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Maximum Torque⚠ unverified

Electrical / Motors · Compute the pull-out (breakdown) torque of an induction motor

Parameters

InputSymbolUnitDefaultDescription
VVV1.0Per-phase stator voltage
R1R11.0Stator winding resistance
R2R21.0Rotor resistance referred to the stator, in ohms (Ohm). Present for interface symmetry; the breakdown-torque expression does not depend on it
X1X11.0Stator leakage reactance
X2X21.0Rotor leakage reactance referred to the stator
ffHz60.0Supply line frequency, in hertz (Hz). Default is 60.0
polespoles4.0Number of magnetic poles of the machine. Default is 4
OutputSymbolUnitDescription
resultTmaxN.mMaximum (breakdown) torque, in newton-metres (N.m)

The science & history

Understanding the Parameters

Derivation (Approaching a Proof)

Take the torque–slip expression $T(s) = \dfrac{3}{\omega_s}\dfrac{V^2 (R_2/s)}{(R_1 + R_2/s)^2 + (X_1+X_2)^2}$ (see Starting Torque). Treating $R_2/s$ as the variable and setting $dT/d(R_2/s) = 0$ gives the condition for the peak:

$$\frac{R_2}{s_{max}} = \sqrt{R_1^2 + (X_1 + X_2)^2},$$

i.e. the peak occurs at slip $s_{max} = R_2/\sqrt{R_1^2+(X_1+X_2)^2}$. Substituting this back and simplifying, the $R_2$ cancels and leaves

$$T_{max} = \frac{3\,V^2}{2\,\omega_s\big(R_1 + \sqrt{R_1^2 + (X_1 + X_2)^2}\big)}.$$

So rotor resistance shifts the peak along the slip axis (used to get high torque at start) but cannot raise the breakdown torque itself — a key design insight.

History

This "maximum torque" result and the slip at which it occurs are classic outcomes of Steinmetz's equivalent‑circuit analysis. Breakdown torque (typically 200–300 % of rated) is a defining spec for motor selection and appears directly in NEMA torque‑class definitions.

Related Concepts: Starting Torque, Slip, Synchronous Speed, Motor Torque

Notes: Registry calculator maximum-torque (unverified; $R$/$X$ mislabelled dimensionless — should be ohms; $R_2$ input is accepted but unused). Uses $V$/$R_1$ as Thévenin approximations.

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