RLC Circuit Calculator
Step and sinusoidal response of series RLC circuits: natural frequency, damping ratio, Q factor, and bandwidth
Step or sinusoidal response, natural frequency, damping, and quality factor for series RLC.
Natural Freq. ωn
447.21 rad/s
Resonant Freq. f₀
71.18 Hz
Damping Ratio ζ
0.2236
Classification
Underdamped
Quality Factor Q
2.236
Bandwidth BW
31.83 Hz
Time Constant τ
10.00 ms
Step Response v_C(t)
Tip: hover to read values, click to pin a point for export
Transient Response Data Table
| t (ms) | v_C (V) |
|---|---|
| 0.000 | 0.000000 |
| 0.500 | 0.024090 |
| 1.000 | 0.092120 |
| 1.500 | 0.196700 |
| 2.000 | 0.329400 |
| 2.500 | 0.481240 |
| 3.000 | 0.643210 |
| 3.500 | 0.806670 |
| 4.000 | 0.963740 |
| 4.500 | 1.107580 |
| 5.000 | 1.232630 |
| 5.500 | 1.334760 |
| 6.000 | 1.411310 |
| 6.500 | 1.461090 |
| 7.000 | 1.484280 |
| 7.500 | 1.482320 |
| 8.000 | 1.457690 |
| 8.500 | 1.413710 |
| 9.000 | 1.354320 |
| 9.500 | 1.283790 |
| 10.000 | 1.206530 |
| 10.500 | 1.126830 |
| 11.000 | 1.048710 |
| 11.500 | 0.975710 |
| 12.000 | 0.910810 |
| 12.500 | 0.856320 |
| 13.000 | 0.813810 |
| 13.500 | 0.784180 |
| 14.000 | 0.767590 |
| 14.500 | 0.763590 |
| 15.000 | 0.771170 |
| 15.500 | 0.788880 |
| 16.000 | 0.814900 |
| 16.500 | 0.847220 |
| 17.000 | 0.883700 |
| 17.500 | 0.922220 |
| 18.000 | 0.960760 |
| 18.500 | 0.997490 |
| 19.000 | 1.030850 |
| 19.500 | 1.059570 |
| 20.000 | 1.082730 |
| 20.500 | 1.099770 |
| 21.000 | 1.110460 |
| 21.500 | 1.114900 |
| 22.000 | 1.113470 |
| 22.500 | 1.106800 |
| 23.000 | 1.095710 |
| 23.500 | 1.081130 |
| 24.000 | 1.064100 |
| 24.500 | 1.045650 |
| 25.000 | 1.026800 |
| 25.500 | 1.008470 |
| 26.000 | 0.991480 |
| 26.500 | 0.976510 |
| 27.000 | 0.964080 |
| 27.500 | 0.954540 |
| 28.000 | 0.948050 |
| 28.500 | 0.944650 |
| 29.000 | 0.944190 |
| 29.500 | 0.946420 |
| 30.000 | 0.950980 |
| 30.500 | 0.957420 |
| 31.000 | 0.965270 |
| 31.500 | 0.974020 |
| 32.000 | 0.983170 |
| 32.500 | 0.992240 |
| 33.000 | 1.000820 |
| 33.500 | 1.008540 |
| 34.000 | 1.015130 |
| 34.500 | 1.020370 |
| 35.000 | 1.024140 |
| 35.500 | 1.026420 |
| 36.000 | 1.027220 |
| 36.500 | 1.026660 |
| 37.000 | 1.024890 |
| 37.500 | 1.022110 |
| 38.000 | 1.018540 |
| 38.500 | 1.014440 |
| 39.000 | 1.010040 |
| 39.500 | 1.005580 |
| 40.000 | 1.001290 |
| 40.500 | 0.997340 |
| 41.000 | 0.993900 |
| 41.500 | 0.991070 |
| 42.000 | 0.988930 |
| 42.500 | 0.987520 |
| 43.000 | 0.986840 |
| 43.500 | 0.986840 |
| 44.000 | 0.987470 |
| 44.500 | 0.988630 |
| 45.000 | 0.990220 |
| 45.500 | 0.992130 |
| 46.000 | 0.994220 |
| 46.500 | 0.996390 |
| 47.000 | 0.998520 |
| 47.500 | 1.000520 |
| 48.000 | 1.002310 |
| 48.500 | 1.003810 |
| 49.000 | 1.005000 |
| 49.500 | 1.005830 |
| 50.000 | 1.006310 |
| 50.500 | 1.006440 |
| 51.000 | 1.006250 |
| 51.500 | 1.005790 |
| 52.000 | 1.005100 |
| 52.500 | 1.004230 |
| 53.000 | 1.003240 |
| 53.500 | 1.002190 |
| 54.000 | 1.001140 |
| 54.500 | 1.000140 |
| 55.000 | 0.999220 |
| 55.500 | 0.998430 |
| 56.000 | 0.997790 |
| 56.500 | 0.997310 |
| 57.000 | 0.997010 |
| 57.500 | 0.996880 |
| 58.000 | 0.996900 |
| 58.500 | 0.997070 |
| 59.000 | 0.997370 |
| 59.500 | 0.997760 |
| 60.000 | 0.998220 |
| 60.500 | 0.998720 |
| 61.000 | 0.999230 |
| 61.500 | 0.999730 |
| 62.000 | 1.000200 |
| 62.500 | 1.000610 |
| 63.000 | 1.000960 |
| 63.500 | 1.001220 |
| 64.000 | 1.001400 |
| 64.500 | 1.001500 |
| 65.000 | 1.001520 |
| 65.500 | 1.001470 |
| 66.000 | 1.001350 |
| 66.500 | 1.001170 |
| 67.000 | 1.000960 |
| 67.500 | 1.000730 |
| 68.000 | 1.000480 |
| 68.500 | 1.000230 |
| 69.000 | 0.999990 |
| 69.500 | 0.999780 |
| 70.000 | 0.999600 |
| 70.500 | 0.999450 |
| 71.000 | 0.999350 |
| 71.500 | 0.999280 |
| 72.000 | 0.999260 |
| 72.500 | 0.999270 |
| 73.000 | 0.999320 |
| 73.500 | 0.999390 |
| 74.000 | 0.999490 |
| 74.500 | 0.999600 |
| 75.000 | 0.999720 |
| 75.500 | 0.999840 |
| 76.000 | 0.999960 |
| 76.500 | 1.000060 |
| 77.000 | 1.000160 |
| 77.500 | 1.000240 |
| 78.000 | 1.000300 |
| 78.500 | 1.000340 |
| 79.000 | 1.000360 |
| 79.500 | 1.000360 |
| 80.000 | 1.000340 |
| 80.500 | 1.000310 |
| 81.000 | 1.000270 |
| 81.500 | 1.000220 |
| 82.000 | 1.000160 |
| 82.500 | 1.000100 |
| 83.000 | 1.000040 |
| 83.500 | 0.999990 |
| 84.000 | 0.999940 |
| 84.500 | 0.999900 |
| 85.000 | 0.999870 |
| 85.500 | 0.999840 |
| 86.000 | 0.999830 |
| 86.500 | 0.999820 |
| 87.000 | 0.999830 |
| 87.500 | 0.999840 |
| 88.000 | 0.999860 |
| 88.500 | 0.999880 |
| 89.000 | 0.999910 |
| 89.500 | 0.999940 |
| 90.000 | 0.999970 |
| 90.500 | 0.999990 |
| 91.000 | 1.000020 |
| 91.500 | 1.000040 |
| 92.000 | 1.000060 |
| 92.500 | 1.000070 |
| 93.000 | 1.000080 |
| 93.500 | 1.000080 |
| 94.000 | 1.000080 |
| 94.500 | 1.000080 |
| 95.000 | 1.000070 |
| 95.500 | 1.000060 |
| 96.000 | 1.000050 |
| 96.500 | 1.000040 |
| 97.000 | 1.000020 |
| 97.500 | 1.000010 |
| 98.000 | 1.000000 |
| 98.500 | 0.999980 |
| 99.000 | 0.999970 |
| 99.500 | 0.999970 |
| 100.000 | 0.999960 |
Formulas
How to Use This Calculator
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Formula Reference
Undamped Natural (Resonant) Frequency
ωn = 1/√(L·C) | f₀ = ωn/(2·π) = 1/(2·π·√(L·C))
Variables: ωn = undamped natural angular frequency (rad/s), f₀ = resonant frequency (Hz), L = inductance (H; entered in mH and divided by 1000), C = capacitance (F; entered in μF and divided by 10⁶). Source: Nilsson & Riedel, Electric Circuits, 10th ed., Ch. 8 (Natural and Step Responses of RLC Circuits)
Neper Frequency, Damping Ratio and Time Constant (Series)
α = R/(2·L) | ζ = α/ωn = (R/2)·√(C/L) = R/(2·√(L/C)) | τ = 1/α = 2·L/R
Variables: α = neper (damping) frequency (Np/s = 1/s), R = series resistance (Ω), L = inductance (H), C = capacitance (F), ζ = damping ratio (dimensionless; ζ < 1 underdamped, ζ = 1 critically damped, ζ > 1 overdamped), τ = decay-envelope time constant (s; displayed in s, ms, μs or ns), ωn = natural angular frequency (rad/s). An overdamped circuit (ζ > 1) has no envelope: it decays as two exponentials, so the page shows instead the slower one's time constant, τ₁ = 1/|s₁| with s₁ = −ωn²/(α + √(α² − ωn²)). Source: Nise, Control Systems Engineering, 8th ed., Ch. 4 (Second-Order Systems); Nilsson & Riedel, Electric Circuits, 10th ed., Ch. 8
Quality Factor and Half-Power Bandwidth (Series Resonance)
Q = (1/R)·√(L/C) = ωn·L/R = 1/(2·ζ) | BW = R/L = ωn/Q | [rad/s]
Variables: Q = quality factor at resonance (dimensionless), R = series resistance (Ω), L = inductance (H), C = capacitance (F), ωn = natural angular frequency (rad/s), ζ = damping ratio (dimensionless), BW = half-power (−3 dB) bandwidth (rad/s; also displayed as BW/(2·π) in Hz). Source: Alexander & Sadiku, Fundamentals of Electric Circuits, 6th ed., Ch. 14 (Series Resonance)
Underdamped Step Response of Capacitor Voltage
v_C(t) = V₀·[1 − e^(−α·t)·(cos(ωd·t) + (α/ωd)·sin(ωd·t))] | ωd = ωn·√(1 − ζ²)
Variables: v_C(t) = capacitor voltage (V), V₀ = step input amplitude (V), t = time (s; plotted and tabulated in s, ms, μs or ns, whichever the window fills), α = R/(2·L) (1/s), ωd = damped natural angular frequency (rad/s), ωn = undamped natural angular frequency (rad/s), ζ = damping ratio (dimensionless). Critically damped branch (ζ = 1): v_C(t) = V₀·[1 − e^(−α·t)·(1 + α·t)]. Source: Nilsson & Riedel, Electric Circuits, 10th ed., Ch. 8 (Step Response of a Series RLC Circuit)
When to Use This Calculator
- •Use the RLC Circuit Calculator to check your hand calculations on homework or exam problems — comparing its result with your own working helps identify arithmetic errors before they propagate.
- •Use it during the early design phase to rapidly iterate on parameters and narrow down feasible configurations before committing time to detailed finite element simulations or full design packages.
- •Use it when reviewing a colleague's calculation or checking a vendor's data sheet for plausibility — a quick sanity check can prevent costly downstream errors.
- •Use it to generate reference data for a technical report or presentation without manual computation, ensuring consistent, reproducible numbers throughout the document.
- •Use it in the field when a quick estimate is needed and a full engineering software package is not available.
About This Calculator
The RLC Circuit Calculator is a precision engineering calculation tool designed for students, engineers, and technical professionals. Step and sinusoidal response of series RLC circuits: natural frequency, damping ratio, Q factor, and bandwidth All calculations are performed using established engineering formulas from the relevant scientific literature and standards. Follow the units printed beside each field. Where a unit selector is provided, the selected unit is converted internally. Results are computed in your browser without sending data to a server, which keeps your inputs private. This calculator is intended as a supplementary tool for learning and design exploration; always verify results against authoritative references for safety-critical applications.
The Theory Behind It
A series RLC circuit contains a resistor, inductor, and capacitor in series, driven by a voltage source. Its natural behavior is determined by the damping ratio ζ and natural frequency ω_n, analogous to a mechanical spring-mass-damper system. Natural frequency ω_n = 1/√(LC). Damping factor α = R/(2L). Damping ratio ζ = α/ω_n = (R/2)·√(C/L). Three damping regimes: underdamped (ζ < 1, oscillatory response, most common), critically damped (ζ = 1, fastest non-oscillatory response), overdamped (ζ > 1, slow non-oscillatory return). For underdamped series RLC, the damped oscillation frequency is ω_d = ω_n·√(1−ζ²). Step response: oscillatory ring-down about final value for underdamped; exponential approach for critical and overdamped. Sinusoidal (steady-state) response: peak amplitude at resonance (ω = ω_n) for underdamped, lower and broader peak for higher damping. RLC circuits are the electrical equivalent of mechanical vibration systems, and the same math applies to both. They are used in signal filters, oscillators, antenna matching networks, and power conditioning. The calculator plots the step response and the response to a sinusoidal source at the resonant frequency, both starting from rest (no current, capacitor uncharged); at resonance the capacitor voltage settles to an amplitude of Q·V₀, 90° behind the source.
Real-World Applications
- •Tuned radio receivers: RLC tank circuits select specific radio frequencies from the broad spectrum picked up by the antenna.
- •Band-pass and band-stop filters: allow or block specific frequency ranges in audio and communication circuits.
- •Voltage regulator smoothing: RLC filtering reduces ripple in DC power supplies after rectification.
- •Crystal radio design: classical wireless radio uses a simple LC tank for tuning without amplification.
- •Transient voltage suppression: RLC circuits absorb voltage spikes and protect sensitive electronics.
Frequently Asked Questions
What is an RLC circuit?
An electrical circuit containing resistance R, inductance L, and capacitance C. These three elements represent dissipation, magnetic energy storage, and electric energy storage respectively. Series and parallel RLC circuits have different response characteristics but are both governed by the same ω_n, ζ, and damping regime concepts as mechanical oscillators.
What's the resonant frequency of an RLC circuit?
ω_r = 1/√(LC), or f_r = 1/(2π√(LC)) in Hz. At this frequency, inductive and capacitive reactances cancel, leaving only resistance. For L = 10 mH and C = 10 μF: f_r = 1/(2π·√(0.01·0.00001)) = 1/(2π·0.0003162) ≈ 503 Hz. At resonance, the circuit has minimum impedance (series) or maximum impedance (parallel).
What's Q for an RLC circuit?
For series RLC: Q = (1/R)·√(L/C) = ω_r·L/R. For parallel RLC: Q = R·√(C/L) = R/(ω_r·L). Q is the ratio of stored to dissipated energy per cycle, measuring how sharply tuned the circuit is. High Q (> 10) gives sharp frequency selectivity; low Q (< 1) gives broad response. Q also relates to the damping ratio: ζ = 1/(2Q).
When does an RLC circuit oscillate?
When underdamped (ζ < 1, equivalent to Q > 0.5). The natural frequency of oscillation is ω_d = ω_n·√(1−ζ²), slightly lower than ω_n. Overdamped circuits (ζ > 1) return to equilibrium without oscillation. Critically damped (ζ = 1) is the fastest non-oscillating response. Most filter designs are underdamped to provide frequency selectivity.
What's the step response of an underdamped RLC?
Oscillating decay about the steady-state value: v(t) = V_ss·(1 − e^(−αt)·(cos(ω_d·t) + (α/ω_d)·sin(ω_d·t))), where V_ss is the final voltage, α = R/(2L), and ω_d = √(ω_n² − α²). The oscillation period is 2π/ω_d, and the amplitude decays exponentially with time constant 1/α. Higher R (or lower L) means faster decay and less ringing.
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References & Further Reading
Wikipedia
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