Understanding RLC Damping Coefficient for Non-Standard Circuits

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SUMMARY

The discussion focuses on determining the damping coefficient (α) for non-standard RLC circuits, specifically when components are arranged in complex configurations. For a series RLC circuit, α is defined as R/2L, while for a parallel circuit, it is 1/2RC. In cases where the circuit configuration is neither strictly series nor parallel, participants suggest converting the circuit to its Thevenin equivalent to simplify analysis. Additionally, deriving the governing differential equation allows for the extraction of the damping ratio and other parameters.

PREREQUISITES
  • Understanding of RLC circuit configurations
  • Familiarity with Thevenin's theorem
  • Knowledge of differential equations
  • Concept of damping ratio and natural frequency
NEXT STEPS
  • Study Thevenin equivalent circuits in depth
  • Learn how to derive differential equations for RLC circuits
  • Explore the relationship between impedance and damping coefficient
  • Investigate advanced RLC circuit configurations and their analysis
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Electrical engineers, circuit designers, and students studying RLC circuits who seek to understand damping coefficients in complex circuit configurations.

samthedummy
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Hey,

Quick question for you guys. How do you find alpha (damping coefficient, Neper frequency) for a circuit that's not strictly parallel or in series? For instance, α for a series RLC circuit is R/2L whereas α for a parallel circuit is 1/2RC; but what if it's different?

Homework Statement



Here's an example of what I mean. Suppose you have an inductor and a capacitor in series that's in parallel with a resistor and a current source (see attached). Although R, L, and C, are in series with each other (in their own loop), R and LC are in parallel with the source. How would you know which α to use? Is there a way to get α in terms of impedance?

Homework Equations



As mentioned before:

\alpha_{series}=\frac{R}{2L}

and:

\alpha_{parallel}=\frac{1}{2RC}

For what it's worth:

\zeta=\frac{\alpha}{\omega_{0}}

where ζ is the damping ratio and:

\omega_{0}=\frac{1}{\sqrt{LC}}

where ω0 is the natural or resonant frequency of the circuit (the same in series and parallel).

The Attempt at a Solution



Since this is more of a conceptual type question, I've tried looking it up in different sources but they all seem to only look at independent series or parallel cases. More curious for myself than anything. Maybe one of you EEs can point me in the right direction/explain this for me. Much appreciated.

Peace.
 
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samthedummy said:
Here's an example of what I mean. Suppose you have an inductor and a capacitor in series that's in parallel with a resistor and a current source (see attached). Although R, L, and C, are in series with each other (in their own loop), R and LC are in parallel with the source. How would you know which α to use? Is there a way to get α in terms of impedance?

Convert the current source and the parallel resistance into its Thevenin equivalent. This will give you a purely serial RLC circuit driven by a voltage source :smile:

There are configurations of R, L, and C that are more tricky. For those you could determine the differential equation governing the circuit and hammer it into standard form (it's a second order differential equation). Then you can pick out the damping ratio, etc., from the parameters.
 

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