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Motor Thermal Time Constant⚠ unverified

Electrical / Motors · Compute the thermal time constant of a motor

Parameters

InputSymbolUnitDefaultDescription
RthRthK/W1.0Thermal resistance
CthCthJ/K1.0Thermal capacitance (heat capacity)
OutputSymbolUnitDescription
resultτsThermal time constant, in seconds (s)

The science & history

Understanding the Parameters

Derivation (Approaching a Proof)

Model the motor as one thermal node: heat is generated at rate $P_{loss}$, stored in capacitance $C_{th}$, and leaks to ambient through $R_{th}$. Energy balance gives a first‑order differential equation identical in form to a charging capacitor:

$$C_{th}\frac{d(\Delta T)}{dt} + \frac{\Delta T}{R_{th}} = P_{loss},$$

whose solution is $\Delta T(t) = P_{loss}R_{th}\big(1 - e^{-t/\tau}\big)$ with

$$\tau = R_{th}\,C_{th}.$$

The mathematics is exactly the RC charging curve (see RC Time Constant), with the thermal–electrical analogy $\Delta T\!\leftrightarrow\!V$, $P\!\leftrightarrow\!I$, $R_{th}\!\leftrightarrow\!R$, $C_{th}\!\leftrightarrow\!C$. The long thermal $\tau$ is why motors survive brief overloads that would be impossible thermally at steady state.

History

Lumped RC thermal models were adapted from circuit theory to machines and power electronics in the mid‑20th century; the thermal time constant underlies motor overload ("$I^2t$") protection, which allows short overloads but trips on sustained ones.

Related Concepts: Temperature Rise, RC Time Constant, Motor Efficiency

Notes: Registry calculator motor-thermal-time-constant (unverified). Single lumped node; detailed models use multiple nodes with separate winding and frame time constants.

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