Laplace transforms: Simple Electrical Network: Difference between revisions
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Now we do the same for <math>I_1</math> where we solve the function in terms of <math>I_1</math> and decomposing the partial fraction resulting in |
Now we do the same for <math>I_1</math> where we solve the function in terms of <math>I_1</math> and decomposing the partial fraction resulting in |
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<math>I_1(s)= \frac{25s+12500}{s(s^2+500s+2500)}=\frac{5}{ |
<math>I_1(s)= \frac{25s+12500}{s(s^2+500s+2500)}=\frac{5}{s}-\frac{5s+2475}{s^2+500s+2500}</math> |
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⚫ | |||
<math> s^2+500s+2500=0</math> |
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<math>\Rightarrow s^2+500s=-2500</math> |
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<math>\Rightarrow s^2+500s+[\frac{500}{2}]^2=-2500+(\frac{500}{2})^2</math> |
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<math>\Rightarrow s^2+500s+62500=6000</math> |
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<math>\Rightarrow (s^2+250)^2-(20\sqrt{15})^2=0</math) |
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we do this by divinding <math>(\frac{b}{2})^2</math> |
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⚫ | |||
Taking the Inverse Laplace transform yields |
Taking the Inverse Laplace transform yields |
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Revision as of 01:06, 10 December 2009
Problem Statement
Using the formulas
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.
Applying the Laplace transform to each equation gives
Solving for
We find the partial decomposition
Let
Comparing the coefficients we get
Thus
Now we do the same for where we solve the function in terms of and decomposing the partial fraction resulting in
In order to make it nicer on us we need to complete the square as follows
Taking the Inverse Laplace transform yields