Angular Momentum of a rotating mass

AI Thread Summary
The discussion revolves around the angular momentum of a rotating mass, specifically a 3.2-kg bob moving in a circular path. The conservation of angular momentum is highlighted, with the initial and final moments of inertia and angular velocities being calculated. A key point raised is the need to account for the angle θ that the cord makes with the vertical, which changes as the tension increases and affects the system's dynamics. The participant realizes that applying Newton's laws will help determine θ and clarify the conservation of angular momentum. The role of gravity and tension in maintaining the bob's circular motion is also emphasized.
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1. Homework Statement

When the 3.2-kg bob is given a horizontal speed of 1.5 m/s, it begins to rotate around the horizontal circular path A. The force F on the cord is increased, the bob rises and then rotates around the horizontal circular path B. (picture included)

Homework Equations


L = I ω v = rω

The Attempt at a Solution


The solution from the book goes into a long procedure with summation of forces to find the angle etc. I tried this

Since there is no moment about the z axis angular momentum is conserved about the z axis. I1ω1 = I2ω2
For a particle I= mr2 so initially, I = (3.2)(0.6sinθ)2 and after I = (3.2)(0.3sinθ)2. For ω, initially it is (0.6)(sinθ)(1.5m/s) at the end is is (0.3sinθ)(v2)

Setting these equal to each other and solving gives v=12m/s But the answer is 2m/s Not sure where I am going wrong. Thank you!
 

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You don't seem to mark theta on your diagram. I assume it is the angle the chord makes with the z axis. If so, it will not be the same in both positions.
As the tension increases, the "orbit" becomes more horizontal and theta changes.
 
Ah that would explain it. I think i need to find theta using Newton's laws. Then I can apply it to the conservation of angular momentum.

Thank You.
 
Remember that the reason the ball is not just spinning with the chord horizontal, is gravity. The tension in the chord is providing the opposition to gravity as well as centripetal force.
 
Kindly see the attached pdf. My attempt to solve it, is in it. I'm wondering if my solution is right. My idea is this: At any point of time, the ball may be assumed to be at an incline which is at an angle of θ(kindly see both the pics in the pdf file). The value of θ will continuously change and so will the value of friction. I'm not able to figure out, why my solution is wrong, if it is wrong .
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