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Diffstat (limited to '3554/CH15/EX15.10/Ex15_10.sce')
-rw-r--r-- | 3554/CH15/EX15.10/Ex15_10.sce | 35 |
1 files changed, 35 insertions, 0 deletions
diff --git a/3554/CH15/EX15.10/Ex15_10.sce b/3554/CH15/EX15.10/Ex15_10.sce new file mode 100644 index 000000000..e395a330e --- /dev/null +++ b/3554/CH15/EX15.10/Ex15_10.sce @@ -0,0 +1,35 @@ +// Exa 15.10
+
+clc;
+clear all;
+
+// Given data
+// Second order inverting Butterworth low pass filter
+// Refering Table 15.1 and 15.3 in page no 517 and 538 respectively
+
+Af=6;// DC gain
+Fc=1.5;// KHz
+Q=10;
+
+// Solution
+
+disp(" According to Table 15.1, the inverting configurations would normally be used to give an inverting low pass output. However, to obtain a gain of 6, an inverting uncommitted opamp has to br used, hence the non-inverting filter configuration must be used.");
+
+// From table 15.4 given on page no 538
+R2=316/Q;
+R3=100/(3.16*Q-1);
+// R1 treated as open circuit
+printf(' \n The R1 is open while R2 and R3 are %.1f ,k Ohms %.1f k Ohms respectively \n',R2,R3);
+// From equations 15.54 given on page no 538 we get R4 and R5
+R4=(5.03)*10^7/(Fc*10^3);//Ohms
+R5=R4;
+printf(' \n The calculated value of R4=R5=%.2f k Ohms \n',R4/1000);
+disp(" use R4=R5=33 k Ohms");
+
+disp(" Let R6=1.8 K ohms");
+R6=1.8; // K ohms
+R7=R6*Af;
+R8=(1/R6 + 1/R7)^-1;
+
+printf(' The values of R6 and R7 are %.1f k Ohms, %.3f K ohms respectively \n',R6,R7);
+printf(' The value of R8 = %.3f k Ohms \n ',R8);
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