No-Slip Rolling & Conservation of Energy

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SUMMARY

The discussion centers on calculating the height \( h_2 \) that a marble of mass \( M \) and radius \( R \) reaches after rolling down from height \( h_1 \) and then moving up a frictionless track. The conservation of mechanical energy is applied, leading to the equation \( Mgh_1 = Mgh_2 + \frac{1}{2}Mv^2 + \frac{1}{2}I\omega^2 \), where \( I \) for a sphere is \( \frac{2}{5}MR^2 \). The final expression for \( h_2 \) is derived as \( h_2 = h_1 - \frac{7}{10}\left(\frac{v^2}{g}\right) \). The discussion emphasizes the importance of recognizing that the marble stops at height \( h_2 \) on the frictionless incline, which is crucial for solving the problem correctly.

PREREQUISITES
  • Understanding of conservation of mechanical energy principles
  • Familiarity with rotational dynamics and moment of inertia, specifically for a solid sphere
  • Knowledge of kinematic relationships between linear and angular motion
  • Basic algebra for manipulating equations and solving for variables
NEXT STEPS
  • Study the concept of conservation of energy in rolling motion
  • Learn about the moment of inertia for different shapes and how it affects motion
  • Explore the implications of frictionless surfaces on rolling objects
  • Investigate the relationship between translational and angular velocity in rolling objects
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Physics students, educators, and anyone interested in understanding the dynamics of rolling motion and energy conservation principles in mechanics.

Kavorka
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I wanted to just make sure I was doing this right. The problem:

A marble of mass M and radius R rolls without slipping down a track from height h1. The marble then goes up a frictionless track to a height h2. Find h2.

I figure this has to be in terms of other variables, here is my work.

initial mechanical energy = final mechanical energy

Mgh1 = Mgh2 + (1/2)Mv^2 + (1/2)Iω^2

I for sphere = (2/5)MR^2

Plug in for I and cancel M's. Plug in v = ωR

gh1 = gh2 + (1/2)v^2 + (1/5)v^2

g(h1 - h2) = (7/10)v^2

h2 = h1 - (7/10)(v^2 / g)

Can the answer be expressed simpler?
 
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Kavorka said:
I wanted to just make sure I was doing this right. The problem:

A marble of mass M and radius R rolls without slipping down a track from height h1. The marble then goes up a frictionless track to a height h2. Find h2.

I figure this has to be in terms of other variables, here is my work.

initial mechanical energy = final mechanical energy

Mgh1 = Mgh2 + (1/2)Mv^2 + (1/2)Iω^2

I for sphere = (2/5)MR^2

Plug in for I and cancel M's. Plug in v = ωR

gh1 = gh2 + (1/2)v^2 + (1/5)v^2

g(h1 - h2) = (7/10)v^2

h2 = h1 - (7/10)(v^2 / g)

Can the answer be expressed simpler?
yes. What is the value of v?
 
angular velocity times radius. That's pretty much all I can think of in terms of substituting in something.
 
Hello Kavorka

Kavorka said:
initial mechanical energy = final mechanical energy

Mgh1 = Mgh2 + (1/2)Mv^2 + (1/2)Iω^2

This is incorrect.

I would suggest you to break the problem in two stages .In the first part the marble rolls from the top at height h1 to the bottom .In the second part it moves up to a height h2.

Just write the energy conservation equation for the first part .What do you get ?
 
The same thing, minus the Mgh2.
 
Kavorka said:
I wanted to just make sure I was doing this right. The problem:

A marble of mass M and radius R rolls without slipping down a track from height h1. The marble then goes up a frictionless track to a height h2. Find h2.

Read carefully the problem: the second track is frictionless. Is it possible rolling without slipping on a frictionless track? Think of a car moving on wet ice...

ehild
 
How am I suppose to find the 2nd height then?
 
This is a two step problem. 1st find the speed at the bottom of the track h2 = 0. Than use energy conservation again on the way up the second track where due to the lack of friction there is no torque and the angular kinetic energy doesn't change.
 
Kavorka said:
How am I suppose to find the 2nd height then?
When the marble reaches height h2, its translational motion comes to a temporary stop. So at that point, the velocity of its center of mass is__?___ and ω is (___see hints given by others____).
 
  • #10
Why does it stop? The problem doesn't say that, it just lists an arbitrary height up a frictionless slope.
 
  • #11
Kavorka said:
Why does it stop? The problem doesn't say that, it just lists an arbitrary height up a frictionless slope.

I asumed it implied it stopped otherwise the solution must be left in terms of the unknown variable 'v' but also in which case your solution is not correct because you have not identified ω properly as noted by others' hints (no friction on incline).
 
  • #12
Kavorka said:
Why does it stop? The problem doesn't say that, it just lists an arbitrary height up a frictionless slope.

Yes it stops. The problem doesn't state it explicitly but it is in between the lines. If the mass hadn't stopped, it would still be moving upwards reaching even higher elevations. It is implicit the h2 is the highest point of the trajectory up the second ramp, so it must stop there.
 
  • #13
Do you end up with height 1 = height 2 then? If not I have no idea what I'm doing.
 

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