Solve RC Circuit Using Laplace Transforms

In summary: Laplace transform, and method of residues. However, your answer was different from the one given in the book, and upon further examination, you found that the partial fraction expansion was incorrect and the correct answer is v(t)=2t-e^{-2t}.
  • #1
photonsquared
15
0
Find v(t) at t=800ms for the circuit in Figure 1.

Ans: 802mV



Writing a single node equation we have

[tex]\frac{v(t)-2tu(t)}{5}+0.1\frac{dv}{dt}=0.[/tex]

Taking the Laplace transform we have

[tex]L\left\{ \frac{v(t)-2tu(t)}{5}+0.1\frac{dv}{dt}=0\right\} .[/tex]

[tex]tu(t)\Rightarrow\frac{1}{s^{2}}[/tex]

[tex]\frac{df}{dt}\Rightarrow sF(s)-f(0^{-})[/tex]

[tex]\frac{V(s)}{5}-\frac{2}{5s^{2}}+0.1sV(s)-0.1v(0^{-})=0[/tex]

Assume that [tex]v(0^{-})=0[/tex] we have

[tex]\frac{V(s)}{5}-\frac{2}{5s^{2}}+0.1sV(s)=0[/tex]

multiplying through by 10 and combing like terms

[tex]V(s)\left(2+s\right)=\frac{4}{s^{2}}[/tex]

Solving for V(s) we have

[tex]V(s)=\frac{4}{s^{2}(s+2)}[/tex]

Applying the method of residues we have

[tex]\frac{4}{s^{2}(s+2)}=\frac{A}{s^{2}}+\frac{B}{s+2}[/tex]

Multiplying throught by [tex]s^{2}[/tex] we have

[tex]\frac{4}{s+2}=A+\frac{Bs^{2}}{s+2}[/tex]

[tex]A=\frac{4-Bs^{2}}{s+2}\mid_{s=0}=2[/tex]

Multiplying through by s+2 we have

[tex]\frac{4}{s^{2}}=\frac{A(s+2)}{s^{2}}+B[/tex]

[tex]B=\frac{4-A(s+2)}{s^{2}}\mid_{s=-2}=1[/tex]

Substituting A and B back into the equation we have

[tex]V(s)=\frac{2}{s^{2}}+\frac{1}{s+2}[/tex]

Applying the known Laplace transform pairs we have

[tex]v(t)=2t+e^{-2t}[/tex]

[tex]v(800ms)=2(0.8)+e^{-2(0.8s)}=1.802V[/tex]





 

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  • #2
I haven't checked all the details, but you seem to have the right idea.

What is the question?
 
  • #3
Well my answer is different from that given in the book. My answer is too high by 1V.
 
  • #4
Your partial fraction expansion is wrong. You should have:

[tex]\frac{4}{s^{2}(s+2)}=\frac{A}{s^{2}}+\frac{C}{s}+\frac{B}{s+2}[/tex]
Using the residues you have A = 2 and B = 1 as you have found.
Rewrite the second member with the common denominator and equate the numerator to 4.
You will find C = -1. This is what you need to find the correct answer.
 
  • #5
Thanks for not giving up on my question.

Kevin
 

1. How do I solve an RC circuit using Laplace transforms?

The first step in solving an RC circuit using Laplace transforms is to write the differential equation that describes the circuit. This equation will include the voltage across the capacitor, the current through the resistor, and the input voltage. Then, apply the Laplace transform to the equation to get an algebraic equation in the Laplace domain. Finally, use inverse Laplace transforms to get the solution in the time domain.

2. What is the benefit of using Laplace transforms to solve an RC circuit?

Laplace transforms allow us to solve differential equations with initial conditions, which is not possible with traditional methods. This makes it easier to find the complete solution of the circuit and analyze its behavior over time.

3. Can Laplace transforms be used for any type of RC circuit?

Yes, Laplace transforms can be used to solve any type of RC circuit, whether it is a series or parallel circuit. The method of solving may vary slightly depending on the type of circuit, but the general approach remains the same.

4. What initial conditions are needed to solve an RC circuit using Laplace transforms?

The initial voltage across the capacitor and the initial current through the resistor are needed as initial conditions to solve an RC circuit using Laplace transforms. These initial conditions can be obtained from the circuit diagram or given in the problem statement.

5. Are there any limitations to using Laplace transforms to solve RC circuits?

One limitation of using Laplace transforms is that it assumes the circuit is in a steady-state condition. This means that the circuit must have reached a stable state before the switch is closed or opened. Additionally, Laplace transforms may not be suitable for circuits with nonlinear elements such as diodes or transistors.

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