Motors Equivalent Model Filippas 2016 Equivalent model Node

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Motors: Equivalent Model Filippas 2016

Motors: Equivalent Model Filippas 2016

Equivalent model Node A Equivalen t to Node B

Equivalent model Node A Equivalen t to Node B

Motor in a circuit Going around the loop: The circuit is comprised of the

Motor in a circuit Going around the loop: The circuit is comprised of the voltage source and the motor. DC voltage source: rise : +V Set up KVL in the one loop – taking into account the equivalent circuit of the motor. Ammeter: zero voltage drop Resistor: voltage drop consistent with the direction of the current : VR + - Back-emf voltage: drop : -Vemf + KVL -

Motor in a circuit From previous: I Ohm’s law + VR - In lab,

Motor in a circuit From previous: I Ohm’s law + VR - In lab, you use the ammeter to measure the current. You also know the value of the source voltage, V. Solve for Vemf:

Motor in a circuit I + VR -

Motor in a circuit I + VR -

Varying magnetic flux F I B I F perp F F Side view No

Varying magnetic flux F I B I F perp F F Side view No field lines go through surface area of coil. F B F perp

Induced voltage So:

Induced voltage So:

Power and efficiency Power dissipator “Useful” power Power generator How do we calculate power

Power and efficiency Power dissipator “Useful” power Power generator How do we calculate power in electrical systems?

Power I I + V This is the picture of a power dissipator. +

Power I I + V This is the picture of a power dissipator. + V This is the picture of a power generator.

Power and efficiency Power dissipator “Useful” power – power dissipated Power generator

Power and efficiency Power dissipator “Useful” power – power dissipated Power generator

Power and efficiency Power dissipator “Useful” power – power dissipated Power generator

Power and efficiency Power dissipator “Useful” power – power dissipated Power generator