diff options
Diffstat (limited to '269')
109 files changed, 553 insertions, 0 deletions
diff --git a/269/CH1/EX1.1/ex.jpeg b/269/CH1/EX1.1/ex.jpeg Binary files differnew file mode 100644 index 000000000..73d76e958 --- /dev/null +++ b/269/CH1/EX1.1/ex.jpeg diff --git a/269/CH1/EX1.1/ex.sce b/269/CH1/EX1.1/ex.sce new file mode 100644 index 000000000..2d6cdd030 --- /dev/null +++ b/269/CH1/EX1.1/ex.sce @@ -0,0 +1,21 @@ +disp("example1.1")
+printf("\n")
+disp("given")
+printf("\n")
+disp("C=C0(1-coswt)")
+disp("angular frequency=500rad/sec")
+w=500;
+t=0:0.001:0.015
+disp("initial capacitance=1 micro farad")
+disp("i=d(CV)/dt")
+disp("supply voltage=3V")
+C0=1*(10^-6)
+C=C0*(1-cos(w*t))
+V=3;
+i= w*C0*V*sin(w*t)//differentiating CV wrt t ,V is constant, i=d(CV)/dt
+subplot(221)
+plot(t,i)
+xtitle('i vs t','t','i')
+subplot(222)
+plot(t,C)//variation of capacitance with time
+xtitle('C vs t','t','C')
\ No newline at end of file diff --git a/269/CH10/EX10.13/ex1.sce b/269/CH10/EX10.13/ex1.sce new file mode 100644 index 000000000..bfaee392e --- /dev/null +++ b/269/CH10/EX10.13/ex1.sce @@ -0,0 +1,19 @@ +Syms t
+s=%s
+H=5
+disp('given')
+disp('H=5')
+disp('poles are -1 and -3')
+disp('The transfer function is ')
+disp('5s/(s+1)(s+3)')
+sysl=syslin('c',5*s/(s+1)*(s+3))
+evans(sysl,100)
+[h]=trfmod(sysl,0)
+//referring the root locus graph
+x=1*imag(exp(-180))
+y=2*imag(exp(-0))
+k1=H*(x/y)
+k2=H*(y/x)
+disp('The current therefore is')
+i=k1*exp(-t)+k2*exp(-3*t)
+disp(i)
diff --git a/269/CH10/EX10.14/ex14a.sce b/269/CH10/EX10.14/ex14a.sce new file mode 100644 index 000000000..9701b2ca4 --- /dev/null +++ b/269/CH10/EX10.14/ex14a.sce @@ -0,0 +1,5 @@ +s=%s
+p=s^4+10*s^3+35*s^2+50*s+24
+h=routh_t(p)
+disp(h)
+disp('from the table the system is stable')
\ No newline at end of file diff --git a/269/CH10/EX10.15/ex15.sce b/269/CH10/EX10.15/ex15.sce new file mode 100644 index 000000000..70aa07d10 --- /dev/null +++ b/269/CH10/EX10.15/ex15.sce @@ -0,0 +1,6 @@ +s=%s
+p=s^3+2*s^2+2*s+40
+h=routh_t(p)
+disp(h)
+disp("from the table there is a sign change ")
+disp("from 2 to -18 and -18 t0 40 and hence system is not stable ")
\ No newline at end of file diff --git a/269/CH10/EX10.16/ex16.sce b/269/CH10/EX10.16/ex16.sce new file mode 100644 index 000000000..af081d933 --- /dev/null +++ b/269/CH10/EX10.16/ex16.sce @@ -0,0 +1,4 @@ +s=%s
+p=3*s^3+2*s^2+1*s+5
+h=routh_t(p)
+disp(h)
diff --git a/269/CH10/EX10.17/ex17.sce b/269/CH10/EX10.17/ex17.sce new file mode 100644 index 000000000..276b32e4d --- /dev/null +++ b/269/CH10/EX10.17/ex17.sce @@ -0,0 +1,7 @@ +s=%s
+p=s^4+s^3+2*s^2+2*s+3
+h=routh_t(p)
+disp(h)
+disp("The element of 1st column 7th row is zero.......its replaced by epsilon(very small quantity)")
+disp("for epsilon<0 seventh element is negative of the 1st column giving 2 sign change implying two positive roots (real) ")
+disp("for epsilon>0 tenth element is zero giving same conclusion")
\ No newline at end of file diff --git a/269/CH10/EX10.18/ex18.sce b/269/CH10/EX10.18/ex18.sce new file mode 100644 index 000000000..328715881 --- /dev/null +++ b/269/CH10/EX10.18/ex18.sce @@ -0,0 +1,11 @@ +s=%s
+p=s^3+2*s^2+2*s+4
+h=routh_t(p)
+disp(h)
+disp("constant term 4 causes the system to be unstable")
+disp("so the polynomial formed is")
+disp("2*s^2+4")
+disp("applyin RH on this polynomial")
+q=s^2+2
+r=routh_t(q)
+disp(r)
diff --git a/269/CH10/EX10.19/ex19.sce b/269/CH10/EX10.19/ex19.sce new file mode 100644 index 000000000..8eda7a4b6 --- /dev/null +++ b/269/CH10/EX10.19/ex19.sce @@ -0,0 +1,10 @@ +s=%s
+p=s^6+5*s^5+11*s^4+25*s^3+36*s^2+30*s+36
+h=routh_t(p)
+disp(h)
+disp("the polynomial obtained is")
+disp("6s^4+30s^2+36")
+disp("applyin RH on this polynomial")
+q=s^2+5*s+6
+r=routh_t(q)
+disp(r)
\ No newline at end of file diff --git a/269/CH12/EX12.1/12_1.jpg b/269/CH12/EX12.1/12_1.jpg Binary files differnew file mode 100644 index 000000000..550289532 --- /dev/null +++ b/269/CH12/EX12.1/12_1.jpg diff --git a/269/CH12/EX12.1/ex1.xcos b/269/CH12/EX12.1/ex1.xcos new file mode 100644 index 000000000..c126977b2 --- /dev/null +++ b/269/CH12/EX12.1/ex1.xcos @@ -0,0 +1 @@ +<?xml version="1.0" encoding="UTF-8"?><XcosDiagram background="-1" finalIntegrationTime="10.0" title="ex1"><mxGraphModel as="model"><root><mxCell id="b736e73:1350b9c47fb:-7fff"/><mxCell id="b736e73:1350b9c47fb:-8000" parent="b736e73:1350b9c47fb:-7fff"/><BasicBlock angle="90" dependsOnU="1" id="b736e73:1350b9c47fb:-7fd4" interfaceFunctionName="Resistor" ordering="1" parent="b736e73:1350b9c47fb:-8000" simulationFunctionName="resistor" simulationFunctionType="DEFAULT" style="Resistor;rotation=90;flip=false;mirror=false"><ScilabString as="exprs" height="1" width="1"><data column="0" line="0" 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\ No newline at end of file diff --git a/269/CH13/EX13.1/1_1.jpg b/269/CH13/EX13.1/1_1.jpg Binary files differnew file mode 100644 index 000000000..78594a2e0 --- /dev/null +++ b/269/CH13/EX13.1/1_1.jpg diff --git a/269/CH13/EX13.1/ex1.sce b/269/CH13/EX13.1/ex1.sce new file mode 100644 index 000000000..acdb34f27 --- /dev/null +++ b/269/CH13/EX13.1/ex1.sce @@ -0,0 +1,8 @@ +s=poly (0,'s')
+F=syslin('c',[1/(3*s+1)])//RC=3 sec
+G=F
+fmin=0.1
+fmax=100
+scf(1);clf;
+bode(G,fmin,fmax)
+show_margins(G)
\ No newline at end of file diff --git a/269/CH13/EX13.2/2_2.jpg b/269/CH13/EX13.2/2_2.jpg Binary files differnew file mode 100644 index 000000000..94a2d4c0c --- /dev/null +++ b/269/CH13/EX13.2/2_2.jpg diff --git a/269/CH13/EX13.2/ex2.sce b/269/CH13/EX13.2/ex2.sce new file mode 100644 index 000000000..3ca10d5f6 --- /dev/null +++ b/269/CH13/EX13.2/ex2.sce @@ -0,0 +1,4 @@ +s=poly(0,'s')
+F=syslin('c',1/(3*s+1))
+y=evans(F)
+disp(y)
\ No newline at end of file diff --git a/269/CH13/EX13.3/3_3.jpg b/269/CH13/EX13.3/3_3.jpg Binary files differnew file mode 100644 index 000000000..6c892417c --- /dev/null +++ b/269/CH13/EX13.3/3_3.jpg diff --git a/269/CH13/EX13.3/ex3.sce b/269/CH13/EX13.3/ex3.sce new file mode 100644 index 000000000..1e9dc4649 --- /dev/null +++ b/269/CH13/EX13.3/ex3.sce @@ -0,0 +1,8 @@ +s=poly (0,'s')
+F=syslin('c',[1*s/(1*s+1)])//RC=3 sec
+G=F
+fmin=0.1
+fmax=100
+scf(1);clf;
+bode(G,fmin,fmax)
+show_margins(G)
\ No newline at end of file diff --git a/269/CH13/EX13.4/4_4.jpg b/269/CH13/EX13.4/4_4.jpg Binary files differnew file mode 100644 index 000000000..78594a2e0 --- /dev/null +++ b/269/CH13/EX13.4/4_4.jpg diff --git a/269/CH13/EX13.4/ex4.sce b/269/CH13/EX13.4/ex4.sce new file mode 100644 index 000000000..acdb34f27 --- /dev/null +++ b/269/CH13/EX13.4/ex4.sce @@ -0,0 +1,8 @@ +s=poly (0,'s')
+F=syslin('c',[1/(3*s+1)])//RC=3 sec
+G=F
+fmin=0.1
+fmax=100
+scf(1);clf;
+bode(G,fmin,fmax)
+show_margins(G)
\ No newline at end of file diff --git a/269/CH13/EX13.7/7_7.jpg b/269/CH13/EX13.7/7_7.jpg Binary files differnew file mode 100644 index 000000000..ae37cd2ba --- /dev/null +++ b/269/CH13/EX13.7/7_7.jpg diff --git a/269/CH13/EX13.7/ex7.sce b/269/CH13/EX13.7/ex7.sce new file mode 100644 index 000000000..a09fadb3f --- /dev/null +++ b/269/CH13/EX13.7/ex7.sce @@ -0,0 +1,5 @@ +s=poly(0,'s')
+F=syslin('c',[(s^2-s+1)/(s^2+s+1)])
+G=F
+evans(G)
+[hm]=trfmod(G ,['f'])
\ No newline at end of file diff --git a/269/CH14/EX14.2/example6_2.sce b/269/CH14/EX14.2/example6_2.sce new file mode 100644 index 000000000..1043700ce --- /dev/null +++ b/269/CH14/EX14.2/example6_2.sce @@ -0,0 +1,10 @@ +disp('chap 14 , ex 2')
+disp(' given')
+disp('The waveform is t for t>0,t<1 and 1 for t>1,t<2')
+function y1=myfunction(t),y1=t^2,endfunction
+function y2=second(t),y2=t^0,endfunction
+i1=intg(0,1,myfunction)//integration from 0 to1 (rms current)
+i2=intg(1,2,second)//integration from 1 to 2(rms current)
+i3=0.5*(i1+i2);
+disp('The rms value of current is')
+disp(sqrt(i3))//i=sqrt(1/2(integ of t^2 from 0 to 1+ integ of 1 from 1 to 2))
\ No newline at end of file diff --git a/269/CH14/EX14.3/example6_3.sce b/269/CH14/EX14.3/example6_3.sce new file mode 100644 index 000000000..691966bb4 --- /dev/null +++ b/269/CH14/EX14.3/example6_3.sce @@ -0,0 +1,25 @@ +disp('chap 14 ex 3')
+disp('given')
+disp('current source i1=5sqrt(2)sin2t')
+disp('driving point impedance Z=3+j/3')
+Pav=25*3//Pav=Irms^2*real(Z)
+disp('Average power is ')
+disp(Pav)
+Q=25*1/3//Q=Irms^2*imag(Z)
+disp('Reactive power is')
+disp(Q)
+s=sqrt(75^2+(25/3)^2)//s=Irms^2*Z, calculation of magnitude of s
+Vrms=s/5
+disp('rms value of voltage is')
+disp(Vrms)
+pf=cos(atan(1/9))//power factor=cos thetaz=cos(tan-(1/9))
+disp('power factor=')
+disp(pf)
+disp('The branch currents are')
+disp('I1=5,I2=10*sqrt(5)/6,I3=10*sqrt(2)/6')
+TPav=50+500/36+400/36//Total avg power=I1^2*2+I2^2*2+13^2*2
+disp('Total average power')
+disp(TPav)
+TQ=500/36-200/36//Total reactive power in the capacitor and inductor branches=Q1-Q2
+disp('Total reactive Power')
+disp(TQ)
\ No newline at end of file diff --git a/269/CH14/EX14.4/example6_4.sce b/269/CH14/EX14.4/example6_4.sce new file mode 100644 index 000000000..9a227c6a5 --- /dev/null +++ b/269/CH14/EX14.4/example6_4.sce @@ -0,0 +1,17 @@ +disp('chapter 14, example 4')
+disp('given')
+disp('Pav=500W, Q=500vars,Pf=0.707 lagging')//power factor=0.707 lag behind Q
+disp('rms value of voltage=2v')
+disp('angular frequency=2rad/sec')
+Q=500
+pf=0.707
+pav=500
+Qt=sqrt((pav/0.9)^2-pav^2)//power factor=pav/sqrt(pav^2+qt^2) and changed power factor = 0.9 lagging .This is done by connecting capacitor
+disp(Qt)
+Qc=Qt-Q
+disp(Qc)
+Vrms=2//rms value of voltage is 2 volts
+W=2//angularfreq=2 rad/sec
+c=Qc/(-Vrms^2*W)*10^-6
+disp('Capacitor required for 0.9 power factor in microfarad is')
+disp(c)
\ No newline at end of file diff --git a/269/CH16/EX16.1/ex1.sce b/269/CH16/EX16.1/ex1.sce new file mode 100644 index 000000000..561c4399f --- /dev/null +++ b/269/CH16/EX16.1/ex1.sce @@ -0,0 +1,33 @@ +clc;
+//Let amplitude be 1
+A=1;
+Dt=0.01;
+T1=4;
+t=0:Dt:T1/4;
+for i=1:length(t)
+ xt(i)=A
+end
+//Calculate Fourier Transform
+Wmax=2*%pi*1;
+K=4;
+k=-(2*K):(K/1000):(2*K);
+W=k*Wmax/K;
+xt=xt';
+XW=xt*exp(-sqrt(-1)*t'*W)*Dt;
+XW_Mag=real(XW);
+W=[-mtlb_fliplr(W),W(2:1001)];
+XW_Mag=[mtlb_fliplr(XW_Mag),XW_Mag(2:1001)];
+subplot(2,1,1);
+a=gca();
+a.data_bounds=[0,0;1,1.5];
+a.y_location="origin";
+plot(t,xt);
+xlabel('t in sec.');
+title('v(t)vs t');
+subplot(2,1,2);
+a=gca();
+a.y_location="origin";
+plot(W*%pi/2,abs (XW_Mag));
+xlabel('Freq in rad/sec');
+ylabel('|F(jw)|')
+title('|F(jw)| vs t');
\ No newline at end of file diff --git a/269/CH16/EX16.1/fig1.jpeg b/269/CH16/EX16.1/fig1.jpeg Binary files differnew file mode 100644 index 000000000..e5d762b33 --- /dev/null +++ b/269/CH16/EX16.1/fig1.jpeg diff --git a/269/CH16/EX16.2/ex2a.sce b/269/CH16/EX16.2/ex2a.sce new file mode 100644 index 000000000..7b992e885 --- /dev/null +++ b/269/CH16/EX16.2/ex2a.sce @@ -0,0 +1,33 @@ +clear;
+clc;
+close;
+A=4;//V0=4 amplitude
+Dt=0.005;
+T1=4;
+t=0:Dt:T1/2;
+for i=1:length(t)
+ xt(i)=A*exp(-0.01*i)
+end
+//continous time Fourier Transform
+Wmax=2*%pi*1;//Analog freq=1HZ
+K=4;
+k=0:(K/1000):K;
+W=k*Wmax/K;
+xt=xt';
+XW=xt*exp(-sqrt(-1)*t'*W)*Dt;
+XW_Mag=real(XW);
+W=[-mtlb_fliplr(W),W(2:1001)];
+XW_Mag=[mtlb_fliplr(XW_Mag),XW_Mag(2:1001)];
+subplot(2,1,1);
+a=gca();
+a.data_bounds=[-4,0;4,2];
+a.y_location="origin";
+plot(t,xt);
+xlabel('t in msec.');
+title('Continous time signal x(t)');
+subplot(2,1,2);
+a=gca();
+a.y_location="origin";
+plot(W,XW_Mag);
+xlabel('Freq in rad/sec');
+title('continous time fourier transform');
\ No newline at end of file diff --git a/269/CH16/EX16.2/ex2f.jpg b/269/CH16/EX16.2/ex2f.jpg Binary files differnew file mode 100644 index 000000000..98d7be1d3 --- /dev/null +++ b/269/CH16/EX16.2/ex2f.jpg diff --git a/269/CH3/EX3.1/ex1.xcos b/269/CH3/EX3.1/ex1.xcos new file mode 100644 index 000000000..b9e62aab0 --- /dev/null +++ b/269/CH3/EX3.1/ex1.xcos @@ -0,0 +1 @@ +<?xml version="1.0" encoding="UTF-8"?><XcosDiagram background="-1" finalIntegrationTime="13.0" title="ex1"><mxGraphModel as="model"><root><mxCell id="5a5c50e:13440d28076:-7fff"/><mxCell id="5a5c50e:13440d28076:-8000" parent="5a5c50e:13440d28076:-7fff"/><GroundBlock dependsOnU="1" id="-65720c4a:134ef37e858:-7f4e" interfaceFunctionName="Ground" ordering="1" parent="5a5c50e:13440d28076:-8000" simulationFunctionName="Ground" simulationFunctionType="DEFAULT" style="Ground;flip=false;mirror=false"><ScilabString as="exprs" height="1" width="1"><data column="0" line="0" value=""/></ScilabString><ScilabDouble as="realParameters" 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\ No newline at end of file diff --git a/269/CH3/EX3.10/ex10_10.jpeg b/269/CH3/EX3.10/ex10_10.jpeg Binary files differnew file mode 100644 index 000000000..0c62ee646 --- /dev/null +++ b/269/CH3/EX3.10/ex10_10.jpeg diff --git a/269/CH3/EX3.10/ex10_10g.jpg b/269/CH3/EX3.10/ex10_10g.jpg Binary files differnew file mode 100644 index 000000000..6bf8e9a93 --- /dev/null +++ b/269/CH3/EX3.10/ex10_10g.jpg diff --git a/269/CH3/EX3.14/ex14.sce b/269/CH3/EX3.14/ex14.sce new file mode 100644 index 000000000..181b9fd41 --- /dev/null +++ b/269/CH3/EX3.14/ex14.sce @@ -0,0 +1,24 @@ +disp("chapter3")
+disp("example 14 ")
+disp("given")
+disp("the equations given are=")
+disp("5i1-2i2-3i3=10")
+disp("-2i1+4i2-i3=0")
+disp("-3i1-i2+6i3=0")
+a=[5 -2 -3; -2 4 -1; -3 -1 6] //matrix
+y=det(a)
+b=[10 -2 -3; 0 4 -1 ;0 -1 6] //matrix for i1 calculation (cramers rule)
+w=det(b)
+i1=w/y
+disp("current i1=")
+disp(i1)
+c=[5 10 -3;-2 0 -1; -3 0 6] //cramers rule
+x=det(c)
+i2=x/y
+disp("current i2=")
+disp(i2)
+d=[5 -2 10; -2 4 0; -3 -1 0]
+z=det(d)
+i3=z/y
+disp("current i3=")
+disp(i3)
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\ No newline at end of file diff --git a/269/CH3/EX3.9/ex9_9.jpeg b/269/CH3/EX3.9/ex9_9.jpeg Binary files differnew file mode 100644 index 000000000..e8b3764df --- /dev/null +++ b/269/CH3/EX3.9/ex9_9.jpeg diff --git a/269/CH3/EX3.9/ex9_9g.jpg b/269/CH3/EX3.9/ex9_9g.jpg Binary files differnew file mode 100644 index 000000000..ad9cb9c2c --- /dev/null +++ b/269/CH3/EX3.9/ex9_9g.jpg diff --git a/269/CH4/EX4.1/ex1.jpg b/269/CH4/EX4.1/ex1.jpg Binary files differnew file mode 100644 index 000000000..140381cd7 --- /dev/null +++ b/269/CH4/EX4.1/ex1.jpg diff --git a/269/CH4/EX4.1/ex1.sce b/269/CH4/EX4.1/ex1.sce new file mode 100644 index 000000000..d6579b140 --- /dev/null +++ b/269/CH4/EX4.1/ex1.sce @@ -0,0 +1,10 @@ +disp("chap 4")
+disp("ex 1")
+disp("the equation for current by kvl is")
+disp("i=v/r*(1-exp(-r*t/L))")// r-resistor,L-inductor
+v=3// assumed supply=5v
+r=10//assumed r=10 ohm
+L=500//assumed inductance=500henry
+t=0:0.1:500
+i=v/r*(1-exp(-r*t/L))
+plot(i)
\ No newline at end of file diff --git a/269/CH4/EX4.2/ex2.jpg b/269/CH4/EX4.2/ex2.jpg Binary files differnew file mode 100644 index 000000000..9cc631d3c --- /dev/null +++ b/269/CH4/EX4.2/ex2.jpg diff --git a/269/CH4/EX4.2/ex2.sce b/269/CH4/EX4.2/ex2.sce new file mode 100644 index 000000000..bdd1ade4b --- /dev/null +++ b/269/CH4/EX4.2/ex2.sce @@ -0,0 +1,16 @@ +disp("chap 4")
+disp("ex 2")
+disp("the current equations obtained by solving diff eqn are")
+disp("i1=v/r1(1-r2/(r1+r2))e^(-r1t/L)")
+disp("i2=v/(r1+r2)(1+r2/r1e^(-(r1+r2)t/L))")
+v=5//assumed supply=5v
+r1=10//assumed r1=10ohms
+r2=50
+L=500//inductance=500 henry
+t=0:0.1:500
+i1=v/r1*(1-(r2/r1+r2*exp(-r1*t/L)))
+subplot(221)
+plot(i1)
+i2=v/(r1+r2)*(1+r2/r1*exp(-(r1+r2)*t/L))
+subplot(222)
+plot(i2)
\ No newline at end of file diff --git a/269/CH4/EX4.3/ex4.xcos b/269/CH4/EX4.3/ex4.xcos new file mode 100644 index 000000000..1d84d4b19 --- /dev/null +++ b/269/CH4/EX4.3/ex4.xcos @@ -0,0 +1 @@ +<?xml version="1.0" encoding="UTF-8"?><XcosDiagram background="-1" finalIntegrationTime="20.0" title="ex4"><mxGraphModel as="model"><root><mxCell id="16147f80:1350b3a3264:-7f12"/><mxCell id="16147f80:1350b3a3264:-7f13" parent="16147f80:1350b3a3264:-7f12"/><BasicBlock angle="270" dependsOnU="1" id="16147f80:1350b3a3264:-7f0a" interfaceFunctionName="Resistor" ordering="1" parent="16147f80:1350b3a3264:-7f13" simulationFunctionName="resistor" simulationFunctionType="DEFAULT" style="Resistor;rotation=270"><ScilabString as="exprs" height="1" width="1"><data column="0" line="0" value="4"/></ScilabString><ScilabDouble as="realParameters" height="1" width="1"><data column="0" line="0" realPart="4.0"/></ScilabDouble><ScilabDouble as="integerParameters" height="0" width="0"/><Array as="objectsParameters" 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\ No newline at end of file diff --git a/269/CH4/EX4.4/ex4_4.jpeg b/269/CH4/EX4.4/ex4_4.jpeg Binary files differnew file mode 100644 index 000000000..1087f32f6 --- /dev/null +++ b/269/CH4/EX4.4/ex4_4.jpeg diff --git a/269/CH4/EX4.4/ex4_4g.jpeg b/269/CH4/EX4.4/ex4_4g.jpeg Binary files differnew file mode 100644 index 000000000..b28b2ead3 --- /dev/null +++ b/269/CH4/EX4.4/ex4_4g.jpeg diff --git a/269/CH5/EX5.1/ex5_5.jpeg b/269/CH5/EX5.1/ex5_5.jpeg Binary files differnew file mode 100644 index 000000000..c58dbad93 --- /dev/null +++ b/269/CH5/EX5.1/ex5_5.jpeg diff --git a/269/CH5/EX5.1/ex5_5g.jpg b/269/CH5/EX5.1/ex5_5g.jpg Binary files differnew file mode 100644 index 000000000..4e777eb4f --- /dev/null +++ b/269/CH5/EX5.1/ex5_5g.jpg diff --git a/269/CH5/EX5.1/example1a.xcos b/269/CH5/EX5.1/example1a.xcos new file mode 100644 index 000000000..a4523b752 --- /dev/null +++ b/269/CH5/EX5.1/example1a.xcos @@ -0,0 +1 @@ +<?xml version="1.0" encoding="UTF-8"?><XcosDiagram background="-1" 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\ No newline at end of file diff --git a/269/CH6/EX6.1/ex1_1.jpeg b/269/CH6/EX6.1/ex1_1.jpeg Binary files differnew file mode 100644 index 000000000..aebfe5a92 --- /dev/null +++ b/269/CH6/EX6.1/ex1_1.jpeg diff --git a/269/CH6/EX6.1/ex1_1g.jpg b/269/CH6/EX6.1/ex1_1g.jpg Binary files differnew file mode 100644 index 000000000..733959ed2 --- /dev/null +++ b/269/CH6/EX6.1/ex1_1g.jpg diff --git a/269/CH6/EX6.1/example1.sce b/269/CH6/EX6.1/example1.sce new file mode 100644 index 000000000..0d703cf31 --- /dev/null +++ b/269/CH6/EX6.1/example1.sce @@ -0,0 +1,29 @@ +disp('by kvl')
+disp('Ldi/dt+Ri+1/c*integ(i)=V')
+disp('given')
+disp('V=1,R=3,L=1,C=0.5')
+disp('Replacing di/dt with s and (di/dt)^2 with s^2')
+disp('we get')
+disp('s^2+3s+2')
+s=poly(0,'s')
+p=s^2+3*s+2
+r=roots(p)
+disp(r)
+disp('therefore the current in general form is')
+disp('i(t)=k1exp(-t)+k2exp(-2t)')
+//k1 and k2 are constants and are evaluated by knowing inital conditions
+disp('initial conditions are')
+disp('di/dt at 0+ is V/L=1')
+disp('i(t) at 0+ is 0')
+disp('on solving we get k1=1,k2=-1')
+t=0:0.1:2
+i=exp(-t)-exp(-2*t)
+subplot(221)
+xtitle("exp(-t)")
+plot2d(exp(-t))
+subplot(222)
+xtitle("exp(-2t)")
+plot2d(exp(-2*t))
+subplot(223)
+xtitle("i")
+plot2d(i)
\ No newline at end of file diff --git a/269/CH6/EX6.3/ex3.xcos b/269/CH6/EX6.3/ex3.xcos new file mode 100644 index 000000000..3b765e8a5 --- /dev/null +++ b/269/CH6/EX6.3/ex3.xcos @@ -0,0 +1 @@ +<?xml version="1.0" encoding="UTF-8"?><XcosDiagram background="-1" finalIntegrationTime="7.0" title="ex3"><mxGraphModel as="model"><root><mxCell id="75c9bd31:1350b5d1940:-7dce"/><mxCell id="75c9bd31:1350b5d1940:-7dcf" parent="75c9bd31:1350b5d1940:-7dce"/><BasicBlock dependsOnU="1" id="75c9bd31:1350b5d1940:-7dcd" interfaceFunctionName="Resistor" ordering="1" parent="75c9bd31:1350b5d1940:-7dcf" simulationFunctionName="resistor" simulationFunctionType="DEFAULT" style="Resistor"><ScilabString as="exprs" height="1" width="1"><data column="0" line="0" value="2"/></ScilabString><ScilabDouble as="realParameters" height="1" width="1"><data column="0" line="0" realPart="2.0"/></ScilabDouble><ScilabDouble as="integerParameters" height="0" width="0"/><Array as="objectsParameters" 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\ No newline at end of file diff --git a/269/CH6/EX6.3/ex3_3.jpeg b/269/CH6/EX6.3/ex3_3.jpeg Binary files differnew file mode 100644 index 000000000..aebfe5a92 --- /dev/null +++ b/269/CH6/EX6.3/ex3_3.jpeg diff --git a/269/CH6/EX6.3/ex3_3g.jpg b/269/CH6/EX6.3/ex3_3g.jpg Binary files differnew file mode 100644 index 000000000..667871675 --- /dev/null +++ b/269/CH6/EX6.3/ex3_3g.jpg diff --git a/269/CH7/EX7.1/example1.sce b/269/CH7/EX7.1/example1.sce new file mode 100644 index 000000000..01d741e35 --- /dev/null +++ b/269/CH7/EX7.1/example1.sce @@ -0,0 +1,10 @@ +Syms t s
+disp('given')
+disp('u(t)=1 for t>=0 else its 0')
+y=laplace(1,t,s)
+disp("The laplace is")
+disp(y)
+disp('similarly')
+disp('laplace of V0 is')
+x=laplace('V0',t,s)
+disp(x)
diff --git a/269/CH7/EX7.10/example10.sce b/269/CH7/EX7.10/example10.sce new file mode 100644 index 000000000..726238167 --- /dev/null +++ b/269/CH7/EX7.10/example10.sce @@ -0,0 +1,5 @@ +syms t
+s=%s
+disp('Heavisides expansion')
+[A]=pfss((2*s^2+3*s+2)/((s+1)^3))
+disp(A(1))
\ No newline at end of file diff --git a/269/CH7/EX7.11/example11.sce b/269/CH7/EX7.11/example11.sce new file mode 100644 index 000000000..022211b63 --- /dev/null +++ b/269/CH7/EX7.11/example11.sce @@ -0,0 +1,3 @@ +s=%s
+[A]=pfss((s+2)/(s^2+2*s+1)*(s+3))
+disp([A])
diff --git a/269/CH7/EX7.12/example12.sce b/269/CH7/EX7.12/example12.sce new file mode 100644 index 000000000..88982695f --- /dev/null +++ b/269/CH7/EX7.12/example12.sce @@ -0,0 +1,10 @@ +Syms t,s
+//on applying KVL we get the laplace transformed current as
+disp(' the laplace transformed current equation is i(s)=s^2+6s+5/(s*(s^2+4s+5))')
+//by partial fraction method
+[A]=pfss(s^2+6*s+5/((s)*(s^2+4*s+5)))
+b=ilt(A (1),s,t)
+c=ilt(A(2),s,t)
+d=b+c
+disp('the time domain expression is')
+disp(d)
diff --git a/269/CH7/EX7.13/example13.sce b/269/CH7/EX7.13/example13.sce new file mode 100644 index 000000000..69f7e948e --- /dev/null +++ b/269/CH7/EX7.13/example13.sce @@ -0,0 +1,7 @@ +Syms t,s
+//by network equations
+disp('by network equations i(s)=1/(s+1)^2+1')
+[A]=pfss((1*s^0+0)/((s+1)^2+1))
+b=ilt(A(1),s,t)
+disp('The inverse laplace is')
+disp(b)
diff --git a/269/CH7/EX7.14/example14.sce b/269/CH7/EX7.14/example14.sce new file mode 100644 index 000000000..7f498c1b6 --- /dev/null +++ b/269/CH7/EX7.14/example14.sce @@ -0,0 +1,10 @@ +Syms t,s
+disp('by network equations kvl and kcl ')
+disp('i2(s)=1000/s*(s^2+40s+300)')
+[A]=pfss((1000*s^0+0)/((s*(s+10)*(s+30))))
+x=ilt(A(1),s,t)
+y=ilt(A(2),s,t)
+z=ilt(A(3),s,t)
+f=x+y+z
+disp('the timedomain expression is')
+disp(f)
diff --git a/269/CH7/EX7.2/example2.sce b/269/CH7/EX7.2/example2.sce new file mode 100644 index 000000000..a2c05ba11 --- /dev/null +++ b/269/CH7/EX7.2/example2.sce @@ -0,0 +1,6 @@ +Syms t,s
+disp('given')
+disp(' f(t)= e^at ,a>0')
+disp('laplace of f(t) is')
+y=laplace('exp(a*t)', t,s)
+disp(y)
diff --git a/269/CH7/EX7.3/example3.sce b/269/CH7/EX7.3/example3.sce new file mode 100644 index 000000000..8071dfa45 --- /dev/null +++ b/269/CH7/EX7.3/example3.sce @@ -0,0 +1,7 @@ +Syms t s
+disp('f1(t)=coswt , f2(t)=sinwt')
+disp('laplace of f1(t) and f2(t) are')
+y=laplace('cos(w*t)',t,s)
+z=laplace('sin(w*t)',t,s)
+disp(y)
+disp(z)
diff --git a/269/CH7/EX7.4/example4.sce b/269/CH7/EX7.4/example4.sce new file mode 100644 index 000000000..38fed5ca4 --- /dev/null +++ b/269/CH7/EX7.4/example4.sce @@ -0,0 +1,5 @@ +Syms s t
+disp('given')
+disp('i(s)=V/R/s+(1/RC) for t>=0')
+z=ilt('(V/R*s^0+0)/(s+(1/RC))',s,t)
+disp(z,"z(t)=")
diff --git a/269/CH7/EX7.5/example5.sce b/269/CH7/EX7.5/example5.sce new file mode 100644 index 000000000..294376891 --- /dev/null +++ b/269/CH7/EX7.5/example5.sce @@ -0,0 +1,9 @@ +Syms t,s
+disp('By KVL the current equation is')
+disp('V/L*(1/s*(s+R/L))')
+//by partial fraction method the expression is split as k0/s+k1/s+(R/L)
+//The values of k0=V/R and k1=-V/R
+//taking inverse laplace
+disp('inverse laplace is')
+z=ilt('(V/R*s^0)/s-(V/R*s^0)/(s+(R/L))',s,t)
+disp(z,"z(t)=")
diff --git a/269/CH7/EX7.7/example7.sce b/269/CH7/EX7.7/example7.sce new file mode 100644 index 000000000..2bc84c65a --- /dev/null +++ b/269/CH7/EX7.7/example7.sce @@ -0,0 +1,5 @@ +syms t
+s=%s
+[A]=pfss((2*s+3)/(s^2+3*s+2))
+disp(A(1))
+disp(A(2))
\ No newline at end of file diff --git a/269/CH7/EX7.8/example8.sce b/269/CH7/EX7.8/example8.sce new file mode 100644 index 000000000..2850d2b4d --- /dev/null +++ b/269/CH7/EX7.8/example8.sce @@ -0,0 +1,4 @@ +syms t
+s=%s
+[A]=pfss((s+2)/((s+1)^2))
+disp(A(1))
diff --git a/269/CH7/EX7.9/example9.sce b/269/CH7/EX7.9/example9.sce new file mode 100644 index 000000000..18d085b24 --- /dev/null +++ b/269/CH7/EX7.9/example9.sce @@ -0,0 +1,4 @@ +syms t
+s=%s
+[A]=pfss((1/(s^2+2*s+5)))
+disp(A(1))
diff --git a/269/CH8/EX8.1/example1.sce b/269/CH8/EX8.1/example1.sce new file mode 100644 index 000000000..4b3ebb865 --- /dev/null +++ b/269/CH8/EX8.1/example1.sce @@ -0,0 +1,18 @@ +Syms t,s
+disp('applyin kvl and solving we get')
+disp('i(s)=1-e^-as/s(s+1) where a is a constant')
+// This can be modified and written as
+a=1
+//by partial fraction
+[A]=pfss((1*s^0+0)/s*(s+1))
+b=ilt(A(1),s,t)
+disp(b)
+d=exp(1*a)//inverse laplace of exp(-sa)
+disp(d)
+//z=ilaplace((%e^-),s,t)
+//disp(z)
+e=ilt((1*s^0+0)/(s+1),s,t)
+f=ilt((d*s^0)/s,s,t)
+g=ilt((d*s^0)/(s+1))
+h=b*d*e*g*f;
+disp(h)
diff --git a/269/CH8/EX8.2/ex2.sce b/269/CH8/EX8.2/ex2.sce new file mode 100644 index 000000000..556e3a864 --- /dev/null +++ b/269/CH8/EX8.2/ex2.sce @@ -0,0 +1,12 @@ +Syms t,s
+disp('i(s)=1/s*(s+1)')
+b=ilt((1*s^0+0)/s,s,t)
+e=ilt((-1*s^0+0)/(s+1),s,t)
+f=b+e
+printf("current in time domain by partial fraction is")
+disp(f,"i(t)=")
+disp('by scaling theorem i1(t)=')
+d=ilt((2*s^0+0)/(2*s),s,t)
+g=ilt((-2*s^0+0)/(2*s+1))
+l=d+g
+disp(l)
diff --git a/269/CH8/EX8.3/ex3.sce b/269/CH8/EX8.3/ex3.sce new file mode 100644 index 000000000..548fb4e2b --- /dev/null +++ b/269/CH8/EX8.3/ex3.sce @@ -0,0 +1,6 @@ +Syms t,s
+disp('By kvl equation\n i(s)=1/s+1')
+f=ilt((s^0)/(s+1),s,t)
+printf("current in time domain by laplace transform is\n")
+printf("i(t)=")
+disp(f)
diff --git a/269/CH8/EX8.5/ex5.sce b/269/CH8/EX8.5/ex5.sce new file mode 100644 index 000000000..1245c5a75 --- /dev/null +++ b/269/CH8/EX8.5/ex5.sce @@ -0,0 +1,15 @@ +Syms t,s
+disp('given')
+disp('i(s)=2s+5/s+1*(s+2)')
+f=(2*s+5)/((s+1)*(s+2))
+[a]=pfss(2*s/(s^2+3*s+2))
+g=a(1)+a(2)
+x=s*f
+y=limit(x,s,0)
+disp('by final value theorem')
+disp(y,"i(inf)=")
+g=ilt(f,s,t)
+disp(g,"time domain exp is")
+h=limit(g,t,%inf)
+disp(h)
+disp('hence verified')
diff --git a/269/CH8/EX8.6/ex6.sce b/269/CH8/EX8.6/ex6.sce new file mode 100644 index 000000000..75a7b4378 --- /dev/null +++ b/269/CH8/EX8.6/ex6.sce @@ -0,0 +1,8 @@ +Syms t,s
+disp('given i2(t)=5-3e^(-2t)')
+f=laplace('5-3*%e^(-2*t)',t,s)
+disp(f,"laplace transformed solution is")
+x=s*f
+disp('by final value theorem')
+y=limit(x,s,0)//final value theorem
+disp(y,"i2(inf)=")
diff --git a/269/CH8/EX8.7/ex7.sce b/269/CH8/EX8.7/ex7.sce new file mode 100644 index 000000000..8ae3dee01 --- /dev/null +++ b/269/CH8/EX8.7/ex7.sce @@ -0,0 +1,25 @@ +s=%s
+Max_Limit = 10;
+h = ones(1,Max_Limit);
+N2 =0:length(h)-1;
+for t = 1: Max_Limit
+ x(t)= exp(-(t -1));
+end
+N1 =0:length(x)-1;
+y = convol(x,h)-1;
+N = 0:length(x)+ length(h)-2;
+figure
+a= gca();
+plot2d (N2 ,h)
+xtitle ( ' Impul s e Re spons e ' , ' t ' , ' h ( t ) ' );
+a. thickness = 2;
+figure
+a= gca ();
+plot2d (N1 ,x)
+xtitle ( ' Input Re spons e ' , ' t ' , ' x ( t ) ' );
+a. thickness = 2;
+figure
+a= gca ();
+plot2d (N(1: Max_Limit ),y (1: Max_Limit ))
+xtitle ( ' Output Re spons e ' , ' t ' , ' y ( t ) ' );
+a. thickness = 2;
diff --git a/269/CH9/EX9.1/ex1.sce b/269/CH9/EX9.1/ex1.sce new file mode 100644 index 000000000..41d00bbf0 --- /dev/null +++ b/269/CH9/EX9.1/ex1.sce @@ -0,0 +1,13 @@ +Syms t,s
+disp('given')
+disp('V=e^-t(sint) R1=1,R2=1,C=0.5,L=2')
+disp('laplace transforming the ckt elements')
+disp('Total impedance is')
+z=((2*s^2+5*s+4)/(2*s^2+s+2))
+disp(z)
+disp('laplace transformed voltage is')
+v=laplace('%e^(-t)*sin(2*t)',t,s)
+disp(v)
+disp('The current can be found as v/z')
+i=v/z
+disp(i,"The total current in s domain")
diff --git a/269/CH9/EX9.3/ex3.sce b/269/CH9/EX9.3/ex3.sce new file mode 100644 index 000000000..1ead7471f --- /dev/null +++ b/269/CH9/EX9.3/ex3.sce @@ -0,0 +1,13 @@ +Syms t ,s
+disp('given')
+disp('V=e^-t(sint) R1=1,R2=1,C=0.5,L=2')
+disp('laplace transforming the ckt elements')
+disp('Total impedance is')
+z=((2*s^2+5*s+4)/(2*s^2+s+2))
+disp(z)
+disp('laplace transformed voltage is')
+v=laplace('%e^(-t)*sin(2*t)',t,s)
+disp(v)
+disp('The current can be found as v/z')
+i=v/z
+disp(i,"The total current in s domain")
diff --git a/269/CH9/EX9.4/ex4.xcos b/269/CH9/EX9.4/ex4.xcos new file mode 100644 index 000000000..72d4fc816 --- /dev/null +++ b/269/CH9/EX9.4/ex4.xcos @@ -0,0 +1 @@ +<?xml version="1.0" encoding="UTF-8"?><XcosDiagram background="-1" finalIntegrationTime="20.0" title="ex4"><mxGraphModel as="model"><root><mxCell id="788ebb49:134fb4fe444:-7fdd"/><mxCell id="788ebb49:134fb4fe444:-7fde" parent="788ebb49:134fb4fe444:-7fdd"/><BasicBlock angle="270" dependsOnU="1" id="788ebb49:134fb4fe444:-7fcb" interfaceFunctionName="Capacitor" ordering="1" parent="788ebb49:134fb4fe444:-7fde" simulationFunctionName="Capacitor" simulationFunctionType="DEFAULT" style="Capacitor;rotation=270;flip=false;mirror=false"><ScilabString as="exprs" height="2" width="1"><data column="0" line="0" value="1"/><data column="0" line="1" value="2"/></ScilabString><ScilabDouble as="realParameters" height="1" width="1"><data column="0" line="0" realPart="1.0"/></ScilabDouble><ScilabDouble as="integerParameters" height="0" 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\ No newline at end of file diff --git a/269/CH9/EX9.4/ex4_4.jpeg b/269/CH9/EX9.4/ex4_4.jpeg Binary files differnew file mode 100644 index 000000000..a006934da --- /dev/null +++ b/269/CH9/EX9.4/ex4_4.jpeg diff --git a/269/CH9/EX9.4/ex4_4g.jpg b/269/CH9/EX9.4/ex4_4g.jpg Binary files differnew file mode 100644 index 000000000..8734953f6 --- /dev/null +++ b/269/CH9/EX9.4/ex4_4g.jpg diff --git a/269/CH9/EX9.6/ex6.sce b/269/CH9/EX9.6/ex6.sce new file mode 100644 index 000000000..c0303e434 --- /dev/null +++ b/269/CH9/EX9.6/ex6.sce @@ -0,0 +1,18 @@ +Syms t,s
+disp('The open ckt voltage is found as')
+disp('1000/s(s+20)')//fig 9.33
+v=1000/(s*(s+20))
+disp('The thevenins impedance is')
+disp('10(s+10)/(s+20)')//fig 9.33
+z=10*(s+10)/(s+20)
+disp('The current through R3 is i1')
+disp('By thevenins theorem ....')
+disp('I1(s)=v/z+z1..........where z1 is the ckt impedance')
+disp('I1(s)=1000/s(s^2+40s+300)')
+I1=1000/(s*(s^2+40*s+300))
+[a]=pfss(1000/(s*(s+10)*(s+30)))
+b=ilt(a(1),s,t)
+c=ilt(a(2),s,t)
+d=ilt(a(3),s,t)
+f=b+c+d
+disp(f,"The current in time domain by thevenins theorem is ")
diff --git a/269/CH9/EX9.7/ex7.sce b/269/CH9/EX9.7/ex7.sce new file mode 100644 index 000000000..4b1f00c06 --- /dev/null +++ b/269/CH9/EX9.7/ex7.sce @@ -0,0 +1,9 @@ +Syms t,s
+disp('C1= C2=8 microfarad,R1=9 megaohm,R2=5 megaohm,V0=75 volts')
+disp('i2(s) the current through resistor R2 is')
+disp('i2(s)=0.208*10^-6/(s+0.045)(s+.0077)')
+[a]=pfss((.208*10^-6*s^0)/(s+0.045)*(s+.0077))
+b=ilt(a(1),s,t)
+//c=ilaplace(a(2),s,t)
+d=b
+disp(d,"By thevenins theorem the current is ")
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