Calculate bandwidth, Q factor, and cutoff frequencies for resonant circuits and filters. Frequency response table, RLC values, and selectivity analysis.
Bandwidth is the range of frequencies over which a resonant circuit or filter responds within a specified attenuation — typically the −3 dB (half-power) points. For a resonator with center frequency f₀ and quality factor Q, the bandwidth is BW = f₀/Q. Higher Q means narrower bandwidth and sharper selectivity.
The quality factor Q represents the ratio of energy stored to energy dissipated per cycle. In an RLC circuit, Q = ω₀L/R (series) or Q = R/(ω₀L) (parallel). Q determines how "peaky" the resonance is: a Q of 10 is broad, a Q of 1000 is narrow, and quartz crystals achieve Q values above 100,000.
This calculator converts between center frequency, bandwidth, and Q factor using any two of the three as input. It also computes RLC component values for a given impedance, provides a frequency response table showing gain vs frequency offset, and compares selectivity across a range of Q values.
Bandwidth calculations involve conversions between Q factor, center frequency, and cutoff frequencies, plus RLC component sizing for a given impedance. The relationships between these quantities are straightforward but involve multiple formulas and unit conversions.
This calculator provides instant conversion between all three representations (Q, bandwidth, cutoff frequencies), computes the required L and C for a series RLC realization, and includes a frequency response table showing attenuation at various offsets from center. The Q comparison table helps understand how selectivity changes with quality factor.
BW = f₀/Q. Q = f₀/BW. f₀ = √(f_L × f_H). BW = f_H − f_L. For series RLC: L = ZQ/ω₀, C = 1/(ω₀²L). Fractional BW = BW/f₀ × 100%.
Result: Bandwidth = 2 MHz, f_L = 99 MHz, f_H = 101 MHz
BW = f₀/Q = 100 MHz / 50 = 2 MHz. The −3 dB points are at f₀ ± BW/2 = 99 MHz and 101 MHz. Fractional bandwidth = 2%.
The quality factor spans an enormous range across different technologies. A simple RC circuit has Q < 1 (overdamped). Air-core inductors typically achieve Q of 50-300 at RF frequencies. Ferrite-core inductors reach Q of 100-500 but suffer from core losses at high frequencies. Ceramic resonators (used in IF filters) have Q around 1000-5000.
Quartz crystals are exceptional: Q values of 50,000-200,000 are common, and specially cut crystals in vacuum reach 2 million. This is why crystal oscillators are used as frequency standards. At optical frequencies, Fabry-Pérot cavities with dielectric mirrors achieve Q values exceeding 10¹¹, enabling ultra-precise spectroscopy and laser stabilization.
Superconducting microwave cavities set the record at Q > 10¹¹, used in particle accelerators and quantum computing. These cavities have essentially zero resistance, so the only losses are from surface currents and dielectric absorption.
The bandwidth of a communication channel fundamentally limits its data-carrying capacity. Shannon's channel capacity theorem states C = BW × log₂(1 + S/N), where S/N is the signal-to-noise ratio. A 20 MHz Wi-Fi channel with 30 dB SNR supports about 200 Mbps theoretical maximum.
Modern communication systems use wide bandwidths to achieve high data rates: 5G NR uses up to 100 MHz bandwidth below 6 GHz and up to 400 MHz in millimeter-wave bands. Fiber optic systems use the enormous bandwidth of the optical spectrum — a single fiber can carry over 100 Tbps by using wavelength-division multiplexing across ~5 THz of bandwidth.
In practice, simple second-order (single RLC) filters are rarely sufficient. Real filters use higher-order designs: Butterworth (maximally flat passband), Chebyshev (steeper rolloff with ripple), Elliptic (steepest rolloff with ripple in both pass and stop bands), and Bessel (maximally flat group delay for minimal signal distortion). The order of the filter determines the ultimate rolloff rate: −20 dB/decade per order (−6 dB/octave per order).
Q (quality factor) is the ratio of energy stored to energy dissipated per radian of oscillation: Q = 2π × (stored energy)/(energy lost per cycle). Higher Q means less loss, sharper resonance, and narrower bandwidth. A tuning fork has Q ~ 1000; a quartz crystal Q ~ 100,000; an optical cavity Q ~ 10⁹.
The −3 dB points are where the power response drops to half maximum (0.707 of peak voltage). This is the standard definition of bandwidth for resonant circuits. At these frequencies, the impedance of the reactive components equals the resistance (for RLC circuits).
Bandwidth determines data throughput: Shannon's theorem states channel capacity C = BW × log₂(1 + SNR). A wider bandwidth carries more information. For example, a 20 MHz Wi-Fi channel supports higher data rates than a 1 MHz AM radio channel.
Fractional bandwidth = BW/f₀ × 100%. A 2 MHz bandwidth at 100 MHz is 2% fractional. At 2.4 GHz, the same 2% fractional bandwidth would be 48 MHz. Fractional bandwidth is useful for comparing filters at different frequencies.
Reduce losses: use lower-resistance inductors (Litz wire, silver-plated, larger gauge), higher-Q capacitors (mica, ceramic C0G), and minimize radiation losses. At microwave frequencies, cavity resonators achieve very high Q by confining fields in conductive enclosures.
A bandpass filter transmits frequencies near f₀ and attenuates others. A band-stop (notch) filter does the opposite: it rejects frequencies near f₀ and passes others. Both are characterized by the same f₀, Q, and bandwidth — only the pass/reject behavior is inverted.