Electromechanical considerations

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Discussion Overview

The discussion revolves around the operation of a DC brush motor as both a motor and a generator, particularly focusing on the relationship between torque, angular velocity, and electrical load. Participants explore the implications of applying different loads to the motor and how this affects the torque required to operate it, as well as considerations for dynamic braking and optimal performance.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant observes that increasing resistance on the rotor leads to higher current and questions whether a larger load will increase the torque required to turn the motor.
  • Another participant suggests that increasing the angular velocity through a higher gear ratio could provide more power while maintaining constant power output.
  • There is a discussion about whether applying more electrical load affects the torque required to turn the motor, with differing opinions on this point.
  • A participant introduces the concept of dynamic braking, explaining that it involves dumping electrical energy into a resistor bank to slow down the mechanical device.
  • One participant provides technical details about the motor, including optimal RPM ranges and load recommendations, while cautioning against exceeding current ratings.
  • Another participant expresses interest in designing a control system for the motor and seeks confirmation of their theoretical understanding.

Areas of Agreement / Disagreement

Participants express differing views on whether increasing electrical load affects the torque required to turn the motor. While some suggest that it does not, others imply that a larger load may necessitate more torque. The discussion remains unresolved with multiple competing perspectives on this topic.

Contextual Notes

Participants reference specific electrical and mechanical parameters, such as current ratings and RPM, but there are no definitive conclusions about the relationship between load and torque requirements. The discussion includes assumptions about the motor's operation that are not fully explored.

Who May Find This Useful

This discussion may be of interest to individuals exploring the practical applications of DC motors and generators, particularly in experimental setups involving human-powered systems and dynamic braking techniques.

Pythagorean
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(please skip straight to the question if you don't want to read the setup)

Backstory:
I'm playing with a motor, both as a motor and a generator. It's from a treadmill, 90 V, 6 Amp.

Observation:
I hook the motor up to a power supply. Apparently it's an independent power supply, because I have little control over the current (it seems to me like I can set the maximum current, but in order to keep the voltage constant, the current changes).

If I put resistance on the rotor, the current goes up. To accelerate the rotor, the current goes up (like when you first turn it on, to overcome the inertia.

I've since refreshed myself on the dependencies between angular velocity, torque, current, and voltage.

Question:
I rigged the motor up as a generator (it worked, so it must not be induction) and power a small light bulb, using bicycle pedals, but it's too easy to spin the rotor, so I'm all velocity and no torque.

If I put a bigger load than a light on the motor, will it put back resistance on the rotor so that I have to apply more torque to get it going?

And, as my intuition suggests, will this supply more current (i.e. my power will more in torque than in angular velocity)?
 
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If you want more power just increase the angular velocity of the generator by gearing it differently. Use a high gear ratio.
 
JCOX said:
If you want more power just increase the angular velocity of the generator by gearing it differently. Use a high gear ratio.

I framed the question under constant power. It's the velocity and torque that would be changing for the same power.
 
ok ... sorry i don't know if i get what you are saying but the way i see it you want the same power output and different tourqe applied on the pedals right?
 
JCOX said:
ok ... sorry i don't know if i get what you are saying but the way i see it you want the same power output and different tourqe applied on the pedals right?

yeah.

My inevitable question will be, "how would I make a break that breaks from the electrical side (i.e., by braking, I generate power)" but I'm building up to that.
 
Oh cool...well i don't know much about generators but i don't think that applying more electrical load to the motor will effect the tourque required to turn the motor at all. I mean when you turn the motor by hand and then apply more load ... does it get harder to turn? I don't think it would.
 
Pythagorean said:
yeah.

My inevitable question will be, "how would I make a break that breaks from the electrical side (i.e., by braking, I generate power)" but I'm building up to that.

What you are describing is called dynamic braking. You basically dump the electrical energy into a resistor bank which causes what ever mechanical device you are using to slow down. Most motor/generator books will have a section on dynamic braking.

CS
 
The motor is a dc brush motor with a permanent magnet stator. To operate the motor as a generator/dynamic load just connect various resistances. I will guess that the optimum RPM is 2000 to 3000 RPM. You shouldn't exceed 6 A load current, or you will exceed the current rating of the brushes and rotor coils. You should be able to get several hundred (200-300) watts out of it. The simplest load(s) would be 120V incandescent lamps with a 100-watt rating. It would be useful to know how much RPM is required to get 90 volts into an incandescent lamp. A better dynamic load would be several parallel NPN bipolar transistors or N-channel FETs (on good heat sinks) connected to the incandescent lamps. This way you could adjust the load setting with a knob.
 
stewartcs said:
What you are describing is called dynamic braking. You basically dump the electrical energy into a resistor bank which causes what ever mechanical device you are using to slow down. Most motor/generator books will have a section on dynamic braking.

CS

Excellent. Thank you. A lot can be done knowing a term (i.e. "dynamic breaking"), makes research a lot easier! The mechanical device will be human legs, but currently it's too easy to turn, so you don't get the full power out of your legs you could if (I assume) a bigger load is put on the generator and more torque is actually required. Your legs have a top speed they can go regardless of torque, so after a certain point you can only get more power from torque.

Bob S said:
The motor is a dc brush motor with a permanent magnet stator. To operate the motor as a generator/dynamic load just connect various resistances. I will guess that the optimum RPM is 2000 to 3000 RPM. You shouldn't exceed 6 A load current, or you will exceed the current rating of the brushes and rotor coils. You should be able to get several hundred (200-300) watts out of it. The simplest load(s) would be 120V incandescent lamps with a 100-watt rating. It would be useful to know how much RPM is required to get 90 volts into an incandescent lamp. A better dynamic load would be several parallel NPN bipolar transistors or N-channel FETs (on good heat sinks) connected to the incandescent lamps. This way you could adjust the load setting with a knob.

Yeah, I've thought about designing a control for it, I just wanted to make sure my theoretical understanding was sound. Thank you for your input!
 

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