Loop-the-Loop: Solving for the Release Height

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Homework Help Overview

The discussion revolves around a physics problem involving a small spherical ball rolling down a ramp and around a loop-the-loop. Participants are tasked with determining the height from which the ball must be released to successfully navigate the loop, considering both translational and rotational kinetic energy.

Discussion Character

  • Exploratory, Conceptual clarification, Assumption checking

Approaches and Questions Raised

  • Participants discuss the application of conservation of energy, questioning how to account for both translational and rotational kinetic energy. Some suggest reviewing previous similar problems for clarity. Others raise concerns about the assumptions made regarding the ball's material properties and the implications of static friction in the context of rolling motion.

Discussion Status

There is an ongoing exploration of the problem with various interpretations being discussed. Some participants have provided insights into the necessary conditions for the ball to complete the loop, while others question the correctness of certain assumptions and calculations. No consensus has been reached, but productive dialogue continues.

Contextual Notes

Participants note the importance of clarifying the ball's material properties and the role of friction in the problem setup. There is also mention of the need for assumptions regarding gravity and the nature of the ball's motion to be explicitly stated.

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Loop-the-Loop

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A small spherical ball of radius r = 1.9 cm rolls without slipping down a ramp and around a loop-the-loop of radius R = 2.6 m. The ball has mass M = 375 g.


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a) How high above the top of the loop must it be released in order that the ball just makes it around the loop?
h = m
5/2*2.6 NO

HELP: Use conservation of energy. Remember that the ball has both translational and rotational kinetic energy. Since it rolls without slipping, the two are related.
HELP: What does it mean to just make it? If you have forgotten, go back and review similar loop-the-loop problems you did without the added complication of rotation. See Lecture 12 for example.


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b) Repeat problem (a) for a disk. Find the ratio of the heights h for the two cases.
hdisk/hsphere =

Can somebody help here!
 
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Have you tried anything, do you have any ideas?
Have you done what the HELP stated? As in have you reviewed the textbooks?
 
Naeem said:
Loop-the-Loop

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A small spherical ball of radius r = 1.9 cm rolls without slipping down a ramp and around a loop-the-loop of radius R = 2.6 m. The ball has mass M = 375 g.


--------------------------------------------------------------------------------
a) How high above the top of the loop must it be released in order that the ball just makes it around the loop?
h = m
5/2*2.6 NO

Well in oder to be sure that you don't fall of the loop your centripetal force needs to be equal to the gravity at the top of the loop : mg = mv²/R...and R is the radius of the loop

so the velocity at the top of the loop is v²=gR

At the bottom you can apply conservation of energy :

1/2mv² =mg2R + 1/2mgR where the last term is the potential + kinetic energy at the top...

thus you have that v² = 5gR

and when you start from a height h you have that 1/2mv² = mgh or v²=2gh...

If you set equal these two last expressions for v² you get 2gh=5gR or h=5/2R

the second part is analoguous but you need to use the inertia of motion here because it is no point-particle that moves here...

regards
marlon
 
for a , i did : h = 5/2R which is 5/2.6 , which I don't think is correct. Am I missing something.
 
h = (5/2)R is correct...
this is the minimal heigth from which you should start out...

regards
 
I did this:

h = (5/2) which is 2.5 * R
here R = 2.6 then h would be

2.5 * 2.6 which equals 6.5, which the computer says is wrong.
 
don't forget rotation

marlon said:
h = (5/2)R is correct...
this is the minimal heigth from which you should start out...
This is incorrect. It would be true for a point particle, but not a rolling ball.

As you found, at the top of the motion [itex]mv^2 = mgR[/itex]; use this to find the minimum total KE at that point: translational ([itex]1/2mv^2[/itex]) plus rotational ([itex]1/2I\omega^2[/itex]).
 
Nitpicking a bit, but shouldn't the question state that the ball is not hollow, and that it's made from uniform material? I suppose you have to make that assumption, or you can't calculate the answer accurately?
 
Yes a dumb question indeed!

Nitpicking a bit, but shouldn't the question state that the ball is not hollow, and that it's made from uniform material? I suppose you have to make that assumption, or you can't calculate the answer accurately?
It should also state that the gravity is some constant otherwise you would have to go with the old [tex]G\frac{m1m2}{d^2}[/tex]
Since friction is not mentioned I'd also like the question to state the aerodynamic properties of the object that is rolling.

Sarcasm indeed, not bulletproof but I'm practicing =)

By the way I wonder, using conservation of energy one assumes there is no friction, but in order for the ball to roll there must be friction, isn't this contradictory?
 
Last edited:
  • #10
The ball is rolling without slipping. This means the point of the ball in contact with the surface is momentarily at rest. Therefore the friction that is producing torque is static. Static friction does no work.
 
  • #11
ceptimus said:
Nitpicking a bit, but shouldn't the question state that the ball is not hollow, and that it's made from uniform material? I suppose you have to make that assumption, or you can't calculate the answer accurately?
Good point. Since the problem explicitly considers rotational KE, it is neither a nitpick nor a dumb question.
 
  • #12
The ball is rolling without slipping. This means the point of the ball in contact with the surface is momentarily at rest. Therefore the friction that is producing torque is static. Static friction does no work.
Cheap solution :P
 
  • #13
Doc Al said:
This is incorrect. It would be true for a point particle, but not a rolling ball.

As you found, at the top of the motion [itex]mv^2 = mgR[/itex]; use this to find the minimum total KE at that point: translational ([itex]1/2mv^2[/itex]) plus rotational ([itex]1/2I\omega^2[/itex]).


Correct Doc Al, I gave the solution for a point particle...i did not realize it was a ball...clearly i did not read the question thouroughly... :rolleyes:

i apologize for my mistake...

regards
marlon
 

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