Angular Frequency

Find angular frequency of source for resonance

Note by Talulah Riley
8 months, 1 week ago

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Comments

@Steven Chase have a look. Thanks in advance.

Talulah Riley - 8 months, 1 week ago

The overall impedance is:

Z=(R+jωL)(j/ωC)R+jωLj/ωC Z = \frac{(R + j \omega L) (-j / \omega C)}{R + j \omega L - j / \omega C }

Do a little trick to make a new expression for Z Z , with the denominator being a real number. This works because when the denominator is multiplied by its complex conjugate, it becomes a real number. We are effectively just creatively multiplying the original expression by 11 .

Z=(R+jωL)(j/ωC)R+jωLj/ωCRjωL+j/ωCRjωL+j/ωC Z = \frac{(R + j \omega L) (-j / \omega C)}{R + j \omega L - j / \omega C } \,\, \frac{R - j \omega L + j / \omega C}{R - j \omega L + j / \omega C}

For resonance, the imaginary part of the new numerator must be zero.

Im[(R+jωL)(j/ωC)(RjωL+j/ωC)]=0 Im\Big[ (R + j \omega L) (-j / \omega C) (R - j \omega L + j / \omega C) \Big ] = 0

Solving for the resonant ω \omega yields:

ω=1LCR2L2 \omega = \sqrt{\frac{1}{L C} - \frac{R^2}{L^2}}

Note that for R=0 R = 0 , this reduces to the familiar LCL C resonance frequency.

Steven Chase - 8 months, 1 week ago

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@Steven Chase Thanks for the solution.
I am getting the same answer by doing the imaginary part of 1Z=0 \large \frac{1}{Z}=0 as well.

Talulah Riley - 8 months, 1 week ago

@Steven Chase what is the meaning of oscillating term?

Talulah Riley - 8 months, 1 week ago

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The part that varies with time

Steven Chase - 8 months, 1 week ago

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@Steven Chase @Steven Chase Thank you so much sir for such giving a precious information :) :)

Talulah Riley - 8 months, 1 week ago
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