The sewing machine had a three-contact plug / terminal block that joins all the wiring:
- AC power from the wall
- Pushbutton power switch
- Foot pedal speed control (carbon-pile rheostat)
- AC motor
- Endcap light

For completeness, the matching socket (not shown) joins two cords:
- AC line cord (two wire, not polarized, no ground)
- Foot pedal
Extract the motor wiring from that block and connect it to a 50 V / 3 A bench supply, with the positive lead to the marked wire conductor:

Cranking the voltage upward from zero:

So that’s about 200 RPM/V, offset by 2800 RPM. Totally unloaded, of course.
The original data:
DC V | DC A | RPM | Notes |
15 | 0.29 | 690 | Barely turning |
20 | 0.28 | 1380 | Finger-stoppable |
25 | 0.29 | 2350 | |
30 | 0.29 | 3450 | |
35 | 0.30 | 4450 | |
40 | 0.29 | 5740 | |
45 | 0.29 | 6780 | Still finger-holdable at start |
50 | 0.29 | 8000 |
I can hold the shaft stopped between my fingers up through 45 V, with 0.54 A locked-rotor current at 25 V. The motor doesn’t have a lot of torque, although it’s operating at less than half the normal RMS voltage.
I should take those numbers with the motor driving the sewing machine to get an idea of the actual current under a more-or-less normal load.
Reversing the power supply leads shows that the motor rotates only counterclockwise, which is exactly what you’d expect: both polarities of the normal AC sine wave must turn the motor in the same direction.