Elliott Sound Products | Dimmer Phase Angle Test |
These results were obtained from a circuit simulator, which allowed me to capture all the data I needed, without having to use test equipment attached to the mains. The results are not quite the same as with a real lamp, because the filament actually changes its resistance with temperature. The table below shows the theoretical power, current and power factor, ignoring the changing resistance.
Phase Angle | Volts RMS | Current RMS | Power | Power Factor |
18° | 19.28 V | 33.47mA | 645.3 mW | 0.08 |
36° | 52.93 V | 91.89 mA | 4.86 W | 0.22 |
54° | 92.53 V | 160.6 mA | 14.86 W | 0.39 |
72° | 132.9 V | 230.7mA | 30.65 W | 0.55 |
90° | 169.7 V | 294.6 mA | 50.00 W | 0.71 |
108° | 199.9 V | 347.0 mA | 69.35 W | 0.83 |
126° | 221.4 V | 384.5 mA | 85.14 W | 0.92 |
144° | 234.1 V | 406.4 mA | 95.14 W | 0.98 |
162° | 339.2 V | 415.3 mA | 99.35 W | 0.99 |
180° | 240.0 V | 416.7 mA | 100.00 W | 1.00 |
For the simulation, I used a 100W load, based on a supply voltage of 240V. This gives a resistance of 576 ohms, which is 100W at 240V. The phase angle is a measure of how many degrees of each half-cycle the dimmer allows through, and is in 10 steps. The power factor is as shown in the table above, and at most usable settings, it's no worse than a typical CFL. Since those pushing for a ban of incandescent lamps have never looked at power factor anyway, to them it is presumably irrelevant.
To explain the table, a cycle of mains power is traditionally divided into 360°, so a half-cycle is 180°. I used 10 steps of 18° for the table, but real dimmers can use any phase angle as set by the control - they are not limited to discrete steps.