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Reactance & resonance

Reactance & resonance: the circuit drawn with the example's values1 kHz10mH1µF
XL 62.8 Ω, XC 159 Ω at 1 kHz; f0 = 1.59 kHz

A coil fights fast changes, a capacitor slow ones; at f0 they cancel.

Opens in the app on 1 December, with Circuit Notebook 1.0 See it worked out

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The example, worked out

Given

Frequency
1 kHz
Inductance L
10 mH
Capacitance C
1 µF

Working

  1. grows with frequency
  2. shrinks with frequency
  3. where they are equal and cancel

Results

XL at 1 kHz62.8 Ω
XC at 1 kHz159 Ω
Resonance f01.59 kHz
Z0 = √(L/C)100 Ω
Series L + C lookscapacitive

The formulas

  1. XL = 2π f Lgrows with frequency
  2. XC = 1 / (2π f C)shrinks with frequency
  3. f0 = 1 / (2π √(L C))where they are equal

The usual traps

  • Below f0 a series LC looks capacitive, above it inductive.
  • Real parts have losses: the resonance is only as sharp as their Q.

Questions

How do I calculate the reactance of an inductor or a capacitor?

XL = 2π f L: grows with frequency. XC = 1 / (2π f C): shrinks with frequency. f0 = 1 / (2π √(L C)): where they are equal.

What does it give for typical values?

XL 62.8 Ω, XC 159 Ω at 1 kHz; f0 = 1.59 kHz. XL at 1 kHz: 62.8 Ω; XC at 1 kHz: 159 Ω.

What are the usual mistakes?

Below f0 a series LC looks capacitive, above it inductive. Real parts have losses: the resonance is only as sharp as their Q.

In the app

Your circuit, drawn live

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The part you can buy

Results rounded to standard values (E12, E24, E96) and power ratings.

The working, shown

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Into your notebook

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Opens in the app on 1 December, with Circuit Notebook 1.0

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