η = (U·Ia − Ia²·Ra − Pv,mech) / (U·Ia)
Resistive armature loss and mechanical loss are subtracted from input electrical power before power is available at the shaft.
Resistive armature loss and mechanical loss are subtracted from input electrical power before power is available at the shaft.
Select a target and calculate.
Resistive armature loss and mechanical loss are subtracted from input electrical power before power is available at the shaft.
U=230 V, Ia=20 A, Ra=0.5 Ω and Pv,mech=150 W give Pel=4,600 W, PCu=200 W, Pab=4,250 W and η≈0.924 or 92.4%.
Steady motoring, constant field flux and temperature-constant Ra; field power, commutation/brush loss and starting transients are excluded.
This calculator extends the DC motor power balance to the shaft: it subtracts both resistive armature loss and mechanical loss from consumed electrical power, giving the actual overall efficiency.
From input power Pel=U·Ia, copper loss Ia²·Ra is subtracted first, giving converted electromagnetic power E·Ia. Subtracting mechanical loss power Pv,mech from that leaves shaft power Pab, and η=Pab/Pel.
η = (U·Ia − Ia²·Ra − Pv,mech) / (U·Ia)
Pel = U·IaPCu = Ia²·Raη = (Pel−PCu−Pv,mech)/Pel| Symbol / input | Meaning |
|---|---|
| Overall efficiency η (0 to 1) | Ratio of delivered shaft power to consumed electrical power at the operating point. |
| Armature voltage U | DC voltage directly at the armature terminals at the steady operating point. |
| Armature current Ia | Measured armature current, excluding separately supplied field current. |
| Armature-circuit resistance Ra | Hot resistance of armature winding, brushes and permanent connection path. |
| Mechanical loss power Pv,mech | Friction, windage and other mechanical losses between converted electromagnetic power and shaft output. |
U and Ia are armature-circuit voltage and current at the same operating point. Ra is the hot armature-circuit resistance. Pv,mech bundles bearing, brush and windage friction and other mechanical losses, and must be known separately, e.g. from a no-load test.
Record U, Ia and Ra at the same steady operating point as for the back-EMF calculator. Determine Pv,mech from a no-load test at the same speed, where all supplied power turns into mechanical loss.
U=230 V, Ia=20 A, Ra=0.5 Ω and Pv,mech=150 W give Pel=4,600 W, copper loss 200 W, shaft power Pab=4,250 W and η≈0.924 or 92.4%.
Low overall efficiency despite small copper loss points to dominant mechanical losses, such as bearing friction or an oversized fan.
U is a voltage, Ia a current, Ra a resistance and Pv,mech a power. η is dimensionless, shown as a ratio between 0 and 1.
Evaluating test-bench measurements, comparing operating points of the same motor and estimating energy demand for a known useful power.
Steady operation with constant field flux and temperature-constant Ra. Field power, commutation/brush voltage loss and starting or load-change transients are excluded.
Common mistake: Do not confuse Pv,mech with copper loss Ia²·Ra; both loss types must be captured separately and both subtracted from Pel. Do not equate the pure back-EMF power E·Ia with shaft power Pab.
Evaluating test-bench measurements, comparing operating points of the same motor and estimating energy demand for a known useful power.
U and Ia are armature-circuit voltage and current at the same operating point. Ra is the hot armature-circuit resistance. Pv,mech bundles bearing, brush and windage friction and other mechanical losses, and must be known separately, e.g. from a no-load test.
Steady operation with constant field flux and temperature-constant Ra. Field power, commutation/brush voltage loss and starting or load-change transients are excluded.