Motor Physics

Lorentz Force

Current in magnetic field creates a force

F=iWdl×B=I×BF=i \int_{W} dl \times B=I\times B

In DC Motors, our torque τI\tau \propto I.

Faraday's Law

ΣEdl=ddtΣBdA\oint_{\partial \Sigma} E \cdot dl=-\frac{d}{dt} \iint_{\Sigma}B \cdot dA

Back EMF

VE=ddtΦBV_E=-\frac{d}{dt} \Phi_B

The Back EMF VEωV_E \propto \omega, where ω\omega is the angularity speed.

Important Relationship in DC Motors

An important relationship existing in DC Motors

Analysis

Analysis

When a motor , its current draw is: Maximum.

Why?

As you can see, when motor stalls, the output torque is very very large and reaches the maximum. Since τI\tau \propto I, we can say that our current draw is maximum.

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