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| A push–pull amplifier produces less ] than a single-ended one. This allows a ] or AB push–pull amplifier to have less distortion for the same power as the same devices used in single-ended configuration. ] dissipate less power for the same output as class A; distortion can be kept low by ] and by biassing the output stage to reduce crossover distortion. | A push–pull amplifier produces less ] than a single-ended one. This allows a ] or AB push–pull amplifier to have less distortion for the same power as the same devices used in single-ended configuration. ] dissipate less power for the same output as class A; distortion can be kept low by ] and by biassing the output stage to reduce crossover distortion. | ||
| A push-pull amplifier is more efficient than a Class A power amplifier because each output device amplifies only half the output waveform and is cut off during the opposite half. It can be shown that the theoretical full power efficiency (AC power in load compared to DC power consumed) of a push-pull stage is approximately 78.5%. This compares with a Class A amplifier which has efficiency of 25% if directly driving the load and no more than 50% for a transformer coupled output. <ref name=Yunik73> Maurice Yunik ''Design of Modern Transistor Circuits'', Prentice-Hall 1973 ISBN 0-13-201285-5 pp. 340-353 </ref> | A push-pull amplifier is more efficient than a Class A power amplifier because each output device amplifies only half the output waveform and is cut off during the opposite half. It can be shown that the theoretical full power efficiency (AC power in load compared to DC power consumed) of a push-pull stage is approximately 78.5%. This compares with a Class A amplifier which has efficiency of 25% if directly driving the load and no more than 50% for a transformer coupled output. <ref name=Yunik73> Maurice Yunik ''Design of Modern Transistor Circuits'', Prentice-Hall 1973 ISBN 0-13-201285-5 pp. 340-353 </ref> A push-pull amplifier draws little power with zero signal, compared to a class A amplifier that draws constant power. Power dissipation in the output devices is roughly one-fifth of the output power rating of the amplifier. <ref name=Yunik73/> A Class A amplifier, by contrast, must use a device capable of dissipating several times the output power. | ||
| The output of the amplifier may be direct-coupled to the load, coupled by a transformer, or connected through a dc blocking capacitor. Where both positive and negative power supplies are used, the load can be returned to the midpoint (ground) of the power supplies. A transformer allows a single polarity power supply to be used, but limits the low-frequency response of the amplifier. Similarly, with a single power supply, a capacitor can be used to block the DC level at the output of the amplifier. <ref>Donald G. Fink, ed. ''Electronics Engineer's Handbook'', McGraw Hill 19745 ISBN 0-07-02980-4 pp. 13-23 through 13-24 </ref> | |||
| Where bipolar junction transistors are used, the bias network must compensate for the negative temperature coefficient of the transistors' base to emitter voltage. This can be done by including a small value resistor between emitter and output. Also, the driving circuit can have silicon diodes mounted in thermal contact with the output transistors, to provide compensation. | |||
| === Push-pull transistor output stages === | === Push-pull transistor output stages === | ||
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A push–pull output is a type of electronic circuit that can drive either a positive or a negative current into a load. Push–pull outputs are present in TTL and CMOS digital logic circuits and in some types of amplifiers, and are usually realized as a complementary pair of transistors, one dissipating or sinking current from the load to ground or a negative power supply, and the other supplying or sourcing current to the load from a positive power supply.
A push-pull amplifier is more efficient than a single-ended "Class A" amplifier. The output power that can be achieved is higher than the continuous dissipation rating of either transistor or tube used alone and increases the power available for a given supply voltage. Symmetrical construction of the two sides of the amplifier means that even-order harmonics are cancelled, which can reduce distortion. DC current is cancelled in the output, allowing a smaller output transformer to be used than in a single-ended amplifier. However, the push-pull amplifier requires a phase-splitting component that adds complexity and cost to the system; use of center-tapped transformers for input and output is a common technique but adds weight and restricts performance. If the two parts of the amplifier do not have identical characteristics, distortion can be introduced as the two halves of the input waveform are amplified unequally. Crossover distortion can be created near the zero point of each cycle as one device is cut off and the other device enters its active region.
Digital circuits
A digital use of a push–pull configuration is the output of TTL and related families. The upper transistor is functioning as an active pull-up, in linear mode, while the lower transistor works digitally. For this reason they aren't capable of supplying as much current as they can sink (typically 20 times less). Because of the way these circuits are drawn schematically, with two transistors stacked vertically, normally with a protection diode in between, they are called "totem pole" outputs.
In simpler digital circuits, especially in CMOS, each transistor is switched on only when its complement is switched off.
A disadvantage of simple push–pull outputs is that two or more of them cannot be connected together, because if one tried to pull while another tried to push, the transistors could be damaged. To avoid this restriction, some push–pull outputs have a third state in which both transistors are switched off. In this state, the output is said to be floating (or, to use a proprietary term, tri-stated).
The alternative to a push–pull output is a single switch that connects the load either to ground (called an open collector or open drain output) or to the power supply (called an open-emitter or open-source output).
Analog circuits
A conventional amplifier stage which is not push–pull is sometimes called single-ended to distinguish it from a push–pull circuit.
In analog push–pull power amplifiers the two output devices (transistors, tubes, FETs) or sets of devices operate in antiphase (i.e. 180° apart). The two antiphase outputs are connected to the load in a way that causes the signal outputs to be added, but distortion components due to non-linearity in the output devices to be subtracted from each other; if the non-linearity of both output devices is similar, distortion is much reduced. Symmetrical push–pull circuits must cancel even order harmonics, like f2, f4, f6 and therefore promote odd order harmonics, like (f1), f3, f5 when driven into the nonlinear range.
A push–pull amplifier produces less distortion than a single-ended one. This allows a class A or AB push–pull amplifier to have less distortion for the same power as the same devices used in single-ended configuration. Class AB and class B dissipate less power for the same output as class A; distortion can be kept low by negative feedback and by biassing the output stage to reduce crossover distortion.
A push-pull amplifier is more efficient than a Class A power amplifier because each output device amplifies only half the output waveform and is cut off during the opposite half. It can be shown that the theoretical full power efficiency (AC power in load compared to DC power consumed) of a push-pull stage is approximately 78.5%. This compares with a Class A amplifier which has efficiency of 25% if directly driving the load and no more than 50% for a transformer coupled output. A push-pull amplifier draws little power with zero signal, compared to a class A amplifier that draws constant power. Power dissipation in the output devices is roughly one-fifth of the output power rating of the amplifier. A Class A amplifier, by contrast, must use a device capable of dissipating several times the output power.
The output of the amplifier may be direct-coupled to the load, coupled by a transformer, or connected through a dc blocking capacitor. Where both positive and negative power supplies are used, the load can be returned to the midpoint (ground) of the power supplies. A transformer allows a single polarity power supply to be used, but limits the low-frequency response of the amplifier. Similarly, with a single power supply, a capacitor can be used to block the DC level at the output of the amplifier.
Where bipolar junction transistors are used, the bias network must compensate for the negative temperature coefficient of the transistors' base to emitter voltage. This can be done by including a small value resistor between emitter and output. Also, the driving circuit can have silicon diodes mounted in thermal contact with the output transistors, to provide compensation.
Push-pull transistor output stages
Categories include:
Transformer-output transistor power amplifiers
It is now very rare to use output transformers with transistor amplifiers, although such amplifiers offer the best opportunity for matching output devices (with only PNP or only NPN devices required).
Totem-pole push-pull output stages
Two matched transistors of the same polarity (or, less often, Vacuum tubes) can be arranged to supply opposite halves of each cycle without the need for an output transformer, although in doing so the driver circuit often is asymmetric and one transistor will be used in a Common-emitter configuration while the other is used as an Emitter follower. This arrangement is less used today than during the 1970s; it can be implemented with few transistors (not so important today) but is relatively difficult to balance and so keep to a low distortion (the highly non-linear TTL circuits such as the 7400 use this arrangement).
Symmetrical push-pull
Each half of the output pair "mirror" the other, in that an NPN (or N-Channel FET) device in one half will be matched by a PNP (or P-Channel FET) in the other. This type of arrangement tends to give lower distortion than quasi-symmetric stages because even harmonics are cancelled more effectively with greater symmetry.
Quasi-symmetrical push-pull
In the past when good quality PNP complements for high power NPN silicon transistors were limited, a workaround was to use identical NPN output devices, but fed from complementary PNP and NPN driver circuits in such a way that the combination was close to being symmetrical (but never as good as having symmetry throughout), and so distortion due to mismatched gain on each half of the cycle could be a significant problem.
Super-symmetric output stages
Employing some duplication in the whole driver circuit, to allow symmetrical drive circuits can improve matching further, although driver asymmetry is a small fraction of the distortion generating process. Using a Bridge-tied load arrangement allows a much greater degree of matching between positive and negative halves, compensating for the inevitable small differences between NPN and PNP devices.
Square-law push-pull
The output devices, usually MOSFETs, are configured so that their square-law transfer characteristics (that generate second harmonic Distortion is used in a single-ended circuit) cancel distortion to a large extent. That is, as the voltage across one transistor's gate-source voltage increases the remaining bias voltage to the complementary device is reduced by that amount and the drain current change in the second device approximately corrects for the non-linearity in the increase of the first.
Push-pull tube (valve) output stages
See article: Valve audio amplifier – technical#The push-pull power amplifier. Vacuum tubes (valves) are not available in complementary types (as are pnp/npn transistors), so the tube push–pull amplifier has a pair of identical output tubes or groups of tubes with the control grids driven in antiphase; these tubes drive current through the two halves of the primary winding of a center-tapped output transformer in such a way that the signal currents add, while the distortion signals due to the non-linear characteristic curves of the tubes subtract. These amplifiers were first designed long before the development of solid-state electronic devices; they are still in use by both audiophiles and musicians who consider them to sound better.
These usually involve an output transformer to drop the output impedance to levels suitable for loudspeakers, although Output-transformerless (OTL) tube stages exist (such as for headphones, for 100 Volt line Public address sound systems, or for rare high-impedance loudspeakers).
Ultra-linear push-pull
Pentodes and Tetrodes can have their screen grid fed from a percentage of the primary voltage on the output transformer, giving efficiency and distortion that is a good compromise between triode (or Triode-strapped) power amplifiers circuits and conventional pentode or tetrode output circuits where the screen is fed from a relatively constant voltage source. See article: Ultra-Linear.
References
- Joe Carr, RF Components and Circuits, Newnes, page 84
- ^ Maurice Yunik Design of Modern Transistor Circuits, Prentice-Hall 1973 ISBN 0-13-201285-5 pp. 340-353
- Donald G. Fink, ed. Electronics Engineer's Handbook, McGraw Hill 19745 ISBN 0-07-02980-4 pp. 13-23 through 13-24
- Ian Hegglun. "Practical Square-law Class-A Amplifier Design". Linear Audio - Volume 1.
See also
- Single-ended triode
- Push–pull converter for more details on implementation
- Open collector
External links
- Push–pull vs. single-ended output in analogue tube amplifiers