Editing Alternating current

{{short description|Electric current that periodically reverses direction}}
{{RefImprove|date=March 2023}}
{{Use American English|date=November 2024}}

[[File:Types of current by Zureks.svg|thumb|Alternating current (green curve). The horizontal axis measures time (it also represents zero voltage/current); the vertical, current or voltage.]]
{{Electromagnetism |Network}}

'''Alternating current''' ('''AC''') is an [[electric current]] that periodically reverses direction and changes its magnitude continuously with time, in contrast to [[direct current]] (DC), which flows only in one direction. Alternating current is the form in which [[electric power]] is delivered to businesses and residences, and it is the form of [[electrical energy]] that consumers typically use when they plug [[kitchen appliance]]s, [[television]]s, [[Fan (machine)|fan]]s and [[electric lamp]]s into a [[wall socket]]. The abbreviations ''AC'' and ''DC'' are often used to mean simply ''alternating'' and ''direct'', respectively, as when they modify ''[[Electric current|current]]'' or ''[[voltage]]''.<ref>{{cite book | title = Basic Electronics & Linear Circuits| author = N. N. Bhargava| author2 = D. C. Kulshreshtha| name-list-style=amp| publisher = Tata McGraw-Hill Education| date = 1983| isbn = 978-0-07-451965-3| page = 90| url = https://books.google.com/books?id=C5bt-oRuUzwC&pg=PA90}}</ref><ref>{{cite book | title = Electrical meterman's handbook| author = National Electric Light Association| publisher = Trow Press| date = 1915 | page = 81| url = https://books.google.com/books?id=ZEpWAAAAMAAJ&pg=PA81}}</ref>

The usual [[waveform]] of alternating current in most electric power circuits is a [[sine wave]], whose positive half-period corresponds with positive direction of the current and vice versa (the full period is called a ''[[wave cycle|cycle]]''). "Alternating current" most commonly refers to power distribution, but a wide range of other applications are technically alternating current although it is less common to describe them by that term.   In many applications, like [[guitar amplifier]]s, different waveforms are used, such as [[Triangle wave|triangular waves]] or [[Square wave (waveform)|square wave]]s. [[Audio frequency|Audio]] and [[radio frequency|radio]] signals carried on electrical wires are also examples of alternating current. These types of alternating current carry information such as sound (audio) or images (video) sometimes carried by [[modulation]] of an AC carrier signal. These currents typically alternate at higher frequencies than those used in power transmission.

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== Transmission, distribution, and domestic power supply ==
{{Main|Electric power transmission|Electric power distribution}}
[[File:Electric Transmission.png|thumb|A schematic representation of long distance electric power transmission. From left to right: G=generator, U=step-up transformer, V=voltage at beginning of transmission line, Pt=power entering transmission line, I=current in wires, R=total resistance in wires, Pw=power lost in transmission line, Pe=power reaching the end of the transmission line,    D=step-down transformer, C=consumers.]]

Electrical energy is distributed as alternating current because AC [[voltage]] may be increased or decreased with a [[transformer]]. This allows the power to be transmitted through [[power line]]s efficiently at [[high voltage]], which reduces the energy lost as heat due to [[electrical resistance|resistance]] of the wire, and transformed to a lower, safer voltage for use. Use of a higher voltage leads to significantly more efficient transmission of power. The power losses (<math>P_{\rm w}</math>) in the wire are a product of the square of the current ( I ) and the [[electrical resistance|resistance]] (R) of the wire, described by the formula:

:<math>P_{\rm w} = I^2 R \, .</math>

This means that when transmitting a fixed power on a given wire, if the current is halved (i.e. the voltage is doubled), the power loss due to the wire's resistance will be reduced to one quarter.

The power transmitted is equal to the product of the current and the voltage (assuming no phase difference); that is,
:<math>P_{\rm t} = IV \, .</math>
Consequently, power transmitted at a higher voltage requires less loss-producing current than for the same power at a lower voltage. Power is often transmitted at hundreds of kilovolts on [[Transmission tower|pylons]], and transformed down to tens of kilovolts to be transmitted on lower level lines, and finally transformed down to 100&nbsp;V – 240&nbsp;V for domestic use.

[[File:Highvoltagetransmissionlines.jpg|thumb|Three-phase high-voltage [[transmission line]]s use alternating currents to distribute power over long distances between [[electric generation]] plants and consumers. The lines in the picture are located in eastern [[Utah]].]]

High voltages have disadvantages, such as the increased insulation required, and generally increased difficulty in their safe handling. In a [[power plant]], energy is generated at a convenient voltage for the design of a [[electric generator|generator]], and then stepped up to a high voltage for transmission. Near the loads, the transmission voltage is stepped down to the voltages used by equipment. Consumer voltages vary somewhat depending on the country and size of load, but generally motors and lighting are built to use up to a few hundred volts between phases. The voltage delivered to equipment such as lighting and motor loads is standardized, with an allowable range of voltage over which equipment is expected to operate. Standard power utilization voltages and percentage tolerance vary in the different [[mains power systems]] found in the world.

[[high-voltage direct current|High-voltage direct-current]] (HVDC) electric power transmission systems have become more viable as technology has provided efficient means of changing the voltage of DC power. Transmission with high voltage direct current was not feasible in the early days of [[electric power transmission]], as there was then no economically viable way to step the voltage of DC down for end user applications such as lighting incandescent bulbs.

[[Three-phase electric power|Three-phase]] electrical generation is very common. The simplest way is to use three separate coils in the generator [[stator]], physically offset by an angle of 120° (one-third of a complete 360° phase) to each other. Three current waveforms are produced that are equal in magnitude and 120° [[out of phase]] to each other. If coils are added opposite to these (60° spacing), they generate the same phases with reverse [[electric polarity|polarity]] and so can be simply wired together. In practice, higher ''pole orders'' are commonly used. For example, a 12-pole machine would have 36 coils (10° spacing). The advantage is that lower rotational speeds can be used to generate the same frequency. For example, a 2-pole machine running at 3600&nbsp;rpm and a 12-pole machine running at 600&nbsp;rpm produce the same frequency; the lower speed is preferable for larger machines. If the load on a three-phase system is balanced equally among the phases, no current flows through the [[neutral point]]. Even in the worst-case unbalanced (linear) load, the neutral current will not exceed the highest of the phase currents. Non-linear loads (e.g. the switch-mode power supplies widely used) may require an oversized neutral bus and neutral conductor in the upstream distribution panel to handle [[Harmonic (electrical power)|harmonics]]. Harmonics can cause neutral conductor current levels to exceed that of one or all phase conductors.

For three-phase at utilization voltages a four-wire system is often used. When stepping down three-phase, a transformer with a Delta (3-wire) primary and a Star (4-wire, center-earthed) secondary is often used so there is no need for a neutral on the supply side. For smaller customers (just how small varies by country and age of the installation) only a [[single-phase electric power|single phase]] and neutral, or two phases and neutral, are taken to the property. For larger installations, all three phases and neutral are taken to the main distribution panel. From the three-phase main panel, both single and three-phase circuits may lead off. [[Split-phase electric power|Three-wire single-phase]] systems, with a single center-tapped transformer giving two live conductors, is a common distribution scheme for residential and small commercial buildings in North America. This arrangement is sometimes incorrectly referred to as ''two phase''. A similar method is used for a different reason on construction sites in the UK. Small power tools and lighting are supposed to be supplied by a local center-tapped transformer with a voltage of 55&nbsp;V between each power conductor and earth. This significantly reduces the risk of [[electric shock]] in the event that one of the live conductors becomes exposed through an equipment fault whilst still allowing a reasonable voltage of 110&nbsp;V between the two conductors for running the tools.

An [[Ground and neutral|additional wire]], called the bond (or earth) wire, is often connected between non-current-carrying metal enclosures and earth ground. This conductor provides protection from electric shock due to accidental contact of circuit conductors with the metal chassis of portable appliances and tools. Bonding all non-current-carrying metal parts into one complete system ensures there is always a low [[electrical impedance]] path to ground sufficient to carry any [[Fault (power engineering)|fault]] current for as long as it takes for the system to clear the fault. This low impedance path allows the maximum amount of fault current, causing the overcurrent protection device (breakers, fuses) to trip or burn out as quickly as possible, bringing the electrical system to a safe state. All bond wires are bonded to ground at the main service panel, as is the neutral/identified conductor if present.

== AC power supply frequencies ==
{{further|Mains electricity by country}}

The [[Utility frequency|frequency of the electrical system]] varies by country and sometimes within a country; most electric power is generated at either 50 or {{val|60|ul=Hz}}. Some countries have a mixture of 50&nbsp;Hz and 60&nbsp;Hz supplies, notably [[Electricity sector in Japan#Transmission|electricity power transmission in Japan]]. 

===Low frequency===
A low frequency eases the design of electric motors, particularly for hoisting, crushing and rolling applications, and commutator-type [[traction motor]]s for applications such as [[railway]]s. However, low frequency also causes noticeable flicker in [[arc lamp]]s and [[incandescent light bulb]]s. The use of lower frequencies also provided the advantage of lower transmission losses, which are proportional to frequency. 

The original Niagara Falls generators were built to produce 25&nbsp;Hz power, as a compromise between low frequency for traction and heavy induction motors, while still allowing incandescent lighting to operate (although with noticeable flicker). Most of the 25&nbsp;Hz residential and commercial customers for Niagara Falls power were converted to 60&nbsp;Hz by the late 1950s, although some{{which|date=December 2011}} 25&nbsp;Hz industrial customers still existed as of the start of the 21st century. 16.7&nbsp;Hz power (formerly 16 2/3&nbsp;Hz) is still used in some European rail systems, such as in [[Austria]], [[Germany]], [[Norway]], [[Sweden]] and [[Switzerland]].{{Citation needed|date=January 2025}}

===High frequency===
Off-shore, military, textile industry, marine, aircraft, and spacecraft applications sometimes use 400&nbsp;Hz, for benefits of reduced weight of apparatus or higher motor speeds. Computer [[Mainframe computer|mainframe]] systems were often powered by 400&nbsp;Hz or 415&nbsp;Hz for benefits of [[ripple (electrical)|ripple]] reduction while using smaller internal AC to DC conversion units.{{citation needed|date=August 2022}}

== Effects at high frequencies ==
{{Main|Skin effect}}

A direct current flows uniformly throughout the cross-section of a homogeneous [[electrical conductivity|electrically conducting]] wire. An alternating current of any frequency is forced away from the wire's center, toward its outer surface. This is because an alternating current (which is the result of the acceleration of [[electric charge]]) creates [[electromagnetic waves]] (a phenomenon known as [[electromagnetic radiation]]). Electric conductors are not conducive to electromagnetic waves (a [[Perfect conductor|perfect electric conductor]] prohibits all electromagnetic waves within its boundary), so a wire that is made of a non-perfect conductor (a conductor with finite, rather than infinite, electrical conductivity) pushes the alternating current, along with their associated electromagnetic fields, away from the wire's center. The phenomenon of alternating current being pushed away from the center of the conductor is called [[skin effect]], and a direct current does not exhibit this effect, since a direct current does not create electromagnetic waves. 

At very high frequencies, the current no longer flows ''in'' the wire, but effectively flows ''on'' the surface of the wire, within a thickness of a few [[skin depth]]s. The skin depth is the thickness at which the current density is reduced by 63%. Even at relatively low frequencies used for power transmission (50&nbsp;Hz – 60&nbsp;Hz), non-uniform distribution of current still occurs in sufficiently thick [[Electrical conductor|conductors]]. For example, the skin depth of a copper conductor is approximately 8.57&nbsp;mm at 60&nbsp;Hz, so high-current conductors are usually hollow to reduce their mass and cost. This tendency of alternating current to flow predominantly in the periphery of conductors reduces the effective cross-section of the conductor. This increases the effective AC [[Electrical resistance|resistance]] of the conductor since resistance is inversely proportional to the cross-sectional area. A conductor's AC resistance is higher than its DC resistance, causing a higher energy loss due to [[Ohmic heating]] (also called I<sup>2</sup>R loss).

{{clear}}

=== Techniques for reducing AC resistance ===
For low to medium frequencies, conductors can be divided into stranded wires, each insulated from the others, with the relative positions of individual strands specially arranged within the conductor bundle. Wire constructed using this technique is called [[Litz wire]]. This measure helps to partially mitigate skin effect by forcing more equal current throughout the total cross section of the stranded conductors. Litz wire is used for making [[Quality factor|high-Q]] [[inductor]]s, reducing losses in flexible conductors carrying very high currents at lower frequencies, and in the windings of devices carrying higher [[radio frequency]] current (up to hundreds of kilohertz), such as switch-mode [[power supply|power supplies]] and [[radio frequency]] [[transformer]]s.

=== Techniques for reducing radiation loss ===
As written above, an alternating current is made of [[electric charge]] under periodic [[acceleration]], which causes [[electromagnetic radiation|radiation]] of [[electromagnetic waves]]. Energy that is radiated is lost. Depending on the frequency, different techniques are used to minimize the loss due to radiation.

==== Twisted pairs ====
At frequencies up to about 1&nbsp;GHz, pairs of wires are twisted together in a cable, forming a [[twisted pair]]. This reduces losses from [[electromagnetic radiation]] and [[inductive coupling]]. A twisted pair must be used with a [[Balanced line|balanced]] signaling system so that the two wires carry equal but opposite currents. Each wire in a twisted pair radiates a signal, but it is effectively canceled by radiation from the other wire, resulting in almost no radiation loss.

==== Coaxial cables ====
[[Coaxial cable]]s are commonly used at [[Audio frequency|audio frequencies]] and above for convenience. A coaxial cable has a conductive wire inside a conductive tube, separated by a [[dielectric]] layer. The current flowing on the surface of the inner conductor is equal and opposite to the current flowing on the inner surface of the outer tube. The electromagnetic field is thus completely contained within the tube, and (ideally) no energy is lost to radiation or coupling outside the tube. Coaxial cables have acceptably small losses for frequencies up to about 5&nbsp;GHz. For [[microwave]] frequencies greater than 5&nbsp;GHz, the losses (due mainly to the dielectric separating the inner and outer tubes being a non-ideal insulator) become too large, making [[Waveguide (electromagnetism)|waveguides]] a more efficient medium for transmitting energy. Coaxial cables often use a perforated dielectric layer to separate the inner and outer conductors in order to minimize the power dissipated by the dielectric.

==== Waveguides ====
[[Waveguide (electromagnetism)|Waveguides]] are similar to coaxial cables, as both consist of tubes, with the biggest difference being that waveguides have no inner conductor. Waveguides can have any arbitrary cross section, but rectangular cross sections are the most common. Because waveguides do not have an inner conductor to carry a return current, waveguides cannot deliver energy by means of an [[electric current]], but rather by means of a ''guided'' [[electromagnetic field]]. Although [[Current density|surface currents]] do flow on the inner walls of the waveguides, those surface currents do not carry power. Power is carried by the guided electromagnetic fields. The surface currents are set up by the guided electromagnetic fields and have the effect of keeping the fields inside the waveguide and preventing leakage of the fields to the space outside the waveguide. Waveguides have dimensions comparable to the [[wavelength]] of the alternating current to be transmitted, so they are feasible only at microwave frequencies. In addition to this mechanical feasibility, [[electrical resistance]] of the non-ideal metals forming the walls of the waveguide causes [[dissipation]] of power (surface currents flowing on lossy [[electrical conductor|conductors]] dissipate power). At higher frequencies, the power lost to this dissipation becomes unacceptably large.

==== Fiber optics ====
At frequencies greater than 200&nbsp;GHz, waveguide dimensions become impractically small, and the [[ohmic heating|ohmic losses]] in the waveguide walls become large. Instead, [[fibre optics|fiber optics]], which are a form of dielectric waveguides, can be used. For such frequencies, the concepts of voltages and currents are no longer used.{{citation needed|date=October 2024}}

==Formulation{{anchor|Mathematics|Mathematics of AC voltages}}==<!--This section is linked from [[Vacuum cleaner]]-->
[[File:Sine voltage.svg|right|thumb|A sinusoidal alternating voltage.{{ordered list
| Peak,
| Peak-to-peak amplitude,
| Effective value,
| Period
}}]]
Alternating currents are accompanied (or caused) by alternating voltages. An AC voltage ''v'' can be described mathematically as a [[function (mathematics)|function]] of time by the following equation:

:<math>v(t) = V_\text{peak}\sin(\omega t)</math>,

where
* <math>V_\text{peak}</math> is the peak voltage (unit: [[volt]]),
* <math>\omega</math> is the [[angular frequency]] (unit: [[radians per second]]). {{paragraph}}The angular frequency is related to the physical frequency, <math>f</math> (unit: [[hertz]]), which represents the number of cycles per second, by the equation <math>\omega = 2\pi f</math>.
* <math>t</math> is the time (unit: [[second]]).

The peak-to-peak value of an AC voltage is defined as the difference between its positive peak and its negative peak. Since the maximum value of <math>\sin(x)</math> is +1 and the minimum value is −1, an AC voltage swings between <math>+V_\text{peak}</math> and <math>-V_\text{peak}</math>. The peak-to-peak voltage, usually written as <math>V_\text{pp}</math> or <math>V_\text{P-P}</math>, is therefore <math>V_\text{peak} - (-V_\text{peak}) = 2 V_\text{peak}</math>.

=== Root mean square voltage{{anchor|Root mean square}} ===
{{further|RMS amplitude}}
{{broader|Root mean square voltage}}
[[File:Sine wave 2.svg|thumb|A sine wave, over one cycle (360°). The dashed line represents the [[root mean square]] (RMS) value at <math>{\sqrt {0.5}}</math> (about 0.707).|alt=A graph of sin(x) with a dashed line at y=sin(45)]]

Below an AC waveform (with no [[DC component]]) is assumed.

The RMS voltage is the square root of the [[mean of a function|mean]] over one cycle of the square of the instantaneous voltage.

{{unordered list
| For an arbitrary periodic waveform <math>v(t)</math> of period <math>T</math>:
: <math>V_\text{rms} = \sqrt{\frac{1}{T} \int_0^{T}{[v(t)]^2 dt}}.</math>
| For a sinusoidal voltage:
: <math>\begin{align}
  V_\text{rms} &= \sqrt{\frac{1}{T} \int_0^{T}[{V_\text{peak}\sin(\omega t + \phi)]^2 dt}}\\
               &= V_\text{peak}\sqrt{\frac{1}{2T} \int_0^{T}[{1 - \cos(2\omega t + 2\phi)] dt}}\\
               &= V_\text{peak}\sqrt{\frac{1}{2T} \int_0^{T}{dt}}\\
               &= \frac{V_\text{peak}}{\sqrt {2}}
\end{align}</math>

where the [[trigonometric identity]] <math>\sin^2(x) = \frac {1 - \cos(2x)}{2}</math> has been used and the factor <math>\sqrt{2}</math> is called the [[crest factor]], which varies for different waveforms.
| For a [[triangle wave]]form centered about zero
: <math>V_\text{rms} = \frac{V_\text{peak}}{\sqrt{3}}.</math>
| For a [[Square wave (waveform)|square wave]]form centered about zero
: <math>V_\text{rms} = V_\text{peak}.</math>
}}

=== Power ===
{{Main|AC power}}

The relationship between voltage and the power delivered is:
:<math>p(t) = \frac{v^2(t)}{R}</math>,

where <math>R</math> represents a load resistance.

Rather than using instantaneous power, <math>p(t)</math>, it is more practical to use a time-averaged power (where the averaging is performed over any integer number of cycles). Therefore, AC voltage is often expressed as a [[root mean square]] (RMS) value, written as <math>V_\text{rms}</math>, because
:<math>P_\text{average} = \frac{{V_\text{rms}}^2}{R}.</math>

;Power oscillation: <math>\begin{align} v(t) &= V_\text{peak}\sin(\omega t) \\ i(t) &= \frac{v(t)}{R} = \frac{V_\text{peak}}{R}\sin(\omega t) \\ p(t) &= v(t)i(t) = \frac{(V_\text{peak})^2}{R}\sin^2(\omega t) = \frac{(V_\text{peak})^2}{2 R} \ (1 - \cos(2 \omega t) ) \end{align}</math>
For this reason, AC power's waveform becomes [[Rectifier#Full-wave rectification|Full-wave rectified]] sine, and its fundamental frequency is double that of the voltage's.


=== Examples of alternating current ===
To illustrate these concepts, consider a 230&nbsp;V AC [[Mains power systems|mains]] supply used in [[Mains power systems#Table of mains voltages, frequencies, and plugs|many countries]] around the world. It is so called because its [[root mean square]] value is 230&nbsp;V. This means that the time-averaged power delivered <math>P_\text{average}</math> is equivalent to the power delivered by a DC voltage of 230&nbsp;V. To determine the peak voltage (amplitude), we can rearrange the above equation to:
:<math>V_\text{peak} = \sqrt{2}\ V_\text{rms}</math>
:<math>P_\text{peak} = \frac{(V_\text{rms})^2}{R}\frac{(V_\text{peak})^2}{(V_\text{rms})^2} = \text{P}_\text{average}\sqrt{2}^2 = \text{2}P_\text{average}.</math>

For 230&nbsp;V AC, the peak voltage <math>V_\text{peak}</math> is therefore <math>230\text{ V}\times\sqrt{2}</math>, which is about 325&nbsp;V, and the peak power <math>P_\text{peak}</math> is <math>230 \times R \times W \times 2</math>, that is 460&nbsp;RW. During the course of one cycle (two cycle as the power) the voltage rises from zero to 325&nbsp;V, the power from zero to 460&nbsp;RW, and both falls through zero. Next, the voltage descends to reverse direction, −325&nbsp;V, but the power ascends again to 460&nbsp;RW, and both returns to zero.

== Information transmission ==
Alternating current is used to transmit [[information]], as in the cases of [[telephone]] and [[cable television]]. Information signals are carried over a wide range of AC frequencies. [[Plain old telephone service|POTS]] telephone signals have a frequency of about 3&nbsp;kHz, close to the [[baseband]] audio frequency. Cable television and other cable-transmitted information currents may alternate at frequencies of tens to thousands of megahertz. These frequencies are similar to the electromagnetic wave frequencies often used to transmit the same types of information [[wireless|over the air]].

== History ==
The first [[alternator]] to produce alternating current was an electric generator based on [[Michael Faraday]]'s principles constructed by the French instrument maker [[Hippolyte Pixii]] in 1832.<ref>{{Cite web |url=http://www.magnet.fsu.edu/education/tutorials/java/pixiimachine/index.html |title=Pixii Machine invented by Hippolyte Pixii, National High Magnetic Field Laboratory |access-date=2012-03-23 |archive-url=https://web.archive.org/web/20080907092008/http://www.magnet.fsu.edu/education/tutorials/java/pixiimachine/index.html |archive-date=2008-09-07 |url-status=dead}}</ref> Pixii later added a [[Commutator (electric)|commutator]] to his device to produce the (then) more commonly used direct current. The earliest recorded practical application of alternating current is by [[Guillaume Duchenne]], inventor and developer of [[electrotherapy]]. In 1855, he announced that AC was superior to [[direct current]] for electrotherapeutic triggering of muscle contractions.<ref>{{cite book|isbn=9780853240631|last=Licht|first=Sidney Herman|chapter=History of Electrotherapy|title=Therapeutic Electricity and Ultraviolet Radiation|edition=2|location=New Haven|year=1967|pages=1–70}}</ref> Alternating current technology was developed further by the Hungarian [[Ganz Works]] company in the 1870s, and, in the 1880s, by [[Sebastian Ziani de Ferranti]], [[Lucien Gaulard]], and [[Galileo Ferraris]].

In 1876, Russian engineer [[Pavel Yablochkov]] invented a lighting system where sets of induction coils were installed along a high-voltage AC line. Instead of changing voltage, the primary windings transferred power to the secondary windings which were connected to one or several [[electric candle]]s (arc lamps) of his own design,<ref name="maglab" /><ref>{{cite journal |url=https://books.google.com/books?id=ksa-S7C8dT8C&pg=RA2-PA283 |page=283 |journal=[[Nature (journal)|Nature]] |issue=534 |volume=21 |title=Gas and Electricity in Paris |date=Jan 22, 1880 |last=De Fonveille |first=W. |access-date=Jan 9, 2009 |bibcode=1880Natur..21..282D |doi=10.1038/021282b0 |doi-access=free}}</ref> used to keep the failure of one lamp from disabling the entire circuit.<ref name="maglab" /> In 1878, the [[Ganz Works|Ganz factory]], Budapest, Hungary, began manufacturing equipment for electric lighting and, by 1883, had installed over fifty systems in [[Austria-Hungary]]. Their AC systems used arc and incandescent lamps, generators, and other equipment.<ref>{{Cite book | url = https://books.google.com/books?id=g07Q9M4agp4C&q=Networks+of+Power:+Electrification+in+Western+Society,+1880-1930+ganz&pg=PA96 | last = Hughes | first = Thomas P. | title = Networks of Power: Electrification in Western Society, 1880–1930 | publisher = The Johns Hopkins University Press | location = Baltimore | year= 1993 | page = 96 | access-date = Sep 9, 2009 | isbn = 0-8018-2873-2}}</ref>

=== Transformers ===
The development of the alternating current [[transformer]] to change voltage from low to high level and back, allowed generation and consumption at low voltages and transmission, over great distances, at high voltage, with savings in the cost of conductors and energy losses. A bipolar open-core [[Transformer|power transformer]] developed by [[Lucien Gaulard]] and [[John Dixon Gibbs]] was demonstrated in London in 1881, and attracted the interest of [[Westinghouse Electric (1886)|Westinghouse]]. They exhibited an AC system powering arc and incandescent lights was installed along five railway stations for the Metropolitan Railway in [[London]] and a single-phase multiple-user AC distribution system [[Turin]] in 1884.<ref>{{Cite journal |last=Allerhand |first=Adam |date=2019 |title=Early AC Power: The First Long-Distance Lines [History] |url=https://ieeexplore.ieee.org/document/8802330 |journal=IEEE Power and Energy Magazine |volume=17 |issue=5 |pages=82–90 |doi=10.1109/MPE.2019.2921059 |issn=1540-7977|url-access=subscription }}</ref> These early induction coils with open magnetic circuits were inefficient at transferring power to [[Electrical load|loads]].{{fact|date=December 2024}} Until about 1880, the paradigm for AC power transmission from a high voltage supply to a low voltage load was a series circuit.{{fact|date=December 2024}} Open-core transformers with a ratio near 1:1 were connected with their primaries in series to allow use of a high voltage for transmission while presenting a low voltage to the lamps.{{fact|date=December 2024}} The inherent flaw in this method was that turning off a single lamp (or other electric device) affected the voltage supplied to all others on the same circuit.{{fact|date=December 2024}} Many adjustable transformer designs were introduced to compensate for this problematic characteristic of the series circuit, including those employing methods of adjusting the core or bypassing the magnetic flux around part of a coil.<ref name="FJU1889" /> The direct current systems did not have these drawbacks, giving it significant advantages over early AC systems.

In the UK, [[Sebastian Ziani de Ferranti|Sebastian de Ferranti]], who had been developing AC generators and transformers in London since 1882, redesigned the AC system at the [[Grosvenor Gallery#Generating station|Grosvenor Gallery power station]] in 1886 for the London Electric Supply Corporation (LESCo) including alternators of his own design and open core transformer designs with serial connections for utilization loads - similar to Gaulard and Gibbs.{{sfnp|Hughes|1993|p=98}} In 1890, he designed [[Deptford Power Station|their power station at Deptford]]<ref>{{cite web|url=http://www.mosi.org.uk/collections/explore-the-collections/ferranti-online/timeline.aspx|title=Ferranti Timeline|archive-url=https://web.archive.org/web/20151003002335/http://www.mosi.org.uk/collections/explore-the-collections/ferranti-online/timeline.aspx|archive-date=2015-10-03| website=Museum of Science and Industry (Manchester)|access-date=February 22, 2012}}</ref> and converted the Grosvenor Gallery station across the Thames into an [[electrical substation]], showing the way to integrate older plants into a universal AC supply system.{{sfnp|Hughes|1993|p=208}}

[[File:ZBD team.jpg|thumb|right|The Hungarian ZBD Team ([[Károly Zipernowsky]], [[Ottó Bláthy]], [[Miksa Déri]]), inventors of the first high efficiency, closed-core shunt connection [[transformer]]]]

[[File:DBZ trafo.jpg|right|thumb|The prototype of the ZBD transformer on display at the Széchenyi István Memorial Exhibition, [[Nagycenk]] in [[Hungary]]]]

In the autumn{{Ambiguous|date=January 2023}} of 1884, [[Károly Zipernowsky]], [[Ottó Bláthy]] and [[Miksa Déri]] (ZBD), three engineers associated with the [[Ganz Works]] of Budapest, determined that open-core devices were impractical, as they were incapable of reliably regulating voltage.{{sfnp|Hughes|1993|p=95}} Bláthy had suggested the use of closed cores, Zipernowsky had suggested the use of [[Shunt (electrical)|parallel shunt connections]], and Déri had performed the experiments;<ref>{{cite book|url=https://archive.org/details/creatingtwentiet0000smil|url-access=registration|quote=ZBD transformer.|last=Smil|first=Vaclav|title=Creating the Twentieth Century: Technical Innovations of 1867–1914 and Their Lasting Impact|location=Oxford |publisher=Oxford University Press|year=2005|page=[https://archive.org/details/creatingtwentiet0000smil/page/71 71]|isbn=978-0-19-803774-3}}</ref> In their joint 1885 patent applications for novel transformers (later called ZBD transformers), they described two designs with closed magnetic circuits where copper windings were either wound around a ring core of iron wires or else surrounded by a core of iron wires.<ref name="FJU1889" /> In both designs, the magnetic flux linking the primary and secondary windings traveled almost entirely within the confines of the iron core, with no intentional path through air (see [[transformer#Toroidal cores|toroidal cores]]). The new transformers were 3.4 times more efficient than the open-core bipolar devices of Gaulard and Gibbs.<ref>{{cite web |last=Jeszenszky|first=Sándor |title=Electrostatics and Electrodynamics at Pest University in the Mid-19th Century |url=http://ppp.unipv.it/Collana/Pages/Libri/Saggi/Volta%20and%20the%20History%20of%20Electricity/V%26H%20Sect2/V%26H%20175-182.pdf |archive-url=https://ghostarchive.org/archive/20221009/http://ppp.unipv.it/Collana/Pages/Libri/Saggi/Volta%20and%20the%20History%20of%20Electricity/V%26H%20Sect2/V%26H%20175-182.pdf |archive-date=2022-10-09 |url-status=live |publisher=[[University of Pavia]]|access-date=Mar 3, 2012}}</ref> The Ganz factory in 1884 shipped the world's first five high-efficiency AC transformers.<ref name="Halacsy (1961)" /> This first unit had been manufactured to the following specifications: 1,400 W, 40&nbsp;Hz, 120:72 V, 11.6:19.4 A, ratio 1.67:1, one-phase, shell form.<ref name="Halacsy (1961)" />

The ZBD patents included two other major interrelated innovations: one concerning the use of parallel connected, instead of series connected, utilization loads, the other concerning the ability to have high turns ratio transformers such that the supply network voltage could be much higher (initially 140 to 2000&nbsp;V) than the voltage of utilization loads (100&nbsp;V initially preferred).<ref>{{cite web |title=Hungarian Inventors and Their Inventions |url=http://www.institutoideal.org/conteudo_eng.php?&sys=biblioteca_eng&arquivo=1&artigo=94&ano=2008 |publisher=Institute for Developing Alternative Energy in Latin America |access-date=Mar 3, 2012 |url-status=dead |archive-url=https://web.archive.org/web/20120322223457/http://www.institutoideal.org/conteudo_eng.php?&sys=biblioteca_eng&arquivo=1&artigo=94&ano=2008 |archive-date=2012-03-22}}</ref><ref>{{cite web |title=Bláthy, Ottó Titusz|url=http://www.omikk.bme.hu/archivum/angol/htm/blathy_o.htm|publisher=Budapest University of Technology and Economics, National Technical Information Centre and Library |access-date=Feb 29, 2012}}</ref> When employed in parallel connected electric distribution systems, closed-core transformers finally made it technically and economically feasible to provide electric power for lighting in homes, businesses and public spaces.<ref>{{cite web |title=Bláthy, Ottó Titusz (1860–1939) |url=http://www.hpo.hu/English/feltalalok/blathy.html |publisher=Hungarian Patent Office |access-date=Jan 29, 2004 |archive-date=December 2, 2010 |archive-url=https://web.archive.org/web/20101202031830/http://www.hpo.hu/English/feltalalok/blathy.html |url-status=dead}}</ref><ref>{{cite web |last=Zipernowsky|first=K.|author2= Déri, M.|author3= Bláthy, O.T. | url=http://www.freepatentsonline.com/0352105.pdf |archive-url=https://ghostarchive.org/archive/20221009/http://www.freepatentsonline.com/0352105.pdf |archive-date=2022-10-09 |url-status=live|title=Induction Coil|publisher=U.S. Patent 352 105, issued Nov. 2, 1886|access-date=July 8, 2009}}</ref>
 
The other essential milestone was the introduction of 'voltage source, voltage intensive' (VSVI) systems'<ref>American Society for Engineering Education. Conference – 1995: Annual Conference Proceedings, Volume 2, (PAGE: 1848)</ref> by the invention of constant voltage generators in 1885.{{sfnp|Hughes|1993|p=96}} In early 1885, the three engineers also eliminated the problem of [[eddy current]] losses with the invention of the lamination of electromagnetic cores.<ref>{{cite book|author=Electrical Society of Cornell University|title=Proceedings of the Electrical Society of Cornell University|publisher=Andrus & Church|year=1896|page=39}}</ref> Ottó Bláthy also invented the first AC [[electricity meter]].<ref>{{cite web |author=Eugenii Katz |url=http://people.clarkson.edu/~ekatz/scientists/blathy.html |title=Blathy |publisher=People.clarkson.edu |access-date=2009-08-04| archive-url = https://web.archive.org/web/20080625015707/http://people.clarkson.edu/~ekatz/scientists/blathy.html| archive-date = June 25, 2008}}</ref><ref>{{cite journal |last=Ricks |first=G.W.D. |title=Electricity Supply Meters |journal=Journal of the Institution of Electrical Engineers |date=March 1896 |volume=25 |number=120 |pages=57–77 |doi=10.1049/jiee-1.1896.0005 |url=https://archive.org/stream/journal06sectgoog#page/n77/mode/1up}} Student paper read on January 24, 1896, at the Students' Meeting.</ref><ref>''The Electrician'', Volume 50. 1923</ref><ref>Official gazette of the United States Patent Office: Volume 50. (1890)</ref>

===Adoption===

The AC power system was developed and adopted rapidly after 1886. In March of that year, Westinghouse engineer [[William Stanley, Jr.|William Stanley]], designing a system based on the Gaulard and Gibbs transformer,<ref>{{cite book|last=Skrabec|first=Quentin R.|title=George Westinghouse: Gentle Genius|publisher=Algora Publishing|year=2007|page=102|isbn=978-0-87586-508-9|url=https://books.google.com/books?id=C3GYdiFM41oC&pg=PA102}}</ref> demonstrated a lighting system in [[Great Barrington, Massachusetts|Great Barrington]]:  A [[Siemens]] generator's voltage of 500 volts was converted into 3000 volts, and then the voltage was stepped down to 500 volts by six Westinghouse transformers. With this setup, the Westinghouse company successfully powered thirty 100-volt incandescent bulbs in twenty shops along the main street of Great Barrington.<ref>{{cite journal |last1=Brusso |first1=Barry|last2=Allerhand |first2=Adam |date=January 2021 |title=A Contrarian History of Early Electric Power Distribution|volume= |issue= |doi= 10.1109/MIAS.2020.3028630|url=https://ieeexplore.ieee.org/document/9292399 |journal=IEEE Industry Applications Magazine |page=13 |publisher=IEEE.org |s2cid=230605234 |access-date=January 1, 2023|archive-date=December 12, 2020 |archive-url=https://web.archive.org/web/20201212083429/https://ieeexplore.ieee.org/stamp/stamp.jsp?arnumber=9292399 |doi-access=free}}</ref><ref>{{cite book|author=Clark W. Gellings|title=The Smart Grid Enabling Energy Efficiency and Demand Response|publisher=[[River Publishers]]|year=2020|page=62|isbn=9781000355314|url=https://books.google.com/books?id=0xkOEAAAQBAJ&dq=siemens+generator+%22great+barrington%22&pg=PT62}}</ref> By the fall of that year Ganz engineers installed a ZBD transformer power system with AC generators in [[Rome]].<ref name="IEC Techline" />

[[File:WestinghouseEarlyACSystem1887-USP373035.png|thumb|Westinghouse Early AC System 1887<br /> ([https://web.archive.org/web/20090325121254/http://www.pat2pdf.org/patents/pat373035.pdf US patent 373035])]]

Based on Stanley's success, the new [[Westinghouse Electric Corporation|Westinghouse Electric]]<ref>{{cite book|title=History of Tinicum Township (PA) 1643–1993|publisher=Tinicum Township Historical Society|year=1993|url=http://tthsdelco.org/wp-content/uploads/2014/02/History%20of%20Tinicum%20Twp.pdf|archive-url=https://web.archive.org/web/20150423202458/http://tthsdelco.org/wp-content/uploads/2014/02/History%20of%20Tinicum%20Twp.pdf|archive-date=April 23, 2015|url-status=live}}</ref> went on to develop alternating current (AC) electric infrastructure throughout the United States. The spread of Westinghouse and other AC systems triggered a push back in late 1887 by [[Thomas Edison]] (a proponent of direct current), who attempted to discredit alternating current as too dangerous in a public campaign called the "[[war of the currents]]". 

In 1888, alternating current systems gained further viability with the introduction of a functional [[AC motor]], something these systems had lacked up till then. The design, an [[induction motor]], was independently invented by [[Galileo Ferraris]] and [[Nikola Tesla]] (with Tesla's design being licensed by Westinghouse in the US). This design was independently further developed into the modern practical [[three-phase]] form by [[Mikhail Dolivo-Dobrovolsky]] and [[Charles Eugene Lancelot Brown]] in Germany on one side,<ref>{{cite book|first1=Arnold|last1=Heertje|first2=Mark|last2=Perlman|title=Evolving Technology and Market Structure: Studies in Schumpeterian Economics|year=1990 |isbn=9780472101924|page=138|publisher=University of Michigan Press}}</ref> and [[Jonas Wenström]] in Sweden on the other, though Brown favored the two-phase system.

The [[Ames Hydroelectric Generating Plant]], constructed in 1890, was among the first hydroelectric alternating current power plants. A long-distance transmission of single-phase electricity from a hydroelectric generating plant in Oregon at Willamette Falls sent power fourteen miles downriver to downtown Portland for street lighting in 1890.<ref>{{Cite journal |date=1915|title=Electric Transmission of Power |journal=General Electric Review |volume=XVIII}}</ref>  In 1891, another transmission system was installed in Telluride Colorado.<ref>{{Cite journal |date=1915|title=Electric Transmission of Power|journal=General Electric|volume=XVIII}}</ref> The first [[Three-phase electric power|three-phase system]] was established in 1891 in [[Frankfurt]], Germany. The [[Tivoli, Lazio|Tivoli]]–[[Rome]] transmission was completed in 1892.<ref name="Holjevac" /> The San Antonio Canyon Generator was the third commercial single-phase hydroelectric AC power plant in the United States to provide long-distance electricity.  It was completed on December 31, 1892, by [[Almarian Decker|Almarian William Decker]] to provide power to the city of [[Pomona, California]], which was 14 miles away. Meanwhile, the possibility of transferring electrical power from a waterfall at a distance was explored at the [[Grängesberg]] mine in Sweden. A {{val|45|ul=m}} fall at Hällsjön, Smedjebackens kommun, where a small iron work had been located, was selected. In 1893,  a three-phase {{val|9.5|ul=Kilovolt{{!}}kv}} system was used to transfer 400 [[horsepower]] a distance of {{val|15|ul=km}}, becoming the first commercial application.<ref>{{cite book | last= Hjulström | first= Filip | title= Elektrifieringens utveckling i Sverige, en ekonomisk-geografisk översikt | year= 1940 | url= https://www.antikvariat.net/sv/rod151504-elektrifieringens-utveckling-i-sverige-en-ekonomisk-geografisk-oversikt-hjulstrom-filip | trans-quote= Excerpt taken from YMER 1941, häfte 2.Utgiven av Sällskapet för antropologi och geografi: Meddelande från Upsala univeristets geografiska institution, N:o 29, published by Esselte ab, Stockholm 1941 no. 135205}}</ref> In 1893, Westinghouse built an alternating current system for the [[Chicago World Exposition]].<ref name="Holjevac" /> In 1893, Decker designed the first American commercial [[three-phase]] power plant using alternating current—the hydroelectric [[Mill Creek No. 1 Hydroelectric Plant]] near [[Redlands, California]].  Decker's design incorporated 10&nbsp;kV three-phase transmission and established the standards for the complete system of generation, transmission and motors used in USA today. The original Niagara Falls [[Adams Power Plant]]  with three two-phase generators was put into operation in August 1895, but was connected to the remote transmission system only in 1896. The [[Jaruga Hydroelectric Power Plant]] in Croatia was set in operation two days later, on 28 August 1895. Its [[electric generator|generator]] (42&nbsp;Hz, 240&nbsp;kW) was made and installed by the Hungarian company [[Ganz]], while the transmission line from the power plant to the City of [[Šibenik]] was {{convert|11.5|km|sp=us}} long, and the municipal distribution grid 3000&nbsp;V/110&nbsp;V included six transforming stations.<ref name="Holjevac" />

Alternating current circuit theory developed rapidly in the latter part of the 19th and early 20th century. Notable contributors to the theoretical basis of alternating current calculations include [[Charles Steinmetz]], [[Oliver Heaviside]], and many others.<ref>{{Cite book|url=https://books.google.com/books?id=f5FqsDPVQ2MC&q=theoretical++alternating+current++Oliver+Heaviside&pg=PA1229|title=Companion Encyclopedia of the History and Philosophy of the Mathematical Sciences|first=I.|last=Grattan-Guinness|date=September 19, 2003|publisher=JHU Press|via=Google Books|isbn=978-0-8018-7397-3}}</ref><ref>{{Cite book|url=https://books.google.com/books?id=lew5IC5piCwC&q=theoretical++alternating+current++Charles+Steinmetz&pg=PA329|title=Mathematics in Historical Context|first=Jeff|last=Suzuki|date=August 27, 2009|publisher=MAA|via=Google Books|isbn=978-0-88385-570-6}}</ref> Calculations in unbalanced three-phase systems were simplified by the [[symmetrical components]] methods discussed by [[Charles LeGeyt Fortescue]] in 1918. <!-- discuss network analyzer and digital computer network analysis -->

== See also ==
{{Portal|Electronics|Energy}}
{{Div col|colwidth=30em}}
* [[AC power]]
* [[Electrical wiring]]
* [[Industrial and multiphase power plugs and sockets|Heavy-duty power plugs]]
* [[Hertz]]
* [[Leading and lagging current]]
* [[Mains electricity by country]]
* [[AC power plugs and sockets]]
* [[Utility frequency]]
* [[War of the currents]]
* [[AC/DC receiver design]]
{{div col end}}

== References ==
{{reflist|refs=
<ref name="maglab">{{cite web |url=http://www.magnet.fsu.edu/education/tutorials/museum/stanleytransformer.html |title=Stanley Transformer |publisher=[[Los Alamos National Laboratory]]; [[University of Florida]] |access-date=Jan 9, 2009 |archive-url=https://web.archive.org/web/20090119134626/http://www.magnet.fsu.edu/education/tutorials/museum/stanleytransformer.html |archive-date=2009-01-19 |url-status=dead}}</ref>
<ref name="FJU1889">{{cite book|url=https://archive.org/details/historyoftransfo00upperich|last=Uppenborn|first=F. J.|title=History of the Transformer|publisher=E. & F. N. Spon|location=London|date=1889|pages=35–41}}</ref>
<ref name="Halacsy (1961)">{{cite journal |last1=Halacsy |first1=A. A. |last2=Von Fuchs |first2=G. H. |date=April 1961 |title=Transformer Invented 75 Years Ago |journal=IEEE Transactions of the American Institute of Electrical Engineers |volume=80 |issue=3 |pages=121–125 |doi=10.1109/AIEEPAS.1961.4500994 |s2cid=51632693}}</ref>
<ref name="IEC Techline">{{cite web |url=http://www.iec.ch/cgi-bin/tl_to_htm.pl?section=technology&item=144 |archive-url=https://web.archive.org/web/20070930171011/http://www.iec.ch/cgi-bin/tl_to_htm.pl?section=technology&item=144 |url-status=dead |archive-date=September 30, 2007 |title=Ottó Bláthy, Miksa Déri, Károly Zipernowsky |publisher=IEC Techline |access-date=Apr 16, 2010}}</ref>
<ref name="Holjevac">{{Cite journal |last1=Holjevac |first1=Ninoslav |last2=Kuzle |first2=Igor |date=2019 |title=Prvi cjeloviti višefazni elektroenergetski sustav na svijetu – Krka Šibenik |url=https://hrcak.srce.hr/238713 |journal=Godišnjak Akademije tehničkih znanosti Hrvatske |language=hr |volume=2019 |issue=1 |pages=162–174 |issn=2975-657X}}</ref>
}}

== Further reading ==
{{refbegin}}
* Willam A. Meyers, ''History and Reflections on the Way Things Were: Mill Creek Power Plant – Making History with AC'', IEEE Power Engineering Review, February 1997, pp. 22–24
{{refend}}

== External links ==
{{Commons category}}
* "''AC/DC: [https://www.pbs.org/wgbh/amex/edison/sfeature/acdc.html What's the Difference]?''". Edison's Miracle of Light, [https://www.pbs.org/wgbh/amex/index.html American Experience]. ([[Public Broadcasting Service|PBS]])
* "''AC/DC: [https://www.pbs.org/wgbh/amex/edison/sfeature/acdc_insideacgenerator.html Inside the AC Generator] {{Webarchive|url=https://web.archive.org/web/20141228182024/http://www.pbs.org/wgbh/amex/edison/sfeature/acdc_insideacgenerator.html |date=2014-12-28 }}''". Edison's Miracle of Light, American Experience. (PBS)
* [http://www.technology.niagarac.on.ca/people/mcsele/Rankine.html Professor Mark Csele's tour of the 25&nbsp;Hz Rankine generating station]
* Blalock, Thomas J., "''[https://web.archive.org/web/20070607042254/http://www.ieee.org/organizations/pes/public/2003/sep/peshistory.html The Frequency Changer Era: Interconnecting Systems of Varying Cycles]''". The history of various frequencies and interconversion schemes in the US at the beginning of the 20th century
* [http://edisontechcenter.org/AC-PowerHistory.html AC Power History and Timeline]
{{Authority control}}

[[Category:Electrical engineering]]
[[Category:Electric current]]
[[Category:Electric power]]
[[Category:AC power]]