Bridged and paralleled amplifiers: Difference between revisions
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Multiple [[electronic amplifier]]s can be connected such that they drive a single floating load (bridge) or a single common load (parallel), to increase the amount of [[power (physics)|power]] available in different situations. This is commonly encountered in [[Audio amplifier|audio]] applications. |
Multiple [[electronic amplifier]]s can be connected such that they drive a single floating load (bridge) or a single common load (parallel), to increase the amount of [[power (physics)|power]] available in different situations. This is commonly encountered in [[Audio amplifier|audio]] applications. |
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== Overview == |
== Overview == |
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Bridged or paralleled modes of working, normally involving audio power amplifiers, are methods of using two or more identical amplifiers to drive the same load simultaneously. This is possible for sets of mono, stereo and multichannel amplifiers since the amplifier outputs are combined on a per load basis. Depending on the method of combining separate amplifiers, bridging or paralleling, different amplification goals can be served. The result is an amplifier that can be further combined with bridging or paralleling. This approach can be beneficial for driving loads for which using a [[Single-ended signaling|single-ended]] amplifier is impossible, impractical or less cost-effective. |
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There are many situations where one amplifier may not be sufficient to drive a given load. For example, an audio amplifier rated for 100 watts (W) into 8 Ω will not be capable of driving any more power into that load unless the supply voltages are increased — this may not always be feasible in practice. So in a design situation which calls for 400 W into 8 Ω, the designer may opt for a bridged configuration using two 100 W/4 Ω amplifiers. |
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Another situation arises when it is desired to keep the [[power (physics)|power]] [[dissipation]] per amplifier unchanged whilst operating into a lower impedance load or, equivalently, to lower dissipation in each amp while operating into the same rated load. So in a design situation which calls for using a 100 W/8 Ω amplifier into 4 Ω, the designer may opt for a paralleled amplifier configuration using two such amplifiers. |
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A '''bridge-tied load''' (BTL), also known as '''bridged transformerless''' and '''bridged mono''', is an output configuration for [[audio amplifier]]s, a form of [[impedance bridging]] used mainly in [[professional audio]] & car applications.<ref>{{cite book |url=https://books.google.com/books?id=K1t0GxyvVbMC&pg=PA87 |page=87 |title=Guide to Sound Systems for Worship |last=Eiche |first=Jon F. |publisher=Hal Leonard Corporation |year=1990 |isbn=0-7935-0029-X |series=Recording and Audio Technology}}</ref> The two channels of a stereo amplifier are fed the same [[monaural]] [[audio signal]], with one channel's [[electrical polarity]] reversed. A [[loudspeaker]] is connected between the two amplifier outputs, ''bridging'' the output terminals. This doubles the available voltage swing at the load compared with the same amplifier used without bridging. The configuration is most often used for [[subwoofer]]s.<ref>{{cite web |url=http://www.directproaudio.com/shop/amplifiers/guide/modes.cfm |title=Stereo, Parallel, and Bridge Mono |work=Amp Guide |publisher=DirectProAudio |accessdate=September 28, 2011}}</ref> |
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For a given output voltage swing, the lower the impedance the higher the amplifier load. Bridging is used to allow an amplifier to drive low loads into higher power, because power is inversely proportional to impedance and proportional to the square of voltage, according to the equation <math>P = V^2/R</math>. This equation also shows that bridging quadruples the theoretical power in an amplifier, however this is true only for low enough loads. For example, for loads where the amplifier reaches its full potential in single-ended mode, there is no gain to be made with bridging. This is because an amplifier can have current limitations. In practical applications, inadequate heating dissipation and power supply also limit the power increase, although if the bridged amplifiers use separate power supplies, which is typical, the limit increase for high loads is power doubling, since every amplifier only delivers half of the total power. |
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Yet another situation may require both the above design goals to be met. In such situations a bridge-parallel configuration is used. |
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===Typical circuit=== |
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'''''Note:''' The [[schematic]]s show a simplified amplifier symbol, similar to that used for [[op-amp]]s. Amplifiers (including [[power amplifier]]s) which have distinct inverting and non-inverting inputs (such as voltage or current feedback circuits), are often depicted using this symbol. The reader must not assume that the discussion applies to standard op-amps alone. Further, any amplifier may be imagined in the schematics since the schematics are only representative of the concepts and not the actual or practical circuits.'' |
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''The + and − signs on the input side represent the non-inverting and inverting inputs of each amplifier. Other components such as [[negative feedback|feedback network]], input/output [[resistor]]s/[[capacitor]]s, etc. are not shown.'' |
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[[Image:Bridge amp.GIF|thumb|200px|Representative schematic of a bridged amplifier configuration.]] |
[[Image:Bridge amp.GIF|thumb|200px|Representative schematic of a bridged amplifier configuration.]] |
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Example: The image shows two identical amplifiers A1 and A2 connected in bridge mode. The system is arranged in such a way that the outputs from the amplifiers are inverted with respect to each other. In other words, as the signal in one amplifier is swinging positively, the signal in the other is swinging negatively. When the output of one amplifier is at +10 volts the output of the other will be at −10 volts, and vice versa. The load is connected between the “hot” (often red) outputs of the two amplifiers, and is subject to the potential '''difference''' between them. If the instantaneous potential at the output of one amplifier is at +10 volts, then the output of the other one will be at −10 volts, and the potential difference across the load will be 20 volts, or double the potential available from a single amplifier. |
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A '''bridged amplifier''' or '''H-bridge''' is a configuration for creating a larger output [[voltage]] swing than that possible with one amplifier by inverting a second amplifier and connecting the [[Electrical load|load]] (such as a [[loudspeaker]]) between the two outputs ('''BTL''' = [[bridge-tied load]]). |
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<ref>{{cite web |url=http://www.rocketroberts.com/techart/amp.htm |title=Audio Power Amplifier Fundamentals |year=2007 |work=Joe's Tech Notes |last=Roberts |first=Joe |accessdate=September 28, 2011}}</ref> |
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The image shows two identical amplifiers A1 and A2 connected in bridge configuration. If a single amplifier is able to produce ±10 V relative to [[ground (electricity)|ground]] (20 V<sub>[[Peak-to-peak|p-p]]</sub>), then the second amplifier will output the same signal, but inverted. If the load is connected between the positive ("hot") outputs of the two amplifiers (instead of connecting between one output and ground), it can see up to 10 V − (−10 V) = ±20 V (or 40 V<sub>p-p</sub>) total, which is twice what each individual amplifier can put out. Driving the load in [[antiphase]] makes each amplifier see only half the load's [[Electrical impedance|impedance]]. |
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The provision of the anti-phase audio input signal can be provided in several ways, which require appropriate knowledge and skill. |
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Because the available voltage swing across the load is doubled for the same power supply voltage, bridged output enables the design of an amplifier producing 4x the power output on the same supply voltage, since [[Electric power#In circuits|power varies as the square of the voltage]]: |
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# by an internal modification such as that described by Rod Elliot at https://sound-au.com/project20.htm; |
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: <math>P = \frac{{V^2 }}{R}</math>. |
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# by a simple active phase splitter circuit, external to the amplifier; |
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# by a phase splitting audio input transformer, external to the amplifier. |
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===Benefits and drawbacks=== |
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(edit) Because the above is so authoritively written, I am loathe to overwrite the "facts"in this section. Perhaps the originator will choose to investigate and clarify. It should read TWICE the power. see other edits below when the formula above is used correctly (end of edit) |
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Since two amplifiers are being used in opposite polarity, using the same power supply, the bridged output is floating. This makes a DC blocking capacitor between the amplifier and the load unnecessary, saving cost and space and avoiding the power reduction at low frequency due to the capacitor.<ref>{{cite book |url=https://books.google.com/books?id=Qpmi4ia2nhcC&pg=PA367 |page=367 |title=Audio Power Amplifier Design Handbook |last=Self |first=Douglas |publisher=Focal Press |year=2009 |isbn=978-0-240-52162-6 |edition=5}}</ref> For the same reason the amplifier outputs should never be grounded or it may damage the amplifier. [[Damping factor]] is cut in half, which is beneficial to the power delivery.<ref name=Bartlett/> |
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===Amplifier design considerations=== |
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This is often provided as an option on [[power amplifier]]s for audio, allowing the two channels to be used in a [[stereophonic sound|stereo]] configuration, or in a single channel bridged configuration to increase the power available. For example, if an amplifier can deliver a maximum of 100 W each into two 8 Ω loads in stereo mode, the same amplifier when bridged will deliver 400 W into a single 8 Ω load. (the same amplifier will deliver 200watts into a 16ohm load. |
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On audio chat forums, some hobbyists claim that operating an amplifier's stereo pair in bridge mode will deliver four times the power of one of the pair's channels. Given an equivalent load, power delivered is proportional to the square of the voltage, and bridge mode operation doubles the voltage presented. On that basis, a pair of amplifier channels operated in bridge mode should deliver four times the power of a single amplifier, driving the same load. However, this ignores an important consideration that because the potential difference at the load is doubled, the current passing through the load (and through each of the amplifier's outputs) will also be doubled. |
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Amplifier circuits are typically designed with the lowest-cost [[Electronic component|components]] needed to provide the desired performance characteristics. The components that carry the output current from the amplifier will tend to be the smallest (cheapest) that will satisfy the peak current draw when the amplifier is running at maximum power, in the designed mode of operation. Operating an amplifier designed for solo operation in bridge mode will mean that the current in the components that drive the output could peak at twice that which they were originally designed for. |
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This output configuration is useful in applications where battery size dictates a lower supply voltage, e.g., automotive or handheld applications. |
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If the components can cope with the additional current beyond the peak current expected for solo operation, then greater power delivery could be achieved. But in the general case, the amplifier can only be expected to work as specified, and operating it beyond the specification will give rise to increased risk of permanent damage to the amplifier circuit. |
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(Edit) The statements above fail to mention that when two amplifiers are connected in bridge mode the output impedance of the pair is DOUBLED. Thus, if "2R" is substituded for "R" in the formula given, (together with the implied "2Vsquared) it will be seen that the output power is also DOUBLED and not quadrupled as stated. |
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As such, if an amplifier designed for solo operation is to be re-purposed for bridge mode operation, the load impedance should be doubled. This should mean that the current draw stays within the limits of the amplifier design. In this scenario, the power delivered by the bridged amplifier pair will be twice the power delivered by a single amplifier channel. |
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However, if a loudspeaker is used that has the impedance specified for just one of the pair the bridged pair WILL see a load impedance of half that the amplifiers are designed for and it will attempt to supply up to 4 times the output. This is no different than saying you may double the output of a given single amplifier by working it into a load of half the rated output impedance. The effect of doing this will depend entirely on the design of amplifier; ie it's overload detection circuit, it's power supply capability and what degree of harmonic didtortion is acceptable. (end of edit) |
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<ref name=Bartlett>{{cite web |url=http://www.prosoundweb.com/article/print/amplifier_power_master_class_not_all_ratings_are_similar |title=Amplifier Power Master Class: Not All Ratings Are Similar |last=Bartlett |first=Bruce |publisher=ProSoundWeb |date=May 1, 2010 |accessdate=September 28, 2011}}</ref> |
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Bridging is a common technique with [[car audio]] systems to increase the available power output, since the supply is limited to that of the [[alternator]] (14.4 VDC) unless a voltage step-up power supply is used. |
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However, in some scenarios, amplifiers are designed specifically to operate in bridge mode. Such amplifiers are specifically designed to be able to deliver the necessary current. In such systems, the bridged pair will be able to deliver four times that power that a single amplifier channel would have been able to deliver. The bridge mode option is often used in PA systems and especially in car audio applications to feed bass loudspeakers at high power. |
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Also, note that when connected in bridge, each amplifier sees half the load impedance and thus delivers double the [[current (electricity)|current]], thereby doubling the dissipation within the amplifier. (edit) This makes no sense. Each amplifier sees half the final load impedance and delivers the SAME output signal current as in normal connection (end of edit) |
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Car audio amplifiers commonly have only a notional 13.8 volt supply, which would ordinarily limit the voltage swing available at the output to + and − 6.9 volts. Whilst it would be possible to achieve higher voltage swings by such means as [[DC-to-DC converter|DC-to-DC conversion]] of the supply voltage, using a bridge mode design allows for twice the voltage swing with a simpler and lower cost design. This design also increases efficiency by avoiding the power losses of a converter. |
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One requirement of this configuration is that the output [[DC offset]] voltage of the amplifiers (edit)not applicable to capacitive or transformer output (end of edit) must always be equal , preferably as close to zero as possible at no signal. Unequal offset will cause some [[direct current]] to flow through the load and the amplifiers, wasting power in all three. Practically, a small offset may be acceptable depending on final requirements or specifications. |
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Amplifiers that use a single supply with an internal DC offset (at half the supply voltage for maximum undistorted voltage swing) must not drive that direct current into the load, so they typically use output coupling [[capacitor]]s so that the speaker sees zero volts DC. In the case of a bridged amplifier, however, this is not necessary, since if both amplifiers have the same offset, the net voltage across the load is zero. |
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== Paralleled amplifier == |
== Paralleled amplifier == |
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[[Image:Parallel amp.GIF|thumb|220px|Representative schematic of a paralleled amplifier configuration.]] |
[[Image:Parallel amp.GIF|thumb|220px|Representative schematic of a paralleled amplifier configuration.]] |
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A '''paralleled amplifier''' configuration uses multiple amplifiers in parallel, i.e., two or more amplifiers operating in-phase into a common load. |
A '''paralleled amplifier''' configuration uses multiple amplifiers in parallel, i.e., two or more amplifiers operating in-phase into a common load. |
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In this mode the available output ''current'' is doubled but the output ''voltage'' remains the same. The output impedance of the pair is now halved. |
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⚫ | The image shows two identical amplifiers A1 and A2 connected in parallel configuration. This configuration is often used when a single amplifier is incapable of being operated into a low impedance load or dissipation per amplifier is to be reduced without increasing the load [[Electrical impedance|impedance]] or reducing power delivered to the load. For example, if two identical amplifiers (each rated for operation into 4 |
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⚫ | The image shows two identical amplifiers A1 and A2 connected in parallel configuration. This configuration is often used when a single amplifier is incapable of being operated into a low impedance load or dissipation per amplifier is to be reduced without increasing the load [[Electrical impedance|impedance]] or reducing power delivered to the load. For example, if two identical amplifiers (each rated for operation into 4 ohm) are paralleled into a 4 ohm load, each amplifier sees an equivalent of 8 ohm since the output current is now shared by both amplifiers — each amplifier supplies half the load current, and the dissipation per amplifier is halved. This configuration (ideally or theoretically) requires each amplifier to be exactly identical to the other(s), or they will appear as loads to each other. Practically, each amplifier must satisfy the following: |
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* Each amplifier must have as little output DC offset as possible (ideally zero offset) at no signal, otherwise the amplifier with the higher offset will try to drive current into the one with lesser offset thereby increasing dissipation. Equal offsets are also not acceptable since this will cause unwanted current (and dissipation) in the load. These are taken care of by adding an offset nulling circuit to each amplifier. |
* Each amplifier must have as little output DC offset as possible (ideally zero offset) at no signal, otherwise the amplifier with the higher offset will try to drive current into the one with lesser offset thereby increasing dissipation. Equal offsets are also not acceptable since this will cause unwanted current (and dissipation) in the load. These are taken care of by adding an offset nulling circuit to each amplifier. |
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* The [[gain]]s of the amplifiers must be as closely matched as possible so that the outputs don't try to drive each other when signal is present. |
* The [[Gain (electronics)|gain]]s of the amplifiers must be as closely matched as possible so that the outputs don't try to drive each other when signal is present. A simple and robust solution is to use paralleled [[Buffer amplifier#Voltage buffer examples|voltage followers]], which by design have exactly unity gain, driven by a common voltage amplification stage. |
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In addition, small resistors (much less than the load impedance, not shown in the schematic) are added in series with each amplifier's output to enable proper current sharing between the amplifiers. These resistances are necessary |
In addition, small resistors (much less than the load impedance, not shown in the schematic) are added in series with each amplifier's output to enable proper current sharing between the amplifiers. These resistances are necessary because the output impedance of the two amplifiers will not, due to manufacturing variation, be perfectly identical. Introduction of output resistors isolates this imbalance and prevents problematic interactions between the two amplifiers. |
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Another method of parallelling amplifiers is to use current drive. With this approach the close matching and resistances are not needed. |
Another method of parallelling amplifiers is to use current drive. With this approach the close matching and resistances are not needed. |
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== Bridge-parallel amplifier == |
== Bridge-parallel amplifier == |
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A '''bridge-parallel amplifier''' |
A '''bridge-parallel amplifier''' topology is a hierarchical combination of the bridged and paralleled amplifier topologies, with at least four single-ended channels needed to produce one bridge-parallel channel. The two topologies complement each other in that the bridging allows for higher voltage output and the paralleling provides the current handling capacity needed to drive low impedances, typical in subwoofer applications. It is more commonly used with IC power amplifiers with stereo outputs operating in bridged mode.<ref>{{cite web|url=https://www.ti.com/product/TPA3255|title=TPA3255 315-W stereo, 600-W mono, 18- to 53.5-V supply, analog input Class-D audio amplifier|publisher=Texas Instruments}}</ref> It can be seen from the preceding sections that a bridged configuration of two amplifier channels delivers four times the power and doubles the dissipation. A paralleled configuration of two amplifier channels delivers the same power and halves dissipation. So when both configurations are combined on a set of four single-ended amplifiers, the power output is increased four-fold but the power dissipation of each constituent amplifier is not increased, and thermal issues are easier to handle. |
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== Practical applications == |
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=== Stereo amplifiers === |
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Two identical amplifiers are most often encountered in a common case, with a common power supply, and would normally be regarded as a stereo amplifier. Any conventional stereo amplifier can be operated in bridge or parallel mode provided that the common loudspeaker terminals (normally black) are connected and common to the ground rail within the amplifier. This would turn the stereo amplifier into a mono amplifier. |
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Some two channel amplifiers, or stereo amplifiers, have the built in facility to operate in bridge mode by operating a switch and observing the input and output connections detailed on the back panel or in the manual. This option is most often found in high power PA equipment or amplifiers designed for car audio applications. Operation in parallel mode requires no special facility and is implemented merely by the appropriate external connection. |
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Stereo amplifiers usually have a common control for [[Gain (electronics)|gain]] and frequently bass/treble and when switched to bridge mode will automatically track each channel identically. Where two channel amplifiers have separate controls, and are switchable to bridge mode, only the controls on one channel will be operational. |
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Where the user implements their own connections for either bridge or parallel mode, and the amplifiers have individual controls, care should be taken that both sets of controls are set identically. |
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== See also == |
== See also == |
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* [[Amplifier]] |
* [[Amplifier]] |
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* [[Audio amplifier]] |
* [[Audio amplifier]] |
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* [[Electronic amplifier]] |
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* [[Single-ended signalling]] |
* [[Single-ended signalling]] |
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== |
==References== |
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{{reflist}} |
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== Further reading == |
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* [https://www.apexanalog.com/resources/appnotes/an20u.pdf Bridge Mode Operation of Power Operational Amplifiers] Apex Microtechnology - application note AN20, October 2012 |
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* [http://www.maximintegrated.com/en/app-notes/index.mvp/id/1122 Optimizing Audio Bridged Tied Load Amplifiers], [[Maxim Integrated]] Products, Inc. application note 1122, Jun 24, 2002. |
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{{DEFAULTSORT:Bridged And Paralleled Amplifiers}} |
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[[Category:Electronic amplifiers]] |
[[Category:Electronic amplifiers]] |
Latest revision as of 19:15, 23 November 2024
Multiple electronic amplifiers can be connected such that they drive a single floating load (bridge) or a single common load (parallel), to increase the amount of power available in different situations. This is commonly encountered in audio applications.
Overview
[edit]Bridged or paralleled modes of working, normally involving audio power amplifiers, are methods of using two or more identical amplifiers to drive the same load simultaneously. This is possible for sets of mono, stereo and multichannel amplifiers since the amplifier outputs are combined on a per load basis. Depending on the method of combining separate amplifiers, bridging or paralleling, different amplification goals can be served. The result is an amplifier that can be further combined with bridging or paralleling. This approach can be beneficial for driving loads for which using a single-ended amplifier is impossible, impractical or less cost-effective.
Bridged amplifier
[edit]A bridge-tied load (BTL), also known as bridged transformerless and bridged mono, is an output configuration for audio amplifiers, a form of impedance bridging used mainly in professional audio & car applications.[1] The two channels of a stereo amplifier are fed the same monaural audio signal, with one channel's electrical polarity reversed. A loudspeaker is connected between the two amplifier outputs, bridging the output terminals. This doubles the available voltage swing at the load compared with the same amplifier used without bridging. The configuration is most often used for subwoofers.[2]
For a given output voltage swing, the lower the impedance the higher the amplifier load. Bridging is used to allow an amplifier to drive low loads into higher power, because power is inversely proportional to impedance and proportional to the square of voltage, according to the equation . This equation also shows that bridging quadruples the theoretical power in an amplifier, however this is true only for low enough loads. For example, for loads where the amplifier reaches its full potential in single-ended mode, there is no gain to be made with bridging. This is because an amplifier can have current limitations. In practical applications, inadequate heating dissipation and power supply also limit the power increase, although if the bridged amplifiers use separate power supplies, which is typical, the limit increase for high loads is power doubling, since every amplifier only delivers half of the total power.
Typical circuit
[edit]Example: The image shows two identical amplifiers A1 and A2 connected in bridge mode. The system is arranged in such a way that the outputs from the amplifiers are inverted with respect to each other. In other words, as the signal in one amplifier is swinging positively, the signal in the other is swinging negatively. When the output of one amplifier is at +10 volts the output of the other will be at −10 volts, and vice versa. The load is connected between the “hot” (often red) outputs of the two amplifiers, and is subject to the potential difference between them. If the instantaneous potential at the output of one amplifier is at +10 volts, then the output of the other one will be at −10 volts, and the potential difference across the load will be 20 volts, or double the potential available from a single amplifier.
The provision of the anti-phase audio input signal can be provided in several ways, which require appropriate knowledge and skill.
- by an internal modification such as that described by Rod Elliot at https://sound-au.com/project20.htm;
- by a simple active phase splitter circuit, external to the amplifier;
- by a phase splitting audio input transformer, external to the amplifier.
Benefits and drawbacks
[edit]Since two amplifiers are being used in opposite polarity, using the same power supply, the bridged output is floating. This makes a DC blocking capacitor between the amplifier and the load unnecessary, saving cost and space and avoiding the power reduction at low frequency due to the capacitor.[4] For the same reason the amplifier outputs should never be grounded or it may damage the amplifier. Damping factor is cut in half, which is beneficial to the power delivery.[5]
Amplifier design considerations
[edit]On audio chat forums, some hobbyists claim that operating an amplifier's stereo pair in bridge mode will deliver four times the power of one of the pair's channels. Given an equivalent load, power delivered is proportional to the square of the voltage, and bridge mode operation doubles the voltage presented. On that basis, a pair of amplifier channels operated in bridge mode should deliver four times the power of a single amplifier, driving the same load. However, this ignores an important consideration that because the potential difference at the load is doubled, the current passing through the load (and through each of the amplifier's outputs) will also be doubled.
Amplifier circuits are typically designed with the lowest-cost components needed to provide the desired performance characteristics. The components that carry the output current from the amplifier will tend to be the smallest (cheapest) that will satisfy the peak current draw when the amplifier is running at maximum power, in the designed mode of operation. Operating an amplifier designed for solo operation in bridge mode will mean that the current in the components that drive the output could peak at twice that which they were originally designed for.
If the components can cope with the additional current beyond the peak current expected for solo operation, then greater power delivery could be achieved. But in the general case, the amplifier can only be expected to work as specified, and operating it beyond the specification will give rise to increased risk of permanent damage to the amplifier circuit.
As such, if an amplifier designed for solo operation is to be re-purposed for bridge mode operation, the load impedance should be doubled. This should mean that the current draw stays within the limits of the amplifier design. In this scenario, the power delivered by the bridged amplifier pair will be twice the power delivered by a single amplifier channel.
However, in some scenarios, amplifiers are designed specifically to operate in bridge mode. Such amplifiers are specifically designed to be able to deliver the necessary current. In such systems, the bridged pair will be able to deliver four times that power that a single amplifier channel would have been able to deliver. The bridge mode option is often used in PA systems and especially in car audio applications to feed bass loudspeakers at high power.
Car audio amplifiers commonly have only a notional 13.8 volt supply, which would ordinarily limit the voltage swing available at the output to + and − 6.9 volts. Whilst it would be possible to achieve higher voltage swings by such means as DC-to-DC conversion of the supply voltage, using a bridge mode design allows for twice the voltage swing with a simpler and lower cost design. This design also increases efficiency by avoiding the power losses of a converter.
Paralleled amplifier
[edit]A paralleled amplifier configuration uses multiple amplifiers in parallel, i.e., two or more amplifiers operating in-phase into a common load.
In this mode the available output current is doubled but the output voltage remains the same. The output impedance of the pair is now halved.
The image shows two identical amplifiers A1 and A2 connected in parallel configuration. This configuration is often used when a single amplifier is incapable of being operated into a low impedance load or dissipation per amplifier is to be reduced without increasing the load impedance or reducing power delivered to the load. For example, if two identical amplifiers (each rated for operation into 4 ohm) are paralleled into a 4 ohm load, each amplifier sees an equivalent of 8 ohm since the output current is now shared by both amplifiers — each amplifier supplies half the load current, and the dissipation per amplifier is halved. This configuration (ideally or theoretically) requires each amplifier to be exactly identical to the other(s), or they will appear as loads to each other. Practically, each amplifier must satisfy the following:
- Each amplifier must have as little output DC offset as possible (ideally zero offset) at no signal, otherwise the amplifier with the higher offset will try to drive current into the one with lesser offset thereby increasing dissipation. Equal offsets are also not acceptable since this will cause unwanted current (and dissipation) in the load. These are taken care of by adding an offset nulling circuit to each amplifier.
- The gains of the amplifiers must be as closely matched as possible so that the outputs don't try to drive each other when signal is present. A simple and robust solution is to use paralleled voltage followers, which by design have exactly unity gain, driven by a common voltage amplification stage.
In addition, small resistors (much less than the load impedance, not shown in the schematic) are added in series with each amplifier's output to enable proper current sharing between the amplifiers. These resistances are necessary because the output impedance of the two amplifiers will not, due to manufacturing variation, be perfectly identical. Introduction of output resistors isolates this imbalance and prevents problematic interactions between the two amplifiers.
Another method of parallelling amplifiers is to use current drive. With this approach the close matching and resistances are not needed.
Bridge-parallel amplifier
[edit]A bridge-parallel amplifier topology is a hierarchical combination of the bridged and paralleled amplifier topologies, with at least four single-ended channels needed to produce one bridge-parallel channel. The two topologies complement each other in that the bridging allows for higher voltage output and the paralleling provides the current handling capacity needed to drive low impedances, typical in subwoofer applications. It is more commonly used with IC power amplifiers with stereo outputs operating in bridged mode.[6] It can be seen from the preceding sections that a bridged configuration of two amplifier channels delivers four times the power and doubles the dissipation. A paralleled configuration of two amplifier channels delivers the same power and halves dissipation. So when both configurations are combined on a set of four single-ended amplifiers, the power output is increased four-fold but the power dissipation of each constituent amplifier is not increased, and thermal issues are easier to handle.
Practical applications
[edit]Stereo amplifiers
[edit]Two identical amplifiers are most often encountered in a common case, with a common power supply, and would normally be regarded as a stereo amplifier. Any conventional stereo amplifier can be operated in bridge or parallel mode provided that the common loudspeaker terminals (normally black) are connected and common to the ground rail within the amplifier. This would turn the stereo amplifier into a mono amplifier.
Some two channel amplifiers, or stereo amplifiers, have the built in facility to operate in bridge mode by operating a switch and observing the input and output connections detailed on the back panel or in the manual. This option is most often found in high power PA equipment or amplifiers designed for car audio applications. Operation in parallel mode requires no special facility and is implemented merely by the appropriate external connection.
Stereo amplifiers usually have a common control for gain and frequently bass/treble and when switched to bridge mode will automatically track each channel identically. Where two channel amplifiers have separate controls, and are switchable to bridge mode, only the controls on one channel will be operational.
Where the user implements their own connections for either bridge or parallel mode, and the amplifiers have individual controls, care should be taken that both sets of controls are set identically.
See also
[edit]References
[edit]- ^ Eiche, Jon F. (1990). Guide to Sound Systems for Worship. Recording and Audio Technology. Hal Leonard Corporation. p. 87. ISBN 0-7935-0029-X.
- ^ "Stereo, Parallel, and Bridge Mono". Amp Guide. DirectProAudio. Retrieved September 28, 2011.
- ^ Roberts, Joe (2007). "Audio Power Amplifier Fundamentals". Joe's Tech Notes. Retrieved September 28, 2011.
- ^ Self, Douglas (2009). Audio Power Amplifier Design Handbook (5 ed.). Focal Press. p. 367. ISBN 978-0-240-52162-6.
- ^ a b Bartlett, Bruce (May 1, 2010). "Amplifier Power Master Class: Not All Ratings Are Similar". ProSoundWeb. Retrieved September 28, 2011.
- ^ "TPA3255 315-W stereo, 600-W mono, 18- to 53.5-V supply, analog input Class-D audio amplifier". Texas Instruments.
Further reading
[edit]- Bridge Mode Operation of Power Operational Amplifiers Apex Microtechnology - application note AN20, October 2012
- Bridge/Parallel Amplifier (BPA-200) Documentation, National Semiconductor application note, September 19, 1997.
- Optimizing Audio Bridged Tied Load Amplifiers, Maxim Integrated Products, Inc. application note 1122, Jun 24, 2002.