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Diffstat (limited to '3682/CH7/EX7.4/Ex7_4.sce')
-rw-r--r-- | 3682/CH7/EX7.4/Ex7_4.sce | 43 |
1 files changed, 43 insertions, 0 deletions
diff --git a/3682/CH7/EX7.4/Ex7_4.sce b/3682/CH7/EX7.4/Ex7_4.sce new file mode 100644 index 000000000..9aaa28843 --- /dev/null +++ b/3682/CH7/EX7.4/Ex7_4.sce @@ -0,0 +1,43 @@ +// Exa 7.4
+
+clc;
+clear;
+
+// Given data
+
+n=2; // Second order Butterworth filter
+fH=1000; // Lower cut off frequency(Hz)
+
+// Solution
+
+printf('Let C = 0.1 μF. \n');
+C=0.1*10^-6; // Farads
+
+// Since fH = 1/(2 * %pi * R*C);
+// Therefore;
+R = 1/(2*%pi*fH*C);
+printf(' The calculated value of R = %.1f kΩ. \n',R/1000);
+
+printf(' From Table 7.1, for n=2, the damping factor alpha = 1.414.');
+alpha=1.414;
+A0 = 3-alpha;
+printf('\n Then the pass band gain A0 = %.3f. \n',A0);
+printf('\n');
+printf(' The transfer function of the normalized second order low-pass Butterworth filter is 1.586 ');
+printf('\n ----------------');
+printf('\n Sn^2+1.414*Sn+1');
+
+// Since Af= 1 + Rf/Ri = 1 + 0.586;
+printf('\n Since A0= 1.586 so Let Rf = 5.86 kΩ and Ri = 10 kΩ to make A0 = 1.586.' );
+
+printf(' \n The circiuit realized is as shown in Fig. 7.4 with component value as mentioned above.');
+
+printf('\n By considering minimum DC offset condition, the modified value of R and C comes out to be R = 1.85 kΩ and C=0.086 μF.');
+printf('\n\n\n Frequency, f in Hz Gain magnitude in dB 20 log(vo/vi)\n');
+// Frequency Response
+x=[0.1*fH,0.2*fH,0.5*fH,1*fH,5*fH,10*fH]
+for i = 1:1:6
+ response(i) = 20*log10(A0/(sqrt(1+(x(i)/fH)^4)));
+ printf(' %d %.2f \n',x(i),response(i));
+end
+
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