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Diffstat (limited to '1370/CH1/EX1.31')
-rwxr-xr-x | 1370/CH1/EX1.31/chapter1_31.sce | 39 |
1 files changed, 39 insertions, 0 deletions
diff --git a/1370/CH1/EX1.31/chapter1_31.sce b/1370/CH1/EX1.31/chapter1_31.sce new file mode 100755 index 000000000..19c964459 --- /dev/null +++ b/1370/CH1/EX1.31/chapter1_31.sce @@ -0,0 +1,39 @@ +//example1.31
+clc
+disp("Method 1: Kirchoffs laws")
+disp("Now apply KVL to the two loops without current source as effect of the currents in various branches.")
+disp("-2(I1-2)-I2+6=0 i.e. 2(I1)+I2=10 ..(1)")
+disp("-3(I1-2-I2)-12+I2=0 i.e. -3(I1)+4(I2)=6 ..(2)")
+disp("-3(I1)+4(10-2(I1))=6")
+i=34/11
+format(7)
+disp(i,"Therefore, I1(in A)=")
+i=10-(2*3.0909)
+disp(i,"and, I2(in A)=")
+disp("Currents through various resistances are,")
+i=3.0909-2
+disp(i,"I(2ohm)[in A]=I1-2=")
+disp("I(1ohm)[in A]=I2=3.8181")
+i=3.0909-2-3.8181
+disp(i,"I(3ohm)[in A]=I1-2-I2=")
+disp("Current through 3ohm is negative i.e. it is flowing in opposite direction to that assumed in the circuit.")
+disp("Method II: Loop analysis")
+disp("From the current source branch,")
+disp("I3= 2 A")
+disp("Applying KVL to the other two loopos without current source,")
+disp("-2(I1)+2(I3)-I1+I2+6=0 i.e. -3(I1)+I2= -10 ..(1)")
+disp("-3(I2)+3(I3)-12-I2+I1=0 i.e. I1-4(I2)=6 ..(2)")
+disp("Solving we get,")
+disp("I1-4(-10+3(I1))=6")
+i=34/11
+disp(i,"I1(in A)=")
+i=(3.0909-6)/4
+disp(i,"and, I2(in A)=")
+disp("Currents through various resistances are,")
+i=3.0909-2
+disp(i,"I(2ohm)[in A]=I1-2=")
+i=3.0909+0.7272
+disp(i,"I(1ohm)[in A]=I1-I2=")
+i=-0.7272-2
+disp(i,"I(3ohm)[in A]=I2-2=")
+disp("The currents are same as obtained by the method 1.")
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