Laplace transforms for transient analysis

In summary: I'm sorry, I don't understand.When you solve for I(s), you're solving for the current in the circuit at a given time, right? You should calculate Vout now.
  • #1
agata78
139
0

Homework Statement



A capacitor of 0.1 F and a resistor of 5 Ω are connected in series; the combination is applied to a step voltage of 20V. Determine the expression for the:

(a) current that flows in the circuit and

(b) the voltage across the capacitor in time domain.

Homework Equations



For question (b)

Would I be correct to use the following equations?

Where:
Vc - is the voltage across the capacitor
V - is the supply voltage
t - is the elapsed time since the application of the supply voltage
RC - is the time constant of the RC charging circuit
e - is the base of the Natural Logarithm = 2.71828

Time Constant
τ = R x C
τ = 5 x 0.5
τ = 2.5 seconds

The voltage formula is given as:
Vc = V(1-e-t/RC)

which equals:
Vc = 20(1-e-t/5)
 
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  • #2
Are you expected to do the problem using Laplace transforms (it's in the thread title), or just write down the result from previous knowledge?

EDIT: Also, 5 x 0.1 is not 5.
 
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  • #3
Yes. The general title for these question states 'Use Laplace transforms for the transient analysis of networks'.

Appologies for the typing error.
 
  • #4
So, the equations you've written are really a result you hope to find using Laplace transforms.

As usual, begin with a circuit equation. Use Laplace domain models for the circuit components and write the appropriate equations...
 
  • #5
I can't find any appropriate equation for this, i don't have any good example for this.

Can you help?
 
  • #6
You write your usual circuit equations just as you would for an AC circuit, but use the Laplace domain version of the component impedances. Where you were using 'jω' before in the expressions for inductor and capacitor impedances, just use the variable 's'.

I know it looks silly at first glance, writing AC-type equations for what is apparently a DC circuit, but the Laplace domain's 's' variable takes in all frequencies and can readily model the transient response that happens when a switch closes. You'll see :smile:

You should have in your text or notes the form that a unit step function takes in the Laplace domain. You'll need that to model the 20V source that's suddenly switched on at time t=0.
 
  • #7
If I(t) is the current at time t, what is the voltage drop across the resistor at time t (in terms of I(t) and R)? What is the voltage drop across the capacitor at time t (in terms of the integral of I(t) with respect to t and C)? Write an equation such that the sum of these two voltage drops is equal to the applied step voltage. Do you know how to take the Laplace Transform of the individual terms in this equation? If so, write the Laplace Transform of the equation.

Chet
 
  • #8
Z = R + (1 / sC)

Z = 5 + (1 / s x 0.1)

Using Ohms Law:

I(s) = Vin / Z

I(s) = 20/s / 5+(1 / s x 0.1)

However:

Vout(s) = I x (1 / sC)

Vout(s) = I x (1 / s x 0.1)

So:

Vout(s) = [ 20/s / (0.1 + (1 / s x 0.1))] x [1 / s x 0.1]

Vout(s) = 20 / s(s x 0.1 x 0.1 + 1)

Vout(s) = 20 / s(s x 0.01 + 1)

Am i right? What value is s in this example?
 
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  • #9
Something's gone wrong in your algebra when you solved for Vout.

Start by simplifying your Z a bit. Note that 1/(s x 0.1) = 10/s. Makes the numbers easy!

You're going to want to solve for I, so you might as well simplify the expression for I(s) before carrying on to the potential across C. Can you reduce the expression for I(s)?
 
  • #10
To solve Z = R + (1 / sC) i need to add (5 + 10/s) = (10+5s/ s)

for Is= (20s/ 10 +5s) = (20s(10-5s) )/ (10+5s) (10-5s) = (200s - 100s2 ) / (100-25s2)

and if s2=(-1) then

Is= (200s+100) / 125
Is it ok so far?
 
  • #11
Use more parentheses to keep your operations straight.
$$I(s) = \frac{V(s)}{Z(s)} = \frac{20}{s} \left(\frac{s}{5 s + 10}\right) = ~~?$$
 
  • #12
Is= = 20 / 5s+10 = (100s-200) / (25s2 -100)

Is=( 4s-8) /-5
 
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  • #13
agata78 said:
Is= = 20 / 5s+10 = (100s-200) / (25s2 -100)

Egads! Just divide the top and bottom of 20 / (5s+10) by five. Hint: It is desirable to have the denominator have factors of the form (s + n).
 
  • #14
This is the same answer I got, but I used a different method. My starting equation was
[tex]\frac{\int_0^t{I(t')dt'}}{C}+RI(t)=Vu(t)[/tex]
where u is the unit step function. Taking the Laplace Transform gives:
[tex]\frac{I(s)}{sC}+RI(s)=\frac{V}{s}[/tex]
Solving for I(s):
[tex]I(s)=\frac{V}{R}\frac{1}{\left(s+\frac{1}{RC}\right)}[/tex]
 
  • #15
Then Is= 4/ (s+2)

Should i calculate now Vout?
 
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  • #16
agata78 said:
Then Is= 4/ (s+2)

Should i calculate now Vout?

You could, or you could find I(t) first. You need to provide it as one of the answers...
 
  • #17
It= ( V/R ) ( 1-e (-Rt/L) )

But i don't have L for this equation. Should i find a different one for It?
 
  • #18
agata78 said:
It= ( V/R ) ( 1-e (-Rt/L) )

But i don't have L for this equation. Should i find a different one for It?

There's no inductor in this circuit.

Find I(t) by finding the inverse Laplace transform of the I(s) that you found above. You should have a table of Laplace transforms to work with.
 
  • #19
What is the Laplace Transform of the function eat?
 
  • #20
ok then,

It= 4e -2t

am i right?
 
  • #21
agata78 said:
ok then,

It= 4e -2t

am i right?

Right. And that should be I(t); it's current as a function of time.
 
  • #22
Trying to calculate now Vout:

(4+/ (s+2) ) x (10/s) = 40 / ( s2 +2s)

how to deal with s2
 
  • #23
agata78 said:
Trying to calculate now Vout:

(4+/ (s+2) ) x (10/s) = 40 / ( s2 +2s)

how to deal with s2

Factor the denominator.

In fact, when you're deriving these things it's a good idea to keep a lookout for factors like s, (s + n), etc., and not combine them. They'll be needed later!
 
  • #24
Im stuck now, I out of ideas what to do next. Help!
 
  • #25
After factoring the denominator, use partial fractions to split the expression into two terms. Both terms should have forms that you can recognize in your Transform tables (If they're good tables you will probably also be able to spot an entry for your expression before the partial fraction procedure is done).
 
  • #26
40 / s2 +2s = -8+16s

am i right so far? What you mean by split the expression? which expression ?
 
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  • #27
agata78 said:
40 / s2 +2s = -8+16s

am i right?

Nope. You want to use partial fractions on the expression:
$$\frac{40}{s(s + 2)}$$
so
$$\frac{40}{s(s + 2)} = \frac{A}{s} + \frac{B}{s + 2}$$

...carry on...
 
  • #28
I don't know if I am doing that right,

after some calculations i have if s= (-2) then B=-20
and if s = 0 then A= 20

is it ok?
 
  • #29
You've found the correct values for A and B, but I don't recognize your method. Usually one multiplies out the expression on the right and then equates like terms of the numerators on the LHS and RHS to create a pair of equations to find A and B (look up the method of partial fractions).

Nevertheless, since you have values for A and B you now have two expressions in the Laplace domain that you should be able to find in your table of Laplace transforms. Write down their time domain translations; they comprise the terms of the current I(t) that you want.
 
  • #30
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  • #31
agata78 said:
I used this website to educate myself a bit more then i remembered from school www.mash.dept.shef.ac.uk/Resources/web-partialfractions.pdf

But does it matter which way i used to calculate A and B.

i(t)= 20e 1 + (-20) -2t

But what next?

Your transformation of the Laplace terms does not look right! You have found the that in the Laplace domain:
$$I(s) = \frac{20}{s} - \frac{20}{s + 2}$$
Find the forms of those two terms in your Laplace Transform tables and convert them to time domain terms. The result should look familiar!
 
  • #32
the only way it could be is:

20-20e(-2t)
 
  • #33
agata78 said:
the only way it could be is:

20-20e(-2t)

Right. Technically each term is multiplied by a unit step function to indicate the the voltage is "switched on" at time t = 0. Mathematically it means that this solution applies only for t ≥ 0.

So, writing it in proper form for a function:

[STRIKE]I(t)[/STRIKE]Vc(t) = 20-20e(-2t) = 20(1 - e(-2t))
[STRIKE]
Now you can move on to finding Vc(t). Use the same methods.[/STRIKE]

EDIT: Sorry about that. I misremembered where we were at in the problem sequence! I think you're done with this one!
 
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  • #34
Yes i was actually trying to ask you why would i have to calculate it again.

Hurrayyyyy!

Thank you so much for help all the way! One to go!
 

Related to Laplace transforms for transient analysis

1. What is a Laplace transform?

A Laplace transform is a mathematical tool used to convert a function of time into a function of complex frequency. It is commonly used in engineering and physics for analyzing systems with time-varying inputs and outputs.

2. How is a Laplace transform used in transient analysis?

In transient analysis, a Laplace transform is used to convert the differential equations governing a system into algebraic equations that can be easily solved. This allows for a more efficient and accurate analysis of the system's behavior over time.

3. What is the difference between a Laplace transform and a Fourier transform?

While both Laplace and Fourier transforms are used to convert functions from the time domain to the frequency domain, they differ in the types of functions they can handle. A Laplace transform can handle functions with exponential growth or decay, whereas a Fourier transform is limited to functions with periodic behavior.

4. How do I perform a Laplace transform?

To perform a Laplace transform, you need to apply the Laplace transform operator to the function of interest and integrate over the entire range of time. This will result in a new function of complex frequency, which can then be used for further analysis.

5. What are some real-world applications of Laplace transforms for transient analysis?

Laplace transforms are commonly used in electrical engineering, control systems, and signal processing to analyze the behavior of circuits, mechanical systems, and signals over time. They are also used in physics to study the dynamics of systems such as oscillators and fluid flow.

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