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-rwxr-xr-xWorking_Examples/293/CH1/EX1.1/eg1_1.sce8
-rwxr-xr-xWorking_Examples/293/CH11/EX11.1/eg11_1.sce11
-rwxr-xr-xWorking_Examples/293/CH11/EX11.2/eg11_2.sce11
-rwxr-xr-xWorking_Examples/293/CH11/EX11.3/eg11_3.sce5
-rwxr-xr-xWorking_Examples/293/CH12/EX12.2/eg12_2.pdfbin0 -> 13151 bytes
-rwxr-xr-xWorking_Examples/293/CH12/EX12.2/eg12_2.xcos1
-rwxr-xr-xWorking_Examples/293/CH12/EX12.3.a/eg12_3a.pdfbin0 -> 17711 bytes
-rwxr-xr-xWorking_Examples/293/CH12/EX12.3.a/eg12_3a.xcos1
-rwxr-xr-xWorking_Examples/293/CH12/EX12.3.b/eg12_3b.pdfbin0 -> 17711 bytes
-rwxr-xr-xWorking_Examples/293/CH12/EX12.3.b/eg12_3b.xcos1
-rwxr-xr-xWorking_Examples/293/CH15/EX15.1/eg15_1.sce42
-rwxr-xr-xWorking_Examples/293/CH15/EX15.3/eg15_3.sce39
-rwxr-xr-xWorking_Examples/293/CH15/EX15.5/eg15_5.sce12
-rwxr-xr-xWorking_Examples/293/CH16/EX16.1/eg16_1.sce56
-rwxr-xr-xWorking_Examples/293/CH16/EX16.2/eg16_2.sce31
-rwxr-xr-xWorking_Examples/293/CH16/EX16.3/eg16_3.sce25
-rwxr-xr-xWorking_Examples/293/CH18/EX18.1/eg18_1.sce50
-rwxr-xr-xWorking_Examples/293/CH19/EX19.1/eg19_1.sce30
-rwxr-xr-xWorking_Examples/293/CH2/EX2.1.a/eg2_1a.sce6
-rwxr-xr-xWorking_Examples/293/CH2/EX2.1.b/eg2_1b.sce10
-rwxr-xr-xWorking_Examples/293/CH2/EX2.1.c/eg2_1c.sce15
-rw-r--r--Working_Examples/293/CH2/EX2.10/eg210.xcos1
-rwxr-xr-xWorking_Examples/293/CH2/EX2.10/eg2_10.pdfbin0 -> 1937 bytes
-rwxr-xr-xWorking_Examples/293/CH2/EX2.10/eg2_10.xcos1
-rwxr-xr-xWorking_Examples/293/CH2/EX2.2/eg2_2.sce17
-rwxr-xr-xWorking_Examples/293/CH2/EX2.3/eg2_3.sce6
-rwxr-xr-xWorking_Examples/293/CH2/EX2.4/eg2_4.sce8
-rwxr-xr-xWorking_Examples/293/CH2/EX2.5/eg2_5.pdfbin0 -> 12768 bytes
-rwxr-xr-xWorking_Examples/293/CH2/EX2.5/eg2_5.sce22
-rwxr-xr-xWorking_Examples/293/CH2/EX2.6/eg2_6.pdfbin0 -> 13662 bytes
-rwxr-xr-xWorking_Examples/293/CH2/EX2.6/eg2_6.sce26
-rwxr-xr-xWorking_Examples/293/CH2/EX2.7/eg2_7.sce17
-rwxr-xr-xWorking_Examples/293/CH2/EX2.8/eg2_8.sce5
-rwxr-xr-xWorking_Examples/293/CH2/EX2.9/eg2_9.sce6
-rwxr-xr-xWorking_Examples/293/CH20/EX20.2/eg20_2.sce36
-rwxr-xr-xWorking_Examples/293/CH20/EX20.3/eg20_3.sce13
-rwxr-xr-xWorking_Examples/293/CH20/EX20.4/eg20_4.sce38
-rwxr-xr-xWorking_Examples/293/CH23/EX23.1/eg23_1.sce12
-rwxr-xr-xWorking_Examples/293/CH24/EX24.2/eg24_2.sce39
-rwxr-xr-xWorking_Examples/293/CH3/EX3.1/eg3_1.sce10
-rwxr-xr-xWorking_Examples/293/CH3/EX3.10/eg3_10.pdfbin0 -> 3380 bytes
-rwxr-xr-xWorking_Examples/293/CH3/EX3.10/eg3_10.xcos1
-rwxr-xr-xWorking_Examples/293/CH3/EX3.11/eg3_11.pdfbin0 -> 1982 bytes
-rwxr-xr-xWorking_Examples/293/CH3/EX3.11/eg3_11.xcos1
-rwxr-xr-xWorking_Examples/293/CH3/EX3.12/eg3_12.sce29
-rwxr-xr-xWorking_Examples/293/CH3/EX3.13/eg3_13.sce15
-rwxr-xr-xWorking_Examples/293/CH3/EX3.14/eg3_14.pdfbin0 -> 2121 bytes
-rwxr-xr-xWorking_Examples/293/CH3/EX3.14/eg3_14.xcos1
-rwxr-xr-xWorking_Examples/293/CH3/EX3.15/eg3_15.pdfbin0 -> 2136 bytes
-rwxr-xr-xWorking_Examples/293/CH3/EX3.15/eg3_15.xcos1
-rwxr-xr-xWorking_Examples/293/CH3/EX3.2/eg3_2.sce10
-rwxr-xr-xWorking_Examples/293/CH3/EX3.3/eg3_3.sce12
-rwxr-xr-xWorking_Examples/293/CH3/EX3.4/eg3_4.sce25
-rwxr-xr-xWorking_Examples/293/CH3/EX3.5/eg3_5.pdfbin0 -> 2119 bytes
-rwxr-xr-xWorking_Examples/293/CH3/EX3.5/eg3_5.xcos1
-rwxr-xr-xWorking_Examples/293/CH3/EX3.6/eg3_6.pdfbin0 -> 2006 bytes
-rwxr-xr-xWorking_Examples/293/CH3/EX3.6/eg3_6.xcos1
-rwxr-xr-xWorking_Examples/293/CH3/EX3.7/eg3_7.pdfbin0 -> 2035 bytes
-rwxr-xr-xWorking_Examples/293/CH3/EX3.7/eg3_7.xcos1
-rwxr-xr-xWorking_Examples/293/CH3/EX3.8/eg3_8.sce17
-rwxr-xr-xWorking_Examples/293/CH3/EX3.9/eg3_9.pdfbin0 -> 4572 bytes
-rwxr-xr-xWorking_Examples/293/CH3/EX3.9/eg3_9.xcos1
-rwxr-xr-xWorking_Examples/293/CH4/EX4.3/eg4_3.sce10
-rwxr-xr-xWorking_Examples/293/CH5/EX5.1/eg5_1.pdfbin0 -> 11097 bytes
-rwxr-xr-xWorking_Examples/293/CH5/EX5.1/eg5_1.xcos1
-rwxr-xr-xWorking_Examples/293/CH5/EX5.2/eg5_2.pdfbin0 -> 28142 bytes
-rwxr-xr-xWorking_Examples/293/CH5/EX5.2/eg5_2.sce9
-rwxr-xr-xWorking_Examples/293/CH5/EX5.2/eg5_2.xcos1
-rwxr-xr-xWorking_Examples/293/CH5/EX5.3/eg5_3.pdfbin0 -> 94474 bytes
-rwxr-xr-xWorking_Examples/293/CH5/EX5.3/eg5_3.xcos1
-rwxr-xr-xWorking_Examples/293/CH5/EX5.5/eg5_5.pdfbin0 -> 47080 bytes
-rwxr-xr-xWorking_Examples/293/CH5/EX5.5/eg5_5.xcos1
-rwxr-xr-xWorking_Examples/293/CH5/EX5.6/eg5_6.pdfbin0 -> 30205 bytes
-rwxr-xr-xWorking_Examples/293/CH5/EX5.6/eg5_6.xcos1
-rwxr-xr-xWorking_Examples/293/CH5/EX5.7/eg5_7.pdfbin0 -> 26343 bytes
-rwxr-xr-xWorking_Examples/293/CH5/EX5.7/eg5_7.xcos1
-rwxr-xr-xWorking_Examples/293/CH5/EX5.8/eg5_8.pdfbin0 -> 31745 bytes
-rwxr-xr-xWorking_Examples/293/CH5/EX5.8/eg5_8.xcos1
-rwxr-xr-xWorking_Examples/293/CH6/EX6.1/eg6_1.sce6
-rwxr-xr-xWorking_Examples/293/CH7/EX7.1/eg7_1.sce6
-rwxr-xr-xWorking_Examples/293/CH7/EX7.10/eg7_10.sce14
-rwxr-xr-xWorking_Examples/293/CH7/EX7.11/eg7_11.sce14
-rwxr-xr-xWorking_Examples/293/CH7/EX7.2/eg7_2.sce9
-rwxr-xr-xWorking_Examples/293/CH7/EX7.3/eg7_3.sce10
-rwxr-xr-xWorking_Examples/293/CH7/EX7.4/eg7_4.sce14
-rwxr-xr-xWorking_Examples/293/CH7/EX7.5/eg7_5.sce16
-rwxr-xr-xWorking_Examples/293/CH7/EX7.6/eg7_6.sce7
-rwxr-xr-xWorking_Examples/293/CH7/EX7.7/eg7_7.sce41
-rwxr-xr-xWorking_Examples/293/CH7/EX7.8/eg7_8.sce12
-rwxr-xr-xWorking_Examples/293/CH7/EX7.9/eg7_9.sce29
-rwxr-xr-xWorking_Examples/293/CH9/EX9.2/eg9_2.sce12
-rwxr-xr-xWorking_Examples/293/CH9/EX9.3/eg9_3.sce38
92 files changed, 981 insertions, 0 deletions
diff --git a/Working_Examples/293/CH1/EX1.1/eg1_1.sce b/Working_Examples/293/CH1/EX1.1/eg1_1.sce
new file mode 100755
index 0000000..8854506
--- /dev/null
+++ b/Working_Examples/293/CH1/EX1.1/eg1_1.sce
@@ -0,0 +1,8 @@
+E0 = 1/(36*%pi*10^9); //permitivity in free space
+k = 4*%pi*E0 ;
+q1 = 1; // charge on the first particle in coulombs
+q2 = 1; // charge on the second particle in coulombs
+d = 1; // distance between the particles in meter
+F = (q1*q2)/(k*d^2); //force between the two particles in newtons
+
+disp(F, "force in free space between the two particles is in Newtons is:") \ No newline at end of file
diff --git a/Working_Examples/293/CH11/EX11.1/eg11_1.sce b/Working_Examples/293/CH11/EX11.1/eg11_1.sce
new file mode 100755
index 0000000..d7a5df0
--- /dev/null
+++ b/Working_Examples/293/CH11/EX11.1/eg11_1.sce
@@ -0,0 +1,11 @@
+//a
+N2 = '101'; //binary ordered sequence
+N = bin2dec(N2); //decimal equivalent of N2
+disp("a")
+disp(N, "decimal equivalent of 101 = ")
+
+//b
+N2 = '11011'; //binary ordered sequence
+N = bin2dec(N2); //decimal equivalent of N2
+disp("b")
+disp(N, "decimal equivalent of 11011 = ") \ No newline at end of file
diff --git a/Working_Examples/293/CH11/EX11.2/eg11_2.sce b/Working_Examples/293/CH11/EX11.2/eg11_2.sce
new file mode 100755
index 0000000..2158620
--- /dev/null
+++ b/Working_Examples/293/CH11/EX11.2/eg11_2.sce
@@ -0,0 +1,11 @@
+//a
+N8 = '432'; //octal number
+N = oct2dec(N8); //decimal representation of N8
+disp("a")
+disp(N,"decimal equivalent of 432 = ")
+
+//b
+N16 = 'C4F'; //hexadecimal number
+N = hex2dec(N16); //decimal representation of N16
+disp("b")
+disp(N,"decimal equivalent of C4F = ")
diff --git a/Working_Examples/293/CH11/EX11.3/eg11_3.sce b/Working_Examples/293/CH11/EX11.3/eg11_3.sce
new file mode 100755
index 0000000..3d06f04
--- /dev/null
+++ b/Working_Examples/293/CH11/EX11.3/eg11_3.sce
@@ -0,0 +1,5 @@
+N = 247;
+N2 = dec2bin(N); //binary equivalent of N
+N8 = dec2oct(N); //octal equivalent of N
+disp(N2, "binary equivalent of 247 = ")
+disp(N8, "octal equivalent of 247 = ") \ No newline at end of file
diff --git a/Working_Examples/293/CH12/EX12.2/eg12_2.pdf b/Working_Examples/293/CH12/EX12.2/eg12_2.pdf
new file mode 100755
index 0000000..7ca568c
--- /dev/null
+++ b/Working_Examples/293/CH12/EX12.2/eg12_2.pdf
Binary files differ
diff --git a/Working_Examples/293/CH12/EX12.2/eg12_2.xcos b/Working_Examples/293/CH12/EX12.2/eg12_2.xcos
new file mode 100755
index 0000000..f105056
--- /dev/null
+++ b/Working_Examples/293/CH12/EX12.2/eg12_2.xcos
@@ -0,0 +1 @@
+<?xml version="1.0" encoding="UTF-8"?><XcosDiagram background="-1" finalIntegrationTime="4.0" title="eg12_2"><!--Xcos - 1.0 - scilab-5.5.2 - 20160406 2040--><mxGraphModel as="model"><root><mxCell id="47283b12:1341c9b3c8b:-78f6"/><mxCell id="47283b12:1341c9b3c8b:-78f7" parent="47283b12:1341c9b3c8b:-78f6"/><BasicBlock blockType="d" id="47283b12:1341c9b3c8b:-78e6" interfaceFunctionName="GENSQR_f" ordering="1" parent="47283b12:1341c9b3c8b:-78f7" simulationFunctionName="gensqr" simulationFunctionType="DEFAULT" style="GENSQR_f;flip=false;mirror=false"><ScilabString as="exprs" height="1" width="1"><data column="0" line="0" value="1"/></ScilabString><ScilabDouble as="realParameters" height="0" width="0"/><ScilabDouble as="integerParameters" height="0" width="0"/><Array as="objectsParameters" scilabClass="ScilabList"/><ScilabDouble as="nbZerosCrossing" height="1" width="1"><data column="0" line="0" realPart="0.0"/></ScilabDouble><ScilabDouble as="nmode" height="1" width="1"><data column="0" line="0" realPart="0.0"/></ScilabDouble><ScilabDouble as="dState" height="1" width="1"><data column="0" line="0" realPart="1.0"/></ScilabDouble><Array as="oDState" scilabClass="ScilabList"/><Array as="equations" scilabClass="ScilabList"/><mxGeometry as="geometry" height="40.0" width="70.0" x="30.0" y="280.0"/></BasicBlock><ControlPort dataType="UNKNOW_TYPE" id="47283b12:1341c9b3c8b:-78e4" ordering="1" parent="47283b12:1341c9b3c8b:-78e6" style="ControlPort;align=center;verticalAlign=top;spacing=10;rotation=90;flip=false;mirror=false"><mxGeometry as="geometry" height="8.0" width="8.0" x="36.0" y="-8.0"/></ControlPort><ExplicitOutputPort dataColumns="1" dataLines="1" dataType="REAL_MATRIX" id="47283b12:1341c9b3c8b:-78e5" ordering="1" parent="47283b12:1341c9b3c8b:-78e6" style="ExplicitOutputPort;align=right;verticalAlign=middle;spacing=10;rotation=0;flip=false;mirror=false"><mxGeometry as="geometry" height="8.0" width="8.0" x="70.0" y="16.0"/></ExplicitOutputPort><BasicBlock blockType="h" 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diff --git a/Working_Examples/293/CH12/EX12.3.b/eg12_3b.pdf b/Working_Examples/293/CH12/EX12.3.b/eg12_3b.pdf
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diff --git a/Working_Examples/293/CH12/EX12.3.b/eg12_3b.xcos b/Working_Examples/293/CH12/EX12.3.b/eg12_3b.xcos
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diff --git a/Working_Examples/293/CH15/EX15.1/eg15_1.sce b/Working_Examples/293/CH15/EX15.1/eg15_1.sce
new file mode 100755
index 0000000..2417766
--- /dev/null
+++ b/Working_Examples/293/CH15/EX15.1/eg15_1.sce
@@ -0,0 +1,42 @@
+//a
+phi = 6*10^-4; //given magnetic flux (in Wb)
+A = 0.001; // cross sectional area (in meter square)
+B = phi/A ; //
+Ha = 10; //magnetic field intensity of material a needed to establish the given magnetic flux
+Hb = 77; // magnetic field intensity of material b
+Hc = 270; // magnetic field intensity of material c
+La = 0.3; //arc length of material a (in meters)
+Lb = 0.2; //arc length of material b (in meters)
+Lc = 0.1; //arc length of material c (in meters)
+
+F = Ha*La + Hb*Lb + Hc*Lc; //magnetomotive force
+disp("a")
+disp(F, "magnetomotive force needed to establish a flux of 6*10^-4(in At) = ")
+
+//b
+N = 100; //no. of turns
+I = F/N; //current in amps
+disp("b")
+disp(I,"current that must be made to flow through the coil(in amps) = ")
+
+//c
+MU0 = 4*%pi*10^-7;
+MUa = B/Ha; //permeability of material a
+MUb = B/Hb; //permeability of material b
+MUc = B/Hc; //permeability of material c
+
+MUra = MUa/MU0; //relative permeability of material a
+MUrb = MUb/MU0; //relative permeability of material b
+MUrc = MUc/MU0; //relative permeability of material c
+
+Ra = Ha*La/phi; //reluctance of material a
+Rb = Hb*Lb/phi; //reluctance of material b
+Rc = Hc*Lc/phi; //reluctance of material c
+
+disp("c")
+disp(MUra,"relative permeability of material a = ")
+disp(MUrb,"relative permeability of material b = ")
+disp(MUrc,"relative permeability of material c = ")
+disp(Ra,"reluctance of material a = ")
+disp(Rb,"reluctance of material b = ")
+disp(Rc,"reluctance of material c = ") \ No newline at end of file
diff --git a/Working_Examples/293/CH15/EX15.3/eg15_3.sce b/Working_Examples/293/CH15/EX15.3/eg15_3.sce
new file mode 100755
index 0000000..db0e188
--- /dev/null
+++ b/Working_Examples/293/CH15/EX15.3/eg15_3.sce
@@ -0,0 +1,39 @@
+mu0 = 4*%pi*10^-7;
+A = 0.0025; //cross sectional area of the coil
+//dimensions of the coil (in meters)
+Lg = 0.002; //air gap length (in meters)
+Lbd = 0.025;
+Lde = 0.1;
+Lef = 0.025;
+Lfk = 0.2;
+Lbc = 0.175;
+Lcab = 0.5;
+
+Lbghc = 2*(Lbd + Lde + Lef + (Lfk/2)) - Lg;//length of the ferromagnetic material involved here
+
+phig = 4*10^-4; //air gap flux (in Wb)
+Bg = phig/A ; //air gap flux density (in tesla)
+Hg = Bg/mu0 ; //feild intensity of the air gap
+mmfg = Hg*Lg ; //mmf produced in the air gap (in At)
+
+Bbc = 1.38 ; //flux density corresponding to cast steel
+
+Hbghc = 125; //field intensity corresponding to flux density of 0.16T in the steel
+mmfbghc = Hbghc*Lbghc ; // mmf corresponding to bghc
+
+mmfbc = mmfg + mmfbghc ; //mmf across path bc
+Hbc = mmfbc/Lbc;
+phibc = Bbc*A ; //flux produced in bc
+
+phicab = phig + phibc; //total fiux existing in leg cab
+Bcab = phicab/0.00375; //flux density
+Hcab = 690;
+mmfcab = Hcab*Lcab; //mmf in leg cab
+
+mmf = mmfbc + mmfcab ; //mmf produced by the coil
+
+disp(mmf,"mmf produced by the coil(in At) = ")
+
+
+
+
diff --git a/Working_Examples/293/CH15/EX15.5/eg15_5.sce b/Working_Examples/293/CH15/EX15.5/eg15_5.sce
new file mode 100755
index 0000000..151ccb4
--- /dev/null
+++ b/Working_Examples/293/CH15/EX15.5/eg15_5.sce
@@ -0,0 +1,12 @@
+//b
+mu0 = 4*%pi*10^-7 ;
+//plunger magnet dimensions (in meters)
+x = 0.025;
+h = 0.05;
+a = 0.025;
+g = 0.00125;
+
+mmf = 1414; //(in At)
+
+F = %pi*a*mu0*(mmf^2)*(h^2)*(1/(x + h)^2)/g; //magnitude of the force
+disp(F, "magnitude of the force (in Newtons) = ") \ No newline at end of file
diff --git a/Working_Examples/293/CH16/EX16.1/eg16_1.sce b/Working_Examples/293/CH16/EX16.1/eg16_1.sce
new file mode 100755
index 0000000..dde1653
--- /dev/null
+++ b/Working_Examples/293/CH16/EX16.1/eg16_1.sce
@@ -0,0 +1,56 @@
+//a
+V1 = 1100; //higher voltage
+V2 = 220; //lower voltage
+a = V1/V2; //turns ratio
+r1 = 0.1; //high voltage winding resistance(in ohms)
+x1 = 0.3; //high voltage leakage reactance(in ohms)
+r2 = 0.004; //low voltage winding resistance(in ohms)
+x2 = 0.012; //low voltage leakage reactance(in ohms)
+
+Re1 = r1 + (a^2)*r2 ; //equivalent winding resistance referred to the primary side
+Xe1 = x1 + (a^2)*x2 ; //equivalent leakage reactance referred to the primary side
+Re2 = (r1/a^2) + r2 ; //equivalent winding resistance referred to the secondary side
+Xe2 = (x1/a^2) + x2 ; //equivalent leakage reactance referred to the secondary side
+
+disp("a")
+disp(Re1,"equivalent winding resistance referred to the primary side")
+disp(Xe1,"equivalent leakage reactance referred to the primary side")
+disp(Re2,"equivalent winding resistance referred to the secondary side")
+disp(Xe2,"equivalent leakage reactance referred to the secondary side")
+
+//b
+P = 100; //power (in kVA)
+I21 = P*1000/V1; //primary winding current rating
+Vre1 = I21*Re1; //equivalent resistance drop (in volts)
+VperR1 = Vre1*100/V1 ; // % equivalent resistance drop
+
+Vxe1 = I21*Xe1; //equivalent reactance drop (in volts)
+VperX1 = Vxe1*100/V1; // % equivalent reactance drop
+
+disp("b")
+disp(Vre1,"equivalent resistance drop expressed in terms of primary quantities(in volts) = ")
+disp(VperR1,"% equivalent resistance drop expressed in terms of primary quantities = ")
+disp(Vxe1,"equivalent reactance drop expressed in terms of primary quantities(in volts) =")
+disp(VperX1,"% equivalent reactance drop expressed in terms of primary quantities = ")
+
+//c
+I2 = a*I21; // secondary winding current rating
+Vre2 = I2*Re2; //equivalent resistance drop (in volts)
+VperR2 = Vre2*100/V2 ; // % equivalent resistance drop
+
+Vxe2 = I2*Xe2; //equivalent reactance drop (in volts)
+VperX2 = Vxe2*100/V2; // % equivalent reactance drop
+
+disp("c")
+disp(Vre2,"equivalent resistance drop expressed in terms of secondary quantities(in volts) = ")
+disp(VperR2,"% equivalent resistance drop expressed in terms of secondary quantities = ")
+disp(Vxe2,"equivalent reactance drop expressed in terms of secondary quantities(in volts) =")
+disp(VperX2,"% equivalent reactance drop expressed in terms of secondary quantities = ")
+
+//d
+Ze1 = complex(Re1,Xe1); //equivalent leakage impedance referred to the primary
+Ze2 = Ze1/a ; //equivalent leakage impedance referred to the secondary
+
+disp("d")
+disp(Ze1,"equivalent leakage impedance referred to the primary = ")
+disp(Ze2,"equivalent leakage impedance referred to the secondary = ") \ No newline at end of file
diff --git a/Working_Examples/293/CH16/EX16.2/eg16_2.sce b/Working_Examples/293/CH16/EX16.2/eg16_2.sce
new file mode 100755
index 0000000..978e1e7
--- /dev/null
+++ b/Working_Examples/293/CH16/EX16.2/eg16_2.sce
@@ -0,0 +1,31 @@
+Pl = 396; //wattmeter reading on open circuit test
+Vl = 120; //voltmeter reading on open circuit test
+Il = 9.65; //ammeter reading o open circuit test
+a = 2400/120; //turns ratio
+
+theata = acos(Pl/(Vl*Il)); //phase difference between voltage and current
+Irl = Il*cos(theata); //resistive part of Im
+Ixl = Il*sin(theata); //reactive part of Im
+
+rl = Vl/Irl; //low voltage winding resistance
+rh = (a^2)*rl; //rl on the high side
+xl = Vl/Ixl; //magnetizing reactance referred to the lower side
+xh = (a^2)*xl; //corresponding high side value
+
+Ph = 810; //wattmeter reading on short circuit test
+Vh = 92; //voltmeter reading on short circuit test
+Ih = 20.8; //ammeter reading on short circuit test
+
+Zeh = Vh/Ih; //equivalent impeadance referred to the higher side
+Zel = Zeh/(a^2); //equivalent impedance referred to the lower side
+Reh = Ph/(Ih^2); //equivalent resistance referred to the higher side
+Rel = Reh/(a^2); //equivalent resistance referred to the lower side
+Xeh = sqrt((Zeh^2) - (Reh^2)); //equivalent reactance referred to the higher side
+Xel = Xeh/(a^2); //equivalent reactance referred to the lower side
+
+disp(Zeh,"equivalent impeadance referred to the higher side = ")
+disp(Zel,"equivalent impedance referred to the lower side = ")
+disp(Reh,"equivalent resistance referred to the higher side = ")
+disp(Rel,"equivalent resistance referred to the lower side = ")
+disp(Xeh,"equivalent reactance referred to the higher side = ")
+disp(Xel,"equivalent reactance referred to the lower side = ")
diff --git a/Working_Examples/293/CH16/EX16.3/eg16_3.sce b/Working_Examples/293/CH16/EX16.3/eg16_3.sce
new file mode 100755
index 0000000..fb5fa91
--- /dev/null
+++ b/Working_Examples/293/CH16/EX16.3/eg16_3.sce
@@ -0,0 +1,25 @@
+//a
+P = 50; //power rating (in kVA)
+Ph = 810; //wattmeter reading on short circuit test
+Pl = 396; //wattmeter reading on open circuit test
+Ih = 20.8; //ammeter reading on short circuit test
+pf = 0.8; //power factor = 0.8 lagging
+
+losses = (Ph + Pl)/1000; //losses in kW
+outputP = P*pf; //output power
+inputP = outputP + losses ; //input power
+
+efficiency = outputP/inputP ;
+disp("a")
+disp(efficiency,"efficiency = ")
+
+//b
+Xeh = 4; //equivalent reactance referred to the higher side
+Reh = 1.87; //equivalent resistance referred to the higher side
+Zeh = complex(Reh, Xeh); //equivalent impedance referred to the higher side
+ih = complex(Ih*pf, -Ih*sqrt(1 - (pf^2)));
+V1 = 2400 + Zeh*ih ; //primary voltage
+
+voltageRegulation = (real(V1)-2400)*100/2400;//percent voltage regulation
+disp("b")
+disp(voltageRegulation,"percent voltage regulaton = ") \ No newline at end of file
diff --git a/Working_Examples/293/CH18/EX18.1/eg18_1.sce b/Working_Examples/293/CH18/EX18.1/eg18_1.sce
new file mode 100755
index 0000000..068b46b
--- /dev/null
+++ b/Working_Examples/293/CH18/EX18.1/eg18_1.sce
@@ -0,0 +1,50 @@
+//a
+V1 = 440/sqrt(3);
+s = 0.025; //slip
+r1 = 0.1;
+r2 = 0.12;
+x1 = 0.35;
+x2 = 0.4;
+
+z = complex(r1 + r2/s, x1 + x2);
+i2 = V1/z; //input line current
+I2 = sqrt(real(i2)^2 + imag(i2)^2); //magnitude of input line current
+disp("a")
+disp(i2,"input line current = ")
+
+i1 = complex(18*cos(-1.484), 18*sin(-1.484)); // magnetizing current
+I1 = sqrt(real(i1)^2 + imag(i1)^2); //magnitude of magnetizing current
+i = i1 + i2; //total current drawn from the voltage source
+I = sqrt(real(i)^2 + imag(i)^2); //magnitude of total current
+theta = atan(imag(i)/real(i)); //phase difference between current and voltage
+pf = cos(theta); //power factor
+disp(pf,"power factor = ")
+if theta >= 0 then
+ disp("leading")
+else disp("lagging")
+end
+
+//b
+f = 60; //hertz
+ns = 1800;
+ws = 2*%pi*ns/f; //stator angular velocity
+Pg = 3*I2^2*r2/s; //power
+T = Pg/ws; //developed electromagnetic torque
+disp("b")
+disp(T,"developed electromagneic torque (in Newton-meter) = ")
+
+//c
+Prot = 950; //rotational losses (in watts)
+Po = Pg*(1 - s) - Prot ; //output power
+HPo = Po/746; //output horse power
+disp("c")
+disp(HPo,"output horse power = ")
+
+//d
+Pc = 1200; //core losses (in W)
+SCL = 3*I^2*r1; //stator copper loss
+RCL = 3*I2^2*r2; //rotar copper loss
+loss = Pc + SCL + RCL + Prot; //total losses
+Pi = real(3*V1*i); //input power
+efficiency = 1 - (loss/Pi);
+disp(efficiency,"efficiency = ") \ No newline at end of file
diff --git a/Working_Examples/293/CH19/EX19.1/eg19_1.sce b/Working_Examples/293/CH19/EX19.1/eg19_1.sce
new file mode 100755
index 0000000..a1f4f18
--- /dev/null
+++ b/Working_Examples/293/CH19/EX19.1/eg19_1.sce
@@ -0,0 +1,30 @@
+//a
+efficiency = 0.9;
+Pi = 200*746/efficiency; //input power
+x = 11; //reactance of the motor
+V1 = 2300/sqrt(3); //voltage rating
+delta = 15*%pi/180; //power angle
+Ef = Pi*x/(3*V1*sin(delta)); //the induced excitation voltage per phase
+disp("a")
+disp(Ef,"the induced excitation voltage per phase = ")
+
+//b
+z = complex(0,x); //impedance of the motor
+ef = complex(Ef*cos(-delta),Ef*sin(-delta));
+
+Ia = (V1 - ef)/z ; //armature current
+disp("b")
+disp(Ia,"armatur current = ")
+
+//c
+theata = atan(imag(Ia)/real(Ia)); //phase difference between Ia and V1
+pf = cos(theata); //power factor
+
+disp("c")
+disp(pf,"power factor = ")
+
+if sin(theata)> 0 then
+ disp("leading")
+else
+ disp("lagging")
+end \ No newline at end of file
diff --git a/Working_Examples/293/CH2/EX2.1.a/eg2_1a.sce b/Working_Examples/293/CH2/EX2.1.a/eg2_1a.sce
new file mode 100755
index 0000000..993d36f
--- /dev/null
+++ b/Working_Examples/293/CH2/EX2.1.a/eg2_1a.sce
@@ -0,0 +1,6 @@
+V = 1; // voltage supply
+R = 10; // resistance in ohms
+I = V/R //current flowing through R
+disp("a)")
+disp(V,"voltage across the resistor (in volts)=")
+disp(I,"current flowing through the resistor (in amps) =")
diff --git a/Working_Examples/293/CH2/EX2.1.b/eg2_1b.sce b/Working_Examples/293/CH2/EX2.1.b/eg2_1b.sce
new file mode 100755
index 0000000..154f28e
--- /dev/null
+++ b/Working_Examples/293/CH2/EX2.1.b/eg2_1b.sce
@@ -0,0 +1,10 @@
+V = 1; // voltage supply
+R1 = 10; // first resistance in ohms
+R2 = 5; //resistance of the second resistor
+Vr1 = V * (R1/(R1 + R2)); //voltage across R1
+Vr2 = V - Vr1; //voltage across R2
+Ir = Vr1/R1; //current flowing through R
+
+disp(Vr1,"voltage across the first resistor (in volts)=")
+disp(Vr2,"voltage across the second resistor (in volts)=")
+disp(Ir,"current flowing through the resistor (in amps) =") \ No newline at end of file
diff --git a/Working_Examples/293/CH2/EX2.1.c/eg2_1c.sce b/Working_Examples/293/CH2/EX2.1.c/eg2_1c.sce
new file mode 100755
index 0000000..a0f263d
--- /dev/null
+++ b/Working_Examples/293/CH2/EX2.1.c/eg2_1c.sce
@@ -0,0 +1,15 @@
+//c - a
+R1 = 10; // first resistance in ohms
+ R2 = 5;
+I = 1; // current source
+V = I*R1; // voltage across R
+disp("c - a)")
+disp(V,"voltage across the resistor (in volts)=")
+disp(I,"current flowing through the resistor (in amps) =")
+
+//c - b
+Vr1 = I*R1; // voltage across R1
+Vr2 = I*R2; //voltage across R2
+disp("c - b)")
+disp(V,"voltage across the resistor (in volts)=")
+disp(I,"current flowing through the resistor (in amps) =") \ No newline at end of file
diff --git a/Working_Examples/293/CH2/EX2.10/eg210.xcos b/Working_Examples/293/CH2/EX2.10/eg210.xcos
new file mode 100644
index 0000000..305262f
--- /dev/null
+++ b/Working_Examples/293/CH2/EX2.10/eg210.xcos
@@ -0,0 +1 @@
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diff --git a/Working_Examples/293/CH2/EX2.10/eg2_10.pdf b/Working_Examples/293/CH2/EX2.10/eg2_10.pdf
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diff --git a/Working_Examples/293/CH2/EX2.10/eg2_10.xcos b/Working_Examples/293/CH2/EX2.10/eg2_10.xcos
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diff --git a/Working_Examples/293/CH2/EX2.2/eg2_2.sce b/Working_Examples/293/CH2/EX2.2/eg2_2.sce
new file mode 100755
index 0000000..3714ebb
--- /dev/null
+++ b/Working_Examples/293/CH2/EX2.2/eg2_2.sce
@@ -0,0 +1,17 @@
+R = 100; // resistance in ohms
+I = 0.3; // current in amps
+P = I^2 * R; // power
+//power specification of the resistors available in the stock
+Pa = 5;
+Pb = 7.5;
+Pc = 10;
+
+if Pa > P then
+ disp("we should select resistor a")
+end
+if Pb > P then
+ disp("we should select resistor b")
+end
+if Pc > P then
+ disp("we should select resistor c")
+end \ No newline at end of file
diff --git a/Working_Examples/293/CH2/EX2.3/eg2_3.sce b/Working_Examples/293/CH2/EX2.3/eg2_3.sce
new file mode 100755
index 0000000..9a2694b
--- /dev/null
+++ b/Working_Examples/293/CH2/EX2.3/eg2_3.sce
@@ -0,0 +1,6 @@
+L = 1; //length of the copper wire in meters
+A = 1 * 10^-4; // cross sectional area of the wire in meter square
+rho = 1.724 * 10^-8; // resistivity of copper in ohm meter
+R = rho*L / A; // resistance of the wire in ohm
+
+disp(R, "resistance of the wire (in ohms)=") \ No newline at end of file
diff --git a/Working_Examples/293/CH2/EX2.4/eg2_4.sce b/Working_Examples/293/CH2/EX2.4/eg2_4.sce
new file mode 100755
index 0000000..2ea3640
--- /dev/null
+++ b/Working_Examples/293/CH2/EX2.4/eg2_4.sce
@@ -0,0 +1,8 @@
+//1 inches = 0.0254meters
+//1 foot = 0.3048 meters
+d = 0.1*0.0254; // diameter of the wire in meters
+L = 10*0.3048; //length of the wire in meters
+rho = 1.724*10^-8; // resistivity of the wire in ohm-meter
+A = %pi*(d/2)^2; // cross sectional area of the wire
+R = rho*L/A; //resistance of the wire in ohm
+disp(R,"resistance of the wire (in ohm)=") \ No newline at end of file
diff --git a/Working_Examples/293/CH2/EX2.5/eg2_5.pdf b/Working_Examples/293/CH2/EX2.5/eg2_5.pdf
new file mode 100755
index 0000000..f55213b
--- /dev/null
+++ b/Working_Examples/293/CH2/EX2.5/eg2_5.pdf
Binary files differ
diff --git a/Working_Examples/293/CH2/EX2.5/eg2_5.sce b/Working_Examples/293/CH2/EX2.5/eg2_5.sce
new file mode 100755
index 0000000..f1659ed
--- /dev/null
+++ b/Working_Examples/293/CH2/EX2.5/eg2_5.sce
@@ -0,0 +1,22 @@
+L = 0.1; // inductance of the coil in henry
+t1 = [0:0.001:0.1];
+t2 = [0.101:0.001:0.3];
+t3 = [0.301:0.001:0.6];
+t4 = [0.601:0.001:0.7];
+t5 = [0.701:0.001:0.9]
+//current variation as a function of time
+i1 = 100*t1;
+i2 = (-50*t2) + 15;
+i3 = -100*sin(%pi*(t3-0.3)/0.3);
+i4 = (100*t4) - 60;
+i5 = (-50*t5) + 45;
+
+t = [t1,t2,t3,t4,t5];
+i = [i1,i2,i3,i4,i5];
+plot(t, i)
+
+dt = 0.001;
+di = diff(i);
+V = L*di/dt; //voltage drop appearing across the inductor terminals
+Tv = [0:0.001:0.899];
+plot(Tv, V, "green") \ No newline at end of file
diff --git a/Working_Examples/293/CH2/EX2.6/eg2_6.pdf b/Working_Examples/293/CH2/EX2.6/eg2_6.pdf
new file mode 100755
index 0000000..7e625db
--- /dev/null
+++ b/Working_Examples/293/CH2/EX2.6/eg2_6.pdf
Binary files differ
diff --git a/Working_Examples/293/CH2/EX2.6/eg2_6.sce b/Working_Examples/293/CH2/EX2.6/eg2_6.sce
new file mode 100755
index 0000000..5094d17
--- /dev/null
+++ b/Working_Examples/293/CH2/EX2.6/eg2_6.sce
@@ -0,0 +1,26 @@
+C = 0.01; // capacitance of the capacitor in Farads
+t1 = [0:0.001:0.1];
+t2 = [0.101:0.001:0.3];
+t3 = [0.301:0.001:0.6];
+t4 = [0.601:0.001:0.7];
+t5 = [0.701:0.001:0.9]
+//current variation as a function of time
+i1 = 100*t1;
+i2 = (-50*t2) + 15;
+i3 = -100*sin(%pi*(t3-0.3)/0.3);
+i4 = (100*t4) - 60;
+i5 = (-50*t5) + 45;
+
+t = [t1,t2,t3,t4,t5];
+i = [i1,i2,i3,i4,i5];
+plot(t, i)
+
+// voltage across the capacitor as a function of time
+V1 = (1/C)*integrate('100*t','t',0,t1);
+V2 = (1/C)*integrate('(-50*t)+15','t',0.101,t2);
+V3 = (1/C)*integrate('-100*sin(%pi*(t-0.3)/0.3)','t',0.301,t3);
+V4 = (1/C)*integrate('(100*t) - 60','t',0.601,t4);
+V5 = (1/C)*integrate('(-50*t) + 45','t',0.701,t5);
+V = [V1, V2, V3, V4, V5];
+
+plot(t, V, "green") \ No newline at end of file
diff --git a/Working_Examples/293/CH2/EX2.7/eg2_7.sce b/Working_Examples/293/CH2/EX2.7/eg2_7.sce
new file mode 100755
index 0000000..3f437fe
--- /dev/null
+++ b/Working_Examples/293/CH2/EX2.7/eg2_7.sce
@@ -0,0 +1,17 @@
+//a
+Ri = 1;
+Rf = 39;
+A = 10^5; //open loop gain of the op-amp
+G = A/(1 + (A*Ri/(Ri+Rf))); //actual voltage gain of the circuit
+disp("a")
+disp(G,"actual voltage of the circuit =")
+
+//b
+G1 = 1 + (Rf/Ri); // voltage gain of the circuit with infinite open loop gain
+disp("b")
+disp(G1,"for ideal case the voltage gain =")
+
+//c
+er = ((G1 - G)/G)*100; //percent error
+disp("c")
+disp(er,"percent error of the ideal value compared to the actual value=") \ No newline at end of file
diff --git a/Working_Examples/293/CH2/EX2.8/eg2_8.sce b/Working_Examples/293/CH2/EX2.8/eg2_8.sce
new file mode 100755
index 0000000..9a60968
--- /dev/null
+++ b/Working_Examples/293/CH2/EX2.8/eg2_8.sce
@@ -0,0 +1,5 @@
+G = 4; // voltage gain of the circuit
+r = G -1; // ratio of the resistances in the non-inverting op-amp circuit
+disp(r,"Rf/Ri =")
+//Result:
+//A suitable choice for R1 is 10K, Hence Rf = 30K
diff --git a/Working_Examples/293/CH2/EX2.9/eg2_9.sce b/Working_Examples/293/CH2/EX2.9/eg2_9.sce
new file mode 100755
index 0000000..b204274
--- /dev/null
+++ b/Working_Examples/293/CH2/EX2.9/eg2_9.sce
@@ -0,0 +1,6 @@
+G = 4;
+r = G; // ratio of the resistances in the inverting op-amp circuit
+disp(r,"Rf/Ri")
+//Result;
+//A suitable choice for Rf=30K and R1=7.5K
+//therefore input resistance R1 = 7.5K
diff --git a/Working_Examples/293/CH20/EX20.2/eg20_2.sce b/Working_Examples/293/CH20/EX20.2/eg20_2.sce
new file mode 100755
index 0000000..396caca
--- /dev/null
+++ b/Working_Examples/293/CH20/EX20.2/eg20_2.sce
@@ -0,0 +1,36 @@
+//a
+Vt = 230; //(in volts)
+Ia = 73; //armature current (in amps)
+If = 1.6; //feild current (in amps)
+Ra = 0.188; //armature circuit resistance(in ohms)
+n = 1150; //rated speed of the rotor(in rpm)
+Po = 20*746; //output power (in watts)
+
+Ea = Vt - (Ia*Ra); //armature voltage
+wm = 2*%pi*n/60; //rated speed of the rotor (in rad/sec)
+T = Ea*Ia/wm ; //electromagnetic torque
+
+disp("a")
+disp(T,"electromagnetic torque = ")
+
+//b
+a = 4; //no. of parallel armature paths
+p = 4; //no. of poles
+z = 882; //no. of armature conductors
+flux = Ea*60*a/(p*z*n); //flux per pole (in Wb)
+
+disp("b")
+disp(flux,"flux per pole = ")
+
+//c
+Prot = (Ea*Ia) - Po; //rotational loss (in watt)
+disp("c")
+disp(Prot,"rotational losses = ")
+
+//d
+losses = Prot + (Ia^2 * Ra) + (Vt * If) ;
+Pi = (Ea*Ia) + (Ia^2 * Ra) + (Vt * If); //input power
+efficiency = 1 - (losses/Pi);
+
+disp("d")
+disp(efficiency,"efficiency = ") \ No newline at end of file
diff --git a/Working_Examples/293/CH20/EX20.3/eg20_3.sce b/Working_Examples/293/CH20/EX20.3/eg20_3.sce
new file mode 100755
index 0000000..5f7c18b
--- /dev/null
+++ b/Working_Examples/293/CH20/EX20.3/eg20_3.sce
@@ -0,0 +1,13 @@
+// final flux = 0.8*initial flux
+Ia1 = 73; //initial armature current (in amps)
+Vt = 230; //(in volts)
+Ra = 0.188; //armature circuit resistance
+n1 = 1150; //initial rotor speed (in rpm)
+Ea1 = 216.3; //initial armature voltage
+
+Ia2 = (1/0.8)*Ia1 ; //final armature current
+Ea2 = Vt - (Ia2*Ra); //final armature voltage
+
+n2 = (Ea2/Ea1)*(1/0.8)*n1; //final rotor speed
+
+disp(n2,"final rotor speed(in rpm) = ") \ No newline at end of file
diff --git a/Working_Examples/293/CH20/EX20.4/eg20_4.sce b/Working_Examples/293/CH20/EX20.4/eg20_4.sce
new file mode 100755
index 0000000..c792906
--- /dev/null
+++ b/Working_Examples/293/CH20/EX20.4/eg20_4.sce
@@ -0,0 +1,38 @@
+//a
+rop = 0.4; //ratio of ON time T0 to cycle time Tp
+Vb =550; //rated terminal voltage of the dc motor
+Ia = 30; //current drawn by the motor (in amps)
+Ra = 1; //armature circuit resistance (in ohms)
+ts = 5.94; //torque and speed parameter of the motor (in N-m/A)
+
+Vm = rop*Vb; //average value of the armature terminal voltage
+Ea = Vm - (Ia*Ra); //induced armature voltage
+
+wm = Ea/ts; //motor speed (in rad/s)
+disp("a")
+disp(wm,"motor speed (in rad/s) = ")
+
+//b
+deltaI = 5; //change of armature current during the ON period
+La = 0.1; //armature winding inductance (in H)
+To = La*deltaI/(Vb - Ea); //ON time
+Tp = To/rop; //cycle time
+
+f = 1/Tp ; //required pulses per second
+disp("b")
+disp(f,"required pulses per second = ")
+
+//c
+rop = 0.7; //new ratio of ON time T0 to cycle time Tp
+Vm = rop*Vb; //average value of the armature terminal voltage
+Ea = Vm - (Ia*Ra); //induced armature voltage
+
+wm = Ea/ts; //motor speed (in rad/s)
+disp("c")
+disp(wm,"motor speed with To/Tp equal to 0.7 (in rad/s) = ")
+
+To = La*deltaI/(Vb - Ea); //ON time
+Tp = To/rop; //cycle time
+
+f = 1/Tp ; //required pulses per second
+disp(f,"required pulses per second with To/Tp equal to 0.7 = ") \ No newline at end of file
diff --git a/Working_Examples/293/CH23/EX23.1/eg23_1.sce b/Working_Examples/293/CH23/EX23.1/eg23_1.sce
new file mode 100755
index 0000000..18ac13b
--- /dev/null
+++ b/Working_Examples/293/CH23/EX23.1/eg23_1.sce
@@ -0,0 +1,12 @@
+deltaGi = 420 - 380; //variation in the without feedback gain
+Gi = 400; //without feedback gain
+T = 400; //transfer function of the closed loop system
+// (variation in T)/T = (change in G)/G * (1/ 1+H*G) = 0.02
+//1 + H*G = R
+R = (deltaGi/Gi)/0.02;
+
+G = T*R; //new direct transmission gain with feedback
+H = (G/T - 1)/G; //feedback factor
+
+disp(G,"new direct transmission gain with feedback = ")
+disp(H,"feedback factors = ") \ No newline at end of file
diff --git a/Working_Examples/293/CH24/EX24.2/eg24_2.sce b/Working_Examples/293/CH24/EX24.2/eg24_2.sce
new file mode 100755
index 0000000..fa8965c
--- /dev/null
+++ b/Working_Examples/293/CH24/EX24.2/eg24_2.sce
@@ -0,0 +1,39 @@
+//a
+//parameter values
+Kp = 0.5; //V/rad
+Ka = 100; //V/V
+Km = 2*10^-4 ; //lb-ft/V
+F = 1.5*10^-4; //lb-ft/rad/s
+J = 10^-5 //slug-ft^2
+
+K = Kp*Ka*Km ; //loop propotional gain
+dr = F/(2*sqrt(K*J)); //damping ratio
+wn = sqrt(K/J);
+ts = 5/(dr*wn);
+wd = wn*sqrt(1 - dr^2); //frequency at which damped oscillations occur
+disp("a")
+disp(wd, "damped oscillations occur at a frequency = ")
+disp(dr,"damping ratio = ")
+
+//b
+Tl = 10^-3; //load disturbance (lb-ft)
+e = Tl/K; //position lag error
+disp("b")
+disp(e,"position lag error (in rad) = ")
+
+//c
+KaNew = (e/0.025)*Ka; //new loop gain
+disp("c")
+disp(KaNew,"new loop gain for which the position lag error is equal to 0.025rad = ")
+
+//d
+drNew = F/(2*sqrt(Kp*KaNew*Km*J)); //new damping ratio
+disp("d")
+disp(drNew,"new damping ratio = ")
+
+//e
+//for a maximum overshoot of 25% , (F + Qo)/2*sqrt(K*J) = 0.4
+Qo = (0.4*2*sqrt(Kp*KaNew*Km*J)) - F ;
+Ko = Qo/(KaNew*K) ; //output gain factor
+disp("e")
+disp(Ko,"output gain factor = ") \ No newline at end of file
diff --git a/Working_Examples/293/CH3/EX3.1/eg3_1.sce b/Working_Examples/293/CH3/EX3.1/eg3_1.sce
new file mode 100755
index 0000000..5f9ef05
--- /dev/null
+++ b/Working_Examples/293/CH3/EX3.1/eg3_1.sce
@@ -0,0 +1,10 @@
+V = 100; // volatage supply in volts
+Rs = 40; //resistance in series in ohms
+// parallel resistances in ohms
+Rp1 = 33.33;
+Rp2 = 50;
+Rp3 = 20;
+Rpinv = (1/Rp1)+(1/Rp2)+(1/Rp3); //reciprocal of equivalent resistance in parallel
+Req = Rs + (1/Rpinv) ;
+I = V/Req; //current flowing from the voltage source in amps
+disp(I,"current flowing from the voltage source(in amps) = ") \ No newline at end of file
diff --git a/Working_Examples/293/CH3/EX3.10/eg3_10.pdf b/Working_Examples/293/CH3/EX3.10/eg3_10.pdf
new file mode 100755
index 0000000..8bdf4a6
--- /dev/null
+++ b/Working_Examples/293/CH3/EX3.10/eg3_10.pdf
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diff --git a/Working_Examples/293/CH3/EX3.10/eg3_10.xcos b/Working_Examples/293/CH3/EX3.10/eg3_10.xcos
new file mode 100755
index 0000000..e07264c
--- /dev/null
+++ b/Working_Examples/293/CH3/EX3.10/eg3_10.xcos
@@ -0,0 +1 @@
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diff --git a/Working_Examples/293/CH3/EX3.11/eg3_11.pdf b/Working_Examples/293/CH3/EX3.11/eg3_11.pdf
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--- /dev/null
+++ b/Working_Examples/293/CH3/EX3.11/eg3_11.pdf
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diff --git a/Working_Examples/293/CH3/EX3.11/eg3_11.xcos b/Working_Examples/293/CH3/EX3.11/eg3_11.xcos
new file mode 100755
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--- /dev/null
+++ b/Working_Examples/293/CH3/EX3.11/eg3_11.xcos
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y="430.0"/></TextBlock></root></mxGraphModel><mxCell as="defaultParent" id="-108078b6:1345b8f2778:-79f9" parent="-108078b6:1345b8f2778:-79f8"/></XcosDiagram> \ No newline at end of file
diff --git a/Working_Examples/293/CH3/EX3.12/eg3_12.sce b/Working_Examples/293/CH3/EX3.12/eg3_12.sce
new file mode 100755
index 0000000..178b314
--- /dev/null
+++ b/Working_Examples/293/CH3/EX3.12/eg3_12.sce
@@ -0,0 +1,29 @@
+//a
+// circuit parameters
+E1 = 120;
+R1 = 40;
+R2 = 20;
+R3 = 60;
+
+Voc = E1*R2/(R2 + R1); //open circuit voltage appearing at terminal 1
+Ri = R3 + (R1*R2/(R1 + R2)); //equivalent resistance looking into the network from terminal pair 01
+
+function I = Il(Rl)
+ I = Voc/(Ri + Rl) //current through Rl
+endfunction
+
+Il1 = Il(10); //Rl = 10 ohm
+Il2 = Il(50); //Rl = 50 ohm
+Il3 = Il(200); //Rl = 200 ohm
+
+disp("a")
+disp(Il1,"Il (Rl = 10ohm) = ")
+disp(Il2,"Il (Rl = 50ohm) = ")
+disp(Il3,"Il (Rl = 200ohm) = ")
+
+//b
+//for maximum power Rl = Ri
+Rl = Ri;
+Plmax = (Voc/(2*Ri))^2 * Ri ; //maximum power to Rl
+disp("b")
+disp(Plmax,"maximum power to Rl(in Watt) = ") \ No newline at end of file
diff --git a/Working_Examples/293/CH3/EX3.13/eg3_13.sce b/Working_Examples/293/CH3/EX3.13/eg3_13.sce
new file mode 100755
index 0000000..7de1797
--- /dev/null
+++ b/Working_Examples/293/CH3/EX3.13/eg3_13.sce
@@ -0,0 +1,15 @@
+//circuit parameters
+//voltage sources
+E1 = 120;
+E2 = 65;
+//resistances
+R1 = 40;
+R2 = 11;
+R3 = 60;
+
+I = (E1/R1) + (E2/R3); //norton's current source
+Req = R1*R3/(R1 + R3); //equivalent resistance
+
+I2 = I*Req/(Req + R2); //current flowing through R2
+
+disp(I2,"current flowing through R2 = ") \ No newline at end of file
diff --git a/Working_Examples/293/CH3/EX3.14/eg3_14.pdf b/Working_Examples/293/CH3/EX3.14/eg3_14.pdf
new file mode 100755
index 0000000..2a35a98
--- /dev/null
+++ b/Working_Examples/293/CH3/EX3.14/eg3_14.pdf
Binary files differ
diff --git a/Working_Examples/293/CH3/EX3.14/eg3_14.xcos b/Working_Examples/293/CH3/EX3.14/eg3_14.xcos
new file mode 100755
index 0000000..717c835
--- /dev/null
+++ b/Working_Examples/293/CH3/EX3.14/eg3_14.xcos
@@ -0,0 +1 @@
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diff --git a/Working_Examples/293/CH3/EX3.15/eg3_15.pdf b/Working_Examples/293/CH3/EX3.15/eg3_15.pdf
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+++ b/Working_Examples/293/CH3/EX3.15/eg3_15.pdf
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diff --git a/Working_Examples/293/CH3/EX3.15/eg3_15.xcos b/Working_Examples/293/CH3/EX3.15/eg3_15.xcos
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y="280.0"/></TextBlock></root></mxGraphModel><mxCell as="defaultParent" id="-108078b6:1345b8f2778:-78b9" parent="-108078b6:1345b8f2778:-78b8"/></XcosDiagram> \ No newline at end of file
diff --git a/Working_Examples/293/CH3/EX3.2/eg3_2.sce b/Working_Examples/293/CH3/EX3.2/eg3_2.sce
new file mode 100755
index 0000000..9a23d58
--- /dev/null
+++ b/Working_Examples/293/CH3/EX3.2/eg3_2.sce
@@ -0,0 +1,10 @@
+V = 100; // volatage supply in volts
+Rs = 40; //resistance in series in ohms
+// parallel resistances in ohms
+Rp1 = 33.33;
+Rp2 = 50;
+Rp3 = 20;
+Rpinv = (1/Rp1)+(1/Rp2)+(1/Rp3); //reciprocal of equivalent resistance in parallel
+Rp = 1/Rpinv; // equivalent esistance in parallel
+Vbc = V*(Rp/(Rs + Rp)); // potential difference across bc
+disp(Vbc,"potential difference across bc = ") \ No newline at end of file
diff --git a/Working_Examples/293/CH3/EX3.3/eg3_3.sce b/Working_Examples/293/CH3/EX3.3/eg3_3.sce
new file mode 100755
index 0000000..980d333
--- /dev/null
+++ b/Working_Examples/293/CH3/EX3.3/eg3_3.sce
@@ -0,0 +1,12 @@
+// resistances in ohms
+R1 = 25;
+R2 = 300;
+R3 = 80;
+R4 = 30;
+R5 = 60;
+
+Rcd = R5*R4/(R5 + R4);
+Rbd1 = Rcd + R3;
+Rbd = Rbd1*R2/(Rbd1 + R2);
+Req = Rbd + R1; // equivalent resistance
+disp(Req, "equivalent resistance = ") \ No newline at end of file
diff --git a/Working_Examples/293/CH3/EX3.4/eg3_4.sce b/Working_Examples/293/CH3/EX3.4/eg3_4.sce
new file mode 100755
index 0000000..38faaca
--- /dev/null
+++ b/Working_Examples/293/CH3/EX3.4/eg3_4.sce
@@ -0,0 +1,25 @@
+// resistances in ohms
+R1 = 25;
+R2 = 300;
+R3 = 80;
+R4 = 30;
+R5 = 60;
+
+P5 = 15; //power dissipated in R5 (in watt)
+
+I5 = sqrt(P5/R5); //current flowing through R5
+V5 = R5*I5 ; //voltage across R5
+Vcd = V5; //voltage across cd
+
+I4 = Vcd/R4; //current flowing through R4
+Icd = I5 + I4; //current flowing through cd
+
+Vbd = (Icd*R3)+Vcd ; //voltage across bd
+Ibd = (Vbd/R2)+Icd; //current through bd
+
+V1 = R1*Ibd; //voltage across R1
+
+E = V1 + Vbd;
+disp(E,"E = ")
+
+//Result : Value of E for which power dissipation in R is 15W = 200V \ No newline at end of file
diff --git a/Working_Examples/293/CH3/EX3.5/eg3_5.pdf b/Working_Examples/293/CH3/EX3.5/eg3_5.pdf
new file mode 100755
index 0000000..81434c8
--- /dev/null
+++ b/Working_Examples/293/CH3/EX3.5/eg3_5.pdf
Binary files differ
diff --git a/Working_Examples/293/CH3/EX3.5/eg3_5.xcos b/Working_Examples/293/CH3/EX3.5/eg3_5.xcos
new file mode 100755
index 0000000..b09dccc
--- /dev/null
+++ b/Working_Examples/293/CH3/EX3.5/eg3_5.xcos
@@ -0,0 +1 @@
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diff --git a/Working_Examples/293/CH3/EX3.7/eg3_7.pdf b/Working_Examples/293/CH3/EX3.7/eg3_7.pdf
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diff --git a/Working_Examples/293/CH3/EX3.7/eg3_7.xcos b/Working_Examples/293/CH3/EX3.7/eg3_7.xcos
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diff --git a/Working_Examples/293/CH3/EX3.8/eg3_8.sce b/Working_Examples/293/CH3/EX3.8/eg3_8.sce
new file mode 100755
index 0000000..78d7228
--- /dev/null
+++ b/Working_Examples/293/CH3/EX3.8/eg3_8.sce
@@ -0,0 +1,17 @@
+//mesh equations:
+//60*I1 - 20*I2 = 20
+//-20*I1 + 80*I2 = -65
+
+R = [60 -20;-20 80];
+E = [120;-65];
+I = inv(R)*E;
+I1 = I(1,:); //current flowing in first mesh
+I2 = I(2,:); //current flowing in second mesh
+
+Ibd = I1 - I2; //current flowing through branch bd
+Iab = I1; //current flowing through branch ab
+Icb = -I2; //current flowing through branch cb
+
+disp(Ibd, "current flowing through branch bd = ")
+disp(Iab,"current flowing through branch ab = ")
+disp(Icb,"current flowing through branch cb = ")
diff --git a/Working_Examples/293/CH3/EX3.9/eg3_9.pdf b/Working_Examples/293/CH3/EX3.9/eg3_9.pdf
new file mode 100755
index 0000000..ec1a8c3
--- /dev/null
+++ b/Working_Examples/293/CH3/EX3.9/eg3_9.pdf
Binary files differ
diff --git a/Working_Examples/293/CH3/EX3.9/eg3_9.xcos b/Working_Examples/293/CH3/EX3.9/eg3_9.xcos
new file mode 100755
index 0000000..57ac65b
--- /dev/null
+++ b/Working_Examples/293/CH3/EX3.9/eg3_9.xcos
@@ -0,0 +1 @@
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diff --git a/Working_Examples/293/CH4/EX4.3/eg4_3.sce b/Working_Examples/293/CH4/EX4.3/eg4_3.sce
new file mode 100755
index 0000000..2aac486
--- /dev/null
+++ b/Working_Examples/293/CH4/EX4.3/eg4_3.sce
@@ -0,0 +1,10 @@
+//ad
+Zab = complex(1,-0.5); //impedance appearing across terminals ab
+Zbg = complex(1); //impedance appearing across terminals bg
+Zbcd = complex(2+1,2); //impedance appearing across terminals bcd
+Zad = Zab + (Zbg*Zbcd/(Zbg + Zbcd)); //impedance appearing across terminals ad
+disp(Zad,"impedance appearing across terminals ad = ")
+
+//dg
+Zdg = Zbg + (Zab*Zbcd/(Zab+Zbcd)); //impedance appearing across termainals dg
+disp(Zdg,"impedance appearing across terminals dg = ") \ No newline at end of file
diff --git a/Working_Examples/293/CH5/EX5.1/eg5_1.pdf b/Working_Examples/293/CH5/EX5.1/eg5_1.pdf
new file mode 100755
index 0000000..6c14bf8
--- /dev/null
+++ b/Working_Examples/293/CH5/EX5.1/eg5_1.pdf
Binary files differ
diff --git a/Working_Examples/293/CH5/EX5.1/eg5_1.xcos b/Working_Examples/293/CH5/EX5.1/eg5_1.xcos
new file mode 100755
index 0000000..bcb39be
--- /dev/null
+++ b/Working_Examples/293/CH5/EX5.1/eg5_1.xcos
@@ -0,0 +1 @@
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diff --git a/Working_Examples/293/CH5/EX5.2/eg5_2.pdf b/Working_Examples/293/CH5/EX5.2/eg5_2.pdf
new file mode 100755
index 0000000..c5a9d74
--- /dev/null
+++ b/Working_Examples/293/CH5/EX5.2/eg5_2.pdf
Binary files differ
diff --git a/Working_Examples/293/CH5/EX5.2/eg5_2.sce b/Working_Examples/293/CH5/EX5.2/eg5_2.sce
new file mode 100755
index 0000000..1010bcd
--- /dev/null
+++ b/Working_Examples/293/CH5/EX5.2/eg5_2.sce
@@ -0,0 +1,9 @@
+C = 10*10^-6 ; //capacitance(in farads)
+R = 0.2*10^6; //resistance (in ohms)
+Vi = 40; //initial voltage of the capacitor (in volts)
+Wc = (1/2)*C*Vi^2; //energy stored in the capacitor
+//current flowing in circuit as a function of time i(t) = 2*10^-4*exp(-t/2)
+//power dissipated in the resistor = R*i^2
+Wr = integrate('R*4*10^-8*exp(-t)','t',0,100)
+disp(Wc,"energy stored in the capacitor(in Joules) = ")
+disp(Wr,"energy dissipated in the resistor(in Joules) = ") \ No newline at end of file
diff --git a/Working_Examples/293/CH5/EX5.2/eg5_2.xcos b/Working_Examples/293/CH5/EX5.2/eg5_2.xcos
new file mode 100755
index 0000000..6a93136
--- /dev/null
+++ b/Working_Examples/293/CH5/EX5.2/eg5_2.xcos
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diff --git a/Working_Examples/293/CH5/EX5.3/eg5_3.pdf b/Working_Examples/293/CH5/EX5.3/eg5_3.pdf
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+++ b/Working_Examples/293/CH5/EX5.3/eg5_3.pdf
Binary files differ
diff --git a/Working_Examples/293/CH5/EX5.3/eg5_3.xcos b/Working_Examples/293/CH5/EX5.3/eg5_3.xcos
new file mode 100755
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diff --git a/Working_Examples/293/CH5/EX5.6/eg5_6.pdf b/Working_Examples/293/CH5/EX5.6/eg5_6.pdf
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diff --git a/Working_Examples/293/CH5/EX5.6/eg5_6.xcos b/Working_Examples/293/CH5/EX5.6/eg5_6.xcos
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@@ -0,0 +1 @@
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diff --git a/Working_Examples/293/CH5/EX5.7/eg5_7.pdf b/Working_Examples/293/CH5/EX5.7/eg5_7.pdf
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diff --git a/Working_Examples/293/CH5/EX5.7/eg5_7.xcos b/Working_Examples/293/CH5/EX5.7/eg5_7.xcos
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diff --git a/Working_Examples/293/CH6/EX6.1/eg6_1.sce b/Working_Examples/293/CH6/EX6.1/eg6_1.sce
new file mode 100755
index 0000000..193b6b7
--- /dev/null
+++ b/Working_Examples/293/CH6/EX6.1/eg6_1.sce
@@ -0,0 +1,6 @@
+function F = laplace(s, T1, T2)
+ //pulse:
+ // f = u(t - T1) - u(t - T2)
+ F = integrate('exp(-s*t)','t',T1,T2); //laplace transform of the pulse
+endfunction
+
diff --git a/Working_Examples/293/CH7/EX7.1/eg7_1.sce b/Working_Examples/293/CH7/EX7.1/eg7_1.sce
new file mode 100755
index 0000000..2b6c2c8
--- /dev/null
+++ b/Working_Examples/293/CH7/EX7.1/eg7_1.sce
@@ -0,0 +1,6 @@
+Vm = 2; // assumption
+//average value of the function
+//v(t) = Vm*alpha/(%pi/3) for 0 <= alpha <= %pi/3
+// = Vm for %pi/3 <= alpha <= %pi/2
+Vav = (2/%pi)*integrate('Vm*alpha*(3/%pi)','alpha',0,%pi/3) + (2/%pi)*integrate('Vm*alpha/alpha','alpha',%pi/3,%pi/2);
+disp(Vav) \ No newline at end of file
diff --git a/Working_Examples/293/CH7/EX7.10/eg7_10.sce b/Working_Examples/293/CH7/EX7.10/eg7_10.sce
new file mode 100755
index 0000000..8471961
--- /dev/null
+++ b/Working_Examples/293/CH7/EX7.10/eg7_10.sce
@@ -0,0 +1,14 @@
+V1 = complex(10);
+V2 = complex(10*cos(-%pi/3),10*sin(-%pi/3));
+Z1 = complex(1,1);
+Z2 = complex(1,-1);
+Z3 = complex(1,2);
+//By appling the nodal analysis we get the following equation:
+//Va((1/Z1)+(1/Z2)+(1/Z3)) = (V1/Z1) + (V2/Z2)
+
+Y = (1/Z1)+(1/Z2)+(1/Z3);
+Va = (1/Y)*((V1/Z1) + (V2/Z2)); //voltage of node a
+
+Ibr = Va/Z3; //current flowing through Z3
+
+disp(Ibr,"current flowing through Z3 = ") \ No newline at end of file
diff --git a/Working_Examples/293/CH7/EX7.11/eg7_11.sce b/Working_Examples/293/CH7/EX7.11/eg7_11.sce
new file mode 100755
index 0000000..8a4f15a
--- /dev/null
+++ b/Working_Examples/293/CH7/EX7.11/eg7_11.sce
@@ -0,0 +1,14 @@
+V1 = complex(10);
+V2 = complex(10*cos(-%pi/3),10*sin(-%pi/3));
+Z1 = complex(1,1);
+Z2 = complex(1,-1);
+Z3 = complex(1,2);
+
+Zth = Z3 + (Z1*Z2/(Z1+Z2)); // thevinin resistance
+
+I = (V1 - V2)/(Z1 + Z2); // current flowing through the circuit when R3 is not connected
+Vth = V1 - I*Z1; //thevinin voltage
+
+Ibr = Vth/Zth; //current flowing through Z3
+
+disp(Ibr,"current flowing through Z3 = ") \ No newline at end of file
diff --git a/Working_Examples/293/CH7/EX7.2/eg7_2.sce b/Working_Examples/293/CH7/EX7.2/eg7_2.sce
new file mode 100755
index 0000000..96d6655
--- /dev/null
+++ b/Working_Examples/293/CH7/EX7.2/eg7_2.sce
@@ -0,0 +1,9 @@
+theta = %pi/6; //phase difference between current and voltage
+pf = cos(theta); //power factor
+disp(pf,"power factor = ")
+
+Vm = 170; //peak voltage
+Im = 14.14; //peak current
+
+Pav = Vm*Im*pf/2; //average power delivered to the circuit
+disp(Pav,"average power delivered to the circuit = ") \ No newline at end of file
diff --git a/Working_Examples/293/CH7/EX7.3/eg7_3.sce b/Working_Examples/293/CH7/EX7.3/eg7_3.sce
new file mode 100755
index 0000000..7ef4543
--- /dev/null
+++ b/Working_Examples/293/CH7/EX7.3/eg7_3.sce
@@ -0,0 +1,10 @@
+// lets assume that i1 and i2 are stationary and the coordinate system is rotating with an angular frquency of w. And i1 lies on the x-axis (i.e. making an angle of 0 degree with the x-axis)
+theta = %pi/3; //phase difference between i1 and i2;
+I1 = 10*sqrt(2); // peak value of i1
+I2 = 20*sqrt(2); // peak value of i2
+I = sqrt(I1^2 + I2^2 + 2*I1*I2*cos(theta)); //peak value of the resultant current
+
+phi = atan(I2*sin(theta)/(I1 + I2*cos(theta)));// phase difference between the resultant and i1(in radians)
+disp(I,"peak value of the resultant current = ")
+disp(phi,"phase difference between the resultant and i1 = ")
+// result : i = I sin(wt + phi) \ No newline at end of file
diff --git a/Working_Examples/293/CH7/EX7.4/eg7_4.sce b/Working_Examples/293/CH7/EX7.4/eg7_4.sce
new file mode 100755
index 0000000..408b4a1
--- /dev/null
+++ b/Working_Examples/293/CH7/EX7.4/eg7_4.sce
@@ -0,0 +1,14 @@
+I1 = 10; //peak value of i1
+I2 = 20; //peak value of i2
+theta = %pi/3; //phase difference between i1 and i2
+// complex representation of the two currents
+i1 = complex(10);
+i2 = complex(20*cos(%pi/3),20*sin(%pi/3));
+
+i = i1 + i2 ; //resultant current
+I = sqrt (real(i)^2 + imag(i)^2); //calculating the peak value of the resultant current by using its real and imaginary parts
+phi = atan(imag(i)/real(i)); //calculatig the phase of the resultant current by using its real and imaginary parts
+disp(i,"resultant current = ")
+disp(I,"peak value of the resultant current = ")
+disp(phi,"phase of the resultant current = ")
+//result : i = Isin(wt + phi)
diff --git a/Working_Examples/293/CH7/EX7.5/eg7_5.sce b/Working_Examples/293/CH7/EX7.5/eg7_5.sce
new file mode 100755
index 0000000..8dc01c2
--- /dev/null
+++ b/Working_Examples/293/CH7/EX7.5/eg7_5.sce
@@ -0,0 +1,16 @@
+I1 = 3; //peak value of i1
+I2 = 5; //peak value of i2
+I3 = 6; //peak value of i3
+theta1 = %pi/6; //phase difference between i2 and i1
+theta2 = -2*%pi/3; //phase difference between i3 and i1
+// complex representation of the currents
+i1 = complex(3);
+i2 = complex(5*cos(%pi/6),5*sin(%pi/6));
+i3 = complex(6*cos(-2*%pi/3),6*sin(-2*%pi/3));
+
+i = i1 + i2 + i3; //resultant current
+I = sqrt (real(i)^2 + imag(i)^2); //calculating the peak value of the resultant current by using its real and imaginary parts
+phi = atan(imag(i)/real(i)); //calculatig the phase of the resultant current by using its real and imaginary parts
+disp(I,"peak value of the resultant current = ")
+disp(phi,"phase of the resultant current = ")
+//result : i = Isin(wt + phi) \ No newline at end of file
diff --git a/Working_Examples/293/CH7/EX7.6/eg7_6.sce b/Working_Examples/293/CH7/EX7.6/eg7_6.sce
new file mode 100755
index 0000000..52b0b90
--- /dev/null
+++ b/Working_Examples/293/CH7/EX7.6/eg7_6.sce
@@ -0,0 +1,7 @@
+//find V*Z1/Z2
+V = complex(45*sqrt(3), -45);
+Z1 = complex(2.5*sqrt(2), 2.5*sqrt(2));
+Z2 = complex(7.5, 7.5*sqrt(3));
+// we have to find V*Z1/Z2
+Z = V*Z1/Z2;
+disp(Z,"V*Z1/Z2 = ") \ No newline at end of file
diff --git a/Working_Examples/293/CH7/EX7.7/eg7_7.sce b/Working_Examples/293/CH7/EX7.7/eg7_7.sce
new file mode 100755
index 0000000..6e6dc46
--- /dev/null
+++ b/Working_Examples/293/CH7/EX7.7/eg7_7.sce
@@ -0,0 +1,41 @@
+//a
+f = 60; //frequency of the volatge source
+V = complex(141);//voltage supply V = 141sin(wt)
+R = 3; //resistance of the circuit
+L = 0.0106; // inductance of the circuit
+Z = complex(R,2*%pi*f*L);//impedance of the circuit = R + jwL
+i = V/Z; //current
+I = sqrt (real(i)^2 + imag(i)^2); //calculating the peak value of the current by using its real and imaginary parts
+phi = atan(imag(i)/real(i)); //calculatig the phase of the resultant current by using its real and imaginary parts
+disp("a")
+disp(I,"effective value of the steady state current = ")
+disp(phi,"relative phase angle = ")
+
+//b
+// expression for the instantaneous current can be written as
+//i = I sin(wt + phi)
+
+//c
+R = complex(3);
+ vr = V*R/Z; // voltage across the resistor
+Vr = sqrt (real(vr)^2 + imag(vr)^2); //peak value of the voltage across the resistor
+phi1 = atan(imag(vr)/real(vr)); //phase of the voltage across the resistor
+
+vl = V - vr; //voltage across the inductor
+Vl = sqrt (real(vl)^2 + imag(vl)^2); //peak value of the voltage across the inductor
+phi2 = atan(imag(vl)/real(vl)); //phase of the voltage across the inductor
+disp("c")
+disp(Vr,"effective value of the voltage drop across the resistor = ")
+disp(phi1,"phase of the voltage drop across the resistor = ")
+disp(Vl,"effective value of the voltage drop across the inductor = ")
+disp(phi2,"phase of the voltage drop across the inductor = ")
+
+//d
+Pav = V*I*cos(phi); //average power dissipated by the circuit
+disp("d")
+disp(Pav,"average power dissipated by the circuit = ")
+
+//e
+pf = cos(phi); //power factor
+disp("e")
+disp(pf,"power factor = ") \ No newline at end of file
diff --git a/Working_Examples/293/CH7/EX7.8/eg7_8.sce b/Working_Examples/293/CH7/EX7.8/eg7_8.sce
new file mode 100755
index 0000000..e33b3cc
--- /dev/null
+++ b/Working_Examples/293/CH7/EX7.8/eg7_8.sce
@@ -0,0 +1,12 @@
+//impedances in the circuit
+Z1 = complex(10,10);
+Z2 = complex(15,20);
+Z3 = complex(3,-4);
+Z4 = complex(8,6);
+
+Ybc = (1/Z2)+(1/Z3)+(1/Z4); //admittance of the parallel combination
+Zbc = (1/Ybc); //impedance of the parallel combination
+
+Z = Z1 + Zbc; // equivalent impedance of the circuit
+
+disp(Z,"equivalent impedance of the circuit = ") \ No newline at end of file
diff --git a/Working_Examples/293/CH7/EX7.9/eg7_9.sce b/Working_Examples/293/CH7/EX7.9/eg7_9.sce
new file mode 100755
index 0000000..ff8d27d
--- /dev/null
+++ b/Working_Examples/293/CH7/EX7.9/eg7_9.sce
@@ -0,0 +1,29 @@
+V1 = complex(10);
+V2 = complex(10*cos(-%pi/3),10*sin(-%pi/3));
+Z1 = complex(1,1);
+Z2 = complex(1,-1);
+Z3 = complex(1,2);
+
+//by mesh analysis we get the following equations:
+//I1*Z11 - I2*Z12 = V1
+//-I1*Z21 + I2*Z22 = -V2; where I1 and I2 are the currrents flowing in the first and second meshes respectively
+Z11 = Z1 + Z1;
+Z12 = Z1 + Z2;
+Z21 = Z12;
+Z22 = Z2 + Z2;
+
+// the mesh equations can be represented in the matrix form as I*Z = V
+Z = [Z11, -Z12; -Z21, Z22]; //impedance matrix
+V = [V1; -V2]; //voltage matrix
+I = inv(Z)*V; //current matrix = [I1;I2]
+
+I1 = I(1,:); // I1 = first row of I matrix
+I2 = I(2,:); // I1 = second row of I matrix
+
+Ibr = I1 - I2; //current flowing through Z3
+
+disp(Ibr,"current flowing through Z3 = ")
+
+
+
+
diff --git a/Working_Examples/293/CH9/EX9.2/eg9_2.sce b/Working_Examples/293/CH9/EX9.2/eg9_2.sce
new file mode 100755
index 0000000..8a35341
--- /dev/null
+++ b/Working_Examples/293/CH9/EX9.2/eg9_2.sce
@@ -0,0 +1,12 @@
+// Quiescent point
+Idq = 0.0034; // drain current
+Vdq = 15; // drain voltage
+Vgq = 1; // gate voltage
+
+Vdd = 24; //drain supply voltage
+
+Rs = Vgq/Idq;
+disp(Rs,"The value of self bais source resistance is(in ohm): ")
+
+Rd = (Vdd - Vdq)/Idq ;
+disp(Rd,"The value of drain load resistance is(in ohm): ") \ No newline at end of file
diff --git a/Working_Examples/293/CH9/EX9.3/eg9_3.sce b/Working_Examples/293/CH9/EX9.3/eg9_3.sce
new file mode 100755
index 0000000..edac541
--- /dev/null
+++ b/Working_Examples/293/CH9/EX9.3/eg9_3.sce
@@ -0,0 +1,38 @@
+//a
+//transistor parameters
+ R2 = 0.625;
+ hie = 1.67;
+ Rb = 4.16;
+ Rl = 2.4;
+ Roe = 150;
+
+ Cc = 25 * 10^-6;
+ rBB = 0.29;
+ rBE = 1.375;
+ Cd = 6900 * 10^-12;
+ Ct = 40 * 10^-12;
+ gm = 0.032;
+
+ Req = (Rl*Roe)/(Rl + Roe);
+ hfe = 44;
+ a = 1 + (R2/Req);
+ b = 1 + (hie/Rb);
+ Aim = -hfe/(a*b); // mid band frequency gain
+ disp("a")
+ disp(Aim,"The mid band frequency gain of the first stage of the circuit is: ")
+
+ //b
+ Tl = 2*%pi*(Req + R2)*Cc*(10^3);
+ Fl = 1/Tl;
+
+ Rp = (Req*R2)/(Req + R2);
+ C = Cd + Ct*(1 + gm*Rp*10^3);
+ d = Rb + hie ;
+ e = rBE * (Rb + rBB)* 10^3 * C ;
+ Fh = d/(2*%pi*e);
+
+ BW = Fh - Fl;
+ disp("b")
+ disp(BW, "The bandwidth of the first stage amplifier in Hz is :")
+
+ \ No newline at end of file
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