RLC Circuit (with variable frequency)

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SUMMARY

The discussion focuses on determining the frequency at which an RLC circuit becomes purely resistive and calculating the effective resistance. The user, Josh, expresses difficulty in simplifying the solution process and seeks alternative methods. The key formula presented involves the impedance Z, where Z is expressed in terms of resistance R, inductance L, and capacitance C, highlighting the relationship between these components at varying frequencies.

PREREQUISITES
  • Understanding of RLC circuit theory
  • Familiarity with complex impedance calculations
  • Knowledge of resonance in electrical circuits
  • Proficiency in algebraic manipulation of complex numbers
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  • Study the conditions for resonance in RLC circuits
  • Learn about the implications of complex impedance in AC circuits
  • Explore methods for simplifying impedance calculations
  • Investigate practical applications of purely resistive circuits in electronics
USEFUL FOR

Electrical engineering students, circuit designers, and anyone involved in analyzing RLC circuits and their frequency response.

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Homework Statement



Find the frequency at which the circuit becomes purely resistive and calculate the effective resistance.

Here is the circuit with the given solution-

23qgif.jpg


The trouble is, whilst the solution is simple enough, there are many places to go wrong, and the whole process is time comsuming. I've managed to simplify a few other answers given in this answer booklet, but for this one, i can't find an easier method.

Any ideas? I can't find a similar example in Hughes.

Thanks,
Josh.
 
Physics news on Phys.org
If Z is real so is 1/Z.

[tex]\frac{1}{Z}=\frac{R-j\omega L}{R^2+(\omega L)^2}+j\omega C=\frac{R}{R^2+(\omega L)^2}+j\omega( C-\frac{ L}{R^2+(\omega L)^2})[/tex]

ehild
 

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