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AExE0106 Amplifiers

Output-stage purpose

An output stage supplies the required load voltage and current while controlling distortion, efficiency, heat, and output impedance. A power amplifier is designed primarily to deliver substantial power to a load; it still has voltage and current relationships, but output power is the design objective.

Class A, B, and AB

Class A, B, and AB conduction intervals

Class Conduction angle per device Quiescent bias Main advantage Main limitation
A \(360^\circ\) In active region Best linearity, no crossover gap High idle dissipation, low efficiency
B \(180^\circ\) At cutoff High theoretical efficiency Crossover distortion near zero
AB \(180^\circ<\theta<360^\circ\) Slightly above cutoff Reduced crossover with better efficiency than A Bias/thermal control needed

Efficiency limits require topology context:

  • series-fed resistive Class A: theoretical maximum \(25\%\);
  • ideal transformer-coupled Class A: theoretical maximum \(50\%\);
  • ideal sinusoidal Class B push-pull: theoretical maximum \(\pi/4=78.5\%\);
  • Class AB lies between Class A and Class B behavior, but has no one universal efficiency percentage.

Class C conducts for less than \(180^\circ\) and normally uses a tuned load to recover a sinusoid. It is efficient for fixed-envelope RF service but is not a linear general-purpose output stage.

Push-pull and crossover distortion

A push-pull stage uses two devices so one handles one polarity/half-cycle and the other handles the opposite polarity/half-cycle. It is a power-amplifier output stage.

In an unbiased complementary Class B emitter follower, neither transistor conducts until the input magnitude reaches approximately one base-emitter drop. This creates a dead zone and crossover distortion around zero.

Class AB applies a small forward bias between the transistor bases so both devices conduct slightly near zero crossing. Common bias elements include diode strings and a \(V_{BE}\) multiplier. Because \(V_{BE}\) changes with temperature, thermal tracking and emitter resistors are important to prevent excessive quiescent current and thermal runaway.

Power BJTs

Power BJTs are designed for higher current, voltage, and power dissipation than small-signal devices. Selection requires more than checking one current rating:

  • maximum \(V_{CE}\), \(I_C\), and power dissipation;
  • safe operating area (SOA), including secondary breakdown;
  • junction temperature and thermal resistance;
  • heat sink and derating;
  • saturation voltage and required base drive;
  • variable and often lower \(\beta\) at high current.

Instantaneous transistor dissipation is approximately

\[ p_Q=v_{CE}i_C. \]

A device can violate its power/SOA limit before reaching its nominal maximum current.

Transformer-coupled push-pull stages

Transformers can:

  • split phase for two output devices;
  • combine their alternating output currents;
  • block DC from the load;
  • match a low load impedance to a higher optimum collector load.

Reflected impedance is

\[ Z_p=\left(\frac{N_p}{N_s}\right)^2Z_L. \]

Tradeoffs include size, cost, finite bandwidth, copper/core loss, leakage inductance, and possible core saturation. Transformer coupling is historically important and remains useful in selected power/RF applications.

Tuned amplifiers

A tuned amplifier uses an LC resonant load and gives high gain over a narrow band around \(f_0\). At resonance, the tank converts device current pulses into a near-sinusoidal voltage. Uses include RF and IF stages, frequency selection, and Class C power amplification.

Do not confuse:

  • wideband amplifier: designed for approximately uniform gain over a range;
  • tuned amplifier: deliberately narrowband and frequency selective.

Operational amplifiers

An op-amp is a very-high-gain differential amplifier:

\[ v_o=A_{OL}(v_+-v_-). \]

Ideal assumptions:

Property Ideal value
Open-loop gain Infinite
Input resistance Infinite; input currents zero
Output resistance Zero
Bandwidth and slew rate Infinite
Input offset and bias current Zero
Common-mode rejection Infinite

Real op-amps have finite gain-bandwidth, slew rate, input common-mode range, output current, and output swing. Always check the data sheet in design work.

With negative feedback, linear operation, and no saturation, the ideal rules are:

\[ i_+=i_-=0, \qquad v_+\approx v_-. \]

The second relation is a virtual short, not a physical connection. It is not valid merely because an op-amp symbol is present; negative feedback and linear operation must exist.

Common configurations:

Circuit Closed-loop gain Phase recognition
Inverting \(A_v=-R_f/R_{in}\) \(180^\circ\) inversion
Noninverting \(A_v=1+R_f/R_g\) No inversion; gain at least 1
Voltage follower \(A_v\approx1\) Buffer; high input, low output impedance
Comparator Usually open-loop Output chooses a saturation state from input polarity

Amplifier examples

  1. An inverting op-amp with \(R_{in}=10\ \text{k}\Omega\) and \(R_f=50\ \text{k}\Omega\) has \(A_v=-5\).
  2. A transformer with \(N_p/N_s=5\) reflects an \(8\ \Omega\) load as \(Z_p=5^2(8)=200\ \Omega\).
  3. A Class B transistor conducts for \(180^\circ\) per cycle, while the pair reconstructs both half-cycles.

Amplifier revision box

  • Class A: \(360^\circ\); B: \(180^\circ\); AB: between them.
  • Class A maximum is \(25\%\) resistive or \(50\%\) transformer-coupled.
  • Ideal Class B push-pull maximum is \(78.5\%\).
  • Push-pull is a power-amplifier arrangement.
  • AB bias reduces the Class B crossover dead zone.
  • Tuned amplifier = narrowband LC load, usually RF/IF.
  • Op-amp virtual short requires negative feedback and unsaturated operation.