Simple AC circuit with L and parasitic R

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    Ac Ac circuit Circuit
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Discussion Overview

The discussion revolves around determining the inductance (L) of a non-ideal inductor in an AC circuit that includes parasitic resistance (R). Participants explore various methods to analyze the circuit, focusing on the phase shift of the output signal at a frequency of 50 kHz. The conversation includes attempts to apply sinusoidal steady-state analysis and voltage division principles.

Discussion Character

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

Main Points Raised

  • One participant presents an approach using voltage division to express the output voltage (Vo) in terms of the input voltage (Vi) and the impedances of the resistor and inductor.
  • Another participant challenges the initial equations, suggesting that impedances in series simply add and proposes using the complex equivalent of Ohm's law to find the current through the circuit.
  • A different participant mentions using sinusoidal steady states and expresses uncertainty about how to handle the phase difference between the voltage across the inductor and the source voltage.
  • One participant clarifies that the parasitic resistance in the inductor is distinct from the regular resistor in the circuit and provides a method to calculate it, leading to a quadratic equation for L.
  • Another participant indicates that their calculations yield negative roots for L, suggesting further investigation is needed.

Areas of Agreement / Disagreement

Participants express differing views on the appropriate methods to analyze the circuit, with some advocating for sinusoidal steady-state techniques while others prefer simpler approaches. There is no consensus on the best method or the final value of L, as calculations yield varying results.

Contextual Notes

Some participants note the complexity introduced by the parasitic resistance and the phase shift, which may affect the accuracy of their calculations. The discussion also highlights the potential for multiple interpretations of the circuit's behavior based on different analytical approaches.

Who May Find This Useful

This discussion may be useful for students and practitioners interested in AC circuit analysis, particularly those dealing with non-ideal components and phase relationships in electrical engineering.

anthonuc
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Homework Statement


[PLAIN]http://sphotos.ak.fbcdn.net/hphotos-ak-snc4/hs894.snc4/72731_10150110340044992_712009991_7710053_709779_n.jpg

The circuit has a non-ideal inductor with parasitic R. v0(t) goes to coswt as the limit of w goes to zero.

The output signal has a +15 degree phase shift at 50kHz.

Determine L

Homework Equations



arctan(z1)-arctan(z2)=arctan[(z1-z2)/(1+z1z2)]

V0(t)= Xa * |H| * cos(wt+angle H)

H = a+bj
angle H = arctan(b/a)

The Attempt at a Solution



I change the impedances to 50 for the resistor and jwL for the inductor. Then using voltage division I get Vo = Vi(jwL/(jwL+50)) where (jwL/(jwL+50)) = H

However when trying to get the angle of H i get arctan(wL/0)-arctan(wL/50) and the arctan identity formula doesn't seem to help as the first value just goes to pi/2. Can I set the angle to 15 degrees and use w = 2pi*f where f =50khz to solve for L?

Trying this I get L = 5.9e-4 Henrys. Does this seem right? Feels low.

I don't know what to make of the first hint either with the limit of w going to zero.

Thanks if you read/help, much appreciated.
 
Last edited by a moderator:
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I don't know what all those equations are for. Impedances in series add. Ztotal = ZR + ZL.

Use the complex equivalent of V=IR: V=IZ, or V(t)=I(t)Ztotal

V(t) = 2cos(wt)

Now you can find the current through the series circuit using V(t)=I(t)Ztotal. This is also the current through the inductor.

Next, apply V=IZ again to find the voltage across the inductor. This time V=Vinductor and Z=iwL. Vinductor will have a different phase from the voltage source. This phase difference is what you are after.
 
Last edited:
Hmm. Well in class we were taught to use sinusoidal steady states to solve these problems which is where the relevant equations came from.

Using your method I get I=IL=(jwL+50)/(2costwt)

Then solving for VL in V=IZ I get

VL = (-w2L2+50jwL) / 2coswt

However I'm not sure what to do with this. This has a different phase from the voltage source?
 
[PLAIN]http://dl.dropbox.com/u/4222062/L-R.PNG

You are asked to work out the inductance, so you can work it out from the above diagram.
 
Last edited by a moderator:
Thanks for the help but I've managed to solve it correctly.

You use sinusoidal steady state to find the parasitic R in the inductor. The R attached in the circuit is not the parasitic R. It's just a regular resistor. There's also some unknown parasitic resistance in the non-ideal inductor.

Parasitic R = Rp

You use Vo = 2coswt*(jwl + Rp) / (jwl + Rp + 50).

Set this equation equal to coswt as w goes to zero and you'll get Rp = 50.

Knowing this value you can plug it back into this equation:

Vo = 2coswt*(jwl + Rp) / (jwl + Rp + 50)

and use H = (jwl + Rp) / (jwl + Rp + 50)

the angle of H = 15 degrees when f = 50Khz where w=2pi*f

the angle of H = arctan(50/(100000*pi*L) - arctan(100/100000*pi*L) = 15 degrees

Then you can use the identity

arctan(z1)-arctan(z2)=arctan[(z1-z2)/(1+z1z2)]

and get a solvable equation for L. You get a quadratic polynomial but it should be easy enough to solve in the end.

I ended up with L = 85mH

Actually I still have to find out what the correct answer will be since my quadratic actually gives me negative roots.

Hope this can be help for future references at least! I appreciate your guys' help.
 
Last edited:

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