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Do a little trick to make a new expression for 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 1.
Z=R+jωL−j/ωC(R+jωL)(−j/ωC)R−jωL+j/ωCR−jωL+j/ωC
For resonance, the imaginary part of the new numerator must be zero.
Im[(R+jωL)(−j/ωC)(R−jωL+j/ωC)]=0
Solving for the resonant ω yields:
ω=LC1−L2R2
Note that for R=0, this reduces to the familiar LC resonance frequency.
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This discussion board is a place to discuss our Daily Challenges and the math and science related to those challenges. Explanations are more than just a solution — they should explain the steps and thinking strategies that you used to obtain the solution. Comments should further the discussion of math and science.
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@Steven Chase have a look. Thanks in advance.
The overall impedance is:
Z=R+jωL−j/ωC(R+jωL)(−j/ωC)
Do a little trick to make a new expression for 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 1.
Z=R+jωL−j/ωC(R+jωL)(−j/ωC)R−jωL+j/ωCR−jωL+j/ωC
For resonance, the imaginary part of the new numerator must be zero.
Im[(R+jωL)(−j/ωC)(R−jωL+j/ωC)]=0
Solving for the resonant ω yields:
ω=LC1−L2R2
Note that for R=0, this reduces to the familiar LC resonance frequency.
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@Steven Chase Thanks for the solution.
I am getting the same answer by doing the imaginary part of Z1=0 as well.
@Steven Chase what is the meaning of oscillating term?
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The part that varies with time
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@Steven Chase Thank you so much sir for such giving a precious information :) :)