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In Kleppner & Kolenkow's Introduction to Mechanics (Amazon link), the general gyroscope motion including nutation was derived using the approximation condition $\Omega T \ll 1$ where $\Omega$ is the precession angular velocity and $T$ is the period of nutation.

How does one describe the gyroscopic motion if the the condition for the approximation is not satisfied? How does one describe the general gyroscopic motion if

  1. the angular momentum of precession is not negligible and
  2. if the gyroscope spins very slowly around its axis, $\omega$ is low?

In general I want to find the formula for most general gyroscope motion. If I let $\omega$ go to zero then I should get the special case of a pendulum.

Kyle Kanos
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user50224
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