An RC filter circuit, composed of a single resistor and capacitor, is a fundamental building block in electronics for shaping the frequency content of a signal. This simulator models both the low-pass (LP) and high-pass (HP) configurations. In the low-pass filter, the capacitor is placed in parallel with the output, allowing low-frequency signals to pass while attenuating high frequencies. Conversely, in the high-pass filter, the capacitor is in series with the input, blocking low frequencies and passing high ones. The core physics is governed by the complex impedance of the capacitor, Z_C = 1/(jωC), where ω is the angular frequency (ω = 2πf). Using voltage division, the transfer function H(ω) = V_out / V_in is derived. For a low-pass filter, H_LP(ω) = 1 / (1 + jωRC). The magnitude of this function, |H_LP| = 1 / √(1 + (ωRC)²), describes the gain. A key learning point is the cutoff frequency, f_c = 1/(2πRC), where the power delivered to a resistive load is halved, corresponding to a gain of 1/√2 or approximately −3 decibels (dB). The simulator visualizes this relationship on a Bode plot (gain in dB vs. log frequency) and shows live sine wave inputs and outputs, illustrating phase shifts introduced by the filter. Simplifications include ideal components (no parasitic inductance or resistance), a purely sinusoidal voltage source, and an assumption of an open-circuit (high-impedance) load to isolate the filter's intrinsic behavior. By interacting, students solidify concepts of AC circuit analysis, complex impedance, frequency-domain behavior, and the practical meaning of bandwidth and filtering.
Who it's for: Undergraduate physics or engineering students studying AC circuit theory, signal processing, or introductory electronics, as well as advanced high school students in AP Physics or similar courses.
Key terms
RC Circuit
Low-Pass Filter
High-Pass Filter
Cutoff Frequency
Bode Plot
Transfer Function
Attenuation
Decibel (dB)
Live graphs
How it works
A first-order RC stage acts as a low-pass (output across C) or high-pass (output across R). The magnitude rolls off at 20 dB/decade beyond the corner f_c = 1/(2πRC). At f_c, gain is 1/√2 ≈ −3.01 dB — the usual cutoff definition.
Why is the cutoff frequency defined at -3 dB, and what does that mean?
The -3 dB point, where the output voltage amplitude is 1/√2 (≈ 0.707) of the input, marks the frequency at which the power delivered to a resistive load is exactly half the maximum power. This is a standard engineering definition for the edge of a filter's passband. It represents a perceptible but not severe reduction in signal strength, making it a practical benchmark for bandwidth.
Can this simple RC filter completely block frequencies beyond the cutoff?
No. A first-order RC filter provides a gradual roll-off of -20 dB per decade of frequency. This means signals far above (for LPF) or below (for HPF) the cutoff are greatly attenuated but never fully eliminated. Sharper cutoffs require more complex, higher-order filters with multiple reactive components.
Where are RC filters used in real-world devices?
They are ubiquitous. Low-pass filters are found in audio systems to remove high-frequency noise (hiss) and in analog-to-digital converters to prevent aliasing. High-pass filters are used in audio crossovers to route bass to woofers and treble to tweeters, and in AC coupling circuits to block unwanted DC voltage offsets while passing the AC signal.
What is the phase shift shown between V_in and V_out, and why does it occur?
The capacitor's voltage and current are 90 degrees out of phase. This causes the filter to introduce a frequency-dependent phase shift. For a low-pass filter, the output lags the input by up to 90 degrees at high frequencies. This phase response is as critical as the amplitude response in applications like feedback control systems or audio processing, where timing relationships matter.