The single phase induction motor is the most widely used electric motor in the world, found in refrigerators, pumps, air conditioners, workshop tools and nearly every ventilation fan. It runs directly from the single-phase supply that powers homes, farms and small businesses, and it needs no brushes, no commutator and very little maintenance. Its simplicity hides an engineering problem, though: a 1 phase induction motor produces no starting torque on its own, which is why a single phase induction motor is not self starting. This guide explains the single phase motor working principle, the main types of single phase induction motors, and how they compare in a single phase vs three phase induction motor choice. It ends with how engineers troubleshoot, test, validate and select a one phase induction motor or single phase induction machine, drawing on Impedyme’s experience in real-time testing and power hardware in the loop.
A single phase induction motor is an AC motor that runs from a single-phase supply and turns electrical energy into shaft rotation through electromagnetic induction. Nothing is wired to the rotating part.
In practice, the 1 phase induction motor has two stator windings, a main (running) winding and an auxiliary (starting) winding, wrapped around a squirrel-cage rotor. It has no brushes, commutator or slip rings. The machine is asynchronous: the rotor always turns a little slower than the stator field. That speed difference, called slip, is what induces rotor current and torque. At rated load, slip is typically 3–6 %.
Ratings run from a few watts in small fans to about 3 kW in pumps and compressors. Supplies are 110–120 V or 220–240 V at 50 or 60 Hz. Pole count and supply frequency set the speed:
| Poles | Synchronous speed (60 Hz) / Typical full-load speed | Synchronous speed (50 Hz) / Typical full-load speed |
|---|---|---|
| 2 | 3600 rpm / ≈3450 rpm | 3000 rpm / ≈2850 rpm |
| 4 | 1800 rpm / ≈1725 rpm | 1500 rpm / ≈1425 rpm |
| 6 | 1200 rpm / ≈1140 rpm | 1000 rpm / ≈950 rpm |
| 8 | 900 rpm / ≈860 rpm | 750 rpm / ≈710 rpm |
Here is a worked example. On a 60 Hz supply, a four-pole motor’s field turns at 1800 rpm. At full load the rotor falls behind by about 4 %, so the nameplate reads close to 1725 rpm. The same motor on 50 Hz reads about 1425 rpm.
Homes, farms, small workshops and most light-commercial buildings get only single-phase service. That makes the single phase induction machine the default motor wherever three-phase power is unavailable. It also has one built-in weakness that shapes the rest of this article: on its own, it cannot start. Every variant described below exists to solve that starting problem.
The single phase induction motor has five assemblies: the stator and its two windings, the squirrel-cage rotor, the bearings and end shields, the enclosure and cooling system, and the starting components (switch or relay plus capacitors). Mechanically it is very close to a small three-phase motor. The only electrical difference is on the stator side, where two windings and their starting hardware take the place of a balanced three-phase winding. North American motors use fractional- and integral-horsepower frame designations. Elsewhere, IEC frame sizes based on shaft height apply. Enclosures are described as open drip-proof or totally enclosed, or by an IEC ingress-protection code such as IP44, IP54 or IP55.
In a 1 phase induction motor, the stator core is a stack of thin, insulated silicon-steel laminations. Laminating the core keeps eddy-current losses down. Small machines commonly have 24 or 36 slots, and insulated copper (sometimes aluminum) coils are distributed through them.
The two windings are built for opposite jobs:
The two windings sit 90 electrical degrees apart in space. That spacing is only half of what a rotating field needs. The other half is a time difference between the two currents. Every starting method in this article, whether resistance, capacitor or shading coil, exists to create a time-phase difference between the currents in these two windings.
The rotor is a laminated steel core whose slots hold aluminum bars (copper in some premium designs), usually die-cast in one shot. End rings short the bars together at both ends. The cage has no electrical connection to the supply; all of its current is induced. The bars are skewed, set at a slight angle along the stack, to reduce cogging, slot-harmonic torques and magnetic whine.
Wound rotors are essentially never used in a single phase induction machine. Slip rings and brushes would add cost, maintenance and sparking to a machine whose whole appeal is being simple and sealed. Rotor resistance is still a design lever, set through bar material and cross-section. Narrow bars or aluminum alloy raise resistance, which boosts starting torque but increases running slip and rotor loss. Large or copper bars do the reverse: lower slip and better efficiency, at the cost of weaker starting torque.
Sleeve bearings, which are oil-impregnated bronze, are quiet and cheap. They suit low-load appliance fans and blowers. Ball bearings handle radial belt pull and axial thrust, and they belong in belt-driven pumps, compressors and workshop machines. The end shields hold the bearings concentric so the rotor sits in a small, uniform air gap, a few tenths of a millimetre in fractional-kilowatt machines. The gap is kept small because air is a poor magnetic path: every extra fraction of a millimetre raises magnetizing current and lowers power factor.
Cooling in a one phase induction motor comes from a shaft-mounted fan. Open drip-proof (ODP) enclosures pull air through the windings and suit clean indoor locations. Totally enclosed fan-cooled (TEFC) enclosures blow air over a finned frame and suit dusty, damp or outdoor sites. Insulation is usually Class B (130 °C) or Class F (155 °C). Most motors also carry a thermal protector, a bimetal disc or thermistor embedded in or against the winding, which opens the circuit on stall or sustained overload. It may reset automatically or manually.
The auxiliary circuit has to be disconnected or reconfigured once the motor is up to speed. Several devices do this:
There are two capacitor families:
| Property | Start capacitor | Run capacitor |
|---|---|---|
| Construction | Non-polarized aluminum electrolytic | Metallized polypropylene film, oil-filled or dry |
| Duty | Intermittent; standard rating is 20 starts per hour of 3 s each | Continuous |
| Typical capacitance | 50–1200 µF | 2.5–100 µF |
| Typical voltage ratings | 110/125, 165, 220/250, 330 VAC | 370 or 440 VAC |
| Tolerance | Wide (often −0/+20 % or a µF range) | Tight (about ±5–6 %) |
The single phase motor working principle starts with the main winding of the single phase induction motor. Alternating current in that winding produces a magnetic flux that stays fixed along the winding axis. It grows, collapses and reverses polarity twice per cycle, but it does not rotate. This pulsating flux cuts the rotor bars and induces currents in them, much as a transformer induces current in a shorted secondary. With the rotor of a 1 phase induction motor at rest, the forces on the bars push equally both ways around the shaft, and nothing happens except heat and hum. Once the rotor is already turning, the same pulsating field produces useful torque in the direction of rotation.
Engineers explain the behavior of a single phase induction machine with two complementary models: the double revolving field theory and the cross-field theory.
A pulsating field fixed in space is mathematically identical to two fields of half its peak strength, rotating in opposite directions at synchronous speed. One is the forward field, the other the backward field. Each one acts on the rotor as if it were a separate three-phase-style motor.
At standstill, the rotor slips equally against both fields. The two torques are equal and opposite, so net torque is zero. Once the rotor turns, say forward, its slip against the forward field becomes small (a few per cent), while its slip against the backward field approaches 2, meaning the backward field sweeps past the rotor at nearly twice synchronous speed. At such high slip, rotor reactance dominates, the backward field induces large but poorly coupled currents, and its torque collapses. Forward torque wins, and the one phase induction motor keeps running in whichever direction it was pushed.
The model also predicts four practical consequences:
The cross-field picture of a single phase induction motor starts from the moving rotor. Spinning rotor conductors cut the stator flux and generate a speed EMF. That EMF drives rotor currents whose flux lies at right angles (in quadrature) to the stator axis and lags the stator flux by roughly a quarter cycle. Two fluxes 90° apart in space and roughly 90° apart in time combine into a field that rotates, close to circular near synchronous speed and fading to nothing at standstill.
The two models fit different jobs. Cross-field theory is the convenient way to understand running behavior and the quadrature field. Double revolving field theory is the one to use for torque-speed curves and equivalent-circuit work.
At standstill in a single phase induction motor, the forward and backward torques are equal and cancel, so the starting torque is zero. The evidence is easy to see on a bench. A 1 phase induction motor with an open starting circuit hums loudly, draws close to full locked-rotor current and heats quickly. Give the shaft a firm spin by hand while it is energized and it accelerates and runs, in whichever direction it was spun.
That stalled state is dangerous. Locked-rotor current is typically five to eight times rated current.
The fix is simple: add a second winding whose current is shifted in time from the main winding current. That is exactly how the five motor types differ.
To read the torque-speed curve of a single phase induction motor, follow it from left to right:
Typical starting torque as a percentage of full-load torque:
Motor Type Starting Torque (% FLT) Breakdown Torque (% FLT)
Shaded-pole 25–50% ≈100–150%
Permanent split capacitor (PSC) 50–100% ≈150–200%
Split-phase 100–175% ≈200–250%
Capacitor-start 200–300%+ ≈200–300%
Capacitor-start, capacitor-run (CSCR) 200–300% ≈200–300%
Load matching follows from the curve. Fans and centrifugal blowers have square-law torque: almost nothing at standstill, rising with the square of speed. A PSC or shaded-pole motor with a gentle curve suits them. Positive-displacement compressors starting against head pressure, loaded conveyors, and pumps with sticky seals or a partial jam need high breakaway torque, which means a capacitor-start or two-value capacitor motor.
The double-frequency torque pulsation is always present in a single phase induction machine. It is strongest in switch-type motors running on the main winding alone and weakest in motors with a well-sized run capacitor. It shows up as 100/120 Hz hum, as vibration passed into the frame, and as fatigue in rigid mounts. That is why appliance and HVAC fan motors are usually held in resilient rubber rings or isolation mounts.
All five types differ in only two ways: how the auxiliary circuit creates the phase shift, and whether it stays connected once the motor is up to speed.
Type Starting characteristics Efficiency, power factor, rating, and uses
Split-phase Phase shift: Aux-winding resistance (≈25–30°); aux circuit: disconnected at speed; starting torque: 100–175% FLT; starting current: high Peak efficiency: 50–60%; power factor: 0.6–0.7; rating: 0.06–0.75 kW; uses: grinders, small belt fans, office machines
Capacitor-start Phase shift: Electrolytic capacitor (≈70–90°); aux circuit: disconnected at speed; starting torque: 200–300%+ FLT; starting current: moderate Peak efficiency: 50–65%; power factor: 0.6–0.7; rating: 0.18–1.5 kW; uses: compressors, jet pumps, conveyors
Two-value capacitor (CSCR) Phase shift: Start + run capacitor; aux circuit: run capacitor stays; starting torque: 200–300% FLT; starting current: moderate Peak efficiency: 60–75%; power factor: 0.8–0.95+; rating: 0.75–3 kW; uses: large pumps, air compressors, machine tools
PSC Phase shift: Run capacitor only; aux circuit: stays connected; starting torque: 50–100% FLT; starting current: low Peak efficiency: 55–70%; power factor: 0.8–0.95+; rating: 10 W–0.75 kW; uses: fans, blowers, HVAC air handlers
Shaded pole Phase shift: Copper shading ring; aux circuit: N/A; starting torque: 25–50% FLT; starting current: low Peak efficiency: 20–40%; power factor: 0.5–0.6; rating: 2–100 W; uses: oven, freezer, and humidifier fans
In a split-phase single phase induction motor, the high-resistance auxiliary winding produces only about 25–30 degrees of displacement between the two currents. That is enough to start the motor, but it makes a weak, elliptical field. A centrifugal switch (or a current relay in small hermetic units) disconnects the winding at roughly three-quarters of synchronous speed. Starting torque is modest. Starting current is high because the two currents are nearly in phase and add almost directly. Starting duty is strictly intermittent. Typical sizes for this 1 phase induction motor are 60 W to 0.75 kW, driving small belt-driven fans, bench grinders, washing machines and office machines. The dominant failure is frequent starting or slow acceleration that cooks the finely wound auxiliary winding.
An electrolytic start capacitor in series with the auxiliary winding pushes that winding’s current ahead of the voltage. That brings the displacement close to 90 degrees, giving the highest starting torque in the family at moderate starting current. The capacitor and auxiliary winding switch out at speed, so running performance is that of a plain single phase induction machine. Start capacitors range from roughly 60–110 µF on 1/4 hp to 216–300 µF on 1 hp 115 V motors, rated 125 or 250 VAC. Their duty limit is typically 20 starts per hour of about three seconds each. Exceeding it is the classic cause of a burst capacitor. Applications include refrigeration and air compressors, jet and well pumps, conveyors and farm equipment.
This type adds a smaller, continuously rated film run capacitor that stays in circuit, alongside the large electrolytic start capacitor that a switch or voltage relay removes. It gets the high starting torque of the capacitor-start design, plus better running power factor and efficiency, lower running current and noticeably reduced 100/120 Hz pulsation, because the motor runs close to balanced two-phase at rated load. The costs are two capacitors, a switch or relay, and a higher price. It is the usual single phase induction motor choice for larger pumps, air compressors, woodworking and metalworking machine tools up to around 3 kW.
A single run capacitor stays in series with the auxiliary winding at all times. With no switch and no relay, it is very reliable and the quietest small one phase induction motor. Because the capacitor is sized for running rather than starting, starting torque is low, which limits PSC motors to fans, blowers and direct-drive loads. Running efficiency and power factor are good. Because nothing switches with speed, the PSC tolerates voltage-based and drive-based speed control. When the main and auxiliary windings are identical, moving the capacitor from one winding to the other reverses rotation. That is how reversible gate and actuator motors work.
The stator of a shaded pole single phase induction machine has salient poles. A heavy copper shading ring around part of each pole face delays the flux in that section, so the field sweeps from the unshaded to the shaded side and drags the rotor along. The motor is extremely simple and cheap, with no capacitor or switch. On the other hand, starting torque is very low, efficiency is poor (often 20–30 %, sometimes lower), and the direction is fixed by where the ring sits. Sizes run from a few watts to about 100 W in oven, refrigerator and freezer evaporator fans, humidifiers and small blowers. Efficiency regulations are steadily pushing these applications toward electronically commutated (EC) motors. An Oak Ridge National Laboratory study of commercial-refrigeration evaporator fans, sponsored by the US Department of Energy, puts state-of-the-art EC motors at approximately 66 % efficiency, against approximately 20 % for shaded-pole units and about 29 % for PSC motors.
The equivalent circuit of a 1 phase induction motor turns the double revolving field theory into a circuit diagram. It starts with the stator: winding resistance and leakage reactance in series, carrying the full line current. After that, the circuit splits into two series-connected sections. One represents the forward field and one the backward field. Each holds half of the magnetizing reactance and half of the rotor leakage reactance and resistance. The rotor resistance in each branch depends on slip. In the forward branch it looks very large near running speed, which represents converted mechanical power. In the backward branch it looks small, close to half its standstill value, which represents braking torque and extra heat.
At standstill the two branches are identical, which makes the zero starting torque obvious. Near rated speed the forward branch takes most of the voltage, and the backward branch becomes a small loss path.
With this circuit, engineers predict input current, power factor, torque, losses and efficiency at any slip from a handful of parameters, without building the single phase induction motor. The same parameters feed simulation models of the motor and its controller, including the real-time models that run on FPGA or CPU targets in Hardware in the loop work, where an appliance board or drive interacts with a simulated machine.
When the auxiliary winding stays connected, as in PSC and two-value motors, the simple model is not enough. The motor is treated as an unbalanced two-phase machine. Main and auxiliary currents are resolved into forward and backward components (the two-winding revolving-field model), and the capacitor and turns ratio appear explicitly.
These two bench tests extract the equivalent-circuit parameters of a single phase induction motor. Both are done with the auxiliary circuit open, except on capacitor-run designs, where the test plan must account for it.
No-load test. Run the one phase induction motor uncoupled at rated voltage and frequency, with the auxiliary circuit out once the motor is up to speed. Record voltage, current, input power and speed. Slip is nearly zero, so the input power is almost entirely core loss plus friction and windage. Repeating the test at several reduced voltages separates the two, because friction and windage stay constant while core loss falls with voltage. The current and power factor define the magnetizing branch.
Blocked-rotor test. Lock the shaft (with the auxiliary winding open, the motor will not start anyway). Raise a reduced voltage until rated current flows, then record voltage, current and power. Magnetizing current is negligible here, so the readings give the series impedance: stator plus rotor resistance and leakage reactance, and full-current copper loss.
Practical cautions:
A three-phase motor produces a constant-amplitude rotating field directly from its supply. A single-phase motor has to fake one. Nearly every difference between the two follows from that.
Attribute Single phase induction motor Three phase induction motor
Self-starting No; needs auxiliary circuit Yes
Field type Pulsating (forward + backward) Constant rotating
Starting torque 25–300 %, depending on type 150–275 % (NEMA Designs A–D)
Efficiency and power factor Lower; 0.5–0.95 PF depending on capacitor Higher; typically 0.75–0.9 PF
Torque ripple and noise Inherent 100/120 Hz pulsation Essentially smooth
Frame size and weight Larger for the same output Smaller, lighter
Locked-rotor current (1 hp, 230 V, NEMA limit) 45 A 31.3 A
Supply availability Everywhere, including homes Industrial and commercial sites
Cost and maintenance Higher per kW; switches and capacitors wear Lower per kW; no starting parts
Practical ceiling ≈3 kW typical; rare above 7.5 kW Megawatts
Above roughly 2 kW, a three-phase motor fed from a single-phase-input drive or a phase converter is usually the better answer. That route changes the installation. The drive’s input current is much higher per conductor than the motor’s line current, so feeders and breakers must be sized from the drive’s single-phase input rating. A three-phase-rated drive run on single-phase input is typically derated to about half its nameplate power. Motor cable length, shielding and grounding need attention. In exchange, the motor gets soft starting, variable speed and no starting switch to fail.
There are three practical routes to control the speed of a single phase induction motor, each with limits:
Slip is unavoidable, because without it the rotor induces no current and makes no torque. As load rises, speed falls a few per cent. Where speed has to be tightly regulated, the usual answer is a different motor technology, such as an EC or permanent-magnet motor, or a three-phase motor on a closed-loop drive, rather than more control added to a single phase induction motor.
The loss budget of a single phase induction machine has five parts:
Typical full-load efficiency ranges from 20–40 % for shaded-pole motors and 50–60 % for fractional split-phase and capacitor-start machines, through 55–70 % for PSC motors, up to about 70–80 % for well-designed two-value capacitor motors at 1–3 kW. A small one phase induction motor loses out to its three-phase equivalent for structural reasons: one winding carries all the current, the backward field adds rotor loss without adding torque, and the larger magnetizing current in small frames drags the power factor down. NEMA reflects this in reverse by requiring small polyphase motors to deliver at least 140 % of the breakdown torque of a single-phase motor with the same rating.
In a single phase induction motor, the run capacitor supplies leading reactive current that offsets the lagging magnetizing current. That lifts the power factor from about 0.6–0.7 in switch-type motors to 0.8–0.95 or higher in PSC and two-value designs, and it lowers line current for the same output.
Expect derating when a 1 phase induction motor runs away from nominal conditions. Motors are generally designed for ±10 % voltage. At low voltage, torque falls with the square of voltage and current rises. At high voltage, magnetizing current and core loss climb. Above a 40 °C ambient or 1000 m altitude, output must be reduced to hold the insulation-class temperature limit.
Efficiency classes are defined by the IEC classification standard for line-operated AC motors (the IE code), which covers motors from 0.12 kW to 1000 kW, including the single phase induction machine. For a four-pole 50 Hz motor, the standard’s IE2 minimums are 59.1 % at 0.12 kW, 72.7 % at 0.37 kW, 79.6 % at 0.75 kW and 84.3 % at 2.2 kW. Losses are measured with the IEC loss test-method standard or the IEEE test procedure for single-phase induction motors, which US Department of Energy rules incorporate by reference for single-phase small electric motors. Since 1 July 2023, the European Union’s motor ecodesign regulation has required single-phase motors rated 0.12 kW and above to reach at least IE2, a level many shaded-pole and split-phase designs cannot reach.
The right single phase induction motor for each industry follows from its torque curve and duty cycle:
Single phase motor hums but won’t start. The starting circuit is not producing a phase-shifted current, or the load is locked. Check for:
A quick test: spin the shaft of the 1 phase induction motor by hand with power applied, using a safe method. If the motor runs, the fault is in the starting circuit.
Runs hot. Possible causes are over- or undervoltage, blocked ventilation or a clogged fan cover, mechanical overload, a start switch that never opens, or shorted turns.
Runs slow or stalls under load. Possible causes are low supply voltage or undersized wiring, a wrong or degraded run capacitor, worn bearings, or a load that exceeds breakdown torque.
Repeated thermal trips. Look for too many starts per hour, high ambient temperature, low voltage during starting, or a failing capacitor that stretches acceleration time.
Noise and vibration. Causes include bearing wear, a loose end shield or through-bolts, rotor rub, and the inherent 100/120 Hz pulsation, which mounts must isolate.
Bulging, leaking or vented capacitor. This means overvoltage, excess start duty, heat or end of life. Replace it with an identical µF value and an equal or higher voltage rating.
Confirming measurements on a one phase induction motor:
A complete validation chain for a single phase induction motor moves from simple checks to long-duration runs:
The supply side matters as much as the motor. Wall power is a poor test source. Its voltage moves with building load, its frequency drifts slightly, its harmonic distortion is unknown, and no two runs see the same conditions. Single phase induction machine behavior is very sensitive to all of these: torque scales with voltage squared, capacitor current scales with frequency, and harmonics add heating. A programmable single-phase AC source or grid emulator lets engineers apply controlled sags, swells, brownouts, short interruptions, frequency deviations, harmonic distortion and identical start sequences hundreds of times. These are the conditions defined in the IEC immunity test standard for voltage dips, short interruptions and voltage variations on equipment drawing up to 16 A per phase, whose test levels are dips to residual voltages of 0 %, 40 %, 70 % and 80 % of nominal; a companion IEC standard covers equipment above 16 A per phase. Impedyme’s grid emulator, part of the CHP Series, provides regenerative single-, split- and three-phase AC sources for this kind of supply-disturbance testing.
Power hardware-in-the-loop (P-HIL) extends this in two directions. First, the mechanical load can be emulated in real time instead of using a mechanical dynamometer: a real-time model of a compressor, pump or fan sets the load torque profile, so a motor can be tested against a jammed pump or a high-head compressor start without building one. Second, the motor itself can be emulated as an electrical load. An FPGA-based motor emulator runs an equivalent-circuit model fast enough to draw realistic currents from a DC motor controller , appliance board or inverter test.That lets the electronics be validated, including fault injection such as an open start winding or a failed capacitor, before a real motor exists. Impedyme’s motor emulator supports induction machine models for this purpose, and Impedyme’s P-HIL systems combine real-time simulation and regenerative power stages so that source, load and machine can be emulated together in one closed loop.
Selection checklist:
To read the nameplate of a single phase induction machine, check rated voltage and frequency, full-load amps, rated speed (which tells you the pole count), output in kW or hp, service factor, insulation class, ambient rating, duty (continuous or short-time), thermal protection type, frame, enclosure, the locked-rotor code letter, and the capacitor µF and voltage ratings.
The pulsating field explains the two defining traits of the single phase induction motor: zero torque at standstill and a constant 100/120 Hz hum while running.
Split-phase, capacitor-start, two-value capacitor, PSC and shaded-pole motors are five answers to the same starting problem. They trade starting torque, efficiency, noise and cost in different proportions.
Selection comes down to matching the torque-speed curve and duty cycle to the load. The proof that a choice works comes from controlled bench testing under realistic supply conditions, not from the nameplate alone.
The one phase induction motor will stay in service wherever only single-phase power is available, and choosing the right 1 phase induction motor or single phase induction machine will still start with its torque curve and duty cycle. Tightening efficiency regulations, however, are steadily moving fractional-kilowatt fan and pump loads toward electronically commutated alternatives to the single phase induction motor.
Why does a single phase induction motor need a capacitor?
The capacitor shifts the auxiliary winding’s current ahead of the main winding’s current in time. Combined with the 90° spatial offset, that shift creates a rotating field and starting torque. Run capacitors also improve power factor and smooth running.
Can a single phase motor run without its capacitor?
A capacitor-start motor will not start without its capacitor, but it runs if spun by hand. A PSC motor might creep or stall, then overheat. Either way, running without the specified capacitor quickly overheats windings and voids the design rating.
How do you reverse a single phase induction motor?
Swap the two leads of the auxiliary winding relative to the main winding, with the motor stopped.On PSC motors with identical windings, move the capacitor to the other winding. Shaded-pole motors need the stator flipped mechanically.
What is the most efficient single phase induction motor type? The capacitor-start capacitor-run (two-value) design is usually most efficient, followed by PSC, because the run capacitor approximates balanced two-phase operation at rated load. Shaded-pole motors are least efficient, often converting under a third of input power into shaft output.
What size capacitor does a 1 hp single phase motor need?
A typical 1 hp 115 V capacitor-start motor uses roughly 216–300 µF rated 125 VAC. A 230 V two-value motor’s run capacitor is often 15–20 µF at 370 or 440 VAC.The nameplate value always takes priority.
How long does a start capacitor last? A start capacitor can last years if the motor starts within its duty limit, typically 20 three-second starts per hour. Heat, excessive starts or a switch that fails to open can destroy it within minutes, often by venting.
Can I use a VFD on a single phase motor? Generally no. Standard drives output three phases and damage run capacitors. PSC fan motors can use dedicated single-phase drives. For anything else, replace the motor with a three-phase unit fed from a single-phase-input drive.
Why do single phase motors hum more than three phase motors? Their field is pulsating rather than uniformly rotating. The interaction of forward and backward fields creates torque ripple at twice supply frequency, which vibrates the stator and mounts as an audible 100 or 120 Hz hum.