R-L Transient Circuit: Find Time Constant & Energy Stored in Inductor

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Homework Help Overview

The discussion revolves around a series R-L transient circuit connected to a voltage source, focusing on the time constant and energy stored in the inductor. The original poster presents a scenario where the current through the inductor reaches a specific value after a given time, prompting questions about the time constant and the implications of the circuit's behavior over time.

Discussion Character

  • Exploratory, Assumption checking, Conceptual clarification

Approaches and Questions Raised

  • Participants explore the relationship between time constants and the behavior of the circuit, questioning how to determine if a given time is after a certain number of time constants. There is discussion about the exponential nature of the current rise and the implications of reaching steady state.

Discussion Status

Participants are actively engaging with the problem, raising questions about the original poster's calculations and assumptions. Some suggest using a rule of thumb regarding time constants, while others clarify the implications of the time values given in the problem. There is a recognition that the time constant must be less than the observed time for the current to reach a steady state.

Contextual Notes

There is an ongoing discussion about the clarity of the problem statement regarding steady state conditions and the assumptions that can be made based on the given time values. Participants note the lack of explicit statements about steady state in some scenarios, leading to further inquiry.

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Homework Statement


A series R-L transient circuit is connected to a voltage source of E= 40V through a switch as shown. Suppose the switch is closed at time t=0μs and it was observed that the current iL flowing through the inductor rises to 4mA at time t=20μs and remains at 4mA after t=20μs.(i) Find the R-L time constant τ in μs for the storage phase. Resistor given is 10kΩ

The Attempt at a Solution


iL=E/R(1-e-t/τ)
0.004=40/10000(1-e-20x10-6/τ)
0.004=0.004(1-e-20x10-6/τ) -> 0.004-0.004=0
0=-e-20x10-6/τ -> Wanted to take ln for both side, ln 0 =error

unable to continue, please help, thanks.(ii) Calculate the amount of energy Wl in nJ, stored in the inductor after 1 minute.
How do we know 1min=60sec>>5time constant?
 

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There's a useful rule of thumb for these exponential curves that essentially states that all the interesting action is over after 5 time constants :wink:
 
I know that after 5 time constants, the inductor will become a short circuit.

But how would i know after 1minute, it's 5 time constant?

And if you don't mind can you help me take a look at my working please. Thanks gneill.
 
Yeah, the exponential term has to decay to 0 in order for the current to approach the asymptotic value of E/R. This happens when the exponent "blah" is large enough that e^-blah = 0. (To put it loosely: (-20 us)/tau → ln0 ≈ -infinity). So the time of 20 us is much much larger than a time constant, so that the exponent will be much larger than -1, and you have many factors of "e" of decay. Typically in these engineering classes they give you a "rule of thumb" that says that you can consider the exponential to have effectively decayed to zero after n time constants. I'm inferring from you comment in part ii that your class is taking n = 5 as your rule of thumb. If that's true, you can solve for tau by assuming that the 20 us is = 5 time constants. Without such a rule of thumb, you can't really solve for a specific value of tau, all you can say is that tau is much smaller than 20 us.

EDIT: scooped by gneill!
 
Then how do i determine whether the time given by the question for example 10s,20s or 30s etc is after 5 tau? It's not clear at all. For this instance he just say that after 1min. But actually 1min >> 5 time constants
 
Last edited:
freshbox said:
Then how do i determine whether the time given by the question for example 10s,20s or 30s etc is after 5 tau? It's not clear at all. For this instance he just say that after 1min. But actually 1min >> 5 time constants

Part (ii) of the question follows part (i) :smile: In part (i) you determined the time constant, and it must be less than 20 μs. One minute is 60 million microseconds, which is much more than 5 times 20 μs. In fact, anything over a tenth of a millisecond is guaranteed to be more than ##5\tau##.
 
oic, btw where have i gone wrong for my working?
 
gneill said:
Part (ii) of the question follows part (i) :smile: In part (i) you determined the time constant, and it must be less than 20 μs. One minute is 60 million microseconds, which is much more than 5 times 20 μs. In fact, anything over a tenth of a millisecond is guaranteed to be more than ##5\tau##.

Agreed, except for this part. It should say, "which is much more than 20 μs", since it is 5τ that equals 20 μs, not τ. Right?
 
cepheid said:
Agreed, except for this part. It should say, "which is much more than 20 μs", since it is 5τ that equals 20 μs, not τ. Right?

I used 5 times 20 μs since 20 μs is a given upper bound for τ (although not a least upper bound) and 5τ is the settling time. But sure, your phrasing is arguably more accurate.
 
  • #10
freshbox said:
oic, btw where have i gone wrong for my working?

You're trying to find ##\tau## such that e-20x10-6 = 0. But the function ##e^{-x}## only approaches zero asymptotically as x goes to infinity. You can't find τ exactly by this method. Use the "excitement's over after 5τ" rule of thumb instead.
 
  • #11
You mean part (i) is actually after 5 time constant already?
 
  • #12
freshbox said:
You mean part (i) is actually after 5 time constant already?

"(i) Find the R-L time constant τ in μs for the storage phase. Resistor given is 10kΩ"

You're told that the current reaches essentially steady state after 20 μs. So τ must be less than 20 μs. In fact, it's about 5 times smaller than 20 μs.
 
  • #13
which part of the question says that the circuit is at steady state?
 
  • #14
freshbox said:
which part of the question says that the circuit is at steady state?

"Suppose the switch is closed at time t=0μs and it was observed that the current iL flowing through the inductor rises to 4mA at time t=20μs and remains at 4mA after t=20μs."
 
  • #15
Ok here's another question. A series RC charging circuit is connected to a voltage source of E = 80V through a switch as sown. Assume there was no charge initially stored in the capactior. Suppose the switch is closed at time =0s and it was observed that the voltage vc across the capacitor, rises to 80v after time t=25millisec.

For this question, it did not say that remains at xxx after t=xxxx. So how would i know it is after 5 time constant (steady state) ?

***Ah ok i understand already, is it because initially there was no charge and since battery is 80v and after 25millisec, it's fully charged hence steady state. ?
 
  • #16
freshbox said:
Ok here's another question. A series RC charging circuit is connected to a voltage source of E = 80V through a switch as sown. Assume there was no charge initially stored in the capactior. Suppose the switch is closed at time =0s and it was observed that the voltage vc across the capacitor, rises to 80v after time t=25millisec.

For this question, it did not say that remains at xxx after t=xxxx. So how would i know it is after 5 time constant (steady state) ?

Because E = 80V and it reached 80V after 25 ms. 80V is as high as it can go; the steady state.
 
  • #17
thanks :)
 

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