Troubleshooting RCL Circuit Homework - Help Needed

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In summary: So the current source is off during t > 0 and the circuit is in it's steady state. In summary, the circuit in question is a series RLC circuit with a current source of 5u(-t) A. The current source is turned off at t = 0 and the circuit is in its steady state. The initial inductor current is zero and the equivalent circuit at t = 0+ is a series RLC circuit without the current source.
  • #1
dwn
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*****Please see 3rd post and ignore calculations on this one******

Homework Statement



Please see image.

Homework Equations



alpha = 1/2RC
omega = 1/√(LC)
iL(t) = e-αt(A1[\SUB]coswdt + A2sinωdt)

The Attempt at a Solution



iL(0) = 5 ∴A1 = 5

Code:
di/dt = e[SUP]-1.8541t[/SUP](-11sin(2.236t) + 2.236A[SUB]2[/SUB]cos(2.236t)) + 1.8541e[SUP]-1.8541t[/SUP](5cos(2.236t) + A[SUB]2[/SUB]sin(2.236t))

Evaluating di/dt at t = 0 :
Code:
2.236A[SUB]2[/SUB] + (1.8541 * 5) = 0 
A[SUB]2[/SUB] = -4.146

Code:
i[SUB]L[/SUB](t) = e[SUP]-1.8541t[/SUP](5cos(2.236t) - 4.146sin(2.236t))

I've messed up somewhere...not sure where though. Please help.
 

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  • #2
I see one mistake right off the bat...α is incorrect, I used ωd. Also, I used ω0 instead of ωd. Aside from that now...anymore errors?

IDK what I was thinking!
 
  • #3
Okay...my second attempt, rushing the first time around :

α, ω0, ωd are unchanged.
A1 = i(0) = 5

Code:
i(t) = e[SUP]-1.25t[/SUP](A[SUB]1[/SUB]cos(1.8541t) + A[SUB]2[/SUB]sin(1.8541t))

Code:
di/dt = -1.25e[SUP]-1.25t[/SUP](A[SUB]1[/SUB]cos(1.8541t) + A[SUB]2[/SUB]sin(1.8541t)) - 1.8541e[SUP]-1.25t[/SUP](-5sin(1.8541t) + A[SUB]2[/SUB])cos(1.8541t))

Evaluate di/dt at t = 0:

Code:
 di/dt = (-1.25*5) - 1.8541A[SUB]2[/SUB]
A[SUB]2[/SUB] = -3.371

:bugeye:
 
  • #4
How do you figure that iL(0) = 5 A?

The ##\alpha## for a series circuit is not the same as for a parallel circuit.

The Wikipedia page for the RLC circuit gives a pretty good overview of the series RLC circuit formulas.
 
  • #5
I just can't hack it with these online courses. I can't begin to explain the benefit of discussing this stuff with a teach or student..:cry:

I digress...well, recognizing that there is not switch and therefore no sudden changes occurring in the circuit (in other words a t = 0-)...it is safe to say that at i(0) there is no current passing through the circuit which means i(0) = 0 → A1 = 0.

What exactly do A1 and A2 represent, individually. Is A1 attributed to initial conditions t≥0 and A1 t≤0?
 
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  • #6
dwn said:
I just can't hack it with these online courses. I can't begin to explain the benefit of discussing this stuff with a teach or student..:cry:

I digress...well, recognizing that there is not switch and therefore no sudden changes occurring in the circuit (in other words a t = 0-)...it is safe to say that at i(0) there is no current passing through the circuit which means i(0) = 0 → A1 = 0

Yup. The initial inductor current is zero. Just a few more things though. Note that the current source is specified as 5u(-t) A. Now u(t) is the unit step function, so there is a "hidden" switching operation that takes place at t = 0. How does the current source behave then? You might also want to consider the voltage on the capacitor at time t = 0. What's the equivalent circuit at t = 0+? Which way will the capacitor voltage want to drive the inductor current?
 
  • #7
gneill said:
Yup. The initial inductor current is zero. Just a few more things though. Note that the current source is specified as 5u(-t) A. Now u(t) is the unit step function, so there is a "hidden" switching operation that takes place at t = 0. How does the current source behave then? You might also want to consider the voltage on the capacitor at time t = 0. What's the equivalent circuit at t = 0+? Which way will the capacitor voltage want to drive the inductor current?

I would just like to say that these questions are really helpful in getting me to ask the right questions when I analyze the circuits.

Okay, I hope I am not missing your point and just stating the (somewhat) obvious, but once the "switch" closes the current will be directed to the capacitor until it is maxed out at which point the current will pass through the resistor and slowly charge the inductor since they like to resist change. Is this the correct flow of current? The current source will drive the capacitor voltage to infinite as t → ∞.

V = 1/C ∫(i * dt) + v(0)
Vc(0) = 0 V

The equivalent circuit would be a series RLC circuit not including the source.

Is this good brain function on my part? haha
 
  • #8
If this is the case, which I hope it is, then when it comes to solving diL/dt at t=0, I will not get an answer for A2.

Code:
di/dt|t = A[SUB]2[/SUB] = V[SUB]c[/SUB](0)/L = V[SUB]c[/SUB](0) - Ri(0)/L = 0
 
  • #9
dwn said:
I would just like to say that these questions are really helpful in getting me to ask the right questions when I analyze the circuits.

Okay, I hope I am not missing your point and just stating the (somewhat) obvious, but once the "switch" closes the current will be directed to the capacitor until it is maxed out at which point the current will pass through the resistor and slowly charge the inductor since they like to resist change. Is this the correct flow of current? The current source will drive the capacitor voltage to infinite as t → ∞.

V = 1/C ∫(i * dt) + v(0)
Vc(0) = 0 V

The equivalent circuit would be a series RLC circuit not including the source.

Is this good brain function on my part? haha

No, I suspect that you're missing the import of the unit step function controlling the current source: 5u(- t) A (note the negative sign on the t!). What will be the value of the current source at all time before t = 0? And after t = 0?
 
  • #10
t < 0 current will be positive 5
t > 0 current will be negative -5
 
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  • #11
dwn said:
t < 0 current will be positive 5
t > 0 current will be negative -5

Nope. The sign of the argument of the function doesn't change the sign of the function itself. The value of the unit step function can only be 0 or +1. So what might be the function of the negative sign on the argument t?
 
  • #12
The current source is turned off at t = 0. The step function is only applicable during -t...?

t < 0 equates to 1

t > 0 equates to 0

guess, I missed all this from previous chapter.
 
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  • #13
dwn said:
The current source is turned off at t = 0. The step function is only applicable during -t...?

Right. For all time t < 0 the current source is producing +5 A. At time t = 0 it "switches" or "steps" to zero amps. And, something that passes zero current essentially disappears from the circuit...

So you should determine what the voltage will be on the capacitor at time t = 0, since that will be the source of energy for the circuit after the "switch".

A useful thing to remember is that if you have a capacitor with an initial voltage on it, an equivalent circuit model for that capacitor is an uncharged capacitor in series with a voltage source of the same voltage. This can sometimes help to clarify your overall equivalent circuit and make writing the equations for the circuit easier.
 
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  • #14
I think have got it now, at least the step functions. That last bit is good to know, I will try to remember that and see if it helps make things a little clearer. I think I need to consider a different major.

Given everything, I really hope this is correct:

Code:
i[SUB]L[/SUB](t) = e[SUP]-t[/SUP](A[SUB]2[/SUB]sin(2t))
di[SUB]L[/SUB](t)/dt = -e[SUP]-t[/SUP](A[SUB]2[/SUB]sin(2t)) + e[SUP]-t[/SUP](2A[SUB]2[/SUB]cos(2t))

if V[SUB]c[/SUB] = 1/C∫i*dt  evaluated at t=0  → 5A/0.2F = 25 V
2A[SUB]2[/SUB] = 25    A[SUB]2[/SUB] = 12.5

Final Answer is...?
iL(t) = e-t(12.5sin(2t))
 
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  • #15
You don't need an integral to evaluate Vc for t = 0. It will have achieved steady state long before t = 0, so use the usual methods to evaluate it: The current through the capacitor and inductor is zero, the capacitor looks like an open circuit and the inductor a short circuit. All the current from the source is passing though the resistor. What's the potential that must appear across the "open" capacitor.

If it helps, you might think of replacing the current source and resistor with a Thevenin equivalent (voltage source in series with a resistor).
 
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  • #16
Hey gneill, I think I got it figured out...I was up until about 3 a.m. trying to figure all of this stuff out. I realize I need to work on first figuring out how the circuit is functioning before jumping into the calculations--I think that's how I get so lost, in addition to staring at this stuff for 8 hours straight! :)

Thanks a lot for all your help!
 

1. What is an RCL circuit?

An RCL circuit is a type of electrical circuit that contains a resistor (R), capacitor (C), and inductor (L). These components interact with each other to create a resonant frequency that affects the flow of current in the circuit.

2. What is the purpose of troubleshooting an RCL circuit?

The purpose of troubleshooting an RCL circuit is to identify and fix any issues or problems that may be affecting the circuit's performance. This can include identifying faulty components, loose connections, or incorrect values for the R, C, and L components.

3. How do I troubleshoot an RCL circuit?

To troubleshoot an RCL circuit, you will need to first gather information about the circuit, such as its components, values, and expected behavior. Then, you can use tools such as a multimeter or oscilloscope to measure the circuit's voltage, current, and other parameters. By comparing these measurements to the expected values, you can identify any potential issues and take steps to fix them.

4. What are common problems that can occur in an RCL circuit?

Some common problems that can occur in an RCL circuit include faulty components, incorrect values for the R, C, or L components, loose connections, and external interference. These issues can cause the circuit to behave differently than expected or not work at all.

5. Can I simulate an RCL circuit to help with troubleshooting?

Yes, it is possible to simulate an RCL circuit using software such as LTSpice or CircuitLab. These programs allow you to model the circuit and simulate its behavior, which can help you identify potential issues and test different solutions without having to physically manipulate the circuit.

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