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This equiment is built from a Panasonic flashlight and a Trelock FC 404 bicycle computer. It includes additional circuitry (see below) to slice the AC voltage from the dynamo and divide it to a lower frequency that the bicycle computer can handle. Initially, I designed this with a cheap no-name bicycle computer. I soon found that this does some terrible rounding at higher speeds. I switched to a branded item, the Trelock FC 404. It displays the decimals of the speed and it does so correctly. To properly set the wheel circumference in the bicycle computer, it's necessary to know the diameter of the dynamo wheel as well as the number of magnet poles. Most sidewall dynamos have 8 poles - you can feel 8 steps per rotation of the wheel (and measure 4 full sine waves per rotation). Refer to the formula below. |

Other tools used for the measurements below are multimeters, oscilloscope, a lab power supply and an adjustable current sink based on the LM317T linear regulator IC.

Observation: AXA HR delivers maximum power at 200 mA load current (note this is after voltage doubling !), B&M Dymotec6 at 180 mA, the cheapy at 160 mA. The absolute power levels show the AXA HR on top and the cheapy on the bottom at any speed. Conclusion: The maximum power is achieved at a specific load current. This depends little on the speed, but mostly on the dynamo. In other words: A dynamo is a current source.
Setup: Dymotec6, voltage doubler (Greinacher type using 2x 1N5818 & 2x 1000uF), 180 mA current sink. Speedmeter connected to dynamo.
Procedure: Run the dynamo at 4, 5, 7, 9, 12, 15, 19, 24, 31, 40, 50 km/h and measure the voltage across the current sink. Plot for each speed the calculated power = measured voltage * 180 mA current.

Conclusion: With perfect matching of the load, Dymotec6 delivers 2.7 W at moderate speed, 5 W at high speed and 6 W at really high speed. This is what can be achieved without modification to the dynamo.
Question: Why does a standard 3 W light system with the Dymotec6 not burn out the bulbs at 50 km/h ? This is because at such high speed, the matching of the load is off (current is too high) so that it can't drain maximum power.
Question: Where goes the lost energy when the load doesn't drain the maximum possible power ? It's not lost. The dynamo spins with less effort. Try and short-circuit the dynamo at full speed, the current of the driving motor will drop a lot.

Continuing this experiment, a standard 80mm computer fan is mounted to provide some cooling as it would be on a moving bike. The power increases and eventually stabilizes at 89% of the start value. The temperature stabilizes at around 40ºC.
The Dymotec6 was chosen for this experiment as it has the best mechanical design of all tested dynamos. It doesn't suffer any noticable deterioration after running at 50 km/h and delivering well above 5 W for 2 hours. A lot of dynamos don't withstand this. Bearings and their lubrication suffer from the high internal temperature, resulting in rapid wear. Once the rotating magnet comes into contact with the stator, friction and internal temperature dramatically increase, the dynamo body melts and eventually the rotor jams. In my setup, this just tears the coupling between motor and dynamo while on a real bike, the dynamo wheel may pop off so that the rotor shaft causes damage to tire, rim or spokes. Bottom line: Avoid using a cheap dynamo to assist the brakes on long descents.