Laplace transforms: Simple Electrical Network

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Problem Statement

Using the formulas

E(t)=LdiRdt+RiC
RCdiRdt+iR−iC=0

Solve the system when V0 = 50 V, L = 4 h, R = 20 Ω, C = 10-4 f, and the currents are initially zero.

Solution

Solve the system when V0 = 50 V, L = 4 h, R = 20 Ω, C = 10-4 f, and the currents are initially zero.

4di1dt+20i2=50

20(10−4)di2dt+i2−i1=0

Applying the Laplace transform to each equation gives

4(sℒ{i1}−i1(0))+20ℒ{i2}=50

⇒4sI1(s)+20I2(s)=50s

0.005(sℒi2−i2(0))+ℒ{i2}−ℒ{i1}=0

⇒−500I1(s)+[s+500]I2(s)=0

Solving for I2(s)

I2(s)=6250s(s2+500s+2500)

We find the partial decomposition

Let I2(s)=6250s(s2+500s+2500)=As+Bs+Cs2+500s+2500

⇒6250=A(s2+500s+2500)+(Bs+C)s

⇒62500=As2+500As+2500A+Bs2+Cs

Comparing the coefficients we get

A=52,B=−5,C=−1250

Thus I2(s)=52s−5s+1250s2+500s+2500

Now we do the same for I1 where we solve the function in terms of I1 and decomposing the partial fraction resulting in

I1(s)=25s+12500s(s2+500s+2500)=5s−5s+2475s2+500s+2500

In order to make it nicer on us we need to complete the square as follows

s2+500s+2500=0

⇒s2+500s=−2500

⇒s2+500s+[5002]2=−2500+(5002)2

⇒s2+500s+62500=6000

⇒(s2+250)2−(2015)2=0</math)wedothisbydivinding<math>(b2)2

Taking the Inverse Laplace transform yields

ℒ−1{I1(s)}=58+39103824sin*(252103*t)


ℒ−1{I2(s)}=

Initial Value Theorem

lims→∞sI(s)=f(0+)

lims→∞25s+12500s(s2+500s+2500)=i(0)

⇒i(0)=0

lims→∞6250s(s2+500s+2500)=i(0)

⇒i(0)=0

Final Value Theorem

lims→0sI(s)=f(∞)

lims→∞25s+12500s(s2+500s+2500)=i(∞)

⇒i(∞)=0

⇒lims→06250s(s2+500s+2500)=i(∞)

⇒i(∞)=0

Bode Plots