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Physics · Ch 4 — Electromagnetic Induction and Alternating Current

Quality Factor or Q-Factor

4.7.10

Quality Factor or Q-Factor

As a series RLC circuit reaches resonance and its current rises to the maximum value Im=Vm/RI_m=V_m/R, the individual voltages developed across L and across C both rise correspondingly, and in fact grow far larger than the applied source voltage itself. This magnification of the L and C voltages at series resonance is called the quality factor, or Q-factor, defined as the ratio of the voltage across L (or, equivalently, across C) at resonance, to the applied voltage:

Q-factor=Voltage across L or C at resonanceApplied voltageQ\text{-factor} = \dfrac{\text{Voltage across L or C at resonance}}{\text{Applied voltage}}

Since the circuit is purely resistive at resonance, the applied voltage there equals the voltage across R, so

Q=XLImRIm=XLR=ωrLR(4.52)Q = \dfrac{X_L I_m}{R I_m} = \dfrac{X_L}{R} = \dfrac{\omega_r L}{R} \qquad (4.52)

Substituting ωr=1/LC\omega_r=1/\sqrt{LC} gives the more commonly quoted form,

Q=1RLC(4.53)Q = \dfrac{1}{R}\sqrt{\dfrac{L}{C}} \qquad (4.53) …

Misc Example 4.23Resonant frequency and Q-factor of a given series RLC circuit

Worked out. A series RLC circuit has a 500 μ\muH inductor, an 80π2\dfrac{80}{\pi^2} pF capacitor and a 628 Ω\Omega resistor, and the resonant frequency and Q-factor are required. The resonant frequency is fr=12πLCf_r=\dfrac{1}{2\pi\sqrt{LC}}; substituting the given L and C and simplifying the resulting expression gives fr≈2500f_r\approx2500 kHz. The Q-factor is Q=ωrL/R=2πfrL/R=(2π)(2500×103)(500×10−6)/628≈12.5Q=\omega_r L/R = 2\pi f_r L/R = (2\pi)(2500\times10^3)(500\times10^{-6})/628 \approx12.5. The example is a direct, two-formula numerical drill applying both the resonant-frequency and Q-factor formulas to the sa …

Misc Example 4.26Q-factor before and after doubling the inductance at fixed resonant frequency

Worked out. A series RLC circuit resonating at 400 kHz has an 80 μ\muH inductor, a 2000 pF capacitor and a 50 Ω\Omega resistor, and the questions ask for (i) the initial Q-factor, (ii) the new capacitance needed to keep the SAME 400 kHz resonant frequency if the inductance is doubled to 160 μ\muH, and (iii) the new Q-factor with these doubled-L, adjusted-C values. (i) Q=1RL/C=150(80×10−6)/(2000×10−12)=4Q=\dfrac{1}{R}\sqrt{L/C} = \dfrac{1}{50}\sqrt{(80\times10^{-6})/(2000\times10^{-12})} = 4. (ii) Keeping frf_r fixed while L doubles requires C2=1/(4π2fr2L2)C_2=1/(4\pi^2f_r^2L_2), which works out to C2≈1000C_2\approx1000 pF -- exactly HALF the original capacitance, as expected since fr∝1/LCf_r\propto1/\sqrt{LC} requires the LC product to stay constant. (iii) The new Q-factor is Q2=1RL2/C2=150(160×10−6)/(1000×10−12)=8Q_2=\dfrac{1}{R}\sqrt{L_2/C_2}=\dfrac{1}{50}\sqrt{(160\times10^{-6})/(1000\times10^{-12})}=8 -- exactly DOUBLE the original Q-factor, showing that doubling L while halving C (to keep …