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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 /1445/CH1/EX1.42/ch1_ex_42.sce | |
parent | b1f5c3f8d6671b4331cef1dcebdf63b7a43a3a2b (diff) | |
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diff --git a/1445/CH1/EX1.42/ch1_ex_42.sce b/1445/CH1/EX1.42/ch1_ex_42.sce new file mode 100644 index 000000000..5ca60c3ac --- /dev/null +++ b/1445/CH1/EX1.42/ch1_ex_42.sce @@ -0,0 +1,39 @@ +//CHAPTER 1- D.C. CIRCUIT ANALYSIS AND NETWORK THEOREMS +//Example 42 + +disp("CHAPTER 1"); +disp("EXAMPLE 42"); + +//VARIABLE INITIALIZATION +v=10; //in Volts +I=0.5; //in Amperes +r1=4; //top LHS resistance in Ohms +r2=2; //top RHS resistance in Ohms +r3=2; //first resistance in Ohms +r4=2; //second resistance in Ohms + +//SOLUTION + +//using Thevenin theorem +rth=(r1*r3)/(r1+r3); +vth=v*(r3/(r1+r3)); +//solving for R directly, +R=(40-(56*I))/(24*I); +disp(sprintf("(i) By Thevenin Theorem, the value of R is %d Ω",R)); + +//using nodal analysis +//solving the quadratic equation formed by comparing eq(1) and eq(2) +//(3)R^2+(-3)R+(0)=0 +a=3; +b=-3; +c=0; +D=(b^2)-(4*a*c); //discriminant +R1=(-b+sqrt(D))/(2*a); +R2=(-b-sqrt(D))/(2*a); +if(R1==1) then +disp(sprintf("(ii) By Nodal analysis, the value of R is %d Ω",R1)); +else +disp(sprintf("(ii) By Nodal analysis, the value of R is %d Ω",R1)); +end; + +//END |