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"Tesla motor" redirects here. For the electric car company, see Tesla, Inc.

Three-phase totally-enclosed fan-cooled (TEFC) induction motor with end cover on the left, and without end cover to show cooling fan on the right. In TEFC motors, interior heat losses are dissipated indirectly through enclosure fins, mostly by forced air convection.

Cutaway view through stator of TEFC induction motor, showing rotor with internal air circulation vanes. Many such motors have a symmetric armature, and the frame may be reversed to place the electrical connection box (not shown) on the opposite side.

An induction motor or asynchronous motor is an AC electric motor in which the electric current in the rotor needed to produce torque is obtained by electromagnetic induction from the magnetic field of the stator winding. An induction motor can therefore be made without electrical connections to the rotor. An induction motor's rotor can be either wound type or squirrel-cage type.

Three-phase squirrel-cage induction motors are widely used as industrial drives because they are self-starting, reliable and economical. Single-phase induction motors are used extensively for smaller loads, such as household appliances like fans. Although traditionally used in fixed-speed service, induction motors are increasingly being used with variable-frequency drives (VFD) in variable-speed service. VFDs offer especially important energy savings opportunities for existing and prospective induction motors in variable-torque centrifugal fan, pump and compressor load applications. Squirrel-cage induction motors are very widely used in both fixed-speed and variable-frequency drive applications.

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 History

A model of Nikola Tesla's first induction motor at the Tesla Museum in Belgrade, Serbia

Squirrel-cage rotor construction, showing only the center three laminations

In 1824, the French physicist François Arago formulated the existence of rotating magnetic fields, termed Arago's rotations. By manually turning switches on and off, Walter Baily demonstrated this in 1879, effectively the first primitive induction motor.

The first commutator-free single-phase AC induction motor was invented by Hungarian engineer Ottó Bláthy; he used the single-phase motor to propel his invention, the electricity meter.

The first AC commutator-free polyphase induction motors were independently invented by Galileo Ferraris and Nikola Tesla, a working motor model having been demonstrated by the former in 1885 and by the latter in 1887. Tesla applied for US patents in October and November 1887 and was granted some of these patents in May 1888. In April 1888, the Royal Academy of Science of Turin published Ferraris's research on his AC polyphase motor detailing the foundations of motor operation. In May 1888 Tesla presented the technical paper A New System for Alternating Current Motors and Transformers to the American Institute of Electrical Engineers (AIEE) describing three four-stator-pole motor types: one having a four-pole rotor forming a non-self-starting reluctance motor, another with a wound rotor forming a self-starting induction motor, and the third a true synchronous motor with a separately excited DC supply to the rotor winding.

George Westinghouse, who was developing an alternating current power system at that time, licensed Tesla's patents in 1888 and purchased a US patent option on Ferraris' induction motor concept. Tesla was also employed for one year as a consultant. Westinghouse employee C. F. Scott was assigned to assist Tesla and later took over development of the induction motor at Westinghouse. Steadfast in his promotion of three-phase development, Mikhail Dolivo-Dobrovolsky invented the cage-rotor induction motor in 1889 and the three-limb transformer in 1890. Furthermore, he claimed that Tesla's motor was not practical because of two-phase pulsations, which prompted him to persist in his three-phase work. Although Westinghouse achieved its first practical induction motor in 1892 and developed a line of polyphase 60 hertz induction motors in 1893, these early Westinghouse motors were two-phase motors with wound rotors until B. G. Lamme developed a rotating bar winding rotor.

The General Electric Company (GE) began developing three-phase induction motors in 1891. By 1896, General Electric and Westinghouse signed a cross-licensing agreement for the bar-winding-rotor design, later called the squirrel-cage rotor. Arthur E. Kennelly was the first to bring out the full significance of complex numbers (using j to represent the square root of minus one) to designate the 90º rotation operator in analysis of AC problems. GE's Charles Proteus Steinmetz greatly developed application of AC complex quantities including an analysis model now commonly known as the induction motor Steinmetz equivalent circuit.

Induction motor improvements flowing from these inventions and innovations were such that a 100-horsepower induction motor currently has the same mounting dimensions as a 7.5-horsepower motor in 1897.

 Principle of operation

 3 phase motor

A three-phase power supply provides a rotating magnetic field in an induction motor

Inherent slip - unequal rotation frequency of stator field and the rotor

In both induction and synchronous motors, the AC power supplied to the motor's stator creates a magnetic field that rotates in synchronism with the AC oscillations. Whereas a synchronous motor's rotor turns at the same rate as the stator field, an induction motor's rotor rotates at a somewhat slower speed than the stator field. The induction motor stator's magnetic field is therefore changing or rotating relative to the rotor. This induces an opposing current in the induction motor's rotor, in effect the motor's secondary winding, when the latter is short-circuited or closed through an external impedance. The rotating magnetic flux induces currents in the windings of the rotor, in a manner similar to currents induced in a transformer's secondary winding(s).

The induced currents in the rotor windings in turn create magnetic fields in the rotor that react against the stator field. The direction of the magnetic field created will be such as to oppose the change in current through the rotor windings, in agreement with Lenz's Law. The cause of induced current in the rotor windings is the rotating stator magnetic field, so to oppose the change in rotor-winding currents the rotor will start to rotate in the direction of the rotating stator magnetic field. The rotor accelerates until the magnitude of induced rotor current and torque balances the applied mechanical load on the rotation of the rotor. Since rotation at synchronous speed would result in no induced rotor current, an induction motor always operates slightly slower than synchronous speed. The difference, or "slip," between actual and synchronous speed varies from about 0.5% to 5.0% for standard Design B torque curve induction motors. The induction motor's essential character is that it is created solely by induction instead of being separately excited as in synchronous or DC machines or being self-magnetized as in permanent magnet motors.

For rotor currents to be induced, the speed of the physical rotor must be lower than that of the stator's rotating magnetic field ($n_{s}$); otherwise the magnetic field would not be moving relative to the rotor conductors and no currents would be induced. As the speed of the rotor drops below synchronous speed, the rotation rate of the magnetic field in the rotor increases, inducing more current in the windings and creating more torque. The ratio between the rotation rate of the magnetic field induced in the rotor and the rotation rate of the stator's rotating field is called "slip". Under load, the speed drops and the slip increases enough to create sufficient torque to turn the load. For this reason, induction motors are sometimes referred to as "asynchronous motors".

An induction motor can be used as an induction generator, or it can be unrolled to form a linear induction motor which can directly generate linear motion. The generating mode for induction motors is complicated by the need to excite the rotor, which begins with only residual magnetization. In some cases, that residual magnetization is enough to self-excite the motor under load. Therefore, it is necessary to either snap the motor and connect it momentarily to a live grid or to add capacitors charged initially by residual magnetism and providing the required reactive power during operation. Similar is the operation of the induction motor in parallel with a synchronous motor serving as a power factor compensator. A feature in the generator mode in parallel to the grid is that the rotor speed is higher than in the driving mode. Then active energy is being given to the grid. Another disadvantage of the induction motor generator is that it consumes a significant magnetizing current I₀ = (20-35)%.

 Synchronous speed

An AC motor's synchronous speed, $f_{s}$, is the rotation rate of the stator's magnetic field,

$f_{s}={2f \over p}$,

where $f$ is the frequency of the power supply, $p$ is the number of magnetic poles, and $f_{s}$ is the synchronous speed of the machine. For $f$ in hertz and $n_{s}$ synchronous speed in RPM, the formula becomes:

$n_{s}={2f \over p}\cdot \left({\frac {60\ \mathrm {seconds} }{\mathrm {minute} }}\right)={120f \over {p}}\cdot \left({\frac {\mathrm {seconds} }{\mathrm {minute} }}\right)$.

For example, for a four-pole, three-phase motor, $p$ = 4 and $n_{s}={120f \over 4}$ = 1,500 RPM (for $f$ = 50 Hz) and 1,800 RPM (for $f$ = 60 Hz) synchronous speed.

The number of magnetic poles, $p$, is equal to the number of coil groups per phase. To determine the number of coil groups per phase in a 3-phase motor, count the number of coils, divide by the number of phases, which is 3. The coils may span several slots in the stator core, making it tedious to count them. For a 3-phase motor, if you count a total of 12 coil groups, it has 4 magnetic poles. For a 12-pole 3-phase machine, there will be 36 coils. The number of magnetic poles in the rotor is equal to the number of magnetic poles in the stator.

The two figures at right and left above each illustrate a 2-pole 3-phase machine consisting of three pole-pairs with each pole set 60° apart.

 Slip

ملف:Couple glissement MAs.svg Slip, $s$, is defined as the difference between synchronous speed and operating speed, at the same frequency, expressed in rpm, or in percentage or ratio of synchronous speed. Thus

$s={\frac {n_{s}-n_{r}}{n_{s}}}\,$

where $n_{s}$ is stator electrical speed, $n_{r}$ is rotor mechanical speed. Slip, which varies from zero at synchronous speed and 1 when the rotor is stalled, determines the motor's torque. Since the short-circuited rotor windings have small resistance, even a small slip induces a large current in the rotor and produces significant torque. At full rated load, slip varies from more than 5% for small or special purpose motors to less than 1% for large motors. These speed variations can cause load-sharing problems when differently sized motors are mechanically connected. Various methods are available to reduce slip, VFDs often offering the best solution.

 Torque

انظر أيضاً: Fleming's left-hand rule for motors

 Standard torque

Speed-torque curves for four induction motor types: A) Single-phase, B) Polyphase cage, C) Polyphase cage deep bar, D) Polyphase double cage

Typical speed-torque curve for NEMA Design B Motor

Transient solution for an AC induction motor from a complete stop to its operating point under a varying load.

The typical speed-torque relationship of a standard NEMA Design B polyphase induction motor is as shown in the curve at right. Suitable for most low performance loads such as centrifugal pumps and fans, Design B motors are constrained by the following typical torque ranges:

• Breakdown torque (peak torque), 175–300% of rated torque
• Locked-rotor torque (torque at 100% slip), 75–275% of rated torque
• Pull-up torque, 65–190% of rated torque.

Over a motor's normal load range, the torque's slope is approximately linear or proportional to slip because the value of rotor resistance divided by slip, $R_{r}'/s$, dominates torque in a linear manner. As load increases above rated load, stator and rotor leakage reactance factors gradually become more significant in relation to $R_{r}'/s$ such that torque gradually curves towards breakdown torque. As the load torque increases beyond breakdown torque the motor stalls.

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 Starting

انظر أيضاً: Motor controller

There are three basic types of small induction motors: split-phase single-phase, shaded-pole single-phase, and polyphase.

In two-pole single-phase motors, the torque goes to zero at 100% slip (zero speed), so these require alterations to the stator such as shaded-poles to provide starting torque. A single phase induction motor requires separate starting circuitry to provide a rotating field to the motor. The normal running windings within such a single-phase motor can cause the rotor to turn in either direction, so the starting circuit determines the operating direction.

Magnetic flux in shaded pole motor.

In certain smaller single-phase motors, starting is done by means of a copper wire turn around part of a pole; such a pole is referred to as a shaded pole. The current induced in this turn lags behind the supply current, creating a delayed magnetic field around the shaded part of the pole face. This imparts sufficient rotational field energy to start the motor. These motors are typically used in applications such as desk fans and record players, as the required starting torque is low, and the low efficiency is tolerable relative to the reduced cost of the motor and starting method compared to other AC motor designs.

Larger single phase motors are split-phase motors and have a second stator winding fed with out-of-phase current; such currents may be created by feeding the winding through a capacitor or having it receive different values of inductance and resistance from the main winding. In capacitor-start designs, the second winding is disconnected once the motor is up to speed, usually either by a centrifugal switch acting on weights on the motor shaft or a thermistor which heats up and increases its resistance, reducing the current through the second winding to an insignificant level. The capacitor-run designs keep the second winding on when running, improving torque. A resistance start design uses a starter inserted in series with the startup winding, creating reactance.

Self-starting polyphase induction motors produce torque even at standstill. Available squirrel-cage induction motor starting methods include direct-on-line starting, reduced-voltage reactor or auto-transformer starting, star-delta starting or, increasingly, new solid-state soft assemblies and, of course, variable frequency drives (VFDs).

Polyphase motors have rotor bars shaped to give different speed-torque characteristics. The current distribution within the rotor bars varies depending on the frequency of the induced current. At standstill, the rotor current is the same frequency as the stator current, and tends to travel at the outermost parts of the cage rotor bars (by skin effect). The different bar shapes can give usefully different speed-torque characteristics as well as some control over the inrush current at startup.

Although polyphase motors are inherently self-starting, their starting and pull-up torque design limits must be high enough to overcome actual load conditions.

In wound rotor motors, rotor circuit connection through slip rings to external resistances allows change of speed-torque characteristics for acceleration control and speed control purposes.

 Speed control

 Resistance

ملف:Variation-couple-uf.svg

Typical speed-torque curves for different motor input frequencies as for example used with variable-frequency drives

Before the development of semiconductor power electronics, it was difficult to vary the frequency, and cage induction motors were mainly used in fixed speed applications. Applications such as electric overhead cranes used DC drives or wound rotor motors (WRIM) with slip rings for rotor circuit connection to variable external resistance allowing considerable range of speed control. However, resistor losses associated with low speed operation of WRIMs is a major cost disadvantage, especially for constant loads. Large slip ring motor drives, termed slip energy recovery systems, some still in use, recover energy from the rotor circuit, rectify it, and return it to the power system using a VFD.

 Cascade

The speed of a pair of slip-ring motors can be controlled by a cascade connection, or concatenation. The rotor of one motor is connected to the stator of the other. If the two motors are also mechanically connected, they will run at half speed. This system was once widely used in three-phase AC railway locomotives, such as FS Class E.333. By the turn of this century, however, such cascade-based electromechanical systems became much more efficiently and economically solved using power semiconductor elements solutions.

 Variable-frequency drive

المقالة الرئيسية: Variable-frequency drive

In many industrial variable-speed applications, DC and WRIM drives are being displaced by VFD-fed cage induction motors. The most common efficient way to control asynchronous motor speed of many loads is with VFDs. Barriers to adoption of VFDs due to cost and reliability considerations have been reduced considerably over the past three decades such that it is estimated that drive technology is adopted in as many as 30–40% of all newly installed motors.

Variable frequency drives implement the scalar or vector control of an induction motor.

With scalar control, only the magnitude and frequency of the supply voltage are controlled without phase control (absent feedback by rotor position). Scalar control is suitable for application where the load is constant.

Vector control allows independent control of the speed and torque of the motor, making it possible to maintain a constant rotation speed at varying load torque. But vector control is more expensive because of the cost of the sensor (not always) and the requirement for a more powerful controller.

 Construction

Typical winding pattern for a three-phase (U, W, V), four-pole motor. Note the interleaving of the pole windings and the resulting quadrupole field.

The stator of an induction motor consists of poles carrying supply current to induce a magnetic field that penetrates the rotor. To optimize the distribution of the magnetic field, windings are distributed in slots around the stator, with the magnetic field having the same number of north and south poles. Induction motors are most commonly run on single-phase or three-phase power, but two-phase motors exist; in theory, induction motors can have any number of phases. Many single-phase motors having two windings can be viewed as two-phase motors, since a capacitor is used to generate a second power phase 90° from the single-phase supply and feeds it to the second motor winding. Single-phase motors require some mechanism to produce a rotating field on startup. Induction motors using a squirrel-cage rotor winding may have the rotor bars skewed slightly to smooth out torque in each revolution.

Standardized NEMA & IEC motor frame sizes throughout the industry result in interchangeable dimensions for shaft, foot mounting, general aspects as well as certain motor flange aspect. Since an open, drip proof (ODP) motor design allows a free air exchange from outside to the inner stator windings, this style of motor tends to be slightly more efficient because the windings are cooler. At a given power rating, lower speed requires a larger frame.

 Rotation reversal

The method of changing the direction of rotation of an induction motor depends on whether it is a three-phase or single-phase machine. A three-phase motor can be reversed by swapping any two of its phase connections. Motors required to change direction regularly (such as hoists) will have extra switching contacts in their controller to reverse rotation as needed. A variable frequency drive nearly always permits reversal by electronically changing the phase sequence of voltage applied to the motor.

In a single-phase split-phase motor, reversal is achieved by reversing the connections of the starting winding. Some motors bring out the start winding connections to allow selection of rotation direction at installation. If the start winding is permanently connected within the motor, it is impractical to reverse the sense of rotation. Single-phase shaded-pole motors have a fixed rotation unless a second set of shading windings is provided.

 Power factor

The power factor of induction motors varies with load, typically from around 0.85 or 0.90 at full load to as low as about 0.20 at no-load, due to stator and rotor leakage and magnetizing reactances. Power factor can be improved by connecting capacitors either on an individual motor basis or, by preference, on a common bus covering several motors. For economic and other considerations, power systems are rarely power factor corrected to unity power factor. Power capacitor application with harmonic currents requires power system analysis to avoid harmonic resonance between capacitors and transformer and circuit reactances. Common bus power factor correction is recommended to minimize resonant risk and to simplify power system analysis.

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 Efficiency

انظر أيضاً: Variable-frequency drive § Energy savings

Full-load motor efficiency is around 85–97%, related motor losses being broken down roughly as follows:

• Friction and windage, 5–15%
• Iron or core losses, 15–25%
• Stator losses, 25–40%
• Rotor losses, 15–25%
• Stray load losses, 10–20%.

For an electric motor, the efficiency, represented by the Greek letter Eta, is defined as the quotient of the output mechanical power and the input electric power, and calculated using this formula:

$\eta =OutputMechanicalPower\div InputElectricalPower$

Various regulatory authorities in many countries have introduced and implemented legislation to encourage the manufacture and use of higher efficiency electric motors. There is existing and forthcoming legislation regarding the future mandatory use of premium-efficiency induction-type motors in defined equipment. For more information, see: Premium efficiency.

 Steinmetz equivalent circuit

Many useful motor relationships between time, current, voltage, speed, power factor, and torque can be obtained from analysis of the Steinmetz equivalent circuit (also termed T-equivalent circuit or IEEE recommended equivalent circuit), a mathematical model used to describe how an induction motor's electrical input is transformed into useful mechanical energy output. The equivalent circuit is a single-phase representation of a multiphase induction motor that is valid in steady-state balanced-load conditions.

The Steinmetz equivalent circuit is expressed simply in terms of the following components:

• Stator resistance and leakage reactance ($R_{s}$, $X_{s}$).
• Rotor resistance, leakage reactance, and slip ($R_{r}$, $X_{r}$ or $R_{r}'$, $X_{r}'$, and $s$).
• Magnetizing reactance ($X_{m}$).

Paraphrasing from Alger in Knowlton, an induction motor is simply an electrical transformer the magnetic circuit of which is separated by an air gap between the stator winding and the moving rotor winding. The equivalent circuit can accordingly be shown either with equivalent circuit components of respective windings separated by an ideal transformer or with rotor components referred to the stator side as shown in the following circuit and associated equation and parameter definition tables.

Steinmetz equivalent circuit

The following rule-of-thumb approximations apply to the circuit:

• Maximum current happens under locked rotor current (LRC) conditions and is somewhat less than $V_{\text{s}}/X$, with LRC typically ranging between 6 and 7 times rated current for standard Design B motors.
• Breakdown torque $T_{\text{max}}$ happens when $s\approx R_{\text{r}}'/X$ and $I_{\text{s}}\approx 0.7\;LRC$ such that $T_{\text{max}}\approx KV_{\text{s}}^{2}/2X$ and thus, with constant voltage input, a low-slip induction motor's percent-rated maximum torque is about half its percent-rated LRC.
• The relative stator to rotor leakage reactance of standard Design B cage induction motors is

  ${\frac {X_{\text{s}}}{X_{\text{r}}'}}\approx {\frac {0.4}{0.6}}$.

• Neglecting stator resistance, an induction motor's torque curve reduces to the Kloss equation

  $T_{\text{em}}\approx {\frac {2T_{\text{max}}}{{\frac {s}{s_{\text{max}}}}+{\frac {s_{\text{max}}}{s}}}}$, where $s_{\text{max}}$ is slip at $T_{\text{max}}$.

Circuit parameter definitions
		Units
$f$	stator source frequency	Hz
$f_{\text{s}}$	stator synchronous frequency	Hz
$n_{\text{r}}$	rotor speed in revolutions per minute	rpm
$n_{\text{s}}$	synchronous speed in revolutions per minute	rpm
$I_{\text{s}}$	stator or primary current	A
$I_{\text{r}}'$	rotor or secondary current referred to stator side	A
$I_{\text{m}}$	magnetizing current	A
$j={\sqrt {-1}}$	imaginary number, or 90° rotation, operator
$K_{\text{TE}}$	$=X_{m}/\left(X_{s}+X_{m}\right)$ Thévenin reactance factor
$m$	number of motor phases
$p$	number of motor poles
$P_{\text{em}}$	electromechanical power	W or hp
$P_{\text{gap}}$	air gap power	W
$P_{\text{r}}$	rotor copper losses	W
$P_{\text{o}}$	input power	W
$P_{\text{h}}$	core loss	W
$P_{\text{f}}$	friction and windage loss	W
$P_{\text{rl}}$	running light watts input	W
$P_{\text{sl}}$	stray-load loss	W
$R_{\text{s}},X_{\text{s}}$	stator or primary resistance and leakage reactance	Ω
$R_{\text{r}}',X_{\text{r}}'$	rotor or secondary resistance & leakage reactance referred to the stator side	Ω
$R_{\text{o}},X_{\text{o}}$	resistance & leakage reactance at motor input	Ω
$R_{\text{TE}},X_{\text{TE}}$	Thévenin equivalent resistance & leakage reactance combining $R_{\text{s}},X_{\text{s}}$ and $X_{m}$	Ω
$s$	slip
$T_{\text{em}}$	electromagnetic torque	Nm or ft-lb
$T_{\text{max}}$	breakdown torque	Nm or ft-lb
$V_{\text{s}}$	impressed stator phase voltage	V
$X_{\text{m}}$	magnetizing reactance	Ω
$X$	$X_{s}+X_{r}'$	Ω
$Z_{\text{s}}$	stator or primary impedance	Ω
$Z_{\text{r}}'$	rotor or secondary impedance referred to the primary	Ω
$Z_{\text{o}}$	impedance at motor stator or primary input	Ω
$Z$	combined rotor or secondary and magnetizing impedance	Ω
$Z_{\text{TE}}$	Thévenin equivalent circuit impedance, $R_{\text{TE}}+X_{\text{TE}}$	Ω
$\omega _{\text{r}}$	rotor speed	rad/s
$\omega _{\text{s}}$	synchronous speed	rad/s
$Y$	$=G+jB={\frac {1}{Z}}={\frac {1}{R+jX}}={\frac {R}{Z^{2}}}-{\frac {jX}{Z^{2}}}$	S or Ʊ
$\left\vert Z\right\vert$	${\sqrt {R^{2}+X^{2}}}$	Ω

Basic electrical equations

$\omega _{\text{s}}={\frac {2\pi n_{\text{s}}}{60}}=2\pi f_{\text{s}}={\frac {4\pi f}{p}}$ Motor input equivalent impedance $Z_{\text{m}}=R_{\text{s}}+jX_{\text{s}}+{\frac {\left({\frac {1}{s}}R_{\text{r}}'+jX_{r}'\right)(jX_{\text{m}})}{{\frac {1}{s}}R_{\text{r}}'+j\left(X_{\text{r}}'+X_{\text{m}}\right)}}$ Stator current $I_{\text{s}}=V_{\text{s}}/Z_{\text{m}}=V_{\text{s}}/\left(R_{\text{s}}+jX_{\text{s}}+{\frac {\left({\frac {1}{s}}R_{\text{r}}'+jX_{\text{r}}'\right)(jX_{\text{m}})}{{\frac {1}{s}}R_{\text{r}}'+j\left(X_{\text{r}}'+X_{m}\right)}}\right)$ Rotor current referred to the stator side in terms of stator current $I_{\text{r}}'={\frac {jX_{m}}{{\frac {1}{s}}R_{\text{r}}'+j\left(X_{\text{r}}'+X_{\text{m}}\right)}}I_{\text{s}}$

Power equations

From Steinmetz equivalent circuit, we have ${\frac {1}{s}}R_{\text{r}}'=R_{\text{r}}'{\frac {1-s}{s}}+R_{\text{r}}'$ That is, air gap power is equal to electromechanical power output plus rotor copper losses ${\begin{aligned}P_{\text{gap}}&=P_{\text{em}}+P_{r}\\P_{r}&=3R_{\text{r}}'I_{\text{r}}^{\prime 2}\\P_{\text{gap}}&={\frac {3R_{\text{r}}'I_{\text{r}}^{\prime 2}}{s}}\\P_{\text{em}}&=3R_{\text{r}}'I_{\text{r}}^{\prime 2}{\frac {1-s}{s}}\\P_{\text{em}}&=P_{\text{gap}}(1-s)\end{aligned}}$ Expressing electromechanical power output in terms of rotor speed $P_{\text{em}}={\frac {3R_{\text{r}}'I_{\text{r}}^{\prime 2}n_{\text{r}}}{sn_{\text{s}}}}$ (watts) $P_{\text{em}}={\frac {3R_{\text{r}}'I_{\text{r}}^{\prime 2}n_{\text{r}}}{746\;sn_{\text{s}}}}$ (hp) Expressing $T_{\text{em}}$ in ft-lb: $P_{\text{em}}={\frac {T_{\text{em}}n_{\text{r}}}{5252}}$ (hp)

Torque equations

$T_{\text{em}}={\frac {P_{\text{em}}}{\omega _{r}}}={\frac {\frac {P_{\text{r}}}{s}}{\omega _{s}}}={\frac {3I_{\text{r}}^{\prime 2}R_{\text{r}}'}{\omega _{\text{s}}s}}$ (newton-meters) In order to be able to express $T_{\text{em}}$ directly in terms of $s$, IEEE recommends that $R_{\text{s}},X_{\text{s}}$ and $X_{\text{m}}$ be converted to the Thévenin equivalent circuit IEEE recommended Thévenin equivalent circuit where $V_{\text{TE}}={\frac {X_{\text{m}}}{\sqrt {R_{\text{s}}^{2}+(X_{\text{s}}+X_{\text{m}})^{2}}}}V_{\text{s}}$ $Z_{\text{TE}}=R_{\text{TE}}+jX_{\text{TE}}={\frac {jX_{\text{m}}\left(R_{\text{s}}+jX_{\text{s}}\right)}{R_{\text{s}}+j\left(X_{\text{s}}+X_{\text{m}}\right)}}$ Since $R_{\text{s}}^{2}\gg {\left(X_{\text{s}}+X_{\text{m}}\right)^{2}}$ and $X_{\text{s}}\ll X_{\text{m}}$, and letting $K_{\text{TE}}={\frac {X_{\text{m}}}{X_{\text{s}}+X_{\text{m}}}}$ $V_{\text{TE}}\approx Z_{\text{TE}}V_{\text{s}}$ and $Z_{\text{TE}}\approx K_{\text{TE}}^{2}R_{\text{s}}+jX_{\text{s}}$ $T_{\text{em}}={\frac {3V_{\text{TE}}^{2}}{\left(R_{\text{TE}}+{\frac {1}{s}}R_{\text{r}}'\right)^{2}+\left(X_{\text{TE}}+X_{r}'\right)^{2}}}\cdot {\frac {1}{s}}R_{\text{r}}'\cdot {\frac {1}{\omega _{\text{s}}}}$ (N·m) For low values of slip: Since $R_{\text{TE}}+R_{\text{r}}'\gg R_{\text{TE}}+X_{\text{r}}'$ and $R_{\text{r}}'\gg R_{\text{TE}}$ $T_{\text{em}}\approx {\frac {1}{\omega _{\text{s}}}}\cdot {\frac {3V_{\text{TE}}^{2}}{R_{\text{r}}'}}s$ (N·m) For high values of slip Since $R_{\text{TE}}+R_{r}'\ll R_{\text{TE}}+X_{r}'$ $T_{\text{em}}\approx {\frac {1}{\omega _{\text{s}}}}\cdot {\frac {3V_{\text{TE}}^{2}}{\left(X_{\text{s}}+X_{\text{r}}'\right)^{2}}}\cdot {\frac {R_{\text{r}}^{\prime 2}}{s}}$ (N·m) For maximum or breakdown torque, which is independent of rotor resistance $T_{\text{max}}={\frac {1}{2\omega _{s}}}\cdot {\frac {3V_{\text{TE}}^{2}}{R_{\text{TE}}+{\sqrt {R_{\text{TE}}^{2}+(X_{\text{TE}}+X_{\text{r}}')^{2}}}}}$ (N·m) Corresponding slip at maximum or breakdown torque is $s={\frac {R_{\text{r}}'}{\sqrt {R_{\text{TE}}^{2}+\left(X_{\text{TE}}+X_{\text{r}}'\right)^{2}}}}$ In foot-pound units $T_{\text{em}}={\frac {21.21\;I_{r}^{\prime 2}R_{\text{r}}'}{n_{\text{r}}s}}$ (ft-lb) $T_{\text{em}}={\frac {7.04\;P_{\text{gap}}}{n_{\text{s}}}}$ (ft-lb)

 Linear induction motor

المقالة الرئيسية: Linear induction motor

Linear induction motors, which work on the same general principles as rotary induction motors (frequently three-phase), are designed to produce straight line motion. Uses include magnetic levitation, linear propulsion, linear actuators, and liquid metal pumping.

 See also

• AC motor
• Circle diagram
• Induction generator
• Premium efficiency
• Variable refrigerant flow

 Classical sources

• Bailey, Benjamin Franklin (1911). The Induction Motor. McGraw-Hill. induction motor.
• Behrend, Bernhard Arthur (1901). The Induction Motor: A Short Treatise on its Theory and Design, With Numerous Experimental Data and Diagrams. McGraw Publishing Company / Electrical World and Engineer.
• Boy de la Tour, Henri (1906). The Induction Motor: Its Theory and Design, Set Forth By a Practical Method of Calculation. Translated Cyprien Odilon Mailloux. McGraw Pub. Co.

 External links

• Who Invented the Polyphase Electric Motor?
• Silvanus Phillips Thompson: Polyphase electric currents and alternate current motors
• Induction motor topics from Hyperphysics website hosted by C.R. Nave, GSU Physics and Astronomy Dept.
• Cowern Papers