How Do You Calculate R and C for a Series Impedance of 500∠-36.1° at 10kHz?

AI Thread Summary
To calculate the resistance (R) and capacitance (C) for a series impedance of 500∠-36.1° at 10kHz, the angular frequency (ω) is determined to be 62832 rad/s. The impedance can be expressed as R - j/(ωC), where the real part corresponds to R and the imaginary part relates to C. The discussion emphasizes that the impedance's real and imaginary components can be treated separately, allowing for two equations to be formed from one impedance equation. This separation simplifies the process of solving for R and C, despite initially appearing to leave one equation with two variables. The key takeaway is that both components can be independently analyzed to find the required values.
zealeth
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Homework Statement



Compute values for R and C such that the total series impedance Z=500\angle(-36.1o) when f=10kHz.

F5llcWq.png


Homework Equations



ω=2\pif
KVL
ZC = -j*(1/(ωC)) = 1/(jωC) where j=\sqrt{-1}

The Attempt at a Solution



Seems like a pretty straightforward problem, I seem to be missing an equation somewhere but not sure what else I could use here.

ω=2*\pi*10*103 = 62832 rad/s
Zeq=500\angle(-36.1o) = R - j/(ωC) = R - j/(62832*C)

And here I am left with 1 equation and 2 variables, any ideas on what else I could use to solve this problem?
 
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zealeth said:

Homework Statement



Compute values for R and C such that the total series impedance Z=500\angle(-36.1o) when f=10kHz.

F5llcWq.png


Homework Equations



ω=2\pif
KVL
ZC = -j*(1/(ωC)) = 1/(jωC) where j=\sqrt{-1}

The Attempt at a Solution



Seems like a pretty straightforward problem, I seem to be missing an equation somewhere but not sure what else I could use here.

ω=2*\pi*10*103 = 62832 rad/s
Zeq=500\angle(-36.1o) = R - j/(ωC) = R - j/(62832*C)

And here I am left with 1 equation and 2 variables, any ideas on what else I could use to solve this problem?

Actually you're left with two equations, each in one variable. Note that the impedance has two terms, one real and one imaginary. The real and imaginary components are separate. For example, the real part of the impedance (the resistance) is independent of frequency.
 
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