RLC Circuit Resonance Simulator

The core of resonance is the impedance of the series RLC circuit. At any frequency, the total impedance Z is the sum of the resistance and the two reactances. Since the inductive reactance ($X_L$) and capacitive reactance ($X_C$) have opposite signs, they can cancel.

$Z$ is the complex impedance (Ω), $R$ is the resistance (Ω), $\omega$ is the angular frequency (rad/s), $L$ is the inductance (H), and $C$ is the capacitance (F). Resonance occurs when the imaginary part is zero.

From the impedance condition, we derive the key resonant frequency. The bandwidth (BW) defines the range of frequencies around resonance where the power is at least half the maximum, and is inversely related to the Q factor.

$\omega_0$ is the resonant angular frequency. $Q$ is the quality factor (dimensionless). BW is the bandwidth (rad/s). A high Q means a narrow, selective resonance, which is crucial for filters.

In an RLC circuit the inductive reactance $X_L=\omega L$ and capacitive reactance $X_C=1/(\omega C)$ vary with frequency. The frequency where they are equal ($X_L=X_C$) is the resonant frequency.

$X_L=X_C \;\Rightarrow\; \omega_0=\dfrac{1}{\sqrt{LC}}, \qquad f_0=\dfrac{1}{2\pi\sqrt{LC}}$

The series impedance is $Z=\sqrt{R^2+(X_L-X_C)^2}$; at resonance the reactances cancel, giving $Z=R$ (minimum) and maximum current. The simulator shows the variation of $Z$, current, and phase with frequency and the resonant point in real time.

The Q factor is a dimensionless measure of how sharp (selective) the resonance is — higher Q means a sharper, narrower peak.

The smaller $R$, the higher the Q and the narrower the band. An AM radio tuning circuit uses a high Q to select a single station; applications needing a wide band lower the Q.

Both have the same resonant frequency $f_0=1/(2\pi\sqrt{LC})$, but their impedance and current behave oppositely. Filter design chooses series or parallel depending on whether a frequency should be passed or blocked.

Radio Tuners: Your radio selects a station by using a tunable RLC circuit (often with a variable capacitor). It resonates at the frequency of the desired radio station, allowing that signal's current to be maximized while rejecting others. The simulator's sharp peak shows this selectivity.

RF/Microwave Filters: In cell phones and WiFi routers, RLC-based bandpass and bandstop filters are essential. They allow specific frequency bands for communication while blocking interference. Engineers use CAE tools to simulate the Q factor and bandwidth exactly as this simulator does.

Antenna Impedance Matching: Antennes are designed to resonate at their operating frequency for efficient power transfer. An RLC matching network ensures the antenna's complex impedance looks purely resistive to the transmitter, minimizing reflected power.

EMC/Noise Suppression: Unwanted resonant circuits can form on printed circuit boards (PCBs) from parasitic inductance and capacitance. CAE software performs parasitic extraction to find these and predict electromagnetic compatibility (EMC) issues, using the same resonance principles shown here.

First, are you under the impression that "the resonant frequency is determined solely by L and C"? It's true that the formula $f_0 = 1 / (2\pi\sqrt{LC})$ does not include the resistance R. However, real-world components always have parasitic elements known as "Equivalent Series Resistance (ESR)". Examples include the winding resistance of a coil or the dielectric loss of a capacitor. If you set the simulator to approach an ideal R=0Ω, the peak impedance theoretically diverges to infinity, which is impossible in a real circuit. In practice, this parasitic resistance determines the Q factor and directly impacts heat generation and efficiency.

Next, it's dangerous to think "series and parallel resonance are simply inverses". In series resonance, the impedance is at a "minimum," resulting in maximum current. In parallel resonance, however, the impedance is at a "maximum," resulting in maximum voltage. If you design a filter without understanding this fundamental difference, it will behave in a completely unintended way. For example, using parallel resonance as a noise filter on a power line makes the impedance maximum at a specific noise frequency, thereby blocking that noise (trap filter). Try switching between both modes in this simulator and observe how the graph shape inverts.

Finally, the discrepancy between simulation and actual measurement. Calculations on paper or results from this tool assume a "lumped-element circuit." However, especially at high frequencies (e.g., tens of MHz and above), wiring length becomes non-negligible compared to the wavelength, and distributed-element effects appear. Furthermore, the influence of parasitic capacitance and mutual inductance between components cannot be ignored. Even if you obtain perfect characteristics in the tool, it's not uncommon for the resonant frequency to shift by a few percent on an actual printed circuit board. Always consider "theoretical values as a first approximation" and plan real-world evaluation as an essential step.