How to find the inductance of this circuit

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    Circuit Inductance
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Discussion Overview

The discussion revolves around finding the inductance of a circuit and the angular frequency at which resonance occurs. Participants explore the relationships between inductance, current, and impedance in both series and parallel configurations, addressing both theoretical and practical aspects of resonance in RLC circuits.

Discussion Character

  • Technical explanation
  • Mathematical reasoning
  • Debate/contested
  • Homework-related

Main Points Raised

  • One participant states that resonance occurs when the inductance L is set to 1/8, leading to a minimum current, and seeks to find a new inductance L1 where the current becomes √2 of its minimum value.
  • Another participant questions the value of the impedance ZL at resonance, suggesting that inductive and capacitive impedances should cancel each other out.
  • Several participants discuss the implications of resonance in series versus parallel circuits, noting that the total impedance can be zero in both configurations.
  • There is a suggestion to simplify calculations by focusing on total current rather than total impedance, especially in parallel circuits.
  • One participant expresses uncertainty about whether to use magnitudes or complex terms when summing currents, leading to a discussion about the preference for complex forms in calculations.
  • After some calculations, a participant initially concludes L1=1/8 but later revises this to L=1/6, which another participant confirms as correct.
  • The condition for resonance, ZL=-ZC, is reiterated, with a participant questioning how to confirm resonance based solely on current reaching a minimum value.
  • A later reply clarifies that minimum current occurs at resonance, reinforcing the relationship between reactances of the inductor and capacitor.

Areas of Agreement / Disagreement

Participants exhibit a mix of agreement and disagreement, particularly regarding the values of inductance and the methods used for calculations. While some participants confirm certain values, others express uncertainty and seek clarification on the resonance conditions.

Contextual Notes

Participants mention various assumptions regarding the circuit configuration and the nature of resonance, but these assumptions are not fully resolved. The discussion reflects a range of approaches to the problem, with some methods appearing more complex than others.

Who May Find This Useful

This discussion may be useful for students and practitioners interested in RLC circuits, resonance phenomena, and the mathematical relationships governing inductance and impedance in electrical engineering.

MissP.25_5
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I got stuck doing this question. Please correct my mistakes and help me out.

1. The angular frequency ω is FIXED to 2 [rad/s] whereas the inductance L is changeable. When L=1/8, resonance occurs in the circuit and the magnitude of current i reaches its minimum value. From this state, L is increased to L=L1 and current i becomes √2 of its minimum value. Find L1.

2. The inductance L is fixed to L1 (found in question 1) while ω is variable. When ω= ω0, the magnitude of current i reaches its minimum value. Find ω0.
 

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Check your value for ZL. (At resonance you'd expect the inductive and capacitive impedances to be complex conjugates (i.e., they'll cancel if added)).

Since you're looking for a ratio in part 2, you might as well just choose a convenient value for the voltage source. Letting e = 1 [V] looks promising. What's the current Io at resonance then?
 
gneill said:
Check your value for ZL. (At resonance you'd expect the inductive and capacitive impedances to be complex conjugates (i.e., they'll cancel if added)).

Since you're looking for a ratio in part 2, you might as well just choose a convenient value for the voltage source. Letting e = 1 [V] looks promising. What's the current Io at resonance then?

At resonance, the ZL+ZC is 0 in a series circuit. Is it the same as in this parallell circuit?
 
MissP.25_5 said:
At resonance, the ZL+ZC is 0 in a series circuit. Is it the same as in this parallell circuit?

You'll find that they also cancel when added in parallel. Try it:
$$Z = \frac{1}{\frac{1}{R} + \frac{1}{ZL} + \frac{1}{ZC}}$$
and at resonance ZC = -ZL ... so ...
 
gneill said:
You'll find that they also cancel when added in parallel. Try it:
$$Z = \frac{1}{\frac{1}{R} + \frac{1}{ZL} + \frac{1}{ZC}}$$
and at resonance ZC = -ZL ... so ...

Is the circuit still in resonant state when L is is increased to L1?I guess not, though, because then L=1/8 and it's back to square 1.
 
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So in a parallel circuit, the total impedance of ZL and ZC is indeed 0. But when L increases to L1, the circuit is no more at resonance, isn't it? Am I doing this right? The method I am using seems to be too long, and I think it's impossible to get it.
 

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MissP.25_5 said:
So in a parallel circuit, the total impedance of ZL and ZC is indeed 0. But when L increases to L1, the circuit is no more at resonance, isn't it? Am I doing this right? The method I am using seems to be too long, and I think it's impossible to get it.

I see that the math got a bit hairy pretty quickly. So if I might suggest... rather than going for the total impedance, you can go for the total current right away.

This is a parallel circuit so every branch has the same potential difference and the branch currents sum. Choosing a suitable potential for the voltage source, say 1 V at 2 rad/sec, will make summing the currents a piece of cake.
 
gneill said:
I see that the math got a bit hairy pretty quickly. So if I might suggest... rather than going for the total impedance, you can go for the total current right away.

This is a parallel circuit so every branch has the same potential difference and the branch currents sum. Choosing a suitable potential for the voltage source, say 1 V at 2 rad/sec, will make summing the currents a piece of cake.

When finding the sum of the currents, should I take the magnitudes of iC and iL or just leave them be as complex terms? I'm still not used to when to use magnitudes, can you give me some tips?
 
MissP.25_5 said:
When finding the sum of the currents, should I take the magnitudes of iC and iL or just leave them be as complex terms? I'm still not used to when to use magnitudes, can you give me some tips?

Almost always you want to keep everything in complex form. An exception is when you are calculating power, but even then you can do that in complex form as well (calculating the complex power and then extracting the effective power as the real term). This avoids having to remember how to deal with power factors applied to the product of the voltage and current magnitudes :wink:
 
  • #10
gneill said:
Almost always you want to keep everything in complex form. An exception is when you are calculating power, but even then you can do that in complex form as well (calculating the complex power and then extracting the effective power as the real term). This avoids having to remember how to deal with power factors applied to the product of the voltage and current magnitudes :wink:

Ok, I'm done with the calculation. I got L1=1/8, this cannot be right ? I used your method of using current and then I just equate the terms with its real and imaginary coefficients. I'm not sure if I did it right, though.
 
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  • #11
MissP.25_5 said:
Ok, I'm done with the calculation. Is L1=1/8 ? I used your method of using current and then I just equate the terms with its real and imaginary coefficients. I'm not sure if I did it right, though.

You can sum the currents as before, but this time it's the magnitude of the current you're looking for. So the magnitude rises to √2 x the initial current. I'm not seeing 1/8 for L1.
 
  • #12
gneill said:
You can sum the currents as before, but this time it's the magnitude of the current you're looking for. So the magnitude rises to √2 x the initial current. I'm not seeing 1/8 for L1.

Of course, because L=1/8 is when the circuit is at resonance. I forgot.
 
  • #13
gneill said:
You can sum the currents as before, but this time it's the magnitude of the current you're looking for. So the magnitude rises to √2 x the initial current. I'm not seeing 1/8 for L1.

Ok, I fixed it. L=1/6, right?
 
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  • #14
MissP.25_5 said:
Ok, I fixed it. L=1/6, right?

Yes!
 
  • #15
gneill said:
Yes!

Now, to find ω0, do I have to use the same method too?
 
  • #16
MissP.25_5 said:
Now, to find ω0, do I have to use the same method too?

This time you have all the component values, and in particular, the inductance and capacitance. At resonance, what condition holds for those two components? (it was mentioned earlier).
 
  • #17
gneill said:
This time you have all the component values, and in particular, the inductance and capacitance. At resonance, what condition holds for those two components? (it was mentioned earlier).

ZL=-ZC is the condition. But, how do you know that it's at resonance? It only says that the current reaches its minimum value. But I used current to find omega and got the answer. Look...
 

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  • #18
MissP.25_5 said:
ZL=-ZC is the condition. But, how do you know that it's at resonance? It only says that the current reaches its minimum value. But I used current to find omega and got the answer. Look...

The only time the current can reach its minimum value is when the circuit is at resonance. That is, the capacitor and inductor impedances mutually cancel and they "disappear" from the circuit. Minimum current for a parallel RLC circuit occurs at resonance.

Knowing that, you know that XL = XC; the reactances are equal. (Reactance is magnitude of the impedance)

So just equate the reactances of the two reactive components.

The result you found is correct, even if you pursued a longer path to it :smile:
 

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