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author | prashantsinalkar | 2017-10-10 12:27:19 +0530 |
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committer | prashantsinalkar | 2017-10-10 12:27:19 +0530 |
commit | 7f60ea012dd2524dae921a2a35adbf7ef21f2bb6 (patch) | |
tree | dbb9e3ddb5fc829e7c5c7e6be99b2c4ba356132c /3554/CH10/EX10.1/Ex10_1.sce | |
parent | b1f5c3f8d6671b4331cef1dcebdf63b7a43a3a2b (diff) | |
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Diffstat (limited to '3554/CH10/EX10.1/Ex10_1.sce')
-rw-r--r-- | 3554/CH10/EX10.1/Ex10_1.sce | 24 |
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diff --git a/3554/CH10/EX10.1/Ex10_1.sce b/3554/CH10/EX10.1/Ex10_1.sce new file mode 100644 index 000000000..1f381d119 --- /dev/null +++ b/3554/CH10/EX10.1/Ex10_1.sce @@ -0,0 +1,24 @@ +// Exa 10.1
+
+clc;
+clear all;
+
+// Given data
+
+// 1st measurement
+f1=1; // in MHZ
+C1=500; // in pf
+// 2nd measurement
+f2=2; //in MHz
+C2=110; // in pf
+
+// Solution
+// Using equation 10.2(page no. 278) to calculate distributed Capacitance
+
+Cs=(C1-4*C2)/3; // Distributed capacitance in pf
+printf('The value of distributed capacitance = %d pf \n',Cs);
+// using equation of resonant frequency given as f1=1/(2*%pi*sqrt(L*(C1+Cs));
+// Therefore
+L=1/(4*(%pi)^2*f1^2*(C1+Cs)); // Inductor value
+
+printf(' The value of L(inductor) is =%.3f micro H \n',L*10^6);
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