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-rw-r--r--165/CH10/EX10.1/ex10_1.sce13
-rw-r--r--165/CH10/EX10.2/ex10_2.sce13
-rw-r--r--165/CH10/EX10.3/ex10_3.sce14
3 files changed, 40 insertions, 0 deletions
diff --git a/165/CH10/EX10.1/ex10_1.sce b/165/CH10/EX10.1/ex10_1.sce
new file mode 100644
index 000000000..b987bd619
--- /dev/null
+++ b/165/CH10/EX10.1/ex10_1.sce
@@ -0,0 +1,13 @@
+//Example 10.1
+clc;
+//Given Data
+C1=600*10^-12;
+C2=100*10^-12;
+f1=2*10^6;
+//Distributed Capacitance Cs
+Cs=(C1-4*C2)/3;
+disp(Cs,'Value of Distributed Capacitance is')
+//We know the resonant frequency is
+//given by f1=1/(2*pi*(L(C1+CS))^.5), hence
+L=1/(((2*%pi*f1)^2)*(C1+Cs));
+printf('\nValue of inductance L is %.12f H',L) \ No newline at end of file
diff --git a/165/CH10/EX10.2/ex10_2.sce b/165/CH10/EX10.2/ex10_2.sce
new file mode 100644
index 000000000..c86fa0835
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+++ b/165/CH10/EX10.2/ex10_2.sce
@@ -0,0 +1,13 @@
+//Example 10.2
+clc;
+//Given Data
+C1=500*10^-12;
+C2=110*10^-12;
+f1=1*10^6;
+//Distributed Capacitance Cs
+Cs=(C1-4*C2)/3;
+disp(Cs,'Value of Distributed Capacitance is')
+//We know the resonant frequency is
+//given by f1=1/(2*pi*(L(C1+CS))^.5), hence
+L=1/(((2*%pi*f1)^2)*(C1+Cs));
+printf('\nValue of inductance L is %.12f H',L) \ No newline at end of file
diff --git a/165/CH10/EX10.3/ex10_3.sce b/165/CH10/EX10.3/ex10_3.sce
new file mode 100644
index 000000000..aba690506
--- /dev/null
+++ b/165/CH10/EX10.3/ex10_3.sce
@@ -0,0 +1,14 @@
+//Example 10.3
+clc;
+//Given Data
+C1=500*10^-12;
+C2=50*10^-12;
+f1=2*10^6;
+f2=6*10^6;
+//Since f2=3f1 we can equate the equations
+//as follows
+// 1/(2*pi*(L(C2+CS))^.5) = 3/(2*pi*(L(C1+CS))^.5)
+// => C1+Cs = 9 (C2 +Cs)
+// or Cs=(C1-9C2)/8
+Cs=(C1-9*C2)/8; //Self Capacitance
+disp(Cs,'Value of Self Capacitance is:') \ No newline at end of file