Rubber ball Rotational Motion Question

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Homework Help Overview

The problem involves a rubber ball rolling off a table and falling a certain distance while completing a specified number of revolutions. The objective is to determine the linear speed of the ball as it rolls off the edge. The subject area includes concepts from rotational motion, energy conservation, and kinematics.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • The original poster attempts to apply energy conservation principles and kinematic equations to find the initial linear speed of the ball. They express confusion over obtaining an imaginary number in their calculations.
  • Some participants question the assumptions regarding the rotational speed of the ball during its fall and the treatment of potential energy in the energy equation.
  • Others suggest considering the constancy of angular velocity as the ball leaves the table to relate linear and angular speeds.

Discussion Status

The discussion is ongoing, with participants providing insights and clarifications. Some guidance has been offered regarding the treatment of potential energy and the relationship between linear and angular speeds. The original poster expresses a breakthrough in understanding, indicating progress in the discussion.

Contextual Notes

The original poster's calculations involve assumptions about energy conservation and the behavior of the ball's rotational motion as it falls. There is an indication of confusion regarding the implications of these assumptions on the results obtained.

Theta
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Note: I refrained from using any of the latex references, so bear with me.

Homework Statement



A rubber ball with a radius of 3.2 cm rolls along the horizontal surface of a table with a constant linear speed v. When the ball rolls off the edge of the table, it falls 0.66 m to the floor below. If the ball completes 0.37 revolutions during its fall, what was its linear speed, v?

a) Variables extracted from the question

r = 3.2 cm = 0.032 m
h = 0.66 m
theta = (2pi)(0.37 revolutions) = (2pi x 0.37) rad

2. Homework Equations and physics principles/concepts

a) Equations

i. d = Vit + 0.5at2
ii. v = rw

b) Physics principles/concepts

i. Law of conservation of energy (?)
ii. Rotational kinetic energy and the moment of inertia (?)
iii. Kinematics (?)

The Attempt at a Solution



a) Energy is conserved, therefore:

Ki + Ui = Kf + Uf

b) There is no potential energy as the bottom of the table. Furthermore, we are analyzing the rotational motion of a rubber ball (ie. I = 0.4mr2). Therefore:

Ki + Ui = Kf
0.5mvi2 + 0.5(0.4mr2)(vi/r)2 = mgh + 0.5mvf2 + 0.5(0.4mr2)(vf/r)2

c) We can clean up the equation by eliminating the mass and radii parameters, and multiplying each term by 2.

vi2 + 0.4vi2 = 2gh + vf2 + 0.4vf2

d) Like terms can be collected and vi can be solved for.

vi = sqrt ((5/7)[(7/5)vf2 - 2gh])

e) We only need the final linear speed now. To determine that, we can use:

vf = rwf

i. As can be seen above, we need to determine wf. To do this, regular kinematics can be applied to find the total time the ball spends in the air.

d = Vit + 0.5at2
d = 0.5at2
t = sqrt (2d/a)
t = sqrt [(2 x 0.66 m) / (9.81 m/s2)]
t = 0.37 s

ii. At the very beginning, the amount of revolutions (in radians) was determined. By dividing the revolutions by the time obtained above, we can obtain wf, and ultimately vf.

vf = rwf
vf = (0.032 m)[(2pi x 0.37) / (0.37 s)]
vf = 0.20 m/s

f) Finally, we can solve for initial linear speed.

vi = sqrt ((5/7)[(7/5)vf2 - 2gh])
vi = sqrt ((5/7)[(7/5)(0.20 m/s)2 - 2(9.81 m/s2)(0.66 m)])
vi = WHAT??!? AN IMAGINARY NUMBER?

So yeah, I do not know what I am doing wrong. Am I misinterpreting the question? Am I approaching the question in the wrong way? Does my logic make any sense?
 
Last edited:
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as the ball falls down, its rotational speed does not increase :)

can u imagine why?

and also, in the energy equation where should we put the potential energy, does the system lose or gain potential energy?

hope that helps :)
 
Theta said:
ii. At the very beginning, the amount of revolutions (in radians) was determined. By dividing the revolutions by the time obtained above, we can obtain wf, and ultimately vf.

vf = rwf
vf = (0.032 m)[(2pi x 0.37) / (0.37 s)]
vf = 0.20 m/s

Since ω does not change, the ball has this same ω when it leaves the table. Can you use that information to find vi=rω?
 
Oh, wow, I think I figured it out.

Thanks for the help you two.
 

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