8.3 Multistage Amplifiers, Frequency Response & Power Amplifiers

Key Takeaways

  • Multistage coupling schemes include Direct Coupling (DC to high frequency, zero cutoff), RC Coupling (DC blocking, standard for audio), and Transformer Coupling (impedance matching, max power transfer, limited bandwidth).
  • The low-frequency response limit is dictated by external coupling/bypass capacitors (f_L = \frac{1}{2\pi R_{Th} C}), whereas high-frequency cutoff is limited by parasitic junction capacitances magnified by the Miller Effect: C_{M1} = C_{bc}(1 - A_v).
  • Amplifier bandwidth is BW = f_H - f_L; cascading N non-interacting identical stages reduces overall bandwidth according to BW_N = BW_1 \sqrt{2^{1/N} - 1}.
  • Power amplifier classes are defined by conduction angle: Class A (360°, max efficiency 25% direct / 50% transformer), Class B (180°, max efficiency 78.5%, push-pull crossover distortion), Class AB (eliminates crossover distortion), Class C (<180°, efficiency >80%, tuned RF), Class D (>90%, switching/PWM).
  • Total Harmonic Distortion (THD) quantifies output signal non-linearity: THD = \frac{\sqrt{V_2^2 + V_3^2 + \dots + V_n^2}}{V_1} \times 100\%.
Last updated: July 2026

8.3 Multistage Amplifiers, Frequency Response & Power Amplifiers

1. Multistage Cascaded Amplifiers & Interstage Coupling

Single-stage amplifiers rarely provide sufficient voltage gain, input impedance, and output driving capability simultaneously. Multiple amplifier stages are cascaded in series, where the output of stage $n$ feeds the input of stage $n+1$.

Stage Loading Effects & Total Gain

When cascading stages, the input impedance of stage 2 ($Z_{in2}$) acts as a parallel AC load on stage 1 ($Z_{out1} \parallel R_{C1} \parallel Z_{in2}$).

  • Total Voltage Gain:

AvT=Av1×Av2×Av3××AvnA_{vT} = A_{v1} \times A_{v2} \times A_{v3} \times \dots \times A_{vn}

  • Gain in Decibels ($dB$):

AvT,dB=20log10AvT=Av1,dB+Av2,dB++Avn,dBA_{vT,dB} = 20 \log_{10}|A_{vT}| = A_{v1,dB} + A_{v2,dB} + \dots + A_{vn,dB}

Interstage Coupling Methods

Coupling MethodLow-Frequency ResponseDC Blocking capabilityImpedance MatchingRelative Cost & SizePrimary Application
Direct CouplingExcellent (Down to $0\text{ Hz}$ / DC)No (DC drift propagates)PoorLow, Compact ICsOp-amps, DC instrumentation
RC CouplingLimited by $C_C$ ($f_L > 0$)Yes (Blocks DC bias)FairLow cost, SmallAudio preamplifiers, General AC
Transformer CouplingPoor (Blocks DC & sub-audio)YesExcellent ($N_1/N_2 = \sqrt{Z_1/Z_2}$)High cost, BulkyRF power amplifiers, Impedance matching

2. Frequency Response & Decibel Analysis

Decibel Fundamentals

  • Voltage Gain in dB: $A_{v,dB} = 20 \log_{10}\left|\frac{V_o}{V_i}\right|$
  • Power Gain in dB: $A_{p,dB} = 10 \log_{10}\left|\frac{P_o}{P_i}\right|$
  • Half-Power (-3 dB) Cutoff Points: At frequencies $f_L$ and $f_H$, voltage gain drops to $\frac{1}{\sqrt{2}} \approx 0.707$ ($70.7%$) of midband gain $A_{mid}$, and power drops to $50%$.

Low-Frequency Response ($f_L$)

Determined by coupling capacitors ($C_S, C_C$) and emitter/source bypass capacitors ($C_E, C_S$). Each RC network introduces a lower cutoff frequency:

fL=12πRThCf_L = \frac{1}{2\pi R_{Th} C}

  • The dominant lower cutoff frequency is the largest value among all lower cutoff frequencies ($f_{L,dom} = \max(f_{L1}, f_{L2}, f_{LE})$).

High-Frequency Response ($f_H$) & The Miller Effect

Determined by internal transistor parasitic junction capacitances ($C_{be}, C_{bc}$ in BJTs; $C_{gs}, C_{gd}$ in FETs) and stray wiring capacitance ($C_w$).

Miller Effect Theorem

For an inverting amplifier with voltage gain $-A_v$ and feedback capacitance $C_f$ ($C_{bc}$ or $C_{gd}$):

  • Input Miller Capacitance:

CM1=Cbc(1Av)=Cbc(1+Av)C_{M1} = C_{bc} (1 - A_v) = C_{bc} (1 + |A_v|)

  • Output Miller Capacitance:

CM2=Cbc(11Av)CbcC_{M2} = C_{bc} \left( 1 - \frac{1}{A_v} \right) \approx C_{bc}

  • Total Input High-Frequency Capacitance:

Cin,hi=Cwi+Cbe+CM1C_{in,hi} = C_{wi} + C_{be} + C_{M1}

  • Upper Cutoff Frequency ($f_H$):

fH=12πRTh,hiCin,hif_H = \frac{1}{2\pi R_{Th,hi} C_{in,hi}}

  • The dominant upper cutoff frequency is the smallest value ($f_{H,dom} = \min(f_{H1}, f_{H2})$).

Bandwidth & Gain-Bandwidth Product

  • Bandwidth: $BW = f_H - f_L \approx f_H$ (since $f_H \gg f_L$).
  • Gain-Bandwidth Product ($GBW$): Constant for a given transistor amplifier stage.

GBW=Av,mid×BW=fTGBW = A_{v,mid} \times BW = f_T

Where $f_T$ is the transition frequency at which short-circuit current gain drops to unity ($0\text{ dB}$).

  • Multistage Bandwidth Shrinkage (N identical non-interacting stages):

fL(overall)=fL21/N1,fH(overall)=fH21/N1f_{L(overall)} = \frac{f_L}{\sqrt{2^{1/N} - 1}}, \quad f_{H(overall)} = f_H \sqrt{2^{1/N} - 1}


3. Large-Signal Power Amplifiers

Power amplifiers operate over large portions of the transistor's characteristic curves to deliver maximum AC power to a load (e.g., loudspeaker, antenna).

Summary of Power Amplifier Classes

ClassConduction Angle ($\theta$)Q-Point LocationTheoretical Max Efficiency ($\eta_{max}$)Primary Distortion CharacteristicPrimary Applications
Class A$360^\circ$ ($2\pi$)Center of AC Load Line$25%$ (Direct) / $50%$ (Transformer)Low non-linear distortionHigh-fidelity audio preamps
Class B$180^\circ$ ($\pi$)At Cutoff ($I_{CQ} = 0$)$\frac{\pi}{4} \approx 78.5%$Crossover Distortion near zero-crossingPush-pull audio power stages
Class AB$180^\circ < \theta < 360^\circ$Slightly above Cutoff$50% - 78.5%$Eliminates crossover distortionStandard audio power amplifiers
Class C$< 180^\circ$ ($80^\circ - 120^\circ$)Deep in Cutoff region$> 80%$High harmonic distortion (Requires LC tank)RF Transmitters, Tuned Amplifiers
Class D$360^\circ$ (Switching PWM)Switches between Cutoff & Saturation$> 90% - 95%$Requires LPF to reconstruct analog audioHigh-efficiency audio, Subwoofers

Class B / AB Push-Pull Power Calculations

  • Maximum AC Output Power:

Po,max=VCC22RLP_{o,max} = \frac{V_{CC}^2}{2 R_L}

  • DC Input Power:

Pdc=VCCIdc=VCC(2Ipπ)=2VCCVpπRLP_{dc} = V_{CC} \cdot I_{dc} = V_{CC} \left( \frac{2 I_p}{\pi} \right) = \frac{2 V_{CC} V_p}{\pi R_L}

  • Maximum Efficiency:

ηmax=Po,maxPdc,max=π478.54%\eta_{max} = \frac{P_{o,max}}{P_{dc,max}} = \frac{\pi}{4} \approx 78.54\%

  • Maximum Power Dissipation Per Transistor ($P_{D,max}$): Occurs at $V_p = \frac{2}{\pi} V_{CC} \approx 0.636 V_{CC}$:

PD,max=VCC2π2RLP_{D,max} = \frac{V_{CC}^2}{\pi^2 R_L}

Harmonic Distortion & Thermal Management

  • Total Harmonic Distortion (THD):

THD=V22+V32+V42++Vn2V1×100%THD = \frac{\sqrt{V_2^2 + V_3^2 + V_4^2 + \dots + V_n^2}}{V_1} \times 100\%

  • Thermal Resistance & Derating: Junction temperature $T_J$ must not exceed maximum limit ($150^\circ\text{C} - 200^\circ\text{C}$):

TJTA=PD(θJC+θCS+θSA)T_J - T_A = P_D (\theta_{JC} + \theta_{CS} + \theta_{SA})

Where $\theta_{JC}$ is junction-to-case, $\theta_{CS}$ is case-to-heatsink, and $\theta_{SA}$ is heatsink-to-ambient thermal resistance ($^\circ\text{C/W}$).

Loading diagram...
Class B Complementary-Symmetry Push-Pull Power Amplifier
Theoretical Maximum Conversion Efficiency across Power Amplifier Classes
Test Your Knowledge

A Common Emitter BJT amplifier stage has a voltage gain of A_v = -120 and a collector-base capacitance of C_bc = 4 pF. Calculate the input Miller capacitance C_M1.

A
B
C
D
Test Your Knowledge

Four identical non-interacting amplifier stages, each having an upper cutoff frequency of f_H = 100 kHz, are cascaded. What is the overall upper cutoff frequency f_H(overall) of the multistage amplifier?

A
B
C
D
Test Your Knowledge

A Class B complementary-symmetry push-pull power amplifier operates with V_CC = 24 V and drives an 8 Ω speaker load. Determine the maximum theoretical power delivered to the load P_o,max and the maximum power dissipated by each transistor P_D,max.

A
B
C
D