Crank Generator Power

A conducting rod is bent in the shape of a semicircle of radius r r and the straight parts along the ends of the diameter of the semicircle are passed through fixed, smooth conducting rings O O and O . O'. A capacitor with capacitance C C is connected to the rings with the help of ideal wires. A resistance R R is in series with the capacitor. The system is placed in a uniform magnetic field of strength B B such that the axis of rotation O O OO' is perpendicular to the direction of the magnetic field.

The semicircle is now rotated about the axis O O OO' with a constant angular velocity of ω \omega . Neglect any self-inductance in the circuit.

What is the average mechanical input power (in Watts) required to keep the semicircle rotating?

Inspiration

Details and Assumptions:

  • Assume AC steady-state operation
  • r = 1 m r = 1 \, \text{m}
  • ω = 120 π rad/s \omega = 120 \, \pi \,\, \text{rad/s}
  • B = 0.1 T B = 0.1 \, \text{T}
  • R = 1.0 Ω R = 1.0 \, \Omega
  • C = 1 60 π F C = \large{\frac{1}{60 \pi}} \, \text{F}


The answer is 1402.69.

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1 solution

Steven Chase
Sep 18, 2018

From the solution to the previous problem, the induced voltage is:

V ( t ) = π ω B R 2 2 s i n ( ω t ) \large{V(t) = - \frac{\pi \omega B R^2}{2} sin(\omega t)}

The RMS voltage is:

V r m s = π ω B R 2 2 2 \large{V_{rms} = \frac{\pi \omega B R^2}{2 \sqrt{2}}}

The capacitive reactance is:

X C = 1 ω C = 1 2 \large{X_C = \frac{1}{\omega C} = \frac{1}{2}}

The impedance magnitude is:

Z = R 2 + X C 2 \large{Z = \sqrt{R^2 + X_C^2}}

Current magnitude:

I r m s = V r m s Z \large{I_{rms} = \frac{V_{rms}}{Z}}

The capacitor contributes nothing to the average power. Only the resistive term matters. P a v = I r m s 2 R = 1402.69 \large{P_{av} = I_{rms}^2 R = 1402.69}

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