation>, <Equation input-equation="v[0]" style="2D Comment">NiMmJSJ2RzYjIiIh</Equation> and the values at the output gate <Equation input-equation="F[2]" style="2D Comment">NiMmJSJGRzYjIiIj</Equation>, <Equation input-equation="v[2]" style="2D Comment">NiMmJSJ2RzYjIiIj</Equation> is</Text-field></Input></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">eq[1]:=input=A[1]&amp;*output;</Font></Text-field></Input><Output><Text-field layout="Maple Output" style="2D Output"><Equation>NiM+JkkjZXFHNiI2IyIiIi9JJmlucHV0R0YmLUkjJipHRiY2JCZJIkFHRiZGJ0knb3V0cHV0R0Ym</Equation></Text-field></Output></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">evalm(eq[1]);</Font></Text-field></Input><Output><Text-field layout="Maple Output" style="2D Output"><Equation>NiMvLUknbWF0cml4RzYkSSpwcm90ZWN0ZWRHRidJKF9zeXNsaWJHNiI2IzckNyMmSSJGR0YpNiMiIiE3IyZJInZHRilGLy1GJTYjNyQ3IywmJkYuNiMiIiMiIiIqJiwmKihJI1BpR0YnRjtJImZHRilGOywoIigrK0QnRjwqJkZARjtGQUY7ISV2XComRkAiIiVGQUZHRjwhIiIiJysrRCosXiMhJisrJkY8RkBGPEZBRjwsJiElK0RGPEZERjxGPEZCRkhGPEY8JkYzRjpGPEY8NyNGTw==</Equation></Text-field></Output></Group><Group><Input><Text-field layout="Normal" style="Normal">This yields for the values of the output gate</Text-field></Input></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">sol[1]:=linsolve(A[1],input);</Font></Text-field></Input><Output><Text-field layout="Maple Output" style="2D Output"><Equation>NiM+Jkkkc29sRzYiNiMiIiItSSdtYXRyaXhHNiRJKnByb3RlY3RlZEdGLEkoX3N5c2xpYkdGJjYjNyQ3IyomLC4qKCZJIkZHRiY2IyIiIUYoSSNQaUdGLCIiJUkiZkdGJkY5RihGNCIoKytEJyooRjRGKEY4IiIjRjpGPSEldlwqKCZJInZHRiZGNkYoRjhGPUY6Rj0hJysrRCoqXiMhKisrK0QiRihGQEYoRjhGKEY6RihGKCoqXiMiJisrJkYoRkBGKEY4IiIkRjpGSUYoRigsKEY7RigqJkY4Rj1GOkY9Rj4qJkY4RjlGOkY5RighIiI3I0ZA</Equation></Text-field></Output></Group><Group><Input><Text-field layout="Normal" style="Normal">This means</Text-field></Input></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">F_rigid[2]:=sol[1][1,1];</Font></Text-field></Input><Output><Text-field layout="Maple Output" style="2D Output"><Equation>NiM+JkkoRl9yaWdpZEc2IjYjIiIjKiYsLiooJkkiRkdGJjYjIiIhIiIiSSNQaUdJKnByb3RlY3RlZEdGMiIiJUkiZkdGJkYzRjBGLCIoKytEJyooRixGMEYxRihGNEYoISV2XCooJkkidkdGJkYuRjBGMUYoRjRGKCEnKytEKipeIyEqKysrRCJGMEY5RjBGMUYwRjRGMEYwKipeIyImKysmRjBGOUYwRjEiIiRGNEZCRjBGMCwoRjVGMComRjFGKEY0RihGNyomRjFGM0Y0RjNGMCEiIg==</Equation></Text-field></Output></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">v_rigid[2]:=sol[1][2,1];</Font></Text-field></Input><Output><Text-field layout="Maple Output" style="2D Output"><Equation>NiM+Jkkodl9yaWdpZEc2IjYjIiIjJkkidkdGJjYjIiIh</Equation></Text-field></Output></Group><Group><Input><Text-field layout="Normal" style="Normal">At last we use our information about the impedance of the output gate</Text-field></Input></Group><Group><Input><Text-field layout="Normal256" prompt="&gt; " style="2D Input"><Equation executable="true" input-equation="eq[2]:=F_rigid[2]=R[r]*v_rigid[2];" style="2D Input">NiM+JiUjZXFHNiMiIiMvJiUoRl9yaWdpZEdGJiomJiUiUkc2IyUickciIiImJSh2X3JpZ2lkR0YmRjA=</Equation></Text-field></Input><Output><Text-field layout="Maple Output" style="2D Output"><Equation>NiM+JkkjZXFHNiI2IyIiIy8qJiwuKigmSSJGR0YmNiMiIiEiIiJJI1BpR0kqcHJvdGVjdGVkR0YzIiIlSSJmR0YmRjRGMUYtIigrK0QnKihGLUYxRjJGKEY1RighJXZcKigmSSJ2R0YmRi9GMUYyRihGNUYoIScrK0QqKl4jISorKytEIkYxRjpGMUYyRjFGNUYxRjEqKl4jIiYrKyZGMUY6RjFGMiIiJEY1RkNGMUYxLChGNkYxKiZGMkYoRjVGKEY4KiZGMkY0RjVGNEYxISIiKiYsJiooRjJGKCIjNSNGMUYoLCYqJkYyRjRGNUYoIiRoJCIpKytdaUYxRkciLysrKytdKD0iKiheIyEyKysrKysrRGMiRjFGNUZHRk1GR0YxRjFGOkYx</Equation></Text-field></Output></Group><Group><Input><Text-field layout="Normal" style="Normal">The solution of this equation yields the velocity at the input gate dependent on the force at the input gate</Text-field></Input></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">sol[2]:=simplify(solve(eq[2],v[0]));</Font></Text-field></Input><Output><Text-field layout="Maple Output" style="2D Output"><Equation>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</Equation></Text-field></Output></Group><Group><Input><Text-field layout="Normal" style="Normal">For the velocity on the output gate we get </Text-field></Input></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">v_r[2]:=simplify(subs(v[0]=sol[2],v_rigid[2]));</Font></Text-field></Input><Output><Text-field layout="Maple Output" style="2D Output"><Equation>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</Equation></Text-field></Output></Group><Group><Input><Text-field layout="Normal" style="Normal">We use this derivation later again, so it makes sense to define this in form of a procedure</Text-field></Input></Group><Group><Input><Text-field bookmark="trans" layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">trans:=proc(A,input,R)</Font></Text-field><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">local sol1,sol2,v1,F1,F2,v2,vs2,eq;</Font></Text-field><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">F1:=input[1,1]:</Font></Text-field><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">v1:=input[2,1]:</Font></Text-field><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">sol1:=linsolve(A,input);</Font></Text-field><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">F2:=sol1[1,1];</Font></Text-field><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">v2:=sol1[2,1];</Font></Text-field><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">eq:=F2=R*v2;</Font></Text-field><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">sol2:=simplify(solve(eq,v1));</Font></Text-field><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">vs2:=simplify(subs(v1=sol2,v2));</Font></Text-field><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">end:</Font></Text-field></Input></Group><Group><Input><Text-field layout="Normal" style="Normal">We show the result for the ground velocity graphically</Text-field></Input></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">PErr:=plot(Re(v_r[2]/F[0]),f=0..100,color=red,legend="real part"):</Font></Text-field></Input></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">PEri:=plot(Im(v_r[2]/F[0]),f=0..100,color=green,legend="imaginary part"):</Font></Text-field></Input></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">PEra:=plot(abs(v_r[2]/F[0]),f=0..100,color=blue,thickness=2,legend="absolute value"):</Font></Text-field></Input></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">display(PErr,PEri,PEra,title="Ground Velocity in m/s");</Font></Text-field></Input><Output><Text-field layout="Maple Plot"><Plot height="400" plot-scale="1.0" plot-xtrans="0.0" plot-ytrans="0.0" type="two-dimensional" width="400">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</Plot></Text-field></Output></Group><Group><Input><Text-field layout="Heading 3" style="Heading 3"/><Text-field layout="Heading 3" style="Heading 3">Vibration Isolation by a Spring</Text-field><Text-field layout="Normal" style="Normal">Next we consider the situation that a spring is set between the machine and the ground . Then we have the matrix of the quadripole parameter of the spring with the stiffness</Text-field></Input></Group><Group><Input><Text-field layout="Normal256" prompt="&gt; " style="2D Input"><Equation executable="true" input-equation="k[2]:=10000:" style="2D Input">NiM+JiUia0c2IyIiIyImKysi</Equation></Text-field></Input></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">A[ex]:=subs({sub1,k=k[2]},evalm(A[spring]));</Font></Text-field></Input><Output><Text-field layout="Maple Output" style="2D Output"><Equation>NiM+JkkiQUc2IjYjSSNleEdGJi1JJ21hdHJpeEc2JEkqcHJvdGVjdGVkR0YsSShfc3lzbGliR0YmNiM3JDckIiIiIiIhNyQqKF4jI0YxIiUrXUYxSSNQaUdGLEYxSSJmR0YmRjFGMQ==</Equation></Text-field></Output></Group><Group><Input><Text-field layout="Normal" style="Normal">and the matrix of the quadripole parameter of the serial connection of the vibration source and the spring</Text-field></Input></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">A[2]:=serialconnection(A[s],A[ex]);</Font></Text-field></Input><Output><Text-field layout="Maple Output" style="2D Output"><Equation>NiM+JkkiQUc2IjYjIiIjLUknbWF0cml4RzYkSSpwcm90ZWN0ZWRHRixJKF9zeXNsaWJHRiY2IzckNyQsJiIiIkYyKipeIyNGMiIlK11GMiwmKihJI1BpR0YsRihJImZHRiZGKCwoIigrK0QnRjIqJkY5RihGOkYoISV2XComRjkiIiVGOkZARjIhIiIiJysrRCosXiMhJisrJkYyRjlGMkY6RjIsJiElK0RGMkY9RjJGMkY7RkFGMkYyRjlGMkY6RjJGMkY3NyQqKEY0RjJGOUYyRjpGMkYy</Equation></Text-field></Output></Group><Group><Input><Text-field layout="Normal" style="Normal">We get the velocity at the output gate by use of the <Hyperlink bold="false" executable="false" family="Times New Roman" hyperlink="true" linktarget="Wks:#trans" size="12" style="Hyperlink">above</Hyperlink> defined procedure</Text-field></Input></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">v_s[2]:=trans(A[2],input,R[r]);</Font></Text-field></Input><Output><Text-field layout="Maple Output" style="2D Output"><Equation>NiM+Jkkkdl9zRzYiNiMiIiMsJCoqLC4qJkkjUGlHSSpwcm90ZWN0ZWRHRi4iIilJImZHRiYiIiciJGgkKiZGLSIiJUYwRjQiKSsrXWkqJkYtRjRGMEYoIisrK0RjQSIwKysrK11pIVIiIiIqJkYtRjFGMEY0ISh2ZnoiKiZGLUYoRjBGKCEtKytdUDRKRjlGMEY5JkkiRkdGJjYjIiIhRjksPl4jITQrKysrKytESiY+RjkqJkYtIiIkRjBGRiIvKysrK11pOiooXiMiJytEISpGOUYtIiImRjBGNEY5KiheIyItKysrXWk6RjlGLUY5RjBGKEY5KiheIyEkaCRGOUYtIiIoRjBGMUY5KiZGLUYxRjBGSyIlMD0qJkYtRihGMEZGIiorK103JCooXiMhKSsrXWlGOUYtRkZGMEY0RjkqKEYtRjQiIzUjRjlGKEYwRkYhLisrXWkhPnIqKEYtRjFGZW5GZm5GMEZLIisrK103RSoqXiMiLCsrK3Y9IkY5Ri1GS0ZlbkZmbkYwRjRGOSooRi1GKEZlbkZmbkYwRjkiMSsrKytdUCVbIiooXiMiMSsrKyt2PW4kKkY5Ri1GKEYwRihGOSooXiMhLisrKyt2ViRGOUYtRjRGMEY0RjkhIiIjRjkiJisrJg==</Equation></Text-field></Output></Group><Group><Input><Text-field layout="Normal" style="Normal">The most important point is now the comparison between the velocity in the case of the rigid position of the machine on the ground with the velocity with the spring between machine and ground.</Text-field><Text-field layout="Normal" style="Normal">In blue, the velocity of the case of the rigid connection is displayed.</Text-field></Input></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">PEsa:=plot(abs(v_s[2]/F[0]),f=0..100,color=cyan,thickness=2,legend="absolute value spring"):</Font></Text-field></Input></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">display(PEsa,PEra,title="Ground Velocity in m/s");</Font></Text-field></Input><Output><Text-field layout="Maple Plot"><Plot height="400" plot-scale="1.0" plot-xtrans="0.0" plot-ytrans="0.0" type="two-dimensional" width="400">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</Plot></Text-field></Output></Group><Group><Input><Text-field layout="Normal" style="Normal">Most interesting is normally the question, what is the relation between the absolute value of the velocity at the output gate in case of the rigid support and the isolated support by use of a spring. This is usually shown in a special logarithmic scale. For details please see the literature, for example [1]. We calculate the quotient between the velocity of the ground in case of rigid connection and that in case of supporting by use of any device, here the spring. Then we have to calculate the logarithm and multiply by 20. This result has no physical dimension. It is called the <Font bold="false" executable="false" family="Times New Roman" foreground="[0,0,0]" size="12" style="_cstyle263" underline="false">insertion loss</Font> for the inserted device. To emphasize this kind of presentation, we use the pseudo dimension dB (decibel). Although this property belongs to the inserted device, it depends on the impedance of the vibration source and the impedance of the recipient, here the ground. Strictly speaking, it is not possible to give the insertion loss of a pure device but only in combination with its use.</Text-field><Text-field layout="Normal" style="Normal">Here we calculate the insertion loss of the spring.</Text-field></Input></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">dv_rs:=simplify(20*log[10](abs(v_r[2]/v_s[2])));</Font></Text-field></Input><Output><Text-field layout="Maple Output" style="2D Output"><Equation>NiM+SSZkdl9yc0c2IiwkKiYtSSNsbkc2JEkqcHJvdGVjdGVkR0YrSShfc3lzbGliR0YlNiMtSSRhYnNHRis2IyomLDIqJkkjUGlHRisiIiZJImZHRiUiIiUiJGgkKiZGNCIiI0Y2RjoiLisrKyt2ViQqJkY0IiIiRjZGOiIpKytdaSooXiMhLisrKytEYyJGPUY0Rj1GNkY9Rj0hMCsrKysrRCJ5Rj0qKl4jIisrK103RUY9RjRGNyIjNSNGPUY6RjYiIiRGPSooRkZGR0Y0RkhGNkY6IisrK10oPSIqKl4jIS0rKytdUGZGPUY0RjpGRkZHRjZGPUY9Rj0sMkYzRjhGOSItKysrK0RKRjxGPkY/Rj1GQkY9KipeIyIqKytdUCNGPUY0RjdGRkZHRjZGSEY9RklGSkZLRj0hIiJGPSwmLUYpNiNGOkY9LUYpNiNGNUY9RlMiIz8=</Equation></Text-field></Output></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">PErsa:=plot(dv_rs,f=0..100,color=cyan,legend="spring",title="Insertion Loss in dB",thickness=2):</Font></Text-field></Input></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">display(PErsa);</Font></Text-field></Input><Output><Text-field layout="Maple Plot"><Plot height="400" plot-scale="1.0" plot-xtrans="0.0" plot-ytrans="0.0" type="two-dimensional" width="400">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</Plot></Text-field></Output></Group><Group><Input><Text-field layout="Heading 3" style="Heading 3"/><Text-field layout="Heading 3" style="Heading 3">Vibration Isolation by a Damper</Text-field><Text-field layout="Normal" style="Normal">Next we consider the situation that a damper is set between the machine and the ground . Of course this idea is more theoretically interesting, because the damper itself cannot carry the static load of a machine. In reality there must be some device that can do that. </Text-field><Text-field layout="Normal" style="Normal">We have the matrix of the quadripole parameter of the damper with the damping residence</Text-field></Input></Group><Group><Input><Text-field layout="Normal256" prompt="&gt; " style="2D Input"><Equation executable="true" input-equation="d[3]:=30:" style="2D Input">NiM+JiUiZEc2IyIiJCIjSQ==</Equation></Text-field></Input></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">A[fx]:=subs({sub1,d=d[3]},evalm(A[damper]));</Font></Text-field></Input><Output><Text-field layout="Maple Output" style="2D Output"><Equation>NiM+JkkiQUc2IjYjSSNmeEdGJi1JJ21hdHJpeEc2JEkqcHJvdGVjdGVkR0YsSShfc3lzbGliR0YmNiM3JDckIiIiIiIhNyQjRjEiI0lGMQ==</Equation></Text-field></Output></Group><Group><Input><Text-field layout="Normal" style="Normal">and the matrix of the quadripole parameter of the serial connection of the vibration source and the damper</Text-field></Input></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">A[3]:=serialconnection(A[s],A[fx]);</Font></Text-field></Input><Output><Text-field layout="Maple Output" style="2D Output"><Equation>NiM+JkkiQUc2IjYjIiIkLUknbWF0cml4RzYkSSpwcm90ZWN0ZWRHRixJKF9zeXNsaWJHRiY2IzckNyQsKCIiIkYyKihJI1BpR0YsIiIjSSJmR0YmRjUsKCIoKytEJ0YyKiZGNEY1RjZGNSEldlwqJkY0IiIlRjZGPEYyISIiIyImK10jRigqLF4jIyElK11GKEYyRjRGMkY2RjIsJiElK0RGMkY5RjJGMkY3Rj1GMiwmRjMiJysrRCosXiMhJisrJkYyRjRGMkY2RjJGREYyRjdGPUYyNyQjRjIiI0lGMg==</Equation></Text-field></Output></Group><Group><Input><Text-field layout="Normal" style="Normal">We get the velocity at the output gate by use of the <Hyperlink bold="false" executable="false" family="Times New Roman" hyperlink="true" linktarget="Wks:#trans" size="12" style="Hyperlink">above</Hyperlink> defined procedure</Text-field></Input></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">v_d[2]:=trans(A[3],input,R[r]);</Font></Text-field></Input><Output><Text-field layout="Maple Output" style="2D Output"><Equation>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</Equation></Text-field></Output></Group><Group><Input><Text-field layout="Normal" style="Normal">The following diagram shows the ground velocities for all the previously considered situations</Text-field></Input></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">PEda:=plot(abs(v_d[2]/F[0]),f=0..100,color=magenta,thickness=2,legend="absolute value damper"):</Font></Text-field></Input></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">display(PEda,PEsa,PEra,title="Ground Velocity in m/s");</Font></Text-field></Input><Output><Text-field layout="Maple Plot"><Plot height="400" plot-scale="1.0" plot-xtrans="0.0" plot-ytrans="0.0" type="two-dimensional" width="400">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</Plot></Text-field></Output></Group><Group><Input><Text-field layout="Normal" style="Normal">Again we calculate the insertion loss of the damper</Text-field></Input></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">dv_rd:=simplify(20*log[10](abs(v_r[2]/v_d[2])));</Font></Text-field></Input><Output><Text-field layout="Maple Output" style="2D Output"><Equation>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</Equation></Text-field></Output></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">PErda:=plot(abs(dv_rd),f=0..100,color=magenta,legend="damper",title="Insertion Loss in dB",thickness=2):</Font></Text-field></Input></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">display(PErda,PErsa);</Font></Text-field></Input><Output><Text-field layout="Maple Plot"><Plot height="400" plot-scale="1.0" plot-xtrans="0.0" plot-ytrans="0.0" type="two-dimensional" width="400">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</Plot></Text-field></Output></Group><Group><Input><Text-field layout="Normal" style="Normal">It seems that the damper, especially in the range of lower frequencies, gives the better reduction of the vibration. Only for higher frequencies, in this example from about 50 Hz, the spring support yields a higher insertion loss than the spring. Unfortunately the damper itself cannot carry the static load, so we need something as a spring. Let's consider what happens when we use a combination of a spring and a damper.</Text-field></Input></Group><Group><Input><Text-field layout="Heading 3" style="Heading 3"/><Text-field layout="Heading 3" style="Heading 3">Vibration Isolation by a KELVIN-VOIGT Device</Text-field><Text-field layout="Normal" style="Normal">Next we consider the situation that a combination of a spring and a damper according the KELVIN-VOIGT model is set between the machine and the ground . Then we have the matrix of the quadripole parameter of the device with the spring stiffness <Equation input-equation="k[2]" style="2D Comment">NiMmJSJrRzYjIiIj</Equation> and the damping residence <Equation input-equation="d[3]" style="2D Comment">NiMmJSJkRzYjIiIk</Equation>.</Text-field></Input></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">A[gx]:=subs({sub1,d=d[3],k=k[2]},evalm(A[KELVINVOIGT]));</Font></Text-field></Input><Output><Text-field layout="Maple Output" style="2D Output"><Equation>NiM+JkkiQUc2IjYjSSNneEdGJi1JJ21hdHJpeEc2JEkqcHJvdGVjdGVkR0YsSShfc3lzbGliR0YmNiM3JDckIiIiIiIhNyQsJCooSSNQaUdGLEYxSSJmR0YmRjEsJiomRjZGMUY3RjEhI2deIyImKysiRjEhIiIhIiNGMQ==</Equation></Text-field></Output></Group><Group><Input><Text-field layout="Normal" style="Normal">and the matrix of the quadripole parameter of the serial connection of the vibration source and the KELVIN-VOIGT device is</Text-field></Input></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">A[4]:=serialconnection(A[s],A[gx]);</Font></Text-field></Input><Output><Text-field layout="Maple Output" style="2D Output"><Equation>NiM+JkkiQUc2IjYjIiIlLUknbWF0cml4RzYkSSpwcm90ZWN0ZWRHRixJKF9zeXNsaWJHRiY2IzckNyQsJiIiIkYyKiosJiooSSNQaUdGLCIiI0kiZkdGJkY3LCgiKCsrRCdGMiomRjZGN0Y4RjchJXZcKiZGNkYoRjhGKEYyISIiIicrK0QqLF4jISYrKyZGMkY2RjJGOEYyLCYhJStERjJGO0YyRjJGOUY+RjJGMkY2RjJGOEYyLCYqJkY2RjJGOEYyISNnXiMiJisrIkYyRj4hIiNGNDckLCQqKEY2RjJGOEYyRkVGPkZKRjI=</Equation></Text-field></Output></Group><Group><Input><Text-field layout="Normal" style="Normal">We get again the velocity at the output gate by use of the <Hyperlink bold="false" executable="false" family="Times New Roman" hyperlink="true" linktarget="Wks:#trans" size="12" style="Hyperlink">above</Hyperlink> defined procedure</Text-field></Input></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">v_KV[2]:=trans(A[4],input,R[r]);</Font></Text-field></Input><Output><Text-field layout="Maple Output" style="2D Output"><Equation>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</Equation></Text-field></Output></Group><Group><Input><Text-field layout="Normal" style="Normal">The following diagram shows the ground velocities</Text-field></Input></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">PEKVa:=plot(abs(v_KV[2]/F[0]),f=0..100,color=brown,thickness=2,legend="absolute value KELVIN-VOIGT"):</Font></Text-field></Input></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">display(PEKVa,PEda,PEsa,PEra,title="Ground Velocity in m/s");</Font></Text-field></Input><Output><Text-field layout="Maple Plot"><Plot height="400" plot-scale="1.0" plot-xtrans="0.0" plot-ytrans="0.0" type="two-dimensional" width="400">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</Plot></Text-field></Output></Group><Group><Input><Text-field layout="Normal" style="Normal">Again we calculate the insertion loss of the device</Text-field></Input></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">dv_rKV:=simplify(20*log[10](abs(v_r[2]/v_KV[2])));</Font></Text-field></Input><Output><Text-field layout="Maple Output" style="2D Output"><Equation>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</Equation></Text-field></Output></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">PErKVa:=plot(dv_rKV,f=0..100,color=brown,legend="KELVIN-VOIGT",title="Insertion Loss in dB",thickness=2):</Font></Text-field></Input></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">display(PErKVa,PErda,PErsa);</Font></Text-field></Input><Output><Text-field layout="Maple Plot"><Plot height="400" plot-scale="1.0" plot-xtrans="0.0" plot-ytrans="0.0" type="two-dimensional" width="400">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</Plot></Text-field></Output></Group><Group><Input><Text-field layout="Normal" style="Normal">As expected this solution is somewhere between the support by a spring and the support by a damper. The advantage of the KELVIN-VOIGT device against the single spring is the fact that there is not so big an incursion in the insertion loss.</Text-field></Input></Group><Group><Input><Text-field layout="Heading 3" style="Heading 3"/><Text-field layout="Heading 3" style="Heading 3">Vibration Isolation by a MAXWELL Device</Text-field><Text-field layout="Normal" style="Normal">Next we consider the situation that a combination of a spring and a damper according the MAXWELL model with the spring stiffness <Equation input-equation="k[2]" style="2D Comment">NiMmJSJrRzYjIiIj</Equation> and the damping residence <Equation input-equation="d[3]" style="2D Comment">NiMmJSJkRzYjIiIk</Equation> is set between the machine and the ground . As with the single damper, this device cannot carry static loads and is not capable for practical use of supporting a machine.</Text-field><Text-field layout="Normal" style="Normal">We have the matrix of the quadripole parameter of the device</Text-field></Input></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">A[hx]:=subs({sub1,d=d[3],k=k[2]},evalm(A[MAXWELL]));</Font></Text-field></Input><Output><Text-field layout="Maple Output" style="2D Output"><Equation>NiM+JkkiQUc2IjYjSSNoeEdGJi1JJ21hdHJpeEc2JEkqcHJvdGVjdGVkR0YsSShfc3lzbGliR0YmNiM3JDckIiIiIiIhNyQsJiNGMSIjSUYxKiheIyNGMSIlK11GMUkjUGlHRixGMUkiZkdGJkYxRjFGMQ==</Equation></Text-field></Output></Group><Group><Input><Text-field layout="Normal" style="Normal">and the matrix of the quadripole parameter of the serial connection of the vibration source and the spring</Text-field></Input></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">A[5]:=serialconnection(A[s],A[hx]);</Font></Text-field></Input><Output><Text-field layout="Maple Output" style="2D Output"><Equation>NiM+JkkiQUc2IjYjIiImLUknbWF0cml4RzYkSSpwcm90ZWN0ZWRHRixJKF9zeXNsaWJHRiY2IzckNyQsJiIiIkYyKiYsJiooSSNQaUdGLCIiI0kiZkdGJkY3LCgiKCsrRCdGMiomRjZGN0Y4RjchJXZcKiZGNiIiJUY4Rj5GMiEiIiInKytEKixeIyEmKysmRjJGNkYyRjhGMiwmISUrREYyRjtGMkYyRjlGP0YyRjIsJiNGMiIjSUYyKiheIyNGMiIlK11GMkY2RjJGOEYyRjJGMkYyRjQ3JEZGRjI=</Equation></Text-field></Output></Group><Group><Input><Text-field layout="Normal" style="Normal">The velocity at the output gate is now</Text-field></Input></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">v_MW[2]:=trans(A[5],input,R[r]);</Font></Text-field></Input><Output><Text-field layout="Maple Output" style="2D Output"><Equation>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</Equation></Text-field></Output></Group><Group><Input><Text-field layout="Normal" style="Normal">The following diagram shows the ground velocities</Text-field></Input></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">PEMWa:=plot(abs(v_MW[2]/F[0]),f=0..100,color=green,thickness=2,legend="absolute value MAXWELL"):</Font></Text-field></Input></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">display(PEMWa,PEKVa,PEda,PEsa,PEra,title="Ground Velocity in m/s");</Font></Text-field></Input><Output><Text-field layout="Maple Plot"><Plot height="400" plot-scale="1.0" plot-xtrans="0.0" plot-ytrans="0.0" type="two-dimensional" 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layout="Normal" style="Normal">We calculate the insertion loss of the device</Text-field></Input></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">dv_rMW:=simplify(20*log[10](abs(v_r[2]/v_MW[2])));</Font></Text-field></Input><Output><Text-field layout="Maple Output" style="2D 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size="12" underline="false">display(PErMWa,PErKVa,PErda,PErsa);</Font></Text-field></Input><Output><Text-field layout="Maple Plot"><Plot height="400" plot-scale="1.0" plot-xtrans="0.0" plot-ytrans="0.0" type="two-dimensional" 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layout="Normal" style="Normal">Up to now this model is the best one for elimating ground vibrations.  Unfortunately it cannot be used because it cannot carry static loads.</Text-field></Input></Group><Group><Input><Text-field layout="Heading 3" style="Heading 3"/><Text-field layout="Heading 3" style="Heading 3">Vibration Isolation by Double Spring Device with one Damper</Text-field><Text-field layout="Normal" style="Normal">Next we consider the situation that a combination of a spring, an additional mass and a second spring in series and parallel to this damper is set between the machine and the ground . This device is shown in Figure 17.</Text-field><Text-field alignment="centred"><Image height="252" 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ggGumxfIpl?`pJ_fTFn@>aRAcigpbYev@ikPytqfMHvXX^OotLpH=tAwhSQGaOYB?eDyiriri;eRMutov_aRsse;gudgTegfEudXmXMOg^GenWXIuSlkwu_WSQHXKYUqhgeduaGKowKhLYTJjUqpewFISitR@dY@lPLXP\\LN<]U?DOAHScTkXdqittYYqquOIiqTepdETKETLHvDYTpaxyilqIvthqJyvwAMjxs:qPZPMe\\semOoPwh@S[UNCiKXqUryq_TSP`PwHuOXXWxO:qXWqOd`nlmV@uXtMqt@qLQMsXnV=JW`PgiUwtRDArNptjdTwQxExmgHsX=qjEVxIq\\uVhtRd=paAksajC@nvEOMeO<YKoYwGmogHXmaqYTJpiNaUQSHs>esvdwwMmwtuLLO`uM<xLLHV>po;AuuIlZUmhYlI@s<hW;qp^Erp`F::::=hgCUjgGS::::>fUOpZWel<::IY:MwRigx=XQygYut`CwvMtc?FYIbgMCd?gC=GAQG>uV;qC:MioUwPitewT;AUOQTEkDf;C^aEaybyHNIutWTxIMTsTsUtPh]n^`n>dJ?dvMpqHxy=PK_\\Xp@W;qkr<J:>ZCgbH_bhPbZO6J</Image></Text-field><Text-field layout="Normal256" style="Normal256">Figure 17</Text-field><Text-field layout="Normal" style="Normal">The spring stiffness  shall be</Text-field></Input></Group><Group><Input><Text-field layout="Normal256" prompt="&gt; " style="2D Input"><Equation executable="true" input-equation="k[a6]:=2*k[2];" style="2D Input">NiM+JiUia0c2IyUjYTZHKiYiIiMiIiImRiU2I0YpRio=</Equation></Text-field></Input><Output><Text-field layout="Maple Output" style="2D Output"><Equation>NiM+Jkkia0c2IjYjSSNhNkdGJiImKysj</Equation></Text-field></Output></Group><Group><Input><Text-field layout="Normal256" prompt="&gt; " style="2D Input"><Equation executable="true" input-equation="k[b6]:=2*k[2];" style="2D Input">NiM+JiUia0c2IyUjYjZHKiYiIiMiIiImRiU2I0YpRio=</Equation></Text-field></Input><Output><Text-field layout="Maple Output" style="2D Output"><Equation>NiM+Jkkia0c2IjYjSSNiNkdGJiImKysj</Equation></Text-field></Output></Group><Group><Input><Text-field layout="Normal" style="Normal">and the damping resistance is again <Equation input-equation="d[3]" style="2D Comment">NiMmJSJkRzYjIiIk</Equation>.</Text-field></Input></Group><Group><Input><Text-field layout="Normal" style="Normal">The mass shall be</Text-field></Input></Group><Group><Input><Text-field layout="Normal256" prompt="&gt; " style="2D Input"><Equation executable="true" input-equation="m[6]:=1:" style="2D Input">NiM+JiUibUc2IyIiJyIiIg==</Equation></Text-field></Input></Group><Group><Input><Text-field layout="Normal" style="Normal">The matrices of the single quadripole parameter are</Text-field><Text-field layout="Normal" style="Normal">first spring:</Text-field></Input></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">Am:=subs(k=k[a6],evalm(A[spring]));</Font></Text-field></Input><Output><Text-field layout="Maple Output" style="2D Output"><Equation>NiM+SSNBbUc2Ii1JJ21hdHJpeEc2JEkqcHJvdGVjdGVkR0YpSShfc3lzbGliR0YlNiM3JDckIiIiIiIhNyQqJl4jI0YuIiYrKyNGLkkmT21lZ2FHRiVGLkYu</Equation></Text-field></Output></Group><Group><Input><Text-field layout="Normal" style="Normal">mass</Text-field></Input></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">An:=subs(m=m[6],evalm(A[mass]));</Font></Text-field></Input><Output><Text-field layout="Maple Output" style="2D Output"><Equation>NiM+SSNBbkc2Ii1JJ21hdHJpeEc2JEkqcHJvdGVjdGVkR0YpSShfc3lzbGliR0YlNiM3JDckIiIiKiZeI0YuRi5JJk9tZWdhR0YlRi43JCIiIUYu</Equation></Text-field></Output></Group><Group><Input><Text-field layout="Normal" style="Normal">second spring</Text-field></Input></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">Ao:=subs(k=k[b6],evalm(A[spring]));</Font></Text-field></Input><Output><Text-field layout="Maple Output" style="2D Output"><Equation>NiM+SSNBb0c2Ii1JJ21hdHJpeEc2JEkqcHJvdGVjdGVkR0YpSShfc3lzbGliR0YlNiM3JDckIiIiIiIhNyQqJl4jI0YuIiYrKyNGLkkmT21lZ2FHRiVGLkYu</Equation></Text-field></Output></Group><Group><Input><Text-field layout="Normal" style="Normal">damper</Text-field></Input></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">Ap:=subs(d=d[3],evalm(A[damper]));</Font></Text-field></Input><Output><Text-field layout="Maple Output" style="2D Output"><Equation>NiM+SSNBcEc2Ii1JJ21hdHJpeEc2JEkqcHJvdGVjdGVkR0YpSShfc3lzbGliR0YlNiM3JDckIiIiIiIhNyQjRi4iI0lGLg==</Equation></Text-field></Output></Group><Group><Input><Text-field layout="Normal" style="Normal">The matrix of the quadripole parameter of the serial connection of the spring, the mass and the second spring is</Text-field></Input></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">Amno:=serialconnection(Am,An,Ao);</Font></Text-field></Input><Output><Text-field layout="Maple Output" style="2D Output"><Equation>NiM+SSVBbW5vRzYiLUknbWF0cml4RzYkSSpwcm90ZWN0ZWRHRilJKF9zeXNsaWJHRiU2IzckNyQsJiokSSZPbWVnYUdGJSIiIyMhIiIiJisrIyIiIkY1KiZeI0Y1RjVGMEY1NyQsJiomXiMjRjVGNEY1RjBGNUY1KihGO0Y1Ri5GNUYwRjVGNUYu</Equation></Text-field></Output></Group><Group><Input><Text-field layout="Normal" style="Normal">And the parallel connection from this with the damper is</Text-field></Input></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">Amnop:=parallelconnection(Amno,Ap);</Font></Text-field></Input><Output><Text-field layout="Maple Output" style="2D Output"><Equation>NiM+SSZBbW5vcEc2Ii1JJ21hdHJpeEc2JEkqcHJvdGVjdGVkR0YpSShfc3lzbGliR0YlNiM3JDckKiYsKiomXiMhJSs/IiIiSSZPbWVnYUdGJSIiI0YzXiMiKSsrK1NGM0Y0IScrKzcqJEY0IiIkRjpGMywoRjZGM0Y0RjhGOUY6ISIiKiYsJiomXiNGOEYzRjRGNUYzRjQhKSsrK1NGM0Y7Rjw3JCwkKiZGO0Y8LCZGNCEmKyslRjlGM0YzI0YzIiM1LCQqJkY7RjwsKl4jIiorKysrJUYzRjQhKCsrPyJGOSIjSSomXiMhJisrI0YzRjRGNUYzRjNGRw==</Equation></Text-field></Output></Group><Group><Input><Text-field layout="Normal" style="Normal">This yields with the source in series</Text-field></Input></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">A[6]:=subs(sub1,serialconnection(A[s],Amnop));</Font></Text-field></Input><Output><Text-field layout="Maple Output" style="2D Output"><Equation>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</Equation></Text-field></Output></Group><Group><Input><Text-field layout="Normal" style="Normal">The velocity at the output gate is</Text-field></Input></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">v_m[2]:=trans(A[6],input,R[r]);</Font></Text-field></Input><Output><Text-field layout="Maple Output" style="2D Output"><Equation>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</Equation></Text-field></Output></Group><Group><Input><Text-field layout="Normal" style="Normal">The following diagram shows the ground velocities for all the up to now  situations</Text-field></Input></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">PEma:=plot(abs(v_m[2]/F[0]),f=0..100,color=red,thickness=2,legend="absolute value double spring with one damper"):</Font></Text-field></Input></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">display(PEma,PEMWa,PEKVa,PEda,PEsa,PEra,title="Ground Velocity in m/s");</Font></Text-field></Input><Output><Text-field layout="Maple Plot"><Plot height="400" plot-scale="1.0" plot-xtrans="0.0" plot-ytrans="0.0" type="two-dimensional" 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layout="Normal" style="Normal">We calculate the insertion loss of the device</Text-field></Input></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">dv_rm:=simplify(20*log[10](abs(v_r[2]/v_m[2])));</Font></Text-field></Input><Output><Text-field layout="Maple Output" style="2D Output"><Equation>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</Equation></Text-field></Output></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">PErma:=plot(dv_rm,f=0..100,color=red,legend="double elastic support",title="Insertion Loss in dB",thickness=2):</Font></Text-field></Input></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">display(PErma,PErMWa,PErKVa,PErda,PErsa);</Font></Text-field><Text-field layout="Normal" style="Normal">This devise is not so easy to classify, because to do this we must consider a lot of different combinations of spring stiffness, damping resistances and Additionally masses. The combination we used in this example seems not to be a very good solution.</Text-field></Input><Output><Text-field layout="Maple Plot"><Plot height="400" plot-scale="1.0" plot-xtrans="0.0" plot-ytrans="0.0" type="two-dimensional" 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layout="Heading 3" style="Heading 3"/><Text-field layout="Heading 3" style="Heading 3">Vibration Isolation by Double Spring-Damper Device</Text-field><Text-field layout="Normal" style="Normal">Next we consider the situation that a combination of a KELVIN-VOIGT device, an additional mass and a second KELVIN-VOIGT device in series is set between the machine and the ground  as shown in Figure 18. </Text-field><Text-field alignment="centred"><Image height="336" 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layout="Normal256" style="Normal256">Figure 18</Text-field><Text-field layout="Normal" style="Normal">The spring stiffness shall be</Text-field></Input></Group><Group><Input><Text-field layout="Normal256" prompt="&gt; " style="2D Input"><Equation executable="true" input-equation="k[a7] := 2*k[2];" style="2D Input">NiM+JiUia0c2IyUjYTdHKiYiIiMiIiImRiU2I0YpRio=</Equation></Text-field></Input><Output><Text-field layout="Maple Output" style="2D Output"><Equation>NiM+Jkkia0c2IjYjSSNhN0dGJiImKysj</Equation></Text-field></Output></Group><Group><Input><Text-field layout="Normal256" prompt="&gt; " style="2D Input"><Equation executable="true" input-equation="k[b7]:=2*k[2];" style="2D Input">NiM+JiUia0c2IyUjYjdHKiYiIiMiIiImRiU2I0YpRio=</Equation></Text-field></Input><Output><Text-field layout="Maple Output" style="2D Output"><Equation>NiM+Jkkia0c2IjYjSSNiN0dGJiImKysj</Equation></Text-field></Output></Group><Group><Input><Text-field layout="Normal" style="Normal">and the damping resistance is</Text-field></Input></Group><Group><Input><Text-field layout="Normal256" prompt="&gt; " style="2D Input"><Equation executable="true" input-equation="d[a7]:=2*d[3];" style="2D Input">NiM+JiUiZEc2IyUjYTdHKiYiIiMiIiImRiU2IyIiJEYq</Equation></Text-field></Input><Output><Text-field layout="Maple Output" style="2D Output"><Equation>NiM+JkkiZEc2IjYjSSNhN0dGJiIjZw==</Equation></Text-field></Output></Group><Group><Input><Text-field layout="Normal256" prompt="&gt; " style="2D Input"><Equation executable="true" input-equation="d[b7]:=2*d[3];" style="2D Input">NiM+JiUiZEc2IyUjYjdHKiYiIiMiIiImRiU2IyIiJEYq</Equation></Text-field></Input><Output><Text-field layout="Maple Output" style="2D Output"><Equation>NiM+JkkiZEc2IjYjSSNiN0dGJiIjZw==</Equation></Text-field></Output></Group><Group><Input><Text-field layout="Normal" style="Normal">The mass shall be</Text-field></Input></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">m[7]:=1;</Font></Text-field></Input><Output><Text-field layout="Maple Output" style="2D Output"><Equation>NiM+JkkibUc2IjYjIiIoIiIi</Equation></Text-field></Output></Group><Group><Input><Text-field layout="Normal" style="Normal">The matrices of the single quadripole parameter are</Text-field><Text-field layout="Normal" style="Normal">first KELVIN-VOIGT device:</Text-field></Input></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">Aq:=subs({k=k[a7],d=d[a7]},evalm(A[KELVINVOIGT]));</Font></Text-field></Input><Output><Text-field layout="Maple Output" style="2D Output"><Equation>NiM+SSNBcUc2Ii1JJ21hdHJpeEc2JEkqcHJvdGVjdGVkR0YpSShfc3lzbGliR0YlNiM3JDckIiIiIiIhNyQsJComSSZPbWVnYUdGJUYuLCZGMyEjZ14jIiYrKyNGLiEiIkY4Ri4=</Equation></Text-field></Output></Group><Group><Input><Text-field layout="Normal" style="Normal">mass</Text-field></Input></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">Ar:=subs(m=m[7],evalm(A[mass]));</Font></Text-field></Input><Output><Text-field layout="Maple Output" style="2D Output"><Equation>NiM+SSNBckc2Ii1JJ21hdHJpeEc2JEkqcHJvdGVjdGVkR0YpSShfc3lzbGliR0YlNiM3JDckIiIiKiZeI0YuRi5JJk9tZWdhR0YlRi43JCIiIUYu</Equation></Text-field></Output></Group><Group><Input><Text-field layout="Normal" style="Normal">second KELVIN-VOIGT device</Text-field></Input></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">As:=subs({k=k[b7],d=d[b7]},evalm(A[KELVINVOIGT]));</Font></Text-field></Input><Output><Text-field layout="Maple Output" style="2D Output"><Equation>NiM+SSNBc0c2Ii1JJ21hdHJpeEc2JEkqcHJvdGVjdGVkR0YpSShfc3lzbGliR0YlNiM3JDckIiIiIiIhNyQsJComSSZPbWVnYUdGJUYuLCZGMyEjZ14jIiYrKyNGLiEiIkY4Ri4=</Equation></Text-field></Output></Group><Group><Input><Text-field layout="Normal" style="Normal">The matrix of the quadripole parameter of the serial connection of the fist KELVIN-VOIGT device, mass and the second  KELVIN-VOIGT device is</Text-field></Input></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">Aqrs:=serialconnection(Aq,Ar,As);</Font></Text-field></Input><Output><Text-field layout="Maple Output" style="2D Output"><Equation>NiM+SSVBcXJzRzYiLUknbWF0cml4RzYkSSpwcm90ZWN0ZWRHRilJKF9zeXNsaWJHRiU2IzckNyQsJiooXiMhIiIiIiJJJk9tZWdhR0YlIiIjLCZGMyEjZ14jIiYrKyNGMkYxRjJGMkYyKiZeI0YyRjJGM0YyNyQsJiomRjNGMkY1RjFGMSooRi5GMkYzRjJGNUYxRjFGLg==</Equation></Text-field></Output></Group><Group><Input><Text-field layout="Normal" style="Normal">This yields with the source in series</Text-field></Input></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">A[7]:=subs(sub1,serialconnection(A[s],Aqrs));</Font></Text-field></Input><Output><Text-field layout="Maple Output" style="2D Output"><Equation>NiM+JkkiQUc2IjYjIiIoLUknbWF0cml4RzYkSSpwcm90ZWN0ZWRHRixJKF9zeXNsaWJHRiY2IzckNyQsKCoqXiMhIiUiIiJJI1BpR0YsIiIjSSJmR0YmRjcsJiomRjZGNUY4RjUhJD8iXiMiJisrI0Y1ISIiRjVGNUY1KiYsJiooRjZGN0Y4RjcsKCIoKytEJ0Y1KiZGNkY3RjhGNyEldlwqJkY2IiIlRjhGR0Y1Rj4iJysrRCosXiMhJisrJkY1RjZGNUY4RjUsJiElK0RGNUZERjVGNUZCRj5GNUY1LCYqKEY2RjVGOEY1RjlGPiEiIyoqLCZGMkY1RjVGNUY1RjZGNUY4RjVGOUY+RlBGNUY1LCYqKF4jRjdGNUY2RjVGOEY1RjUqJkZARjVGUkY1RjU3JEZORlI=</Equation></Text-field></Output></Group><Group><Input><Text-field layout="Normal" style="Normal">The velocity at the output gate is</Text-field></Input></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">v_z[2]:=trans(A[7],input,R[r]);</Font></Text-field></Input><Output><Text-field layout="Maple Output" style="2D Output"><Equation>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</Equation></Text-field></Output></Group><Group><Input><Text-field layout="Normal" style="Normal">The following diagram shows the ground velocities</Text-field></Input></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">PEza:=plot(abs(v_z[2]/F[0]),f=0..100,color=maroon,thickness=2,legend="absolute value double spring-damper device"):</Font></Text-field></Input></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">display(PEza,PEma,PEMWa,PEKVa,PEda,PEsa,PEra,title="Ground Velocity in m/s");</Font></Text-field></Input><Output><Text-field layout="Maple Plot"><Plot height="400" plot-scale="1.0" plot-xtrans="0.0" plot-ytrans="0.0" type="two-dimensional" 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layout="Normal" style="Normal">We calculate the insertion loss of the device</Text-field></Input></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">dv_rz:=simplify( 20*log[10](abs(v_r[2]/v_z[2])) ):</Font>
</Text-field></Input></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">PErza:=plot(dv_rz,f=0..100,color=maroon,legend="double spring-damper device",title="Insertion Loss in dB",thickness=2):</Font></Text-field></Input></Group><Group><Input><Text-field layout="Normal" prompt="&gt; " style="Maple Input"><Font italic="false" size="12" underline="false">display(PErza,PErma,PErMWa,PErKVa,PErda,PErsa);</Font></Text-field></Input><Output><Text-field layout="Maple Plot"><Plot height="400" plot-scale="1.0" plot-xtrans="0.0" plot-ytrans="0.0" type="two-dimensional" 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layout="Normal" prompt="&gt; " style="Maple Input"/></Input></Group><Group><Input><Text-field layout="Normal" style="Normal">Consider that this device has the same additional mass as the device above. The only difference between both models is the fact that the damper here is divided in two, just as the spring, so the motion of the additional mass is directly damped in this model. The advantage is easy to see in the insertion loss. We get with this device for frequencies higher than about 60 Hz the best values for the insertion loss. Such devices are often used for the isolation of machines in very sensitive areas, for example, in ships. The vibration of the motor of a ship otherwise can easily be transmitted through all the ship.</Text-field><Text-field layout="Normal" style="Normal"/><Text-field layout="Normal" style="Normal">But once again: Remember that all numerical values are only academic examples. Real devises have more complicated properties than we can show here. For exdample, the spring itself is a mass, every real damper has a certain stiffness, and I don't believe that one can find in reality a vibration source with such a simple form of the impedancethe as described here .</Text-field></Input></Group><Group><Input><Text-field layout="Heading 1" style="Heading 1">Literature</Text-field><Text-field layout="Normal" style="Normal"><Font encoding="ISO8859-1">[1] M. Heckl, H.A. M\374ller, </Font><Font bold="false" executable="false" family="Times New Roman" foreground="[0,0,0]" size="12" style="_cstyle256" underline="false">Taschenbuch der Technischen Akustik</Font>, p. 571-595, Springer-Verlag, 2nd Edition, Berlin 1994</Text-field><Text-field layout="Normal" style="Normal">[2] E. Seidel, <Font bold="false" encoding="ISO8859-1" executable="false" family="Times New Roman" foreground="[0,0,0]" size="12" style="_cstyle258" underline="false">Wirksamkeit von Konstruktionen zur Schwingungs- und K\366rperschalld\344mmung in Maschinen und Ger\344ten</Font><Font encoding="ISO8859-1">, Schriftenreihe der Bundesanstalt f\374r Arbeitsschutz und Arbeitsmedizin, Dortmund/Berlin 1999</Font></Text-field></Input></Group><Text-field/><Text-field/><Text-field/></Worksheet>