diff options
Diffstat (limited to 'Working_Examples/215')
267 files changed, 1435 insertions, 0 deletions
diff --git a/Working_Examples/215/CH10/EX10.1/Figure10_1.jpg b/Working_Examples/215/CH10/EX10.1/Figure10_1.jpg Binary files differnew file mode 100755 index 0000000..b04ab78 --- /dev/null +++ b/Working_Examples/215/CH10/EX10.1/Figure10_1.jpg diff --git a/Working_Examples/215/CH10/EX10.1/Figure10_1_xcos.jpg b/Working_Examples/215/CH10/EX10.1/Figure10_1_xcos.jpg Binary files differnew file mode 100755 index 0000000..64c6983 --- /dev/null +++ b/Working_Examples/215/CH10/EX10.1/Figure10_1_xcos.jpg diff --git a/Working_Examples/215/CH10/EX10.1/ex10_1.xcos b/Working_Examples/215/CH10/EX10.1/ex10_1.xcos new file mode 100755 index 0000000..a12314e --- /dev/null +++ b/Working_Examples/215/CH10/EX10.1/ex10_1.xcos @@ -0,0 +1 @@ +<?xml version="1.0" encoding="UTF-8"?><XcosDiagram background="-1" finalIntegrationTime="10.0" title="ex10_1"><!--Xcos - 1.0 - scilab-5.5.2 - 20160406 2040--><mxGraphModel as="model"><root><mxCell id="-1fad1256:134d7ff92c3:-7ffd"/><mxCell id="-1fad1256:134d7ff92c3:-7ffe" 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\ No newline at end of file diff --git a/Working_Examples/215/CH10/EX10.4/ex10_4.sce b/Working_Examples/215/CH10/EX10.4/ex10_4.sce new file mode 100755 index 0000000..0d091c8 --- /dev/null +++ b/Working_Examples/215/CH10/EX10.4/ex10_4.sce @@ -0,0 +1,14 @@ +clc
+//Example 10.4
+//Determine phasor current and time-domain current
+printf("Given")
+disp('Voltage is 8(-50 deg),Frequency is 100rad/s,Inductance is 4H')
+L=4;
+w=100;
+Vamp=8;Vang=-50;
+//Let current be I
+Iamp=Vamp/(w*L)
+Iang=-90+Vang
+printf("I=%3.2f(%d deg) A \n",Iamp,Iang)
+//In time domain
+printf("i(t)=%3.2f *cos(%d*t%d) A",Iamp,w,Iang);
\ No newline at end of file diff --git a/Working_Examples/215/CH10/EX10.6/Figure10_6.jpg b/Working_Examples/215/CH10/EX10.6/Figure10_6.jpg Binary files differnew file mode 100755 index 0000000..a2686fa --- /dev/null +++ b/Working_Examples/215/CH10/EX10.6/Figure10_6.jpg diff --git a/Working_Examples/215/CH10/EX10.6/Figure10_6_xcos.jpg b/Working_Examples/215/CH10/EX10.6/Figure10_6_xcos.jpg Binary files differnew file mode 100755 index 0000000..4ecc4e8 --- /dev/null +++ b/Working_Examples/215/CH10/EX10.6/Figure10_6_xcos.jpg diff --git a/Working_Examples/215/CH10/EX10.6/ex10_6.xcos b/Working_Examples/215/CH10/EX10.6/ex10_6.xcos new file mode 100755 index 0000000..3a58d14 --- /dev/null +++ b/Working_Examples/215/CH10/EX10.6/ex10_6.xcos @@ -0,0 +1 @@ +<?xml version="1.0" encoding="UTF-8"?><XcosDiagram background="-1" finalIntegrationTime="10.0" title="ex10_6"><!--Xcos - 1.0 - scilab-5.5.2 - 20160406 2040--><mxGraphModel as="model"><root><mxCell id="-1fad1256:134d7ff92c3:-7ef8"/><mxCell 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\ No newline at end of file diff --git a/Working_Examples/215/CH11/EX11.1/ex11_1.sce b/Working_Examples/215/CH11/EX11.1/ex11_1.sce new file mode 100755 index 0000000..57ef313 --- /dev/null +++ b/Working_Examples/215/CH11/EX11.1/ex11_1.sce @@ -0,0 +1,27 @@ +clc
+//Example 11.1
+//Calculate the powerr absorbed by capacitor and resistor
+printf("Given")
+disp('Capacitor 5uF, Resistor 200 ohm, Voltage source is 40+60*u(t)')
+C=5*10^-6;R=200;
+//For t<0 the value of u(t) is zero hence at t=0- the value of voltage is 40V
+//For t=0+ the voltage is 100V
+//At t=0+ the capacitor cannot charge instantaneously hence resistor voltage is 60V
+disp('For t=0+')
+VR=60;
+i0=VR/R
+T=R*C
+t=1.2*10^-3
+disp('The value of current is i(t)=i0*exp(-t/T)')
+ival=i0*exp(-t/T)
+printf("Value of resistor current at 1.2ms=%3.2f mA \n",ival*10^3)
+//Let PR be the power absorbed by the resistor
+PR=ival^2*R
+printf("Value of resistive power at 1.2ms=%3.2f W \n",PR)
+//Out of the 100V available at t>0 the voltage across the capacitor is
+disp('vC(t)=100-60*exp(-t/T)')
+vCval=100-60*exp(-t/T)
+printf("Value of capacitor voltage at 1.2ms=%3.2f V \n",vCval)
+//Let PC be the power absorbed by the capacitor
+PC=ival*vCval
+printf("Value of capacitive power at 1.2ms=%3.2f W \n",PC)
\ No newline at end of file diff --git a/Working_Examples/215/CH11/EX11.2/Figure11_21.jpg b/Working_Examples/215/CH11/EX11.2/Figure11_21.jpg Binary files differnew file mode 100755 index 0000000..9d428ea --- /dev/null +++ b/Working_Examples/215/CH11/EX11.2/Figure11_21.jpg diff --git a/Working_Examples/215/CH11/EX11.2/Figure11_22.jpg b/Working_Examples/215/CH11/EX11.2/Figure11_22.jpg Binary files differnew file mode 100755 index 0000000..64962b8 --- /dev/null +++ b/Working_Examples/215/CH11/EX11.2/Figure11_22.jpg diff --git a/Working_Examples/215/CH11/EX11.2/ex11_2.sce b/Working_Examples/215/CH11/EX11.2/ex11_2.sce new file mode 100755 index 0000000..d9afdb0 --- /dev/null +++ b/Working_Examples/215/CH11/EX11.2/ex11_2.sce @@ -0,0 +1,29 @@ +clc
+//Example 11.2
+//Calculate the average power
+printf("Given")
+disp('v=4*cos(%pi/6*t), V=4(0 deg), Z=2(60 deg)')
+Vamp=4;Vang=0;Zamp=2;Zang=60;
+//Let I be the phasor current
+Iamp=Vamp/Zamp
+Iang=Vang-Zang
+P=0.5*Vamp*Zamp*cos((Zang*%pi)/180)
+printf("P=%d W \n",P);
+t=-1:1:15
+t1=-3:1:12
+v=Vamp*cos(%pi/6*t)
+//i=2*cos((%pi/6)*t-(%pi/3))
+i=Iamp*cos(%pi/6*t+((Iang*%pi)/180))
+figure
+a= gca ();
+plot (t,v,t,i)
+xtitle ('v,i vs t' ,'t' ,'v,i');
+a. thickness = 2;
+//Instantaneous power p=v*i
+//On solving
+p=2+4*cos(%pi/3*t+((Iang*%pi)/180))
+figure
+a= gca ();
+plot (t,p)
+xtitle ('p vs t' ,'t' ,'p');
+a. thickness = 2;
diff --git a/Working_Examples/215/CH11/EX11.3/ex11_3.sce b/Working_Examples/215/CH11/EX11.3/ex11_3.sce new file mode 100755 index 0000000..4fb84d3 --- /dev/null +++ b/Working_Examples/215/CH11/EX11.3/ex11_3.sce @@ -0,0 +1,11 @@ +clc
+//Example 11.3
+//Calculate the Average Power
+printf("Given")
+disp('ZL=8-i*11 ohm, I=5(20 deg)A')
+R=8;Iamp=5;
+//We need to calculate the average power
+//In the calculation of average power the resistance part of impedace only occurs
+//Let P be the average power
+P=0.5*Iamp^2*R
+printf("Average Power=%d W \n",P)
\ No newline at end of file diff --git a/Working_Examples/215/CH11/EX11.4/Figure11_41.jpg b/Working_Examples/215/CH11/EX11.4/Figure11_41.jpg Binary files differnew file mode 100755 index 0000000..626b297 --- /dev/null +++ b/Working_Examples/215/CH11/EX11.4/Figure11_41.jpg diff --git a/Working_Examples/215/CH11/EX11.4/Figure11_42.jpg b/Working_Examples/215/CH11/EX11.4/Figure11_42.jpg Binary files differnew file mode 100755 index 0000000..47abc90 --- /dev/null +++ b/Working_Examples/215/CH11/EX11.4/Figure11_42.jpg diff --git a/Working_Examples/215/CH11/EX11.4/ex11_4.sce b/Working_Examples/215/CH11/EX11.4/ex11_4.sce new file mode 100755 index 0000000..d51e615 --- /dev/null +++ b/Working_Examples/215/CH11/EX11.4/ex11_4.sce @@ -0,0 +1,21 @@ +clc
+//Example 11.4
+//Calculate the Average power absorbed and average power supplied by source
+//From figure 11.6
+//By applying mesh analysis
+I1mag=11.18;I1ang=-63.43;I2mag=7.071;I2ang=-45;R=2;Vleft=20;Vright=10;
+//Current through 2 ohm resistor
+printf("I1-I2=%d(%d ang) A \n",5,-90)
+//Average power absorbed by resistor
+PR=0.5*5^2*R
+printf("Average power absorbed by resistor=%d W \n",PR)
+//Power supplied by left source
+Pleft=0.5*Vleft*I1mag*cos(0-I1ang*%pi/180)
+//Power supplied by right source
+Pright=0.5*Vright*I2mag*cos(0+I2ang*%pi/180)
+printf("Power supplied by sources \t Pleft=%d W \t Pright=%3.1f W",Pleft,Pright);
+
+
+
+
+
diff --git a/Working_Examples/215/CH11/EX11.6/ex11_6.sce b/Working_Examples/215/CH11/EX11.6/ex11_6.sce new file mode 100755 index 0000000..dc3252c --- /dev/null +++ b/Working_Examples/215/CH11/EX11.6/ex11_6.sce @@ -0,0 +1,9 @@ +clc
+//Example 11.6
+//Calculate the Average power
+printf("Given")
+disp('Resistor value is 4 ohm, i1=2*cos(10t)-3*cos(20t) A')
+R=4;im1=2;im2=-3;
+//Let P be the average power delievered
+P=0.5*im1^2*R+0.5*im2^2*R
+printf("Average power=%d W",P)
diff --git a/Working_Examples/215/CH11/EX11.7/ex11_7.sce b/Working_Examples/215/CH11/EX11.7/ex11_7.sce new file mode 100755 index 0000000..d64e258 --- /dev/null +++ b/Working_Examples/215/CH11/EX11.7/ex11_7.sce @@ -0,0 +1,10 @@ +clc
+//Example 11.7
+//Calculate the Average power
+printf("Given")
+disp('Resistor value is 4 ohm, i2=2*cos(10t)-3*cos(10t) A')
+disp('On solving we get i2=-cos(10t)')
+R=4;im=-1
+//Let P be the average power delievered
+P=0.5*im^2*R
+printf("Average power=%d W",P)
\ No newline at end of file diff --git a/Working_Examples/215/CH11/EX11.8/ex11_8.sce b/Working_Examples/215/CH11/EX11.8/ex11_8.sce new file mode 100755 index 0000000..4e38138 --- /dev/null +++ b/Working_Examples/215/CH11/EX11.8/ex11_8.sce @@ -0,0 +1,26 @@ +clc
+//Example 11.8
+//Calculate average power, power supplied by source and the power factor
+printf("Given")
+disp('Voltage source is 60 V,Load values are 2-i ohm and 1+5i ohm')
+Vamp=60;Vang=0;
+//Let Z be the cobined resistance
+Z=2-%i+1+5*%i
+[Zmag Zph]=polar(Z)
+Isamp=Vamp/Zmag;
+Isang=Vang-Zph;
+printf("Ieff=%3.0f A rms and angle of Is is %3.2f degree\n",Isamp,(Isang*180)/%pi);
+//Let Pupper be the power delievered to the upper load
+Rtop=2;
+Pupper=Isamp^2*Rtop
+printf("Average Power delievered to the top load=%3.0f W \n",Pupper)
+//Let Plower be the power delievered to the lower load
+Rright=1;
+Plower=Isamp^2*Rright
+printf("Average Power delievered to the right load=%3.0f W \n",Plower)
+//Let Papp be the apparent power
+Papp=Vamp*Isamp
+printf("Apparent Power =%3.0f VA \n",Papp)
+//Let pf be the power factor
+pf=(Pupper+Plower)/Papp
+printf("power factor=%3.1f lag \n",pf)
\ No newline at end of file diff --git a/Working_Examples/215/CH11/EX11.9/ex11_9.sce b/Working_Examples/215/CH11/EX11.9/ex11_9.sce new file mode 100755 index 0000000..e2aad97 --- /dev/null +++ b/Working_Examples/215/CH11/EX11.9/ex11_9.sce @@ -0,0 +1,34 @@ +clc
+//Example 11.9
+printf("Given")
+disp('Power of induction motor=50kW ,power factor is 0.8 lag,Source voltage is 230V')
+disp('The wish of the consumer is to raise the power factor to 0.95 lag')
+//Let S1 be the complex power supplied to the indiction motor
+V=230;Pmag=50*10^3;pf=0.8;
+Pang=(acos(pf)*180)/%pi
+S1mag=Pmag/pf
+S1ph=Pang
+x=S1mag * cos (( Pang * %pi ) /180) ;
+y=S1mag * sin (( Pang * %pi ) /180) ;
+z= complex (x,y)
+disp(z ,'S1=')
+//To achieve a power factor of 0.95
+pf1=0.95
+//Now the total complex power be S
+P1ang=(acos(pf1)*180)/%pi
+Smag=Pmag/pf1
+Sph=P1ang
+a=Smag * cos (( P1ang * %pi ) /180) ;
+b=Smag * sin (( P1ang * %pi ) /180) ;
+c= complex (a,b)
+disp(c,'S=')
+//Let S2 be the complex power drawn by the corrective load
+S2=c-z
+disp(S2,'S2=')
+disp('Let a phase angle of voltage source selected be 0 degree')
+//Let I2 be the current
+I2=-S2/V
+//Let Z2 be the impedance of corrective load
+Z2=V/I2
+disp(Z2,'Z2=')
+
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\ No newline at end of file diff --git a/Working_Examples/215/CH12/EX12.2/ex12_2.sce b/Working_Examples/215/CH12/EX12.2/ex12_2.sce new file mode 100755 index 0000000..b15fba9 --- /dev/null +++ b/Working_Examples/215/CH12/EX12.2/ex12_2.sce @@ -0,0 +1,29 @@ +clc
+//Example 12.2
+//Calculate total power dissipated
+disp('Given')
+disp('Van=200 with angle 0 degree and Zp=100with angle 60 degree')
+Zpamp=100;Zpang=60
+//Since one of the phase voltage is given, we need to find other phase voltages
+Vanamp=200;Vbnamp=200 ; Vcnamp=200;
+Vanang=0;Vbnang=-120;Vcnang=-240;
+disp('The phase voltages are')
+printf("Van=%d /_%d deg V\tVbn=%d /_%d deg V\tVcn=%d /_%d deg V\t",Vanamp,Vanang,Vbnamp,Vbnang,Vcnamp,Vcnang)
+
+//Now we will find line voltages
+//Let line voltage be Vline
+Vline=200*sqrt(3)
+//By constructing a phasor diagram
+disp('The line voltages are')
+printf("\n Vab=%d /_%d deg V\tVbc=%d /_%d deg V\tVca=%d /_%d deg V\t",Vline,30,Vline,-90,Vline,-210)
+
+//Let the line current be IaA
+IaAamp=Vanamp/Zpamp
+IaAang=Vanang-Zpang
+//Since the given system is a balanced three phase system
+//From phasor diagram as shown in figure 12.16
+disp('The line currents are')
+printf("\n IaA=%d /_%d deg V\tIbB=%d /_%d deg V\tIcC=%d /_%d deg V\t",IaAamp,IaAang,IaAamp,IaAang-120,IaAamp,IaAang-240)
+//Let power absorbeed by phase A is PAN
+PAN=Vanamp*IaAamp*cos(((Vanang+IaAang)*%pi)/180)
+printf("\n Total average power = %d W",3*PAN)
diff --git a/Working_Examples/215/CH12/EX12.3/ex12_3.sce b/Working_Examples/215/CH12/EX12.3/ex12_3.sce new file mode 100755 index 0000000..2f4a0a3 --- /dev/null +++ b/Working_Examples/215/CH12/EX12.3/ex12_3.sce @@ -0,0 +1,16 @@ +clc
+//Example 12.3
+//Calculate the line current and phase impedance
+disp('Given')
+disp('Line voltage = 300V, Power factor=0.8(lead), Phase power = 1200W')
+Vline=300;pf=0.8;PW=1200;
+Vp=Vline/sqrt(3)
+PerPhpower=PW/3;
+//Line current can be found as
+IL=PerPhpower/(pf*Vp)
+printf("Line current= %3.2f A \n",IL)
+//Let Zp be the phase impedance
+Zpmag=Vp/IL
+//Sice power factor is 'leading'
+Zpang=-(acos(0.8)*180)/%pi
+printf("Phase impedance = %d/_%3.2f deg ohm",Zpmag,Zpang);
\ No newline at end of file diff --git a/Working_Examples/215/CH12/EX12.4/ex12_4.sce b/Working_Examples/215/CH12/EX12.4/ex12_4.sce new file mode 100755 index 0000000..69de13e --- /dev/null +++ b/Working_Examples/215/CH12/EX12.4/ex12_4.sce @@ -0,0 +1,21 @@ +clc
+//Example 12.4
+//Calculate the line current
+//Continuing from example 12.3
+Vp=300/sqrt(3);
+IL=2.89;pf=0.8
+disp('A balanced 600W lighting load is added in parallel with the existing load')
+disp('600W if balanced then 200W will be consumed by each phase')
+Vpadd=200;
+//From figure 12.17
+I1=Vpadd/Vp
+disp('Load current is unchanged')
+I2mag=IL
+I2ph=(acos(pf)*180)/%pi
+x=I2mag * cos (( I2ph * %pi ) /180) ;
+y=I2mag * sin (( I2ph * %pi ) /180) ;
+z= complex (x,y)
+disp(z)
+ILnew=I1+z
+[ILmag ILph]=polar(ILnew)
+printf("Line current=%3.2f /_%3.2f deg A \n ",ILmag,ILph*(180/%pi));
\ No newline at end of file diff --git a/Working_Examples/215/CH12/EX12.5/ex12_5.sce b/Working_Examples/215/CH12/EX12.5/ex12_5.sce new file mode 100755 index 0000000..3a8a555 --- /dev/null +++ b/Working_Examples/215/CH12/EX12.5/ex12_5.sce @@ -0,0 +1,18 @@ +clc
+//Example 12.5
+//Calculate amplitude of line current
+disp('Given')
+disp('Line voltage = 300V, Power factor=0.8(lag), Phase power = 1200W')
+Vline=300;pf=0.8;PW=1200;
+disp('1200W will be consumed as 400W in each phase')
+Vp=400
+//Phase current be Ip
+Ip=Vp/(Vline*pf)
+//Let amplitude of line current be IL
+IL=Ip*sqrt(3)
+printf("Line current=%3.2f A \n",IL)
+//Let Zp be the phase impedance
+Zpmag=Vline/Ip
+//Sice power factor is 'lagging'
+Zpang=(acos(0.8)*180)/%pi
+printf("Phase impedance = %d(%3.2f deg)ohm",Zpmag,Zpang);
\ No newline at end of file diff --git a/Working_Examples/215/CH12/EX12.6/ex12_6.sce b/Working_Examples/215/CH12/EX12.6/ex12_6.sce new file mode 100755 index 0000000..acc556e --- /dev/null +++ b/Working_Examples/215/CH12/EX12.6/ex12_6.sce @@ -0,0 +1,20 @@ +clc
+//Example 12.6
+//Calculate amplitude of line current
+disp('Given')
+disp('Line voltage = 300V, Power factor=0.8(lag), Phase power = 1200W')
+Vline=300;pf=0.8;PW=1200;
+Vph=Vline/sqrt(3)
+disp('1200W will be consumed as 400W in each phase')
+Vp=400
+//Let phase current be Ip
+Ip=Vp/(Vph*pf)
+printf("Phase current=%3.2f A \n",Ip)
+//Let Zp be the phase impedance
+Zpmag=Vph/Ip
+//Sice power factor is 'lagging'
+Zpang=(acos(0.8)*180)/%pi
+printf("Phase impedance = %d(%3.2f deg)ohm\n",Zpmag,Zpang);
+//PW=sqrt(3)*VL*IL*pf
+IL=PW/(sqrt(3)*Vline*pf)
+printf("Line current=%3.2f A \n",IL)
\ No newline at end of file diff --git a/Working_Examples/215/CH12/EX12.7/ex12_7.sce b/Working_Examples/215/CH12/EX12.7/ex12_7.sce new file mode 100755 index 0000000..a0ff8e6 --- /dev/null +++ b/Working_Examples/215/CH12/EX12.7/ex12_7.sce @@ -0,0 +1,34 @@ +clc
+//Example 12.7
+//Determine wattmeter reading and total power drawn by the load
+disp('Given')
+disp('Vab=230(0 deg)V')
+Vline=230
+//Since positive phase sequence is used
+disp('The line voltages are')
+printf("\n Vab=%d (%d deg)V\tVbc=%d (%d deg) V\tVca=%d (%d deg)V\t",Vline,0,Vline,-120,Vline,120)
+Vacamp=Vline;
+Vacang=-60;
+Vbcamp=Vline;
+Vbcang=-120;
+//Now we will evaluate phase current
+//Let IaA be the phase current
+Vanamp=Vline/sqrt(3)
+Vanph=-30
+//From figure 12.28
+Zph=4+%i*15
+[Zphmag Zphang]=polar(Zph)
+IaAamp=Vanamp/Zphmag
+IaAang=Vanph-(Zphang*180)/%pi
+IbBang=IaAang+240
+printf("\nIaA=%3.2f(%3.2f deg)A\n",IaAamp,IaAang);
+//Power rating of each wattmeter is now calculated
+//Power measured by wattmeter #1
+P1=Vline*IaAamp*cos(((Vacang-IaAang)*%pi)/180)
+printf("P1=%d W \n",P1)
+//Power measured by wattmeter #2
+P2=Vline*IaAamp*cos(((Vbcang-IbBang)*%pi)/180)
+printf("P2=%3.2f W \n",P2)
+//Net power be P
+P=P1+P2
+printf("P=%3.2f W \n",P)
\ No newline at end of file diff --git a/Working_Examples/215/CH13/EX13.2/ex13_2.sce b/Working_Examples/215/CH13/EX13.2/ex13_2.sce new file mode 100755 index 0000000..ef2b56b --- /dev/null +++ b/Working_Examples/215/CH13/EX13.2/ex13_2.sce @@ -0,0 +1,22 @@ +clc
+//Example 13.2
+disp('Given')
+disp('Input voltage is 10V')
+Viamp=10
+//From figure 13.7
+//Writing the left mesh equations
+disp('(1+10i)*I1-90i*I2=10')
+//Writing the right mesh equations
+disp('(400+1000i)*I2-90i*I1=0')
+i=%i
+A=[1+10*i -90*i;-90*i 400+1000*i]
+i2mat=[1+10*i 10; -90*i 0]
+//Find i2
+i2=det(i2mat)/det(A)
+[mag Theta]=polar(i2)
+Theta=(Theta*180)/%pi
+//The value of resistor is 400 ohm
+R=400;
+//Let V=V2/V1
+Vamp=R*mag/Viamp
+printf("Ratio of output voltage to input is %3.2f with angle %3.2f degrees",Vamp,Theta);
\ No newline at end of file diff --git a/Working_Examples/215/CH13/EX13.4/ex13_4.sce b/Working_Examples/215/CH13/EX13.4/ex13_4.sce new file mode 100755 index 0000000..f342ef2 --- /dev/null +++ b/Working_Examples/215/CH13/EX13.4/ex13_4.sce @@ -0,0 +1,19 @@ +clc
+//Example 13.4
+disp('Given')
+disp('L1=0.4H L2=2.5H k=0.6 i1=4i2=20*cos(500t-20)mA')
+L1=0.4;L2=2.5;k=0.6;
+disp('a)')
+t=0;
+i2=5*cos(500*t-(20*%pi)/180)
+printf("i2(0)=%3.2f mA \n",i2)
+disp('b)')
+M=k*sqrt(L1*L2)
+//v1(t)=L1*d/dt(i1)+M*d/dt(i2)
+v1=-L1*20*500*10^-3*sin(500*t-(20*%pi)/180)-M*5*500*10^-3*sin(500*t-(20*%pi)/180)
+printf("v1(0)=%3.2f V \n",v1)
+disp('c')
+//The total energy can be found as
+w=(L1*(4*i2)^2)/2+ (L2*(i2)^2)/2+M*(4*i2)*(i2)
+printf("w=%3.2f uJ \n",w)
+
diff --git a/Working_Examples/215/CH13/EX13.5/ex13_5.sce b/Working_Examples/215/CH13/EX13.5/ex13_5.sce new file mode 100755 index 0000000..ab7366d --- /dev/null +++ b/Working_Examples/215/CH13/EX13.5/ex13_5.sce @@ -0,0 +1,13 @@ +clc
+//Example 13.5
+printf("Given")
+disp('L1=30 mH L2=60 mH M=40 mH')
+L1=30*10^-3; L2=60*10^-3; M=40*10^-3;
+//The equivalent T network is
+UL=L1-M
+UR=L2-M
+CS=M
+printf("The T network has \n")
+printf("%d mH in the upper left arm\n",UL*10^3)
+printf("%3.0f mH in the upper right arm\n",UR*10^3)
+printf("%d mH in the center stem\n",CS*10^3)
\ No newline at end of file diff --git a/Working_Examples/215/CH13/EX13.6/ex13_6.sce b/Working_Examples/215/CH13/EX13.6/ex13_6.sce new file mode 100755 index 0000000..3fad804 --- /dev/null +++ b/Working_Examples/215/CH13/EX13.6/ex13_6.sce @@ -0,0 +1,15 @@ +clc
+//Example 13.6
+printf("Given")
+disp('L1=30 mH L2=60 mH M=40 mH')
+L1=30*10^-3; L2=60*10^-3; M=40*10^-3;
+//Let X=L1*L2-M^2
+X=L1*L2-M^2
+//The equivalent PI network is
+LA=X/(L2-M)
+LB=X/M
+LC=X/(L1-M)
+printf("The PI network has \n")
+printf("LA=%3.0f mH\n",LA*10^3)
+printf("LB=%3.0f mH \n",LB*10^3)
+printf("LC=%3.0f mH\n",LC*10^3)
\ No newline at end of file diff --git a/Working_Examples/215/CH13/EX13.7/Figure13_7.jpg b/Working_Examples/215/CH13/EX13.7/Figure13_7.jpg Binary files differnew file mode 100755 index 0000000..8f2f461 --- /dev/null +++ b/Working_Examples/215/CH13/EX13.7/Figure13_7.jpg diff --git a/Working_Examples/215/CH13/EX13.7/Figure13_7_xcos.jpg b/Working_Examples/215/CH13/EX13.7/Figure13_7_xcos.jpg Binary files differnew file mode 100755 index 0000000..7a04312 --- /dev/null +++ b/Working_Examples/215/CH13/EX13.7/Figure13_7_xcos.jpg diff --git a/Working_Examples/215/CH13/EX13.7/ex13_7.xcos b/Working_Examples/215/CH13/EX13.7/ex13_7.xcos new file mode 100755 index 0000000..d175425 --- /dev/null +++ b/Working_Examples/215/CH13/EX13.7/ex13_7.xcos @@ -0,0 +1 @@ +<?xml version="1.0" encoding="UTF-8"?><XcosDiagram background="-1" finalIntegrationTime="30.0" title="ex13_7"><!--Xcos - 1.0 - scilab-5.5.2 - 20160406 2040--><mxGraphModel as="model"><root><mxCell id="26015439:134e2b4e9d8:-7fd8"/><mxCell 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\ No newline at end of file diff --git a/Working_Examples/215/CH13/EX13.8/ex13_8.sce b/Working_Examples/215/CH13/EX13.8/ex13_8.sce new file mode 100755 index 0000000..50f1928 --- /dev/null +++ b/Working_Examples/215/CH13/EX13.8/ex13_8.sce @@ -0,0 +1,13 @@ +clc
+//Example 13.8
+disp('Given')
+disp('Vin=50V Zg=100 ohm')
+Vin=50;Zg=100;
+//From figure 13.32
+disp('When the secondary circuit and ideal transformer is replaced by a Thevenin equivalent then the primary circuit sees a 100 ohm impedance')
+//The turns ratio is a
+a=10;
+disp('We place the secondary circuit and ideal transformer by a Thevenin equivalent circuit')
+Vth=-a*Vin
+Zth=(-a)^2*Zg
+printf("The secondary circuit has voltage source %d V rms with %d kohm resistance in series with it along with %d kohm load resistance",Vth,Zth*10^-3,10)
\ No newline at end of file diff --git a/Working_Examples/215/CH14/EX14.10/ex14_10.sce b/Working_Examples/215/CH14/EX14.10/ex14_10.sce new file mode 100755 index 0000000..e3d28c7 --- /dev/null +++ b/Working_Examples/215/CH14/EX14.10/ex14_10.sce @@ -0,0 +1,7 @@ +clc
+//Example 14.10
+//Install Symbolic toolbox
+//Determine the transform of rectangular pulse
+syms t s
+v=integ(exp(-s*t),t,2,%inf)-integ(exp(-s*t),t,5,%inf)
+disp(v,'V(s)=')
\ No newline at end of file diff --git a/Working_Examples/215/CH14/EX14.11/ex14_11.sce b/Working_Examples/215/CH14/EX14.11/ex14_11.sce new file mode 100755 index 0000000..566e19f --- /dev/null +++ b/Working_Examples/215/CH14/EX14.11/ex14_11.sce @@ -0,0 +1,14 @@ +clc
+//Example 14.11
+//Install Symbolic toolbox
+//Calculate f(inf)
+syms s t ;
+disp('Given function is f(t)=1-exp(-a*t)')
+u=laplace(1)
+v=laplace(exp(-2*t))
+F=u-v
+x=s*F
+//From final value theorem
+y=limit(x,s,0)
+disp(y,'f(inf)=')
+
diff --git a/Working_Examples/215/CH14/EX14.2/ex14_2.sce b/Working_Examples/215/CH14/EX14.2/ex14_2.sce new file mode 100755 index 0000000..9ea9a08 --- /dev/null +++ b/Working_Examples/215/CH14/EX14.2/ex14_2.sce @@ -0,0 +1,8 @@ +//Example 14.2
+//Install Symbolic toolbox
+//Find the Laplace transform
+syms t s
+clc
+z=integ(2*exp(-s*t),t,3,%inf)
+//The second term will result in zero
+disp(z,'F(s)=')
\ No newline at end of file diff --git a/Working_Examples/215/CH14/EX14.3/ex14_3.sce b/Working_Examples/215/CH14/EX14.3/ex14_3.sce new file mode 100755 index 0000000..d5e6adb --- /dev/null +++ b/Working_Examples/215/CH14/EX14.3/ex14_3.sce @@ -0,0 +1,11 @@ +clc
+//Example 14.3
+//Install Symbolic toolbox
+//Find the Inverse Laplace transform
+syms s
+a=7/s
+b=31/(s+17)
+x=ilaplace(a)
+y=ilaplace(b)
+g=x-y
+disp(g,'g(t)=')
\ No newline at end of file diff --git a/Working_Examples/215/CH14/EX14.4/ex14_4.sce b/Working_Examples/215/CH14/EX14.4/ex14_4.sce new file mode 100755 index 0000000..40aa3c0 --- /dev/null +++ b/Working_Examples/215/CH14/EX14.4/ex14_4.sce @@ -0,0 +1,12 @@ +clc
+//Example 14.4
+//Install Symbolic toolbox
+//Find the Inverse Laplace transform
+syms s t
+a=2
+b=4/s
+x=ilaplace(b)
+//Inverse laplace transform of a constant is
+disp('inverse laplace(2)=2*delta(t)')
+disp('Answer is')
+disp(x+'2*delta(t)')
diff --git a/Working_Examples/215/CH14/EX14.5/ex14_5.sce b/Working_Examples/215/CH14/EX14.5/ex14_5.sce new file mode 100755 index 0000000..7caf6fe --- /dev/null +++ b/Working_Examples/215/CH14/EX14.5/ex14_5.sce @@ -0,0 +1,12 @@ +clc
+//Example 14.5
+//Install Symbolic toolbox
+//Find the Inverse Laplace transform
+syms s
+s=%s;
+P =(7*s+5)/(s^2+s);
+Pp=pfss (P)
+p1=ilaplace (Pp(1))
+p2=ilaplace (Pp(2))
+p=p1+p2
+disp(p,'p(t)=');
\ No newline at end of file diff --git a/Working_Examples/215/CH14/EX14.6/ex14_6.sce b/Working_Examples/215/CH14/EX14.6/ex14_6.sce new file mode 100755 index 0000000..9155f12 --- /dev/null +++ b/Working_Examples/215/CH14/EX14.6/ex14_6.sce @@ -0,0 +1,12 @@ +clc
+//Example 14.6
+//Install Symbolic toolbox
+//Find the Inverse Laplace transform
+syms s
+s=%s;
+V =2/(s^3+12*s^2+36*s);
+Vp=pfss (V)
+v1=ilaplace (Vp(1))
+v2=ilaplace (Vp(2))
+v=v1+v2
+disp(v,'v(t)=');
\ No newline at end of file diff --git a/Working_Examples/215/CH14/EX14.7/ex14_7.sce b/Working_Examples/215/CH14/EX14.7/ex14_7.sce new file mode 100755 index 0000000..1d50710 --- /dev/null +++ b/Working_Examples/215/CH14/EX14.7/ex14_7.sce @@ -0,0 +1,16 @@ +clc
+//Example 14.7
+//Install Symbolic toolbox
+//Find the current through 5 ohm resistor
+syms s
+s=%s
+//From figure 14.3
+//Writing the KVL equation and taking the Laplace transform
+I=1.5/(s*(s+2))+5/(s+2)
+I1=1.5/(s*(s+2))
+I2=5/(s+2)
+I1p=pfss(I1)
+i1=ilaplace(I1p(1))
+i2=ilaplace(I1p(2)+I2)
+i=i1+i2
+disp(i,'i(t)=')
\ No newline at end of file diff --git a/Working_Examples/215/CH14/EX14.8/ex14_8.sce b/Working_Examples/215/CH14/EX14.8/ex14_8.sce new file mode 100755 index 0000000..d163f8c --- /dev/null +++ b/Working_Examples/215/CH14/EX14.8/ex14_8.sce @@ -0,0 +1,11 @@ +clc
+//Example 14.8
+//Install Symbolic toolbox
+//Find the current for t>0
+syms s
+s=%s
+//From figure 14.5
+//Writing the KVL equation and taking the Laplace transform
+I=-2/(s+4)
+i=ilaplace(I)
+disp(i,'i(t)=')
\ No newline at end of file diff --git a/Working_Examples/215/CH14/EX14.9/ex14_9.sce b/Working_Examples/215/CH14/EX14.9/ex14_9.sce new file mode 100755 index 0000000..0c6166c --- /dev/null +++ b/Working_Examples/215/CH14/EX14.9/ex14_9.sce @@ -0,0 +1,16 @@ +clc
+//Example 14.9
+//Install Symbolic toolbox
+//Find the voltage v(t)
+syms s
+s=%s
+//From figure 14.6
+//Writing the KCL equation and taking the Laplace transform
+V=4/(s*(s+4))+9/(s+4)
+V1=4/(s*(s+4))
+V2=9/(s+4)
+V1p=pfss(V1)
+v1=ilaplace(V1p(1))
+v2=ilaplace(V1p(2)+V2)
+v=v1+v2
+disp(v,'v(t)=')
\ No newline at end of file diff --git a/Working_Examples/215/CH15/EX15.1/ex15_1.sce b/Working_Examples/215/CH15/EX15.1/ex15_1.sce new file mode 100755 index 0000000..c500be9 --- /dev/null +++ b/Working_Examples/215/CH15/EX15.1/ex15_1.sce @@ -0,0 +1,20 @@ +clc
+//Example 15.1
+//Install Symbolic toolbox
+//Calculate the voltage
+//From figure 15.3
+//Writing the KVL equation for the voltage and taking the Laplace transform
+syms s
+s=%s
+disp('V=(2*s*(s+9.5)/((s+8)*(s+0.5)))-2')
+//On solving
+V=(2*s-8)/((s+8)*(s+0.5))
+Vp=pfss (V)
+Vp1=ilaplace(Vp(1))
+Vp2=ilaplace(Vp(2))
+v=Vp1+Vp2
+disp(v,'v(t)=')
+
+
+
+
diff --git a/Working_Examples/215/CH15/EX15.10/ex15_10.sce b/Working_Examples/215/CH15/EX15.10/ex15_10.sce new file mode 100755 index 0000000..c507fa0 --- /dev/null +++ b/Working_Examples/215/CH15/EX15.10/ex15_10.sce @@ -0,0 +1,17 @@ +clc
+//Example 15.10
+//Since the input function is given the Laplace transform is found
+syms s t
+s=%s
+vin=6*exp(-t)
+Vin=laplace(vin)
+//Connecting the impulse voltage pulse to the circuit and converting to s-domain
+//If vin=delta(t)..the impulse source
+V0=2/((2/s)+2)
+//As source voltage is 1V
+H=V0
+V=Vin*H
+Vp=pfss ((6*s)/(s+1)^2)
+Vp1=ilaplace(Vp(1))
+v0=Vp1
+disp(v0,'v0(t)=')
\ No newline at end of file diff --git a/Working_Examples/215/CH15/EX15.2/ex15_2.sce b/Working_Examples/215/CH15/EX15.2/ex15_2.sce new file mode 100755 index 0000000..ff6b08c --- /dev/null +++ b/Working_Examples/215/CH15/EX15.2/ex15_2.sce @@ -0,0 +1,15 @@ +clc
+//Example 15.2
+//Install Symbolic toolbox
+//Calculate the voltage
+//Selecting the current based model
+//From figure 15.6(b)
+//Writing the KCL equation for the voltage and taking the Laplace transform
+syms s
+s=%s
+Vc=-2*(s-3)/(s*(s+2/3))
+Vcp=pfss (Vc)
+Vcp1=ilaplace(Vcp(1))
+Vcp2=ilaplace(Vcp(2))
+vc=Vcp1+Vcp2
+disp(vc,'vc=')
\ No newline at end of file diff --git a/Working_Examples/215/CH15/EX15.4/ex15_4.sce b/Working_Examples/215/CH15/EX15.4/ex15_4.sce new file mode 100755 index 0000000..fe351bf --- /dev/null +++ b/Working_Examples/215/CH15/EX15.4/ex15_4.sce @@ -0,0 +1,14 @@ +clc
+//Example 15.4
+//Install Symbolic toolbox
+//Calculate the voltage
+//From figure 15.9
+//Applying nodal equation and solving for vx
+syms s
+s=%s
+Vx=(10*s^2+4)/(s*(2*s^2+4*s+1))
+Vxp=pfss (Vx)
+Vxp1= ilaplace (Vxp(1))
+Vxp2= ilaplace (Vxp(2))
+vx=Vxp1+Vxp2
+disp(vx,'vx=')
diff --git a/Working_Examples/215/CH15/EX15.6/ex15_6.sce b/Working_Examples/215/CH15/EX15.6/ex15_6.sce new file mode 100755 index 0000000..039494c --- /dev/null +++ b/Working_Examples/215/CH15/EX15.6/ex15_6.sce @@ -0,0 +1,15 @@ +clc
+//Example 15.6
+//Install Symbolic toolbox
+//Calculate the voltage
+//Performing source transformatiom on the s-domain circuit
+//Solving for V(s)
+syms s
+s=%s
+V=(180*s^4)/((s^2+9)*(90*s^3+18*s^2+40*s+4))
+Vp=pfss (V)
+Vp1=ilaplace(Vp(1))
+Vp2=ilaplace(Vp(2))
+Vp3=ilaplace(Vp(3))
+v=Vp1+Vp2+Vp3
+disp(v,'v(t)=')
diff --git a/Working_Examples/215/CH15/EX15.9/ex15_9.sce b/Working_Examples/215/CH15/EX15.9/ex15_9.sce new file mode 100755 index 0000000..a3e04d8 --- /dev/null +++ b/Working_Examples/215/CH15/EX15.9/ex15_9.sce @@ -0,0 +1,14 @@ +clc
+//Example 15.9
+//Install Symbolic toolbox
+//Find the inverse Laplace transform
+syms s
+s=%s
+//Let a=1 and b=3
+a=1;b=3;
+V=1/((s+a)*(s+b))
+Vp=pfss (V)
+Vp1=ilaplace(Vp(1))
+Vp2=ilaplace(Vp(2))
+v=Vp1+Vp2
+disp(v,'v(t)=')
\ No newline at end of file diff --git a/Working_Examples/215/CH16/EX16.1/ex16_1.sce b/Working_Examples/215/CH16/EX16.1/ex16_1.sce new file mode 100755 index 0000000..2a112bd --- /dev/null +++ b/Working_Examples/215/CH16/EX16.1/ex16_1.sce @@ -0,0 +1,14 @@ +clc
+//Example 16.1
+disp('Given')
+disp('L=2.5mH Q0=5 C=0.01uF')
+L=2.5*10^-3; Q0=5; C=0.01*10^-6;
+w0=1/sqrt(L*C)
+printf("w0= %3.1f krad/s \n",w0*10^-3);
+f0=w0/(2*%pi)
+alpha=w0/(2*Q0)
+printf("alpha= %3.1f Np/s \n",alpha);
+wd=sqrt(w0^2-alpha^2)
+printf("wd= %3.1f krad/s \n",wd*10^-3);
+R=Q0/(w0*C)
+printf("R= %3.2f ohm \n",R*10^-3);
\ No newline at end of file diff --git a/Working_Examples/215/CH16/EX16.10/Figure16_10.jpg b/Working_Examples/215/CH16/EX16.10/Figure16_10.jpg Binary files differnew file mode 100755 index 0000000..e3cbf61 --- /dev/null +++ b/Working_Examples/215/CH16/EX16.10/Figure16_10.jpg diff --git a/Working_Examples/215/CH16/EX16.10/ex16_10.sce b/Working_Examples/215/CH16/EX16.10/ex16_10.sce new file mode 100755 index 0000000..323d398 --- /dev/null +++ b/Working_Examples/215/CH16/EX16.10/ex16_10.sce @@ -0,0 +1,11 @@ +clc
+//Example 16.10
+s=poly(0,'s')
+h=syslin('c',(10*s)/((1+s)*(s^2+20*s+10000)))
+disp(h)
+fmin=0.01
+fmax=10^4
+scf(1);clf;
+//Calculate Bode plot
+bode(h,fmin,fmax)
+
diff --git a/Working_Examples/215/CH16/EX16.11/ex16_11.sce b/Working_Examples/215/CH16/EX16.11/ex16_11.sce new file mode 100755 index 0000000..e5676bc --- /dev/null +++ b/Working_Examples/215/CH16/EX16.11/ex16_11.sce @@ -0,0 +1,17 @@ +clc
+//Example 16.11
+disp('Given')
+disp('A high pass filter with cutoff frequency of 3k Hz')
+//Cutoff frequency(wc)=1/(R*C)
+//Let us select some standard value of resistor
+disp('Let R=4.7k ohm')
+fc=3*10^3;R=4.7*10^3;
+wc=2*%pi*fc
+C=1/(R*wc)
+printf("\n C=%3.2f nF ",C*10^9);
+s=poly(0,'s')
+h=syslin('c',(R*C*s)/((1+s*R*C)))
+disp(h)
+HW = frmag(h,512);
+w=0: %pi /511: %pi ;
+plot(w,HW)
diff --git a/Working_Examples/215/CH16/EX16.12/ex16_12.sce b/Working_Examples/215/CH16/EX16.12/ex16_12.sce new file mode 100755 index 0000000..54fcd0b --- /dev/null +++ b/Working_Examples/215/CH16/EX16.12/ex16_12.sce @@ -0,0 +1,26 @@ +clc
+//Example 16.12
+disp('Given')
+disp('Bandwidth = 1M Hz and high frequency cutoff = 1.1M Hz')
+B=10^6;fH=1.1*10^6
+//B=fH-fL
+fL=fH-B
+printf("Low frequency cutoff fL= %d kHz \n",fL*10^-3);
+wL=2*%pi*fL
+printf("wL= %3.2f krad/s \n",wL*10^-3);
+wH=2*%pi*fH
+printf("wH= %3.3f Mrad/s \n",wH*10^-6);
+//Now we need to find values for R,L and C
+//Let X=1/LC
+B=2*%pi*(fH-fL)
+X=(wH-B/2)^2-(B^2/4)
+disp(X)
+disp('Let L=1H')
+L=1;
+C=1/(L*X)
+disp(C,'C=')
+//B=R/L
+R=L*B
+printf("R= %3.3f Mohm \n",R*10^-6);
+
+
diff --git a/Working_Examples/215/CH16/EX16.13/ex16_13.sce b/Working_Examples/215/CH16/EX16.13/ex16_13.sce new file mode 100755 index 0000000..a46d15d --- /dev/null +++ b/Working_Examples/215/CH16/EX16.13/ex16_13.sce @@ -0,0 +1,26 @@ +clc
+//Example 16.13
+disp('Given')
+disp('Voltage gain = 40dB and cutoff frequency = 10k Hz')
+Av_dB=40
+Av=10^(Av_dB/20)
+f=10*10^3
+B=2*%pi*f
+//From figure 16.41(a)
+disp('1+Rf/R1=100(Gain)')
+//From figure 16.41(b)
+//The transfer function is
+disp('V+= Vi*(1/sC)/(1+1/sC)')
+//Combining two transfer functions
+disp('V0 = Vi*(1/sC)/(1+1/sC)*(1+Rf/R1)')
+//The maximum value of the combined transfer function is
+disp('Maximum value is V0 = Vi*(1+Rf/R1)')
+disp('Let R1=1k ohm')
+R1=10^3
+Rf=(Av-1)*R1
+printf("Rf= %d kohm \n",Rf*10^-3);
+disp('C=1 uF')
+C=10^-6
+//B=1/(R2*C)
+R2=1/(C*B)
+printf("R2= %3.2f ohm \n",R2);
\ No newline at end of file diff --git a/Working_Examples/215/CH16/EX16.2/ex16_2.sce b/Working_Examples/215/CH16/EX16.2/ex16_2.sce new file mode 100755 index 0000000..40b43f4 --- /dev/null +++ b/Working_Examples/215/CH16/EX16.2/ex16_2.sce @@ -0,0 +1,21 @@ +clc
+//Example 16.2
+disp('Given')
+disp('R=40Kohm L=1H C=1/64 uF w=8.2krad/s')
+R=40*10^3; L=1; C=1/64 *10^-6; w=8.2*10^3;
+//The value of Q0 must be at least 5
+Q0=5;
+w0=1/sqrt(L*C)
+printf("w0= %3.1f krad/s \n",w0*10^-3);
+f0=w0/(2*%pi)
+B=w0/Q0
+printf("Bandwidth= %3.1f krad/s \n",B*10^-3);
+//Number of half bandwidths be N
+N=2*(w-w0)/B
+disp(N)
+//Admittance Y(s)=(1+i*N)/R
+//Finding the magnitude and angle
+magY=sqrt(1+N^2)/R
+angY=atan(N)*(180/%pi)
+disp(angY,'angY=')
+printf("admittance value=%3.2f uS",magY*10^6)
\ No newline at end of file diff --git a/Working_Examples/215/CH16/EX16.3/ex16_3.sce b/Working_Examples/215/CH16/EX16.3/ex16_3.sce new file mode 100755 index 0000000..f81eeff --- /dev/null +++ b/Working_Examples/215/CH16/EX16.3/ex16_3.sce @@ -0,0 +1,24 @@ +clc
+//Example 16.3
+disp('Given')
+disp('R=10 ohm L=2mH C=200 nF w=48 krad/s vs=100*cos(wt) mV')
+R=10; L=2*10^-3; C=200*10^-9; w=48*10^3;
+vsamp=100;
+w0=1/sqrt(L*C)
+printf("w0= %3.1f krad/s \n",w0*10^-3);
+Q0=w0*L/R
+printf("Q0=%d \n",Q0)
+B=w0/Q0
+printf("Bandwidth= %3.1f krad/s \n",B*10^-3);
+//Number of half bandwidths be N
+N=2*(w-w0)/B
+disp(N)
+//Impedance Z(s)=(1+i*N)*R
+//Finding the magnitude and angle
+magZ=sqrt(1+N^2)*R
+angZ=atan(N)*(180/%pi)
+disp(angZ,'angZ=')
+printf("Equivalent impedance value=%3.2f ohm \n",magZ)
+//Approx current magnitude is
+Iamp=vsamp/magZ
+printf("\n Approx current magnitude= %3.2f mA \n",Iamp);
\ No newline at end of file diff --git a/Working_Examples/215/CH16/EX16.4/ex16_4.sce b/Working_Examples/215/CH16/EX16.4/ex16_4.sce new file mode 100755 index 0000000..3f6628e --- /dev/null +++ b/Working_Examples/215/CH16/EX16.4/ex16_4.sce @@ -0,0 +1,17 @@ +clc
+//Example 16.4
+disp('Given')
+disp('R1=2 ohm R2=3 ohm L=1H C=125mF')
+R1=2;R2=3 ; L=1;C=125*10^-3;
+w0=sqrt(1/(L*C)-(R1/L)^2)
+printf("w0=%d rad/s \n",w0)
+//Input admittance is 1/R2+i*w*C+1/(R+I*w*L)
+Y=1/3+%i/4+1/(2+%i*2)
+printf("Y= %3.4f S \n",Y)
+//Now input impedance at resonance
+Z=1/Y
+printf("Z= %3.4f ohm \n",Z)
+//Resonant frequency f=1/sqrt(L*C)
+f=1/sqrt(L*C)
+printf("f=%3.2f rad/s \n",f);
+
diff --git a/Working_Examples/215/CH16/EX16.5/ex16_5.sce b/Working_Examples/215/CH16/EX16.5/ex16_5.sce new file mode 100755 index 0000000..b3b172d --- /dev/null +++ b/Working_Examples/215/CH16/EX16.5/ex16_5.sce @@ -0,0 +1,13 @@ +clc
+//Example 16.5
+disp('Given')
+disp('R=5 ohm L=100mH w=100 rad/s')
+Rs=5; Ls=100*10^-3 ;w=100;
+//Let Xs be the capacitive and inductive reactance
+Xs=w*Ls
+Q=Xs/Rs
+//As Q is greater than 5 we can approximate as
+Rp=Q^2*Rs
+Lp=Ls
+printf("The parallel equivalent is \n");
+printf("Rp= %d ohm \t Lp=%d mH",Rp,Lp*10^3);
\ No newline at end of file diff --git a/Working_Examples/215/CH16/EX16.6/ex16_6.sce b/Working_Examples/215/CH16/EX16.6/ex16_6.sce new file mode 100755 index 0000000..26c1153 --- /dev/null +++ b/Working_Examples/215/CH16/EX16.6/ex16_6.sce @@ -0,0 +1,26 @@ +clc
+//Example 16.6
+disp('Given')
+disp('Km=20 Kf=50')
+Km=20; Kf=50;
+s=poly(0,'s')
+//From figure 16.20(a)
+C=0.05; L=0.5;
+//Performing magnitude as well as frequency scaling simultaneously
+Cscaled =C/(Km*Kf)
+Lscaled = L*Km/Kf
+printf("Scaled values are \n")
+printf("Cscaled =%d uF \t Lscaled =%d mH \n",Cscaled*10^6,Lscaled*10^3)
+//Converting the Laplace transform of the circuit
+//From figure 16.20(c)
+disp('Vin=V1+0.5s*(1-0.2*V1)')
+disp('V1=20/s')
+//On substituting V1 in equation of Vin
+
+Zin=(s^2-4*s+40)/(2*s)
+disp(Zin,'Zin=')
+//Now we need to scale Zin
+//We will multiply Zin by Km and replace s by s/Kf
+Zinscaled=horner(Km*Zin,s/Kf)
+disp(Zinscaled,'Zinscaled')
+
diff --git a/Working_Examples/215/CH16/EX16.8/Figure16_8.jpg b/Working_Examples/215/CH16/EX16.8/Figure16_8.jpg Binary files differnew file mode 100755 index 0000000..5a397bf --- /dev/null +++ b/Working_Examples/215/CH16/EX16.8/Figure16_8.jpg diff --git a/Working_Examples/215/CH16/EX16.8/ex16_8.sce b/Working_Examples/215/CH16/EX16.8/ex16_8.sce new file mode 100755 index 0000000..0b01847 --- /dev/null +++ b/Working_Examples/215/CH16/EX16.8/ex16_8.sce @@ -0,0 +1,14 @@ +clc
+//Example 16.8
+//From figure 16.26
+disp('Writing the expression for voltage gain')
+disp('Vout/Vin=4000*(-1/200)*(5000*10^8/s)/((5000+10^8/s)*(5000+10^6/20s))')
+//On simplification
+s=poly(0,'s')
+h=syslin('c',(-2*s)/((1+s/10)*(1+s/20000)))
+disp(h)
+fmin=0.01
+fmax=10^7
+scf(1);clf;
+bode(h,fmin,fmax)
+
diff --git a/Working_Examples/215/CH17/EX17.1/ex17_1.sce b/Working_Examples/215/CH17/EX17.1/ex17_1.sce new file mode 100755 index 0000000..d2697fc --- /dev/null +++ b/Working_Examples/215/CH17/EX17.1/ex17_1.sce @@ -0,0 +1,20 @@ +//Example 17.1
+clc
+//From figure 17.3
+disp('The mesh equations are')
+disp('V1=10*I1-10*I2')
+disp('0=-10*I1+17*I2-2*I3-5*I4')
+disp('0=-2*I2+7*I3-I4')
+disp('0=-5*I2-I3+26*I4')
+//We need to find input impedance
+disp('Zin=delz/del11')
+//In matrix form
+A=[10 -10 0 0 ;-10 17 -2 -5; 0 -2 7 -1;0 -5 -1 26]
+delz=det(A)
+printf("\n delz=%f ohm^4",delz);
+//Eliminating first row and first column to find del11
+B=[17 -2 -5;-2 7 -1;-5 -1 26]
+del11=det(B)
+printf("\n del11=%f ohm^3",del11);
+Zin=delz/del11
+printf("\n Zin=%f ohm",Zin);
diff --git a/Working_Examples/215/CH17/EX17.10/ex17_10.sce b/Working_Examples/215/CH17/EX17.10/ex17_10.sce new file mode 100755 index 0000000..9f1c174 --- /dev/null +++ b/Working_Examples/215/CH17/EX17.10/ex17_10.sce @@ -0,0 +1,26 @@ +clc
+//Example 17.10
+//From figure 17.32
+disp('Consider Network A')
+//Writing the mesh equations
+disp('V1=12*I1+10*I2')
+disp('V2=10*I1+14*I2')
+//Arranging in the standard form
+//V1=t11*V2-t12*I2
+//I1=t21*V2-t22*I2
+//Therefore t parameters of Network A is
+t11A=1.2;t12A=6.8;t21A=0.1;t22A=1.4;
+disp('Consider Network B')
+//Writing the mesh equations
+disp('V1=24*I1+20*I2')
+disp('V2=20*I1+28*I2')
+//Arranging in the standard form
+//V1=t11*V2-t12*I2
+//I1=t21*V2-t22*I2
+//Therefore t parameters of Network B is
+t11B=1.2;t12B=13.6;t21B=0.05;t22B=1.4;
+tA=[1.2 6.8;0.1 1.4]
+tB=[1.2 13.6;0.05 1.4]
+disp('t parameters of cascaded network is t=tA*tB')
+t=tA*tB
+disp(t)
\ No newline at end of file diff --git a/Working_Examples/215/CH17/EX17.2/ex17_2.sce b/Working_Examples/215/CH17/EX17.2/ex17_2.sce new file mode 100755 index 0000000..9f7c012 --- /dev/null +++ b/Working_Examples/215/CH17/EX17.2/ex17_2.sce @@ -0,0 +1,20 @@ +//Example 17.2
+clc
+//From figure 17.5
+disp('The mesh equations are')
+disp('V1=10*I1-10*I2')
+disp('0=-10*I1+17*I2-2*I3-5*I4')
+disp('0=-2*I2+7*I3-I4')
+disp('0=-0.5*I3+1.5*I4')
+//We need to find input impedance
+disp('Zin=delz/del11')
+//In matrix form
+A=[10 -10 0 0 ;-10 17 -2 -5; 0 -2 7 -1;0 0 -0.5 1.5]
+delz=det(A)
+printf("\n delz=%f ohm^3",delz);
+//Eliminating first row and first column to find del11
+B=[17 -2 -5;-2 7 -1;0 -0.5 1.5]
+del11=det(B)
+printf("\n del11=%f ohm^2",del11);
+Zin=delz/del11
+printf("\n Zin=%f ohm",Zin);
diff --git a/Working_Examples/215/CH17/EX17.3/ex17_3.sce b/Working_Examples/215/CH17/EX17.3/ex17_3.sce new file mode 100755 index 0000000..dd17bd1 --- /dev/null +++ b/Working_Examples/215/CH17/EX17.3/ex17_3.sce @@ -0,0 +1,22 @@ +//Example 17.3
+clc
+//From figure 17.7
+disp('The nodal equations are')
+disp('I1=0.35*V1-0.2*V2-0.05*V3')
+disp('I2=-0.2*V1+1.7*V2-1*V3')
+disp('I3=-0.05*V1-1*V2+1.3*I3')
+//We need to find input impedance
+disp('Yin=dely/del11')
+disp('Zin=1/Yin')
+//In matrix form
+A=[0.35 -0.2 -0.05;-0.2 1.7 -1;-0.05 -1 1.3]
+dely=det(A)
+printf("\n dely=%f S^3",dely);
+//Eliminating first row and first column to find del11
+B=[1.7 -1;-1 1.3]
+del11=det(B)
+printf("\n del11=%f S^2",del11);
+Yin=dely/del11
+printf("\n Yin=%f S",Yin);
+Zin=1/Yin
+printf("\n Zin=%f ohm",Zin);
diff --git a/Working_Examples/215/CH17/EX17.4/Figure17_4.jpg b/Working_Examples/215/CH17/EX17.4/Figure17_4.jpg Binary files differnew file mode 100755 index 0000000..aa5fa64 --- /dev/null +++ b/Working_Examples/215/CH17/EX17.4/Figure17_4.jpg diff --git a/Working_Examples/215/CH17/EX17.4/Figure17_4_xcos.jpg b/Working_Examples/215/CH17/EX17.4/Figure17_4_xcos.jpg Binary files differnew file mode 100755 index 0000000..b568ea3 --- /dev/null +++ b/Working_Examples/215/CH17/EX17.4/Figure17_4_xcos.jpg diff --git a/Working_Examples/215/CH17/EX17.4/ex17_4.xcos b/Working_Examples/215/CH17/EX17.4/ex17_4.xcos new file mode 100755 index 0000000..5533d44 --- /dev/null +++ b/Working_Examples/215/CH17/EX17.4/ex17_4.xcos @@ -0,0 +1 @@ +<?xml version="1.0" encoding="UTF-8"?><XcosDiagram background="-1" finalIntegrationTime="30.0" title="ex17_4"><!--Xcos - 1.0 - scilab-5.5.2 - 20160406 2040--><mxGraphModel as="model"><root><mxCell id="-536a7494:134d5b6a3e7:-7ff9"/><mxCell id="-536a7494:134d5b6a3e7:-7ffa" 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\ No newline at end of file diff --git a/Working_Examples/215/CH17/EX17.7/ex17_7.sce b/Working_Examples/215/CH17/EX17.7/ex17_7.sce new file mode 100755 index 0000000..91e9fad --- /dev/null +++ b/Working_Examples/215/CH17/EX17.7/ex17_7.sce @@ -0,0 +1,14 @@ +clc
+//Example 17.7
+//From figure 17.16
+disp('Given a linear model of a transistor we need not explicitly find the aadmittance parameters ')
+disp('-y12 corresponds to admittance of 2k ohm resistor')
+disp('y11+y12 corresponds to admittance of 500 ohm resistor')
+disp('y21-y12 correponds to gain of dependent voltage source')
+disp('y22+y12 corresponds to admittance of 10k ohm resistor')
+//Writing down in equation form
+y12=-1/2000
+y11=1/500-y12
+y21=0.0395+y12
+y22=1/10000-y12
+printf("\n y11= %3.2f mS \n y12= %3.2f mS \n y21= %3.2f mS \n y22= %3.2f mS",y11*10^3,y12*10^3,y21*10^3,y22*10^3);
\ No newline at end of file diff --git a/Working_Examples/215/CH17/EX17.8/ex17_8.sce b/Working_Examples/215/CH17/EX17.8/ex17_8.sce new file mode 100755 index 0000000..245234f --- /dev/null +++ b/Working_Examples/215/CH17/EX17.8/ex17_8.sce @@ -0,0 +1,36 @@ +clc +//Example 17.8 +Vs = poly(0,'Vs') +disp('Given') +disp('Z=[10^3 10;-10^6 10^4 ]') +z11=10^3 ; z12=10;z21=-10^6;z22=10^4 +//Using the given matrix we can write the mesh equations as +disp('V1=10^3*I1+10*I2') +disp('V2=-10^6*I1+10^4*I2') +//The input to an two port network is an ideal sinusoidal voltage source in series with 500 ohm +//Mathematically +disp('The characterizing equations are') +disp('Vs=500*I1+V1') +//The output to an two port network is a 10k ohm resistor +//Mathematically +disp('V2=-10^4*I2') +Zg=500; +//Expressing V1,V2,I1,I2 in terms of Vs +V1=0.75*Vs +I1=Vs/2000 +V2=-250*Vs +I2=Vs/40 +disp('Voltage gain Gv=V2/V1') +Gv=V2/V1 +disp(Gv,'Gv=') +disp('Current gain Gi=I2/I1') +Gi=I2/I1 +disp(Gi,'Gi=') +disp('Power gain Gp=Real[-0.5*V2*I2*]/Real[0..5*V1*I1*]') +Gp=(-0.5*V2*I2)/(0.5*V1*I1) +disp(Gp,'Gp=') +disp('Input impedance is Zin=V1/I1') +Zin=V1/I1 +disp('Output impedance is Zout=z22-((z12*z21)/(z11+Zg))') +Zout=z22-((z12*z21)/(z11+Zg)) +printf("\n Zout= %3.2f kohm",Zout*10^-3)
\ No newline at end of file diff --git a/Working_Examples/215/CH17/EX17.9/ex17_9.sce b/Working_Examples/215/CH17/EX17.9/ex17_9.sce new file mode 100755 index 0000000..a8bbcac --- /dev/null +++ b/Working_Examples/215/CH17/EX17.9/ex17_9.sce @@ -0,0 +1,13 @@ +clc
+//Example 17.9
+//From figure 17.27
+//Writing the mesh equations
+disp('V1=5*I1+4*I2')
+disp('V2=4*I1+10*I2')
+//Arranging in the standard form
+//V1=h11*I1+h12*V2
+//I2=h21*I1+h22*V2
+//Therefore h parameters are
+h11=3.4;h12=0.4;h21=-0.4;h22=0.1;
+h=[h11 h12;h21 h22]
+disp(h)
\ No newline at end of file diff --git a/Working_Examples/215/CH18/EX18.1/Figure18_1.jpg b/Working_Examples/215/CH18/EX18.1/Figure18_1.jpg Binary files differnew file mode 100755 index 0000000..c74d5e8 --- /dev/null +++ b/Working_Examples/215/CH18/EX18.1/Figure18_1.jpg diff --git a/Working_Examples/215/CH18/EX18.1/ex18_1.sce b/Working_Examples/215/CH18/EX18.1/ex18_1.sce new file mode 100755 index 0000000..67b8d26 --- /dev/null +++ b/Working_Examples/215/CH18/EX18.1/ex18_1.sce @@ -0,0 +1,45 @@ +clear +close +clc +//Example 18.1 +//From the figure 18.2 +disp('The equation of v(t) considering one period can be written as') +disp('v(t)=Vm*cos(5*%pi*t) for -0.1<=t<=0.1') +disp('v(t)=0 for 0.1<=t<=0.3') +//Assuming the value of Vm is 1 + +//Evaluating the constants an and bn +//bn=0 for all n +//an=(2*Vm*cos(n*%pi/2))/(%pi*(1-n^2)) +//a0=Vm/%pi +t=-1:0.02:1; +Vm=ones(1,length(t)); +v0t=Vm/%pi; +v1t=(Vm.*cos(5*%pi*t)).*0.5; +v0t_v1t=v0t+v1t; +v2t=(2/(3*%pi))*(Vm.*cos(10*%pi*t)); +v0t_v1t_v2t=v0t+v1t+v2t; +v3t=(2/(15*%pi))*(Vm.*cos(20*%pi*t)); +v0t_v1t_v2t_v3t=v0t+v1t+v2t-v3t; +figure +a = gca (); +a. y_location = "origin"; +a. x_location = "origin"; +a. data_bounds =[ -1,0;1 0.5]; +plot (t,v0t) +xtitle('vot vs t','t in s','vot') +figure +a = gca (); +a. y_location = "origin"; +a. x_location = "origin"; +a. data_bounds =[ -1,-0.5;1 0.5]; +plot (t,v0t_v1t) +a. y_location = "origin"; +a. x_location = "origin"; +a. data_bounds =[ -1,-0.5;1 0.5]; +plot (t,v0t_v1t_v2t,'r.->') +a. y_location = "origin"; +a. x_location = "origin"; +a. data_bounds =[ -1,-0.5;1 0.5]; +plot (t,v0t_v1t_v2t_v3t,'d') +xtitle('v(t)','t in s','v(t) in V')
\ No newline at end of file diff --git a/Working_Examples/215/CH18/EX18.2/Figure18_2.jpg b/Working_Examples/215/CH18/EX18.2/Figure18_2.jpg Binary files differnew file mode 100755 index 0000000..16292c9 --- /dev/null +++ b/Working_Examples/215/CH18/EX18.2/Figure18_2.jpg diff --git a/Working_Examples/215/CH18/EX18.2/Figure18_2_xcos.jpg b/Working_Examples/215/CH18/EX18.2/Figure18_2_xcos.jpg Binary files differnew file mode 100755 index 0000000..72970e2 --- /dev/null +++ b/Working_Examples/215/CH18/EX18.2/Figure18_2_xcos.jpg diff --git a/Working_Examples/215/CH18/EX18.2/ex18_2.xcos b/Working_Examples/215/CH18/EX18.2/ex18_2.xcos new file mode 100755 index 0000000..6acbccd --- /dev/null +++ b/Working_Examples/215/CH18/EX18.2/ex18_2.xcos @@ -0,0 +1 @@ +<?xml version="1.0" encoding="UTF-8"?><XcosDiagram background="-1" finalIntegrationTime="6.5" title="ex18_2"><!--Xcos - 1.0 - scilab-5.5.2 - 20160406 2040--><mxGraphModel as="model"><root><mxCell id="f4a86ca:134efd7fc02:-7ffd"/><mxCell 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\ No newline at end of file diff --git a/Working_Examples/215/CH18/EX18.5/Figure18_5.jpg b/Working_Examples/215/CH18/EX18.5/Figure18_5.jpg Binary files differnew file mode 100755 index 0000000..ef0a506 --- /dev/null +++ b/Working_Examples/215/CH18/EX18.5/Figure18_5.jpg diff --git a/Working_Examples/215/CH18/EX18.5/ex18_5.sce b/Working_Examples/215/CH18/EX18.5/ex18_5.sce new file mode 100755 index 0000000..580a1f6 --- /dev/null +++ b/Working_Examples/215/CH18/EX18.5/ex18_5.sce @@ -0,0 +1,34 @@ +clc;
+//Example 18.5
+//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/Working_Examples/215/CH18/EX18.6/ex18_6.sce b/Working_Examples/215/CH18/EX18.6/ex18_6.sce new file mode 100755 index 0000000..91ce75c --- /dev/null +++ b/Working_Examples/215/CH18/EX18.6/ex18_6.sce @@ -0,0 +1,20 @@ +clc
+syms s t
+printf("Given")
+disp('v(t)=4*exp(-3*t)*u(t)')
+v=4*exp(-3*t)
+
+F=4*(integ(exp(-(3+%i*1)*s),s,0,%inf))
+//The secind term tends to zero
+disp(F,'F=')
+//Let W be the total 1 ohm energy in the input signal
+W=integ(v^2,t,0,%inf)
+disp(W,'W=')
+//Let Wo be the total energy
+//As the frequency range is given as 1 Hz<|f|<2 Hz
+//Considering symmetry
+Wo=(1/%pi)*integ((16/(9+s^2)),s,2*%pi,4*%pi)
+disp(Wo,'Wo=')
+
+
+
diff --git a/Working_Examples/215/CH18/EX18.8/Figure18_8.jpg b/Working_Examples/215/CH18/EX18.8/Figure18_8.jpg Binary files differnew file mode 100755 index 0000000..b56b076 --- /dev/null +++ b/Working_Examples/215/CH18/EX18.8/Figure18_8.jpg diff --git a/Working_Examples/215/CH18/EX18.8/Figure18_8_xcos.jpg b/Working_Examples/215/CH18/EX18.8/Figure18_8_xcos.jpg Binary files differnew file mode 100755 index 0000000..9fe790d --- /dev/null +++ b/Working_Examples/215/CH18/EX18.8/Figure18_8_xcos.jpg diff --git a/Working_Examples/215/CH18/EX18.8/ex18_8.xcos b/Working_Examples/215/CH18/EX18.8/ex18_8.xcos new file mode 100755 index 0000000..faf272f --- /dev/null +++ b/Working_Examples/215/CH18/EX18.8/ex18_8.xcos @@ -0,0 +1 @@ +<?xml version="1.0" encoding="UTF-8"?><XcosDiagram background="-1" finalIntegrationTime="5.0" title="ex18_8"><!--Xcos - 1.0 - scilab-5.5.2 - 20160406 2040--><mxGraphModel as="model"><root><mxCell id="f4a86ca:134efd7fc02:-7e65"/><mxCell id="f4a86ca:134efd7fc02:-7e66" 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\ No newline at end of file diff --git a/Working_Examples/215/CH2/EX2.1/ex2_1.sce b/Working_Examples/215/CH2/EX2.1/ex2_1.sce new file mode 100755 index 0000000..b6e0cfd --- /dev/null +++ b/Working_Examples/215/CH2/EX2.1/ex2_1.sce @@ -0,0 +1,35 @@ +//Example 2.1
+//Computation of power absorbed by each part
+//From figure 2.13a
+V=2;I=3;
+//We have Power(P)=V*I
+P=V*I
+printf("a) Power =%dW\n",P)
+if P>0 then
+ printf("Power is absorbed by the element\n")
+else
+ printf("Power is supplied by the element\n");
+end
+
+clear P;
+//From figure 2.13b
+V=-2;I=-3;
+//We have Power(P)=V*I
+P=V*I
+printf("b) Power =%dW\n",P)
+if P>0 then
+ printf("Power is absorbed by the element\n")
+else
+ printf("Power is supplied by the element\n")
+end
+
+//From figure 2.13c
+V=4;I=-5;
+//We have Power(P)=V*I
+P=V*I
+printf("c) Power =%dW\n",P)
+if P>0 then
+ printf("Power is absorbed by the element\n")
+else
+ printf("Power is supplied by the element\n")
+end
diff --git a/Working_Examples/215/CH2/EX2.2/ex2_2.sce b/Working_Examples/215/CH2/EX2.2/ex2_2.sce new file mode 100755 index 0000000..3f56789 --- /dev/null +++ b/Working_Examples/215/CH2/EX2.2/ex2_2.sce @@ -0,0 +1,12 @@ +//Example 2.2
+//Calculate vL
+disp("Given")
+disp("v2=3V")
+v2=3;
+//From figure 2.19b
+disp("Considering the right hand part of the circuit ")
+disp("vL=5v2")
+vL=5*v2;
+disp("On substitution")
+printf("vL=%dV\n",vL);
+
diff --git a/Working_Examples/215/CH2/EX2.3/ex2_3.sce b/Working_Examples/215/CH2/EX2.3/ex2_3.sce new file mode 100755 index 0000000..87a2176 --- /dev/null +++ b/Working_Examples/215/CH2/EX2.3/ex2_3.sce @@ -0,0 +1,15 @@ +//Example 2.3
+//Calculate the voltage and power dissipated acreoss the resistor terminals
+//From figure 2.24b
+disp("Given")
+disp("R=560 ohm ; i=428mA")
+R=560;i=428*10^-3;
+//Voltage across a resistor is
+disp("v=R*i")
+v=R*i;
+printf("Voltage across a resistor=%3.3fV\n",v)
+
+//Power dissipated by the resistor is
+disp("p=v*i")
+p=v*i;
+printf("Power dissipated by the resistor=%3.3fW\n",p)
diff --git a/Working_Examples/215/CH2/EX2.4/ex2_4.sce b/Working_Examples/215/CH2/EX2.4/ex2_4.sce new file mode 100755 index 0000000..6d0448e --- /dev/null +++ b/Working_Examples/215/CH2/EX2.4/ex2_4.sce @@ -0,0 +1,16 @@ +//Example 2.4
+//Calculate the power dissipated within the wire
+//From figure 2.27
+disp("Given")
+disp("Total length of the wire is 4000 feet")
+disp("Current drawn by lamp is 100A")
+//Considering American Wire Gauge system(AWG)
+//Referring Table 2.4
+disp("4AWG=0.2485ohms/1000ft")
+l=4000; i=100 ; rl=0.2485/1000;
+//Let R be the wire resistance
+R=l*rl;
+//Let p be the power dissipated within the wire
+disp("p=i^2*R")
+p=i^2*R
+printf("Power dissipated within the wire=%dW\n",p)
diff --git a/Working_Examples/215/CH3/EX3.1/Figure3_1.jpg b/Working_Examples/215/CH3/EX3.1/Figure3_1.jpg Binary files differnew file mode 100755 index 0000000..e842185 --- /dev/null +++ b/Working_Examples/215/CH3/EX3.1/Figure3_1.jpg diff --git a/Working_Examples/215/CH3/EX3.1/Figure3_1_xcos.jpg b/Working_Examples/215/CH3/EX3.1/Figure3_1_xcos.jpg Binary files differnew file mode 100755 index 0000000..ad928b1 --- /dev/null +++ b/Working_Examples/215/CH3/EX3.1/Figure3_1_xcos.jpg diff --git a/Working_Examples/215/CH3/EX3.1/ex3_1.xcos b/Working_Examples/215/CH3/EX3.1/ex3_1.xcos new file mode 100755 index 0000000..d69979b --- /dev/null +++ b/Working_Examples/215/CH3/EX3.1/ex3_1.xcos @@ -0,0 +1 @@ +<?xml version="1.0" encoding="UTF-8"?><XcosDiagram background="-1" finalIntegrationTime="30.0" title="ex3_1"><!--Xcos - 1.0 - scilab-5.5.2 - 20160406 2040--><mxGraphModel as="model"><root><mxCell id="-3721b5e:1319cfae9ac:-7fff"/><mxCell id="-3721b5e:1319cfae9ac:-8000" 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\ No newline at end of file diff --git a/Working_Examples/215/CH6/EX6.10/ex6_10.sce b/Working_Examples/215/CH6/EX6.10/ex6_10.sce new file mode 100755 index 0000000..f0225a8 --- /dev/null +++ b/Working_Examples/215/CH6/EX6.10/ex6_10.sce @@ -0,0 +1,31 @@ +clc
+//Example 6.10
+//Calculate the voltage across 20 ohm capacitor
+//Consider the circuit to be solved by superposition principle
+disp('Consider the current source 2(90 deg)only')
+//From figure 6.32
+//Let I1 be the current through -i*4 capacitive reactance
+Imag=2;Iph=90;
+i=%i
+x=Imag * cos (( Iph * %pi ) /180) ;
+y=Imag * sin (( Iph * %pi ) /180) ;
+I= complex (x,y)
+I1=(I*(i*15))/(i*5+i*15-i*4)
+//Let V20 be the voltage across -i*4 capacitive reactance
+V200=(-i*4)*I1
+printf("V20=%3.2fV \n",V200)
+disp('Consider the 20 V voltage source only')
+V=20;
+//From figure 6.35
+//let V201 be the voltage across -i*5 capacitive reactance
+V201=-V
+printf("V201=%d V \n",V201)
+disp('Consider the current source 1(90 deg)only')
+I1mag=1;I1ang=90;
+//From figure 6.37
+//Let V202 be the voltage across -i*5 capacitive reactance
+V202=(-i*5)*I1mag*i
+printf("V202=%3.2fV \n",V202)
+//Let V20 be the voltage across -i*20 capacitive reactance
+V20=V200+V201+V202
+printf("\n V20=%3.2fV \n",V20)
diff --git a/Working_Examples/215/CH6/EX6.11/Figure6_11.jpg b/Working_Examples/215/CH6/EX6.11/Figure6_11.jpg Binary files differnew file mode 100755 index 0000000..712bcf3 --- /dev/null +++ b/Working_Examples/215/CH6/EX6.11/Figure6_11.jpg diff --git a/Working_Examples/215/CH6/EX6.11/Figure6_11_xcos.jpg b/Working_Examples/215/CH6/EX6.11/Figure6_11_xcos.jpg Binary files differnew file mode 100755 index 0000000..868e43b --- /dev/null +++ b/Working_Examples/215/CH6/EX6.11/Figure6_11_xcos.jpg diff --git a/Working_Examples/215/CH6/EX6.11/ex6_11.xcos b/Working_Examples/215/CH6/EX6.11/ex6_11.xcos new file mode 100755 index 0000000..54e6293 --- /dev/null +++ b/Working_Examples/215/CH6/EX6.11/ex6_11.xcos @@ -0,0 +1 @@ +<?xml version="1.0" encoding="UTF-8"?><XcosDiagram background="-1" finalIntegrationTime="30.0" title="ex6_11"><!--Xcos - 1.0 - scilab-5.5.2 - 20160406 2040--><mxGraphModel as="model"><root><mxCell id="2602728:132d47c9ecc:-7fff"/><mxCell id="2602728:132d47c9ecc:-8000" 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\ No newline at end of file diff --git a/Working_Examples/215/CH6/EX6.17/ex6_17.sce b/Working_Examples/215/CH6/EX6.17/ex6_17.sce new file mode 100755 index 0000000..cc83739 --- /dev/null +++ b/Working_Examples/215/CH6/EX6.17/ex6_17.sce @@ -0,0 +1,23 @@ +clc
+//Example 6.17
+//Verification of Reciprocity theorem
+I=20
+//From figure 6.59
+disp('The current divides between the two parallel impedances')
+//Let I2 be the current through i5 ohm
+I2=(20*%i*(10+%i*5))/(10+%i*5+%i*5-%i*2)
+//Let Vx be the voltage across -i2 ohm capacitive reactance
+Vx=I2*(-%i*2)
+[Vxmag Vxang]=polar(Vx)
+printf("Vx=%3.2f(%3.2f deg)V \n",Vxmag,(Vxang*180)/%pi)
+//To verify Reciprocity theorem remove the current source and place it parallel with -i2 ohm capacitive reactance
+//From figure 6.60
+//Let I2 be the current flowing through resistor of 10 ohm
+I2=(20*%i*(-%i*2))/(10+%i*5+%i*5-%i*2)
+//let Vx1 be the deired output voltage across 10 ohm resistor and i5 inductive reactance
+Vx1=I2*(10+%i*5)
+[Vx1mag Vx1ang]=polar(Vx1)
+printf("Vx1=%3.2f(%3.2f deg)V \n",Vx1mag,(Vx1ang*180)/%pi)
+//Comparing the values of Vx and Vx1
+disp('Vx=Vx1')
+disp('Hence Reciprocity theorem is verified')
\ No newline at end of file diff --git a/Working_Examples/215/CH6/EX6.18/ex6_18.sce b/Working_Examples/215/CH6/EX6.18/ex6_18.sce new file mode 100755 index 0000000..b137cf6 --- /dev/null +++ b/Working_Examples/215/CH6/EX6.18/ex6_18.sce @@ -0,0 +1,23 @@ +clc
+//Example 6.18
+//Verification of Reciprocity theorem
+I=10
+//From figure 6.61
+disp('The current divides between the two parallel impedances')
+//Let I2 be the current through 4 ohm
+I2=(10*5)/(4-%i*4+5)
+//Let Vx be the voltage across -i4 ohm capacitive reactance
+Vx=I2*(-%i*4)
+[Vxmag Vxang]=polar(Vx)
+printf("Vx=%3.2f(%3.2f deg)V \n",Vxmag,(Vxang*180)/%pi)
+//To verify Reciprocity theorem remove the current source and place it parallel with -i4 ohm capacitive reactance
+//From figure 6.62
+//Let I1 be the current flowing through resistor of 5 ohm
+I1=(10*(-%i*4))/(5+4-%i*4)
+//let Vx1 be the deired output voltage across 5 ohm resistor
+Vx1=I1*5
+[Vx1mag Vx1ang]=polar(Vx1)
+printf("Vx1=%3.2f(%3.2f deg)V \n",Vx1mag,(Vx1ang*180)/%pi)
+//Comparing the values of Vx and Vx1
+disp('Vx=Vx1')
+disp('Hence Reciprocity theorem is verified')
\ No newline at end of file diff --git a/Working_Examples/215/CH6/EX6.19/ex6_19.sce b/Working_Examples/215/CH6/EX6.19/ex6_19.sce new file mode 100755 index 0000000..d7e6f08 --- /dev/null +++ b/Working_Examples/215/CH6/EX6.19/ex6_19.sce @@ -0,0 +1,28 @@ +clc
+//Example 6.19
+//Calculate total current through load
+//On applying source transformation
+//From figure 6.65
+i=%i
+V1=10;V2mag=5;V2ph=90;V3mag=14.4;V3ph=225;
+x=V2mag * cos (( V2ph * %pi ) /180) ;
+y=V2mag * sin (( V2ph * %pi ) /180) ;
+V2= complex (x,y)
+a=V3mag * cos (( V3ph * %pi ) /180) ;
+b=V3mag * sin (( V3ph * %pi ) /180) ;
+V3= complex (a,b)
+G1=1/2;G2=1/(2+i*3);G3=1/(2-i*2);
+//By applying Millman Theorem
+disp('V=((V1*G1)+(V2*G2)+(V3*G3))/(G1+G2+G3)')
+V=((V1*G1)+(V2*G2)+(V3*G3))/(G1+G2+G3)
+[Vmag Vang]=polar(V)
+R=1/(G1+G2+G3)
+printf("V=%3.2f(%3.2f deg)V",Vmag,(Vang*180)/%pi)
+disp(R,'R=')
+//Consider the resultant circuit from figure 6.66
+disp('Let the total current through 3+i4 be I')
+//Applying KVL to the circuit
+I=V/(3+i*4+R)
+[Imag Iang]=polar(I)
+printf("I=%3.2f(%3.2f deg)V",Imag,(Iang*180)/%pi)
+
diff --git a/Working_Examples/215/CH6/EX6.20/Figure6_20.jpg b/Working_Examples/215/CH6/EX6.20/Figure6_20.jpg Binary files differnew file mode 100755 index 0000000..d9eb111 --- /dev/null +++ b/Working_Examples/215/CH6/EX6.20/Figure6_20.jpg diff --git a/Working_Examples/215/CH6/EX6.20/Figure6_20_xcos.jpg b/Working_Examples/215/CH6/EX6.20/Figure6_20_xcos.jpg Binary files differnew file mode 100755 index 0000000..d9b6195 --- /dev/null +++ b/Working_Examples/215/CH6/EX6.20/Figure6_20_xcos.jpg diff --git a/Working_Examples/215/CH6/EX6.20/ex6_20.xcos b/Working_Examples/215/CH6/EX6.20/ex6_20.xcos new file mode 100755 index 0000000..3934266 --- /dev/null +++ b/Working_Examples/215/CH6/EX6.20/ex6_20.xcos @@ -0,0 +1 @@ +<?xml version="1.0" encoding="UTF-8"?><XcosDiagram background="-1" finalIntegrationTime="1.0" title="ex6_20"><!--Xcos - 1.0 - scilab-5.5.2 - 20160406 2040--><mxGraphModel as="model"><root><mxCell id="6611b517:134eb867750:-7ffd"/><mxCell id="6611b517:134eb867750:-7ffe" 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\ No newline at end of file diff --git a/Working_Examples/215/CH6/EX6.22/ex6_22.sce b/Working_Examples/215/CH6/EX6.22/ex6_22.sce new file mode 100755 index 0000000..65afbec --- /dev/null +++ b/Working_Examples/215/CH6/EX6.22/ex6_22.sce @@ -0,0 +1,16 @@ +clc
+//Example 6.22
+//Writing KVL for the circuit
+disp('10*i=30')
+//On solving
+i=3;R=10;V1=25;V2=5;
+printf("Power absorbed by 10 ohm resistor is %d W \n",i^2*R)
+printf("Power delivered by 25 V source is %d W \n",V1*i)
+printf("Power delivered by 5 V source is %d W \n",V2*i)
+//Let P be the total power
+P=i^2*R-(V1*i+V2*i)
+if P==0 then
+ disp('Tellegen theorem is valid')
+else
+ disp('Tellegen theorem is not valid')
+end
\ No newline at end of file diff --git a/Working_Examples/215/CH6/EX6.23/Figure6_23.jpg b/Working_Examples/215/CH6/EX6.23/Figure6_23.jpg Binary files differnew file mode 100755 index 0000000..db00076 --- /dev/null +++ b/Working_Examples/215/CH6/EX6.23/Figure6_23.jpg diff --git a/Working_Examples/215/CH6/EX6.23/Figure6_23_xcos.jpg b/Working_Examples/215/CH6/EX6.23/Figure6_23_xcos.jpg Binary files differnew file mode 100755 index 0000000..c2712f4 --- /dev/null +++ b/Working_Examples/215/CH6/EX6.23/Figure6_23_xcos.jpg diff --git a/Working_Examples/215/CH6/EX6.23/ex6_23.xcos b/Working_Examples/215/CH6/EX6.23/ex6_23.xcos new file mode 100755 index 0000000..8559aaf --- /dev/null +++ b/Working_Examples/215/CH6/EX6.23/ex6_23.xcos @@ -0,0 +1 @@ +<?xml version="1.0" encoding="UTF-8"?><XcosDiagram background="-1" finalIntegrationTime="30.0" title="ex6_23"><!--Xcos - 1.0 - scilab-5.5.2 - 20160406 2040--><mxGraphModel as="model"><root><mxCell id="6611b517:134eb867750:-7be6"/><mxCell 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\ No newline at end of file diff --git a/Working_Examples/215/CH7/EX7.1/Figure7_1.jpg b/Working_Examples/215/CH7/EX7.1/Figure7_1.jpg Binary files differnew file mode 100755 index 0000000..0873bcf --- /dev/null +++ b/Working_Examples/215/CH7/EX7.1/Figure7_1.jpg diff --git a/Working_Examples/215/CH7/EX7.1/ex7_1.sce b/Working_Examples/215/CH7/EX7.1/ex7_1.sce new file mode 100755 index 0000000..97c904a --- /dev/null +++ b/Working_Examples/215/CH7/EX7.1/ex7_1.sce @@ -0,0 +1,10 @@ +clc
+syms s t
+//part(a)
+i=diff(5*s^0,s)
+disp(i,'i=')
+//prt(b)
+i1=diff(4*sin(3*t),t)
+t=-2:.1:5
+ plot (t,12*cos(3*t))
+xtitle('i vs t','t(s)','i(A)')
\ No newline at end of file diff --git a/Working_Examples/215/CH7/EX7.11/Figure7_11.jpg b/Working_Examples/215/CH7/EX7.11/Figure7_11.jpg Binary files differnew file mode 100755 index 0000000..260cfa8 --- /dev/null +++ b/Working_Examples/215/CH7/EX7.11/Figure7_11.jpg diff --git a/Working_Examples/215/CH7/EX7.11/Figure7_11_xcos.jpg b/Working_Examples/215/CH7/EX7.11/Figure7_11_xcos.jpg Binary files differnew file mode 100755 index 0000000..bdb38b1 --- /dev/null +++ b/Working_Examples/215/CH7/EX7.11/Figure7_11_xcos.jpg diff --git a/Working_Examples/215/CH7/EX7.11/ex7_11.xcos b/Working_Examples/215/CH7/EX7.11/ex7_11.xcos new file mode 100755 index 0000000..d566a07 --- /dev/null +++ b/Working_Examples/215/CH7/EX7.11/ex7_11.xcos @@ -0,0 +1 @@ +<?xml version="1.0" encoding="UTF-8"?><XcosDiagram background="-1" finalIntegrationTime="1.0" title="ex7_11"><!--Xcos - 1.0 - scilab-5.5.2 - 20160406 2040--><mxGraphModel as="model"><root><mxCell id="3a97bac1:134ed06dad1:-7ffd"/><mxCell 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\ No newline at end of file diff --git a/Working_Examples/215/CH7/EX7.2/Figure7_21.jpg b/Working_Examples/215/CH7/EX7.2/Figure7_21.jpg Binary files differnew file mode 100755 index 0000000..019312a --- /dev/null +++ b/Working_Examples/215/CH7/EX7.2/Figure7_21.jpg diff --git a/Working_Examples/215/CH7/EX7.2/Figure7_22.jpg b/Working_Examples/215/CH7/EX7.2/Figure7_22.jpg Binary files differnew file mode 100755 index 0000000..df53fef --- /dev/null +++ b/Working_Examples/215/CH7/EX7.2/Figure7_22.jpg diff --git a/Working_Examples/215/CH7/EX7.2/ex7_2.sce b/Working_Examples/215/CH7/EX7.2/ex7_2.sce new file mode 100755 index 0000000..db720e4 --- /dev/null +++ b/Working_Examples/215/CH7/EX7.2/ex7_2.sce @@ -0,0 +1,24 @@ +clc
+t = 0:0.000001:0.002;
+deff('y=u(t)','y=1*(t>=0)');
+y =0.02*(u(t) - u(t-0.002));
+figure
+a=gca()
+subplot(111)
+plot2d(t,y,5,rect=[0 0 0.004 0.03])
+xtitle('i vs t','t in ms','i in mA')
+
+syms s
+//For t<=0 ms
+v=0
+//For the region in the rectangular pulse i.e 0<t<=2 ms
+v=integ(s^0,s)*4000
+//For t>2 ms
+v=8
+s=0:0.000001:0.002
+
+figure
+a=gca()
+subplot(111)
+plot(s,(4000*s),s+0.002,8)
+xtitle('v vs t','t in ms','v in V')
diff --git a/Working_Examples/215/CH7/EX7.3/Figure7_3.jpg b/Working_Examples/215/CH7/EX7.3/Figure7_3.jpg Binary files differnew file mode 100755 index 0000000..966c7f9 --- /dev/null +++ b/Working_Examples/215/CH7/EX7.3/Figure7_3.jpg diff --git a/Working_Examples/215/CH7/EX7.3/ex7_3.sce b/Working_Examples/215/CH7/EX7.3/ex7_3.sce new file mode 100755 index 0000000..a0192d7 --- /dev/null +++ b/Working_Examples/215/CH7/EX7.3/ex7_3.sce @@ -0,0 +1,18 @@ +clc
+//Example 7.3
+//Let wc be the energy stored in capacitor
+C=20*10^-6; R=10^6;
+t=0:0.001:0.5
+v=100*sin(2*%pi*t)
+wc=0.5*C*v^2
+plot(t,wc)
+xtitle('wC vs t','t in sec','wC in J')
+//Let iR be the current in the resistor
+iR=v/R
+//Let pR be the power dissipated in the resistor
+pR=iR^2*R
+//If wR is the energy dissipated in the resistor
+syms s
+wR=integ(100*(sin(2*%pi*s))^2,s,0,0.5)
+disp(wR,'wR=')
+
diff --git a/Working_Examples/215/CH7/EX7.7/ex7_7.sce b/Working_Examples/215/CH7/EX7.7/ex7_7.sce new file mode 100755 index 0000000..68fa332 --- /dev/null +++ b/Working_Examples/215/CH7/EX7.7/ex7_7.sce @@ -0,0 +1,18 @@ +clc
+//Example 7.7
+printf("Given")
+disp('i=12*sin(%pi*t/6),R=0.1 ohm,L=3H')
+t=0:.1:6
+i=12*sin(%pi*t/6),R=0.1;L=3;
+//Let wL be the energy stored in the inductor
+wL=0.5*L*i^2
+plot(t,wL)
+//From the above graph
+wLmax=216;tmax=3;
+printf("Maximum value at %d J at %d sec",wLmax,tmax)
+//Let pR be the power dissipated in the resistor
+pR=i^2*R
+//Energy converted to heat in 6 sec interval in the resistor is
+syms s
+wR=integ(14.4*(sin(%pi/6*s))^2,s,0,6)
+disp(wR,'wR')
diff --git a/Working_Examples/215/CH8/EX8.1/Figure8_1.jpg b/Working_Examples/215/CH8/EX8.1/Figure8_1.jpg Binary files differnew file mode 100755 index 0000000..b1d5ea5 --- /dev/null +++ b/Working_Examples/215/CH8/EX8.1/Figure8_1.jpg diff --git a/Working_Examples/215/CH8/EX8.1/Figure8_1_xcos.jpg b/Working_Examples/215/CH8/EX8.1/Figure8_1_xcos.jpg Binary files differnew file mode 100755 index 0000000..fb14193 --- /dev/null +++ b/Working_Examples/215/CH8/EX8.1/Figure8_1_xcos.jpg diff --git a/Working_Examples/215/CH8/EX8.1/ex8_1.xcos b/Working_Examples/215/CH8/EX8.1/ex8_1.xcos new file mode 100755 index 0000000..8fb1946 --- /dev/null +++ b/Working_Examples/215/CH8/EX8.1/ex8_1.xcos @@ -0,0 +1 @@ +<?xml version="1.0" encoding="UTF-8"?><XcosDiagram background="-1" finalIntegrationTime="0.001" title="ex8_1"><!--Xcos - 1.0 - scilab-5.5.2 - 20160406 2040--><mxGraphModel as="model"><root><mxCell id="77dd482d:134d2cc3c9e:-7f99"/><mxCell id="77dd482d:134d2cc3c9e:-7f9a" 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\ No newline at end of file diff --git a/Working_Examples/215/CH9/EX9.1/ex9_1.sce b/Working_Examples/215/CH9/EX9.1/ex9_1.sce new file mode 100755 index 0000000..a20494a --- /dev/null +++ b/Working_Examples/215/CH9/EX9.1/ex9_1.sce @@ -0,0 +1,18 @@ +//Example 9.1
+//Calculate resistor values for underdamped and overdamped responses
+printf("Given")
+disp('L=10mH and C=100uF')
+L=10*10^-3;C=100*10^-6
+w0=sqrt(1/(L*C))
+printf("w0=%drad/s\n",w0)
+//alpha(a)=1/(2*R*C)
+disp('For an overdamped response')
+disp('a > w0')
+//On solving
+disp('Hence')
+disp('R<5ohm')
+disp('For an underdamped response')
+disp('a < w0')
+//On solving
+disp('Hence')
+disp('R>5ohm')
\ No newline at end of file diff --git a/Working_Examples/215/CH9/EX9.2/Figure9_2.jpg b/Working_Examples/215/CH9/EX9.2/Figure9_2.jpg Binary files differnew file mode 100755 index 0000000..b111279 --- /dev/null +++ b/Working_Examples/215/CH9/EX9.2/Figure9_2.jpg diff --git a/Working_Examples/215/CH9/EX9.2/Figure9_2_xcos.jpg b/Working_Examples/215/CH9/EX9.2/Figure9_2_xcos.jpg Binary files differnew file mode 100755 index 0000000..1434d4f --- /dev/null +++ b/Working_Examples/215/CH9/EX9.2/Figure9_2_xcos.jpg diff --git a/Working_Examples/215/CH9/EX9.2/ex9_2.xcos b/Working_Examples/215/CH9/EX9.2/ex9_2.xcos new file mode 100755 index 0000000..8567cfc --- /dev/null +++ b/Working_Examples/215/CH9/EX9.2/ex9_2.xcos @@ -0,0 +1 @@ +<?xml version="1.0" encoding="UTF-8"?><XcosDiagram background="-1" finalIntegrationTime="0.001" title="ex9_2"><!--Xcos - 1.0 - scilab-5.5.2 - 20160406 2040--><mxGraphModel as="model"><root><mxCell id="2adc5834:134f2773fd2:-7ffd"/><mxCell id="2adc5834:134f2773fd2:-7ffe" 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\ No newline at end of file diff --git a/Working_Examples/215/CH9/EX9.4/Figure9_4.jpg b/Working_Examples/215/CH9/EX9.4/Figure9_4.jpg Binary files differnew file mode 100755 index 0000000..f4fc8be --- /dev/null +++ b/Working_Examples/215/CH9/EX9.4/Figure9_4.jpg diff --git a/Working_Examples/215/CH9/EX9.4/ex9_4.sce b/Working_Examples/215/CH9/EX9.4/ex9_4.sce new file mode 100755 index 0000000..7b8316a --- /dev/null +++ b/Working_Examples/215/CH9/EX9.4/ex9_4.sce @@ -0,0 +1,13 @@ +clc
+//Example 9.4
+//Calculate settling time
+t=0:0.1:5
+ic=2*exp(-t)-4*exp(-t)
+plot(t,ic)
+xtitle('ic vs t','t in s','ic in A')
+//Let ts be the settling time
+//From the graph the maximum value is|-2|=2A
+//'ts' is the time when ic has decreased to 0.02A
+//On solving for 'ts'
+ts=-log(0.02/4)
+printf("ts=%3.2f s\n",ts)
diff --git a/Working_Examples/215/CH9/EX9.6/Figure9_6.jpg b/Working_Examples/215/CH9/EX9.6/Figure9_6.jpg Binary files differnew file mode 100755 index 0000000..06cec48 --- /dev/null +++ b/Working_Examples/215/CH9/EX9.6/Figure9_6.jpg diff --git a/Working_Examples/215/CH9/EX9.6/Figure9_6_xcos.jpg b/Working_Examples/215/CH9/EX9.6/Figure9_6_xcos.jpg Binary files differnew file mode 100755 index 0000000..c889314 --- /dev/null +++ b/Working_Examples/215/CH9/EX9.6/Figure9_6_xcos.jpg diff --git a/Working_Examples/215/CH9/EX9.6/ex9_6.xcos b/Working_Examples/215/CH9/EX9.6/ex9_6.xcos new file mode 100755 index 0000000..003f103 --- /dev/null +++ b/Working_Examples/215/CH9/EX9.6/ex9_6.xcos @@ -0,0 +1 @@ +<?xml version="1.0" encoding="UTF-8"?><XcosDiagram background="-1" finalIntegrationTime="5.0" title="ex9_6"><!--Xcos - 1.0 - scilab-5.5.2 - 20160406 2040--><mxGraphModel as="model"><root><mxCell id="-7cfb447d:134ed64a89d:-7ffd"/><mxCell id="-7cfb447d:134ed64a89d:-7ffe" 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