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-rwxr-xr-x83/CH3/EX3.1/example_3_1.sce22
-rwxr-xr-x83/CH3/EX3.1/result_example_3_1.txt10
-rwxr-xr-x83/CH3/EX3.2/example_3_2.sce21
-rwxr-xr-x83/CH3/EX3.2/result_exapmle_3_2.txt9
-rwxr-xr-x83/CH3/EX3.3/example_3_3.sce31
-rwxr-xr-x83/CH3/EX3.3/result_example_3_3.txt8
6 files changed, 101 insertions, 0 deletions
diff --git a/83/CH3/EX3.1/example_3_1.sce b/83/CH3/EX3.1/example_3_1.sce
new file mode 100755
index 000000000..fc0512a14
--- /dev/null
+++ b/83/CH3/EX3.1/example_3_1.sce
@@ -0,0 +1,22 @@
+//Chapter 3
+//Example 3.1
+//page 87
+//To calculate the capacitance to neutral of a single phase line
+clear;clc;
+r=0.328; //radius of the conductors
+D=300; //distance between the conductors
+h=750; //height of the conductors
+
+//calculating capacitance neglecting the presence of ground
+//using Eq (3.6)
+Cn=(0.0242/(log10(D/r)));
+printf("\nCapacitance to neutral /km of the given single phase line neglecting presence of the earth (using Eq 3.6) is = %0.5f uF/km\n\n",Cn);
+
+//using Eq (3.7)
+Cn=(0.0242)/log10((D/(2*r))+((D^2)/(4*r^2)-1)^0.5);
+printf("Capacitance to neutral /km of the given single phase line neglecting presence of the earth (using Eq 3.7) is = %0.5f uF/km\n\n",Cn);
+
+//Consudering the effect of earth and neglecting the non uniformity of the charge
+Cn=(0.0242)/log10(D/(r*(1+((D^2)/(4*h^2)))^0.5));
+printf("Capacitance to neutral /km of the given single phase line considering the presence of the earth and neglecting non uniformity of charge distribution (using Eq 3.26b) is = %0.5f uF/km\n\n",Cn);
+
diff --git a/83/CH3/EX3.1/result_example_3_1.txt b/83/CH3/EX3.1/result_example_3_1.txt
new file mode 100755
index 000000000..9afdbd2be
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+++ b/83/CH3/EX3.1/result_example_3_1.txt
@@ -0,0 +1,10 @@
+
+
+Capacitance to neutral /km of the given single phase line neglecting presence of the earth (using Eq 3.6) is = 0.00817 uF/km
+
+Capacitance to neutral /km of the given single phase line neglecting presence of the earth (using Eq 3.7) is = 0.00817 uF/km
+
+Capacitance to neutral /km of the given single phase line considering the presence of the earth and neglecting non uniformity of charge distribution (using Eq 3.26b) is = 0.00820 uF/km
+
+
+
diff --git a/83/CH3/EX3.2/example_3_2.sce b/83/CH3/EX3.2/example_3_2.sce
new file mode 100755
index 000000000..e31235042
--- /dev/null
+++ b/83/CH3/EX3.2/example_3_2.sce
@@ -0,0 +1,21 @@
+//Chapter 3
+//Example 3.2
+//page 88
+//To claculate the capacitance to neutral and charging current of a three phase transmission line
+clear;clc;
+d=350; //distance between adjacent lines
+r=1.05/2; //radius of the conductor
+v=110e3; //line voltage;
+f=50;
+
+Deq=(d*d*2*d)^(1/3); //GMD or equivalent
+
+Cn=(0.0242/log10(Deq/r));
+
+Xn=1/(2*%pi*f*Cn*10^(-6)); // Cn is in uF hence we add 10^6 while printing
+
+Ic=(v/sqrt(3))/Xn;
+
+printf("\nCapacitance to neutral is = %f uF/km\n\n",Cn);
+printf("Capacitive rectance of the line is = %f ohm/km to neutral\n\n",Xn);
+printf("Charging Current = %0.2f A/km\n\n",Ic); \ No newline at end of file
diff --git a/83/CH3/EX3.2/result_exapmle_3_2.txt b/83/CH3/EX3.2/result_exapmle_3_2.txt
new file mode 100755
index 000000000..36aad3e31
--- /dev/null
+++ b/83/CH3/EX3.2/result_exapmle_3_2.txt
@@ -0,0 +1,9 @@
+
+
+Capacitance to neutral is = 0.008276 uF/km
+
+Capacitive rectance of the line is = 384635.679536 ohm/km to neutral
+
+Charging Current = 0.17 A/km
+
+
diff --git a/83/CH3/EX3.3/example_3_3.sce b/83/CH3/EX3.3/example_3_3.sce
new file mode 100755
index 000000000..07e3791c8
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+++ b/83/CH3/EX3.3/example_3_3.sce
@@ -0,0 +1,31 @@
+//Chapter 3
+//Example 3.3
+//page 88
+//To claculate the capacitance to neutral and charging current of a double circuit three phase transmission line
+clear;clc;
+
+//After deriving the equation for Cn from the textbook and starting calculation from Eq 3.36 onwards
+
+r=0.865*10^(-2); frequency=50; v=110e3;
+h=6; d=8; j=8; //Referring to fig given in the textbook
+
+i=((j/2)^2+((d-h)/2)^2)^(1/2);
+f=(j^2+h^2)^(1/2);
+g=(7^2+4^2)^(1/2);
+
+
+Cn=4*%pi*8.85*10^(-12)/(log((((i^2)*(g^2)*j*h)/((r^3)*(f^2*d)))^(1/3)));
+
+Cn=Cn*1000 ; //Cn is in per m.to convert it to per km,we multiply by 1000
+WCn=2*%pi*frequency*Cn;
+
+Icp=(v/sqrt(3))*WCn;
+
+Icc=Icp/2;
+
+printf("\nTotal capacitance to neutral for two conductors in parallel = %0.6f uF/km \n\n",Cn*10^(6));
+printf("Charging current/phase = %0.3f A/km \n\n",Icp);
+printf("Charging current/conductor = %0.4f A/km \n\n",Icc);
+
+
+
diff --git a/83/CH3/EX3.3/result_example_3_3.txt b/83/CH3/EX3.3/result_example_3_3.txt
new file mode 100755
index 000000000..6602fe5d9
--- /dev/null
+++ b/83/CH3/EX3.3/result_example_3_3.txt
@@ -0,0 +1,8 @@
+
+
+Total capacitance to neutral for two conductors in parallel = 0.018088 uF/km
+
+Charging current/phase = 0.361 A/km
+
+Charging current/conductor = 0.1804 A/km
+