Push–pull output: Difference between revisions

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{{Short description|Type of electronic circuit}}

{{Other uses of|push–pull|Push–pull (disambiguation){{!}}Push–pull}}

{{RefimproveMore citations needed|date=November 2017}}

[[File:Pushpull (English).pngsvg|right|thumb|A Class B push–pull output driver using a pair of complementary PNP and NPN [[bipolar junction transistor]]s configured as [[emitter follower]]s]]

A '''push–pull''' amplifier is a type of [[electronic circuit]] that uses a pair of active devices that alternately supply current to, or absorb current from, a connected load. Push–pullThis outputs are present in [[Transistor-transistor logic|TTL]] and [[CMOS]] digital [[logic circuit]]s and in some typeskind of [[electronic amplifier|amplifiers]], andcan areenhance usually realized as a complementary pair of [[transistor]]s, one dissipating or ''sinking'' current fromboth the load to ground or a negative power supply,capacity and the other supplying or ''sourcing'' current to the load from a positive powerswitching supplyspeed.

Push–pull outputs are present in [[Transistor-transistor logic|TTL]] and [[CMOS]] digital [[logic circuit]]s and in some types of [[electronic amplifier|amplifiers]], and are usually realized by a complementary pair of [[transistor]]s, 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 [[Amplifier class#Power amplifier classes|"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.<ref>Joe Carr, ''RF Components and Circuits'', Newnes, page 84</ref> 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 [[transformer]]s 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.

A push–pull amplifier is more efficient than a single-ended [[Amplifier class#Power amplifier classes#Class A|"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.<ref>Joe Carr, ''RF Components and Circuits'', Newnes, page 84</ref> 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 [[transformer]]s 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.

[[File:Tube push pull poweramplifier.PNG|thumb|alt=Schematic diagram of vacuum-tube amplifier| A vacuum tube amplifier often used a center-tapped output transformer to combine the outputs of tubes connected in push–pull.]]

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[[Image:MagnavoxFrontcropped.jpg|thumb|A Magnavox stereo tube push–pull amplifier, circa 1960, utilizes two [[EL84|6BQ5]] output tubes per channel]]

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| image1 = Vacuum tube push-pull amplifier 1924.jpg

| caption1 = Transformer coupled vacuum tube push-pull audio amplifier from 1924. The two [[triode]] output tubes are on right.

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[[Image:MagnavoxFrontcropped.jpg|thumb| caption2 = A Magnavox stereo tube push–pull amplifier, circa 1960, utilizes two [[EL84|6BQ5]] output tubes per channel]]. The two pairs of push-pull tubes are visible in front of the output transformers.

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Push–pull circuits are widely used Thankuinin many amplifier output stages. A pair of [[audion]] tubes connected in push–pull is described in [[Edwin H. Colpitts]]' US patent 1137384 granted in 1915, although the patent does not specifically claim the push–pull connection.<ref>Donald Monroe McNicol, ''Radios' Conquest of Space: The Experimental Rise in Radio Communication'' Taylor & Francis, 1946 page 348</ref> The technique was well- known at that time <ref>http://www.leagle.com/xmlResult.aspx?page=5&xmldoc=193278360F2d723_1537.xml&docbase=CSLWAR1-1950-1985&SizeDisp=7 WESTERN ELECTRIC CO. v. WALLERSTEIN retrieved 12/12/12</ref> and the principle had been claimed in an 1895 patent predating electronic amplifiers.<ref>US Patent 549,477 ''Local Transmitter Circuit for Telephones.'', W. W. Dean</ref> Possibly the first commercial product using a push–pull amplifier was the [[RCA]] ''Balanced amplifier'' released in 1924 for use with their [[Radiola III]] regenerative broadcast receiver.<ref>[http://web.eecs.umich.edu/~srs/Antiques/templ.php?pid=223&collection=Radios Radios - RCA Radiola Balanced Amplifier 1924]</ref> By using a pair of low-power vacuum tubes in push–pull configuration, the amplifier allowed the use of a loudspeaker instead of headphones, while providing acceptable battery life with low standby power consumption.<ref>Gregory Malanowski ''The Race for Wireless: How Radio Was Invented (or Discovered?)'', AuthorHouse, 2011 {{ISBN|1463437501}} pages 66-67, page 144</ref> The technique continues to be used in audio, radio frequency, digital and power electronics systems today.

== Digital circuits ==

[[File:7400 Circuit.svg|right|thumb|Circuit of [[Transistor–transistor logic|TTL]] [[NAND gate]] has a 'totem pole output' stage ''(right)'' consisting of two NPN transistors in push pull. When at least one of the inputs is low, transistor ''V''₁ is turned on, ''V''₂ is turned off, ''V''₃ is turned on and ''V''₄ off, pulling output voltage high. When both inputs are high, ''V''₂ is on, ''V''₃ is off and ''V''₄ is turned on, pulling output low.]]

[[File:7400 Circuit.svg|right|thumb|The TTL output stage is a rather complicated push–pull circuit known as a 'totem pole output' (the transistors, diode, and resistor in the right-most slice of this TTL [[logic gate]] circuit). It sinks currents better than it sources current.]]

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 are not capable of supplyingsourcing 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 level shifting diode in between, they are called "'''totem pole'''"<!-- [[Totem pole output]] redirects here---> outputs.

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 are not 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 level shifting diode in between, they are called "'''totem pole'''"<!-- [[Totem pole output]] redirects here---> outputs.

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, [[Three-state logic|''tri-stated'']]).

TheAn alternative to a push–pull output is a single switch that disconnects or connects the [[Electrical load|load]] either to ground (called an [[open collector]] or [[open drain]] output), or a single switch that disconnects or connects the load 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 triode|single-ended]] to distinguish it from a push–pull circuit.

In analog push–pull power amplifiers the two output 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 f22f, f44f, f66f and therefore promote odd order harmonics, like (f1)f, f33f, f55f when driven into the nonlinear range.

A push–pull amplifier produces less [[distortion]] than a single-ended one. This allows a [[Class-APower amplifier classes#Class A|class-A]] or [[Power amplifier classes#Class AB|AB]] push–pull amplifier to have less distortion for the same power as the same devices used in single-ended configuration. Distortion can occur at the moment the outputs switch: the "hand-off" is not perfect. This is called crossover distortion. [[Class BPower amplifier classes#Class B and AB|Class AB]] and [[Power amplifier classes#Class B|class B]] dissipate less power for the same output than class A; general distortion can be kept low by [[negative feedback]], and crossover distortion can be reduced by biassingadding thea output'bias stagecurrent' to reducesmoothen crossoverthe distortionhand-off.

A class - B 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 1975 {{ISBN|978-0-07-020980-0}} 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.

{{Further|OCL amplifier}}

=== Push–pull transistor output stages ===

[[File:Aura VA 100 Evolution 2 (4061759992) - closeup of output stage.jpg|thumb|upright=1.5|Typical transistor output stage of one channel of a 65 watt stereo amplifier from 1993. The 2 MOSFET push-pull output transistors (''FET2, FET4'') are bolted to the black [[heat sink]]. They are driven by transistors ''Q2, Q5, Q6,'' and ''Q7'']]

{{refimprovemore citations needed section|date=November 2012}}

Categories include:

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==== Square-law push–pull ====

The output devices, usually [[MOSFET]]s or [[vacuum tube]]s, are configured so that their [[Power-law#square-law|square-law]] transfer characteristics (that generate second-harmonic [[distortion]] if used in a single-ended circuit) cancel distortion to a large extent. That is, as one transistor's gate-source voltage increases, the drive to the other device is reduced by the same amount and the drain (or plate) current change in the second device approximately corrects for the non-linearity in the increase of the first.<ref>{{cite journal | author=Ian Hegglun | title=Practical Square-law Class-A Amplifier Design | journal=Linear Audio - Volume |volume=1}}</ref>

=== Push–pull tube (valve) output stages ===

{{seeSee also|Valve audio amplifier – technical#The push–pull power amplifier}}

[[Vacuum tube]]s (valves) are not available in complementary types (as are pnpPNP/npnNPN transistors), so the tube push–pull amplifier has a pair of identical output tubes or groups of tubes with the [[control grid]]s driven in antiphase. These tubes drive current through the two halves of the primary winding of a center-tapped output transformer. Signal currents add, while the distortion signals due to the non-linear [[Current–voltage characteristic|characteristic curve]]s 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 [[audiophile]]s and musicians who consider them to sound better.

Vacuum tube push–pull amplifiers usually use an output transformer, although [[Output transformerless|Output-transformerless (OTL)]] tube stages exist (such as the SEPP/SRPP and the White Cathode Follower below).{{citation needed|date=December 2012}} The phase-splitter stage is usually another vacuum tube but a transformer with a center-tapped secondary winding was occasionally used in some designs. Because these are essentially square-law devices, the comments regarding [[Distortion#Cancellation of even-order harmonic distortion|distortion cancellation]] mentioned [[Push–pull output#Square-law push–pull|above]] apply to most push–pull tube designs when operated in [[Class-APower amplifier classes#Class A|class A]] (i.e. neither device is driven to its non-conducting state).

A '''Single Ended Push–Pull''' ('''SEPP''', '''SRPP''' or '''mu-follower'''<ref>{{cite web|title=SRPP Decoded|url=http://www.tubecad.com/may2000/|website=The Tube CAD Journal|accessdateaccess-date=7 November 2016}}</ref>) output stage, originally called the '''Series-Balanced amplifier''' (US patent 2,310,342, Feb 1943). is similar to a totem-pole arrangement for transistors in that two devices are in series between the power supply rails, but the input drive goes ''only to one of the devices,'' the bottom one of the pair; hence the (seemingly contradictory) Single-Ended description. The output is taken from the cathode of the top (not directly driven) device, which acts part way between a constant current source and a cathode follower but receiving some drive from the plate (anode) circuit of the bottom device. The drive to each tube therefore might not be equal, but the circuit tends to keep the current through the bottom device somewhat constant throughout the signal, increasing the power gain and reducing distortion compared with a true single-tube single-ended output stage.

The transformer-less circuit with two tetrode tubes dates back to 1933: "THE USE OF A VACUUM TUBE AS A PLATE-FEED IMPEDANCE." by J.W.Horton in the Journal of the Franklin Institute 1933 volume 216 Issue 6

The '''White Cathode Follower''' (Patent 2,358,428, Sep 1944 by E. L. C. White) is similar to the SEPP design above, but the signal input is to the ''top'' tube, acting as a cathode follower, but one where the bottom tube (in common cathode configuration) if fed (usually via a step-up transformer) from the current in the plate (anode) of the top device. It essentially reverses the roles of the two devices in SEPP. The bottom tube acts part way between a constant current sink and an equal partner in the push–pull workload. Again, the drive to each tube therefore might not be equal.

The '''White Cathode Follower''' (Patent 2,358,428, Sep. 1944 by E. L. C. White) is similar to the SEPP design above, but the signal input is to the ''top'' tube, acting as a cathode follower, but one where the bottom tube (in common cathode configuration) ifis fed (usually via a step-up transformer) from the current in the plate (anode) of the top device. It essentially reverses the roles of the two devices in SEPP. The bottom tube acts part way between a constant current sink and an equal partner in the push–pull workload. Again, the drive to each tube therefore might not be equal.

Transistor versions of the SEPP and White follower do exist, but are rare.

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== See also ==

* [[Single-ended triode]]

* [[Push–pull converter]] for more details on implementation

* [[Open collector]]

== References ==

*[[Single-ended triode]]

*[[Push–pull converter]] for more details on implementation

*[[Open collector]]

==References==

{{Reflist}}

== External links ==

{{DEFAULTSORT:Push-pull output}}