Physics & Mechanics

RLC Circuit Calculator

Calculate the total impedance of a series RLC circuit containing a resistor, inductor, and capacitor at a specific AC frequency.

Ω
H
F
Hz
Inductive Reactance (X_L)
37.699
Capacitive Reactance (X_C)26.526 Ω
Total Impedance (Z)100.622 Ω

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Complex AC Circuits

An RLC circuit is an electrical circuit consisting of a Resistor ($R$), an Inductor ($L$), and a Capacitor ($C$), connected in series or parallel. These three components interact in a way that makes the circuit behave very differently depending on the frequency of the input signal.

The Role of Each Component

  • Resistor ($R$): Dissipates energy as heat. Its opposition is the same regardless of frequency.
  • Inductor ($L$): Opposes high frequencies. Its reactance ($X_L$) increases as frequency goes up.
  • Capacitor ($C$): Blocks low frequencies. Its reactance ($X_C$) decreases as frequency goes up.

At a very specific frequency (the Resonant Frequency), the inductor and capacitor perfectly cancel each other out, and the circuit's impedance is determined purely by the resistor.

The Formula (Series RLC)

Z=R2+(XLXC)2\begin{aligned} Z = \sqrt{R^2 + (X_L - X_C)^2} \end{aligned}

Where:
Z=
Total Impedance (Ohms)
R=
Resistance
XLX_L=
Inductive Reactance (2πfL)
XCX_C=
Capacitive Reactance (1/2πfC)

Example Calculation

A series RLC circuit has $R=100 , \Omega$, $L=0.1 , \text{H}$, and $C=10 , \mu\text{F}$ running at $60 , \text{Hz}$.

  1. Calculate XL ($2\pi f L$): $2 \times \pi \times 60 \times 0.1 \approx 37.7 , \Omega$.
  2. Calculate XC ($1 / 2\pi f C$): $1 / (2 \times \pi \times 60 \times 0.00001) \approx 265.3 , \Omega$.
  3. Calculate Total Z: $\sqrt{100^2 + (37.7 - 265.3)^2} \approx 248.5 , \Omega$.

Frequently Asked Questions

They are the building blocks of radio tuning circuits. By adjusting the capacitance or inductance, you can make the circuit resonate at a specific frequency, allowing you to 'tune in' to one radio station while ignoring others.

The 'Quality Factor' (Q) describes how 'sharp' the resonance is. A high Q circuit is very selective (good for radio), while a low Q circuit responds to a wider range of frequencies.

Because they contain both a spring-like component (Capacitor) and a flywheel-like component (Inductor), energy can bounce back and forth between them. If you give the circuit an electrical 'poke', it will oscillate or 'ring' at its natural frequency.