Power amplifiers and linear voltage regulators
Power amplifier classes A, B, AB, C and D, Class B power and dissipation, crossover distortion, and series linear regulators with dropout, efficiency and current limiting.
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Why it matters
Instruments must drive real loads, such as actuators, valve positioners, loudspeakers and long cables, and every analog circuit in them needs clean, stable supply rails. Power amplifiers are judged by how much of the supply power reaches the load and how much becomes heat; linear regulators turn a rippling, drifting rectifier output into the quiet DC that precision analog circuits need, at the cost of dissipating the difference.
Key ideas
Classes of operation (by the fraction of the cycle each output device conducts):
- Class A: conducts for the full 360°. Biased at mid-supply, very linear, but draws full current even with no signal. Maximum efficiency 25 % with a resistive (series-fed) load, 50 % with a transformer- or inductor-coupled load.
- Class B: each device conducts for 180°. A complementary push-pull pair (npn pushes, pnp pulls) shares the cycle; with no signal there is no quiescent current, so efficiency is high: up to π/4 = 78.5 %.
- Class AB: each device conducts for slightly more than 180°. Two diodes (or a V_BE multiplier) between the bases pre-bias both transistors at the edge of conduction, eliminating the crossover distortion that Class B shows near zero crossings, where neither transistor conducts until the input exceeds about ±0.6 V. Efficiency is close to Class B; this is the usual audio output stage.
- Class C: conducts for less than 180°. Very efficient, but only usable with a tuned (LC) load at radio frequencies.
- Class D: the output devices switch fully on or off with pulse-width modulation, and an LC filter recovers the signal. Efficiency above 90 %.
Class B power balance. With ±V_CC supplies, load R_L and output peak V_p, the load receives V_p²/(2R_L) while the supplies deliver 2V_CC·V_p/(πR_L), so efficiency rises linearly with V_p. Transistor dissipation is not largest at full output: it peaks at V_p = 2V_CC/π, where total device dissipation is 2V_CC²/(π²R_L), about 40 % of the maximum output power (20 % per transistor). Heat sinks are sized from this figure.
Thermal runaway. In a BJT stage, rising temperature lowers V_BE and raises current, which raises temperature further. Class AB stages use small emitter resistors and thermally coupled bias diodes to prevent it.
Linear (series) regulator. Four blocks: a stable reference (Zener or bandgap), a sampling divider R₁–R₂ on the output, an error amplifier comparing the two, and a series pass transistor that drops the excess voltage. Negative feedback holds the sampled output equal to the reference, so V_o = V_ref(1 + R₁/R₂). Protection includes current limiting (a sense resistor that turns on a transistor at about 0.6–0.7 V) and thermal shutdown.
Dropout and efficiency. The pass device needs a minimum input-output difference, the dropout voltage: about 2 V for a classic 78xx regulator, as low as 0.1–0.3 V for a low-dropout (LDO) regulator. Efficiency is roughly V_o/V_in and the pass device dissipates (V_in − V_o)·I_L, so linear regulators are best for small headroom or low current, while switching regulators handle large step-downs efficiently but add switching noise.
Three-terminal regulators. Fixed types (78xx positive, 79xx negative) and adjustable types (LM317) hold a fixed reference voltage (1.25 V for the LM317, from its datasheet) between OUT and ADJ.
Formulas
η = P_out / P_dc — efficiency (P in W).
η_max = 25 % (Class A, resistive load), 50 % (Class A, transformer-coupled), π/4 = 78.5 % (Class B).
P_out = V_p² / (2·R_L) — sinusoidal output power (W); V_p peak output (V).
P_dc = 2·V_CC·V_p / (π·R_L) — Class B push-pull, supplies ±V_CC.
η = (π/4)·(V_p / V_CC) — Class B efficiency at any amplitude.
P_out(max) = V_CC² / (2·R_L), P_D,total(max) = 2·V_CC² / (π²·R_L) at V_p = 2V_CC/π.
V_o = V_ref·(1 + R₁/R₂) — series regulator; R₁ top, R₂ bottom of the sampling divider.
V_o = 1.25 V·(1 + R₂/R₁) + I_ADJ·R₂ — LM317-type adjustable regulator (I_ADJ ≈ 50 µA, often neglected).
P_pass = (V_in − V_o)·I_L, η ≈ V_o / V_in — linear regulator.
I_limit ≈ V_BE / R_sc ≈ 0.7 V / R_sc — current-limit threshold.
Worked examples
Example 1 (standard: Class B). A complementary push-pull Class B stage runs from ±20 V into 8 Ω and delivers a 16 V peak sine. Find P_out, P_dc, efficiency and the dissipation per transistor. What is the worst-case total device dissipation?
P_out = V_p²/(2R_L)= 256/16 = 16 W.P_dc = 2V_CC·V_p/(πR_L)= 2 × 20 × 16/(π × 8) = 25.5 W.η= 16/25.5 = 62.8 % (check: (π/4)(16/20) = 62.8 %).- Device dissipation = 25.5 − 16 = 9.5 W total, 4.7 W per transistor.
- Worst case:
P_D,total(max) = 2V_CC²/(π²R_L)= 800/(9.87 × 8) = 10.1 W (5.1 W each), at V_p = 12.7 V.
Answer: P_out = 16 W, P_dc ≈ 25.5 W, η ≈ 62.8 %, 4.7 W per transistor; worst case 10.1 W total.
Example 2 (GATE level: series regulator). An op-amp series regulator uses a 5.1 V Zener reference and a sampling divider R₁ = R₂ = 10 kΩ. The input is 15 V and the load draws 0.5 A. A 1.2 Ω current-sense resistor sets the limit. Find V_o, pass-transistor dissipation, efficiency and the current limit. Also find the output of an LM317 with R₁ = 240 Ω and R₂ = 720 Ω.
V_o = V_ref(1 + R₁/R₂)= 5.1 × 2 = 10.2 V.P_pass = (V_in − V_o)·I_L= (15 − 10.2) × 0.5 = 2.4 W.η ≈ V_o/V_in= 10.2/15 = 68 %.I_limit ≈ 0.7/R_sc= 0.7/1.2 = 0.58 A.- LM317:
V_o = 1.25(1 + 720/240)= 1.25 × 4 = 5.0 V (I_ADJ neglected).
Answer: V_o = 10.2 V, P_pass = 2.4 W, η ≈ 68 %, I_limit ≈ 0.58 A; LM317 output 5.0 V.
Common mistakes
- Using 78.5 % as the efficiency at any output level; it applies only at full swing (V_p = V_CC).
- Assuming transistor dissipation is greatest at maximum output; it peaks at V_p = 2V_CC/π.
- Mixing peak and rms values in P = V²/R.
- Calling the input-output difference the dropout voltage; dropout is the minimum difference the regulator needs.
- Writing V_o = V_ref·R₁/R₂ instead of V_ref(1 + R₁/R₂).
- Forgetting crossover distortion when a Class B stage has no bias network.
For GATE IN
Expect efficiency, output power and dissipation numericals for Class A and Class B stages, the conduction angle of each class, crossover distortion, and series-regulator questions: output voltage from a reference and divider, pass-device dissipation, current limiting and LM317 settings. Practise the Class B power equations until you can find the dissipation peak without notes.
Quick check
- A Class B stage has V_CC = 12 V and V_p = 6 V. Efficiency?
- Maximum efficiency of a series-fed Class A amplifier?
- A 5 V regulator runs from 9 V at 0.3 A. Pass-device dissipation?
- Conduction angle of a Class AB output transistor?
Answers: 1. About 39.3 %. 2. 25 %. 3. 1.2 W. 4. Slightly more than 180° (less than 360°).
Interview questions
All Analog Electronics interview questionsTry answering each one aloud before you open it.
1.What is a power amplifier and what are its main functions?Concept
A power amplifier is an electronic device that increases the power of a signal. Its main function is to take a low-power input signal and produce a higher-power output signal, which can drive loads like speakers or antennas. Power amplifiers are essential in applications where the signal needs to be transmitted over long distances or to drive high-power devices.
2.Explain the difference between Class A, Class B, and Class AB power amplifiers.Concept
Class A amplifiers conduct over the entire input cycle, providing high linearity but low efficiency. Class B amplifiers conduct for half of the input cycle, offering better efficiency but introducing crossover distortion. Class AB amplifiers combine the two, conducting for more than half but less than the full cycle, balancing efficiency and linearity.
3.What is a linear voltage regulator and how does it work?Concept
A linear voltage regulator is a device that maintains a constant output voltage regardless of changes in input voltage or load conditions. It works by using a variable resistor (transistor) to drop excess voltage, dissipating it as heat, and providing a stable output voltage. Linear regulators are simple and provide low noise output but are less efficient than switching regulators.
4.Why are heat sinks used in power amplifiers?Application
Heat sinks are used in power amplifiers to dissipate excess heat generated during operation. Power amplifiers can produce significant heat due to high power levels, and without proper heat dissipation, this can lead to thermal runaway and damage the device. Heat sinks increase the surface area for heat dissipation, helping to maintain safe operating temperatures.
5.What happens if a linear voltage regulator is used with an input voltage close to its dropout voltage?Application
If a linear voltage regulator is used with an input voltage close to its dropout voltage, it may not be able to maintain a stable output voltage. The dropout voltage is the minimum difference between input and output voltage required for the regulator to function properly. Operating near this limit can lead to output voltage fluctuations and instability.
6.Why might a designer choose a Class D amplifier over a Class A amplifier?Application
A designer might choose a Class D amplifier over a Class A amplifier due to its higher efficiency. Class D amplifiers use pulse-width modulation to achieve efficiencies greater than 90%, making them ideal for battery-powered devices and applications where heat dissipation is a concern. In contrast, Class A amplifiers, while offering high linearity, are much less efficient and generate more heat.
7.Explain the concept of thermal runaway in power amplifiers.Concept
Thermal runaway in power amplifiers occurs when an increase in temperature causes a further increase in power dissipation, leading to even higher temperatures. This positive feedback loop can result in the destruction of the amplifier if not controlled. It is often managed by using heat sinks, thermal shutdown circuits, or biasing techniques to stabilize the temperature.
8.Calculate the power dissipation in a linear voltage regulator with an input voltage of 12 V, output voltage of 5 V, and output current of 1 A.Numerical
Power dissipation (P) in a linear voltage regulator can be calculated using the formula P = (Vin - Vout) × Iout. Here, Vin = 12 V, Vout = 5 V, and Iout = 1 A. So, P = (12 V - 5 V) × 1 A = 7 W. The regulator dissipates 7 watts of power as heat.
9.A complementary Class B push-pull amplifier runs from ±20 V supplies and drives an 8 Ω load. Calculate the maximum output power.Numerical
Maximum output occurs when the output swings to the rails, V_p ≈ V_CC = 20 V (ignoring saturation drops). P_max = V_p²/(2R_L) = 400/16 = 25 W. At this point efficiency is the theoretical π/4 = 78.5 %, so the supplies deliver about 31.8 W. In practice the swing is a volt or two short of the rails, so the real maximum is a little lower.
10.What are the advantages and disadvantages of using a linear voltage regulator compared to a switching regulator?Application
Linear voltage regulators are simple, provide low noise output, and have fast transient response. However, they are less efficient, especially with large input-output voltage differences, as they dissipate excess voltage as heat. Switching regulators, on the other hand, are more efficient and can handle larger voltage differences, but they are more complex and can introduce switching noise into the output.
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