Laplace transforms: Simple Electrical Network: Difference between revisions

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<math>\Rightarrow s^2+500s+62500=6000</math>
<math>\Rightarrow s^2+500s+62500=6000</math>


<math>\Rightarrow (s^2+250)^2-(20\sqrt{15})^2=0</math)
<math>\Rightarrow (s+250)^2-(100\sqrt{6})^2=0</math>


we do this by divinding <math>(\frac{b}{2})^2</math>
Thus


Taking the Inverse Laplace transform yields
<math>I_2(s)=\frac{5}{2s}-5\frac{s+250}{(s+250)^2-(100\sqrt{6})^2}-\frac{5\sqrt{6}}{12}\frac{100\sqrt{6}}{(s+250)^2-(100\sqrt{6})^2}</math>


<math>\mathcal{L}^{-1}\left\{I_1(s)\right\}=\frac{5}{8}+\frac{39\sqrt{103}}{824}sin*(\frac{25}{2}\sqrt{103}*t)</math>


Taking the Inverse Laplace transform gives


<math>\mathcal{L}^{-1}\left\{I_2(s)\right\}=</math>
<math>\mathcal{L}^{-1}\left\{I_2(s)\right\}= i_2(t) =\frac{5}{2}-5e^{-250t}cosh100\sqrt{6}t-\frac{5\sqrt{6}}{12}5e^{-250t}sinh100\sqrt{6}t</math>


==Initial Value Theorem==
==Initial Value Theorem==

Revision as of 17:25, 11 December 2009

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

⇒(s+250)2−(1006)2=0

Thus

I2(s)=52s−5s+250(s+250)2−(1006)2−56121006(s+250)2−(1006)2


Taking the Inverse Laplace transform gives

ℒ−1{I2(s)}=i2(t)=52−5e−250tcosh1006t−56125e−250tsinh1006t

Initial Value Theorem

lims→∞sI(s)=f(0+)

lims→∞s25s+12500s(s2+500s+2500)=i(0)

⇒i(0)=0

lims→∞s6250s(s2+500s+2500)=i(0)

⇒i(0)=0

Final Value Theorem

lims→0sI(s)=f(∞)

lims→∞s25s+12500s(s2+500s+2500)=i(∞)

⇒i(∞)=0

lims→0s6250s(s2+500s+2500)=i(∞)

⇒i(∞)=0

Bode Plots