Engineering Design a circuit w/1 Ohm impedance

AI Thread Summary
The discussion revolves around designing a circuit with an equivalent impedance of 1Ω at ω=100 rad/s, incorporating at least one inductor. Participants express confusion about how to start the problem and the relationships between resistors, capacitors, and inductors. Key equations for impedance are shared, but there is uncertainty about how to apply them effectively. Suggestions include selecting values for L and C that will cancel each other out at the specified frequency while ensuring a 1Ω resistor is included. The conversation highlights the challenge of understanding circuit behavior and the resonance conditions in RLC circuits.
hogrampage
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Homework Statement


Design a suitable combination of resistors, capacitors, and/or inductors which has an equivalent impedance at ω=100 rad/s of 1Ω using at least one inductor.

Homework Equations


Zeq=ZR+ZL+ZC
ZR=R
ZL=jωL
ZC=-j/ωC

The Attempt at a Solution


I really am not sure how to start. I can see this being a fairly simple problem, but I just can't seem to wrap my head around it. I have read through the chapter numerous times, and I don't see anything else that could help at all.
 
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1= R + jwL +j/wC

1= R + j(wL+1/wC)

1= R + j(100L+1/100C)

easy one can be R =1, L=.01, C= -0.01
which equals 1 = 1+ j(0)
 
hogrampage said:

Homework Statement


Design a suitable combination of resistors, capacitors, and/or inductors which has an equivalent impedance at ω=100 rad/s of 1Ω using at least one inductor.

Homework Equations


Zeq=ZR+ZL+ZC
ZR=R
ZL=jωL
ZC=-j/ωC

The Attempt at a Solution


I really am not sure how to start. I can see this being a fairly simple problem, but I just can't seem to wrap my head around it. I have read through the chapter numerous times, and I don't see anything else that could help at all.

What do you know about LC or RLC circuits? Any special properties come to mind?
 
ω0=\frac{1}{\sqrt{LC}}

and

\alpha=\frac{1}{2RC}

Underdamped when \alpha<ω0, which has imaginary components.
 
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What conditions exist when a series RLC circuit are at resonance (ω = ωo)?
 
At resonance, XL=XC, but that would just make them cancel out so I'm not sure what to do.
 
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hogrampage said:
At resonance, XL=XC, but that would just make them cancel out so I'm not sure what to do.

Well, if they cancel out, what remains?...
 
R, but I'm supposed to use at least one inductor. I must be over-analyzing this (I think about these things too much lol).
 
hogrampage said:
R, but I'm supposed to use at least one inductor. I must be over-analyzing this (I think about these things too much lol).

Hmm, doesn't the "L" in "LC" count as an inductor?
 
  • #10
Yes, but I'm lost as to how to find the value(s). It isn't making sense to me. I don't even know which equation(s) to use. I have looked at the equations in the book and examples, and they aren't helping at all. No matter what, they always know at least one of the impedance values.

EDIT: Am I going anywhere with the below equation?

Zeq=jω\frac{1}{4\pi^{2}f^{2}C}-\frac{j}{ωC}

where Zeq=1.
 
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  • #11
I'm not sure what's confusing you :confused: Choose any L and a corresponding C that cancels it for the given frequency of operation --- then bang in a 1 Ohm resistor and you're home free.
 

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