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Free Class-AB Amplifier Bias & Vbe Multiplier Tool Electronics & Embedded
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Free Class-AB Amplifier Bias & Vbe Multiplier Tool

Size Vbe multiplier transistor bias networks ($V_{bias} = V_{BE} (1 + R_1/R_2)$), eliminate crossover distortion, and calculate quiescent current ($I_q$) per Oliver criteria.

🔊 Output Stage Topology & Supply

V
±45V ≈ 100W into 8Ω
Ω
Ballast resistor (0.22 – 0.47 Ω)
mA
Oliver criterion ~26mV / R_E
V_be Multiplier Resistor Network
Ω
Fixed lower resistor
V
Sense transistor V_BE

📊 Bias Voltages & Power Dissipation

Total Bias Spread (V_bias)
-- V
Drop across 2×R_E: -- mV
Idle Power (per pair)
-- W
Heatsink load at idle
V_be Multiplier Component Tuning
Upper Resistor / Trimmer (R_1): -- Ω
Trimmer Sizing (500Ω - 5kΩ): Use -- potentiometer
Oliver Optimum Quiescent Current: -- mA optimal
Class-AB bias voltage and thermal feedback tracking verified.

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Class-AB Audio Power Amplifier Biasing & Oliver's Criterion

In a complementary push-pull audio amplifier, pure Class-B operation results in audible crossover distortion because both NPN and PNP output transistors remain non-conductive when the audio waveform passes through zero volts ($pm 0.6 ext{V}$ dead zone).

The V_be Multiplier ("Rubber Diode") Circuit

To maintain a slight quiescent idle current ($I_q$) through the output devices, an adjustable voltage reference called a $V_{BE}$ multiplier is placed between the driver bases: $$V_{bias} = V_{BE,mult} \cdot \left( 1 + \frac{R_1}{R_2} \right)$$ Mounting this multiplier transistor directly onto the main output heatsink ensures thermal negative feedback: as the power transistors heat up, the sense transistor also heats up, dropping $V_{bias}$ at approximately $-2.0 ext{ mV}/^circ ext{C}$ per junction, preventing destructive thermal runaway.

Oliver's Optimal Biasing Rule

Distortion pioneer Douglas Self and Bernard Oliver demonstrated that there is an exact optimal voltage drop across the emitter ballasting resistors ($R_E$) that minimizes gain doubling and transition ripple: $$V_{RE,opt} \approx 26\text{ mV} \implies I_{q,opt} = \frac{26\text{ mV}}{R_E}$$ For a standard $R_E = 0.22\,\Omega$, the optimal quiescent current is approximately $118\text{ mA}$ (or $\sim 26\text{ mV}$ across both resistors combined for CFPs).

Frequently Asked Questions

Why should I never over-bias a Class-AB amplifier into high idle current?

Counter-intuitively, excessive bias does not reduce distortion; it causes "gm-doubling" distortion where both output transistors conduct simultaneously during small signals, creating higher total harmonic distortion (THD) than correctly biased optimal Class-AB operation.

Why are emitter resistors (RE) mandatory in BJT output stages?

BJT collector current increases exponentially with temperature. Emitter resistors provide local negative current feedback (degenerative feedback): as current rises, the voltage drop across RE increases, reducing the net V_BE drive voltage and preventing thermal runaway and current hogging in parallel output pairs.

What capacitor should be placed across the Vbe multiplier?

A 100nF to 1uF film or ceramic capacitor is wired directly across the collector-emitter of the multiplier transistor to bypass AC audio currents and prevent the multiplier from acting as an inductive impedance at high audio frequencies.