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author | priyanka | 2015-06-24 15:03:17 +0530 |
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committer | priyanka | 2015-06-24 15:03:17 +0530 |
commit | b1f5c3f8d6671b4331cef1dcebdf63b7a43a3a2b (patch) | |
tree | ab291cffc65280e58ac82470ba63fbcca7805165 /29/CH6/EX6.10.10/exa6_10_10.sce | |
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initial commit / add all books
Diffstat (limited to '29/CH6/EX6.10.10/exa6_10_10.sce')
-rwxr-xr-x | 29/CH6/EX6.10.10/exa6_10_10.sce | 48 |
1 files changed, 48 insertions, 0 deletions
diff --git a/29/CH6/EX6.10.10/exa6_10_10.sce b/29/CH6/EX6.10.10/exa6_10_10.sce new file mode 100755 index 000000000..27bf1d5f4 --- /dev/null +++ b/29/CH6/EX6.10.10/exa6_10_10.sce @@ -0,0 +1,48 @@ +//caption:determine_transfer_function,Wn,zeta
+//example 6.10.10
+//page 179
+//J=moment of inertia,f=C,Ke=error detector gain,Wn=natural frequency, zeta=damping ratio,Km=torque constant
+syms J f s
+Ke=5.73;
+Km=0.045;
+n=sym('N1/N2')
+n=subs(n,'N1/N2',1/10);
+J=0.25*float(n^2);//referred to motor side
+f=1*float(n^2);//referred to motor side
+//from the block diagram given in fig 6.10.6 on page 179,
+a=(Ke*Km)
+b=1/(J*s^2+f*s)
+c=(b*float(a))
+G=(n*c);
+G=simple(G)
+H=1;
+d=(1+G*H);
+d=simple(d);
+CL=G/d;
+CL=simple(CL)
+disp(CL,"C(s)/R(s)=");
+e=poly([328800 127516 31879],'s','coeff')
+printf("the characterstics eq. is:\n");
+disp(e);
+f=coeff(e)
+Wn=sqrt((f(1,1)/f(1,3)))//natural_frequency
+zeta=((f(1,2)/f(1,3))/(2*Wn))//damping ratio
+//part(b)
+syms Td
+g=1+s*Td
+h=(g*G)
+i=1+h*H
+i=simple(i);
+CL2=(h/i)
+CL2=simple(CL2);
+disp(CL2,"C(s)/R(s)=");
+poly(0,'s');
+l=s^2+(10.32*Td+4)*s+10.32;
+printf("on simplyfying the characterstics eq. is:");
+disp(float(l));
+Wn1=sqrt(10.32)//natural_frequency
+//2*zeta1*Wn1=10.32*Td+4
+zeta1=1;//as damping is critical
+Td=(2*zeta1*Wn1-4)/10.32;
+disp(Td,"time const. of advanced phase circuit,Td=");
+
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