AC Source/ Variable Resistance

Join the discussion
Registration is free. Ask a follow-up in this thread, or start your own.
8 replies · 4K views
americanforest
Messages
220
Reaction score
0

Homework Statement


http://www.imagehosting.com/out.php/i1196840_3326.jpg
In the figure, a generator with an adjustable frequency of oscillation is connected to a variable resistance R, a capacitor of C = 2.50 μF, and an inductor of inductance L. The amplitude of the current produced in the circuit by the generator is at half-maximum level when the generator's frequency is 2.3 or 2.5 k Hz. What is L?

Homework Equations


1. [tex]I=\frac{\xi_{m}}{Z}cos(\omega_{d}t-\varphi)[/tex]

2. [tex]Z=\sqrt{R_{v}^2+\chi^2}[/tex]

3. [tex]\chi=L\omega-\frac{1}{C\omega}[/tex]

4. [tex]\omega_{r}=\frac{1}{\sqrt{LC}}[/tex]

5. [tex]\Delta\omega=\frac{R}{L}[/tex]

6. [tex]\omega=2\pi\nu[/tex]

Where [tex]\Delta\omega[/tex] is the spread of [tex]\omega[/tex] at .7 times the maximum current (at [tex]\omega_{r}[/tex])

The Attempt at a Solution



[tex]I_{res}=\frac{\xi_{m}}{R}[/tex]

At the given frequencies we have

[tex]I=\frac{I_{res}}{2}=\frac{\xi_{m}}{2R}=\frac{\xi_{m}}{\sqrt{R_{v}^2+\chi_{1,2}^2}}[/tex]

The voltage amplitudes cancel and we have one equation and two unknowns.

I was thinking about using equation 5 but that is only for the gap between the two frequencies for [tex]I_{m}=.7I_{res}[/tex] which isn't the case here.
 
Last edited:
Physics news on Phys.org
learningphysics said:
I'm not seeing the picture. I think the link you used is wrong.

Problem corrected. Sorry
 
As per your equations, at half amplitude you have:

2R = net impedance

so plugging in your two frequencies into this equation... you get two equations. You have two equations with 2 unknowns (L and R). You can solve for L.
 
The equation I come up with at the end is [tex]L=\frac{1}{C^{2}\omega_{1}^{2}\omega_{2}^{2}}[/tex]. Is this right? I seem to be getting the wrong answer with this equation?

I wish I had some kind of elf to do tedious algebra for me...
 
americanforest said:
The equation I come up with at the end is [tex]L=\frac{1}{C^{2}\omega_{1}^{2}\omega_{2}^{2}}[/tex]. Is this right? I seem to be getting the wrong answer with this equation?

I wish I had some kind of elf to do tedious algebra for me...

EDIT: wait: shouldn't it be [tex]L = \frac{1}{C\omega_{1}\omega_{2}}[/tex]
 
Last edited:
learningphysics said:
EDIT: wait: shouldn't it be [tex]L = \frac{1}{C\omega_{1}\omega_{2}}[/tex]

Indeed it should. Thanks. That kind of mistake is typical of me...
 
oops ... you know that (at resonance), LC = 1/w^2 , with w~2*pi*2.3 KHz ...
at the half-max current (hi_f and lo_f) , chi = (+/-) sqrt(3) R
(... from #2, 4R^2 is mostly inductive at higher frequencies than resonance.)
the algebra isn't very tedious when you eliminate the sqrt(3)R first