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A gyro with angular momentum \( I\omega = 0.5 \ \mathrm{kg\,m^2/s} \) is subjected to a torque of \( 0.02 \ \mathrm{N\,m} \). The precession rate is

  • A.0.10 rad/s
  • B.0.04 rad/s
  • C.0.01 rad/s
  • D.25 rad/s

Answer: B

Correct answer: 0.04 rad/s

Precession rate is the applied torque divided by the angular momentum:

\[ \Omega = \frac{T}{I\omega} = \frac{0.02}{0.5} = 0.04\ \mathrm{rad/s} \]

The inverse dependence on angular momentum is what makes a fast, heavy rotor a good reference: the same disturbing torque produces less precession. It is also why a gyro whose rotor is slowing becomes progressively less reliable, drifting faster as its momentum falls.

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