Precession of a spinning projectile, other dynamics problems

AI Thread Summary
The discussion focuses on the dynamics of a spinning projectile, specifically addressing the lack of clarity in Beer and Johnston's textbook regarding precession. The problem involves determining the rate of spin and precession of a 60-lb projectile with given parameters. The solution for the rate of precession is derived from the relationship between angular velocity components, leading to a calculated value of 0.1596 rad/s. The user expresses confusion about why only the y-component of angular velocity contributes to precession rather than a simultaneous lateral and horizontal spin. The request for further clarification highlights the need for a deeper understanding of angular momentum and precession dynamics.
aeroegnr
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Ok, I'm using Beer and Johnston's engineering Mechanics/Dynamics book for class, and i don't particularly enjoy it's lack of explanation for the following problem:


The graphic shows a bullet flying to the right with the x coordinate pointing along its long axis and the y-axis perpendicular. The velocity is theta degrees below the x axis

"The 60-lb projectile shown has a radius of gyration of 2.4in. about its axis of symmetry Gx and radius of gyration of 10in. about the transverse axis Gy. Its angular velocity \omega can be resolved into two components: One component, directed along Gx, measures the rate of spin of the projectile, while the other component, directed along GD, measures its rate of precession. Knowing that \theta=5 degrees and the angular momentum of the projectile about its mass center G is Hg= (0.640 lb-ft-s)i - (0.018 lb-ft-s)j, determine:
a) the rate of spin
b) the rate of precession"


Now, the book provides no explanation of precession up to this point, and its absolutely driving me insane not knowing why the answer is what it is.

The answer in the back of the book for b is found by taking the j component of velocity \omega_\hat{j} and then using this equation where \omega_\hat{p} is the angular velocity in the direction of the moment of precession.

\omega_\hat{p}*sin(\theta)=\omega_\hat{j}

The answer given in the back of the book for this therefore is .1596 rad/s.

I do not understand why this is so. The angular velocity in the y direction is
the farthest from the axis of precession, so why does it provide the only source of precession? Why does this precess and not just spin laterally and in horizontally at the same time?

If anyone can provide insight, I would be very thankful.

I also have more questions if you can answer this one.
 
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