Moving Down a Ramp: Answers & Explanations

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SUMMARY

The discussion centers on the physics of objects moving down a ramp, specifically analyzing the energy transformations involved in rolling versus sliding. Key equations include the conservation of energy, represented as Ei = Ef, and the moment of inertia for solid and hollow spheres, I_solid sphere = 2/5mr^2 and I_hollow sphere = 2/3mr^2. The final heights of the objects are determined to be 5/7 and 3/5 of the original height for the solid and hollow spheres, respectively, while blocks maintain their original height. The conversation highlights the importance of free-body diagrams and energy considerations in understanding motion on slopes.

PREREQUISITES
  • Understanding of conservation of energy principles in physics
  • Familiarity with moment of inertia calculations for different shapes
  • Knowledge of kinematic equations, particularly v^2 = v_0^2 + 2ax
  • Ability to interpret free-body diagrams and forces acting on objects
NEXT STEPS
  • Study the implications of rotational inertia on motion in "Physics of Rolling Objects"
  • Learn about free-body diagram techniques for analyzing forces on inclined planes
  • Explore energy conservation in non-friction scenarios using "Conservation of Mechanical Energy"
  • Investigate the differences between rolling and sliding motion in "Dynamics of Rolling Motion"
USEFUL FOR

Students of physics, educators teaching mechanics, and anyone interested in the dynamics of rolling objects and energy transformations on slopes.

JessicaHelena
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Homework Statement



Please look at the problem attached as a screenshot.

Homework Equations



Assuming frictionless, Ei = Ef, which means objects that are the same will end up in the same heights (so we can group A&C, B&D, and E&F).
For A&C and E&F, mgh = KE_rot + KE_trans
For B&D, it is mgh = KE_trans.
Also, v = rw (I know it's omega, but for convenience, I'll write it as w).
I _solid sphere = 2/5mr^2
I_hollow sphere = 2/3mr^2

The Attempt at a Solution


After all these equations set up, now it's pretty much plugging things in. For A&C ,

mgh = 1/2mv^2 + 1/2Iw^2
mgh = 1/2mv^2 + 1/5mr^2w^2
gh = 1/2v^2 + 1/5 r^2(v/r)^2
gh = 1/2v^2 + 1/5v^2 = 7/10v^2
so v^2 = 10gh/7
then KE at the end is then 1/2mv^2 = 5mgh/7, and that can be converted to the new GPE. so the height will be 5/7 the original height.

For E&F, I can use a similar process, only now I = 2/3mr^2. That gives me a KE of 3/5mgh, so the new (final) height will be 3/5 the original height.

For the blocks (B&D), there's only KE_trans, so Ei = Ef and mgh = 1/2mv^2. With no rot KE to lose trans KE to, the final height should be the same as the original height.

Thus, in order, it is B&D, A&C, E&F.

Could someone please check if I don't have any flaws in my reasoning?
 

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Where does the rotational energy go for the sphere on the upward slope?
 
Oh... so would it be that all objects (regardless of their shape) would end up with a same height that's identical to their original heights?
 
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JessicaHelena said:
Oh... so would it be that all objects (regardless of their shape) would end up with a same height that's identical to their original heights?

Yes, but can you explain what happens on the up-slope? You need a free-body diagram to show what gravity and friction are doing.
 
It's accelerating down the slope even though it will continue moving up. So would that mean the objects don't quite reach the same height?

Using F_net = ma, I get that a = g*sin(theta), and I guess we could use v^2 = v_0^2 + 2ax (Where v = v^2 = 0) to get the x and then use trig to get the actual height, but wouldn't there be a better way using energy?
 
JessicaHelena said:
It's accelerating down the slope even though it will continue moving up. So would that mean the objects don't quite reach the same height?

Using F_net = ma, I get that a = g*sin(theta), and I guess we could use v^2 = v_0^2 + 2ax (Where v = v^2 = 0) to get the x and then use trig to get the actual height, but wouldn't there be a better way using energy?

You can use energy considerations as an explanation (and not talk about forces). But, it's interesting to consider the forces as well:

On the downslope a sphere accelerates more slowly if it rolls (instead of slips).

On the upslope, the sphere must decelerate more slowly than it would under gravity alone in order to reach the same height. How does this happen?
 
Wouldn't it be similar to the downslope scenario — because the sphere is still rolling uphill, there'd be less of translation velocity, so it would decelerate more slowly as well?

But I'm a little lost, to be honest, when you say "On the downslope a sphere accelerates more slowly if it rolls (instead of slips)." It would certainly have less v_trans, but I don't think accelerating more quickly/slowly has much to do with the magnitude of v, and in that case, my answer above would be wrong too.
 
JessicaHelena said:
Wouldn't it be similar to the downslope scenario — because the sphere is still rolling uphill, there'd be less of translation velocity, so it would decelerate more slowly as well?

But I'm a little lost, to be honest, when you say "On the downslope a sphere accelerates more slowly if it rolls (instead of slips)." It would certainly have less v_trans, but I don't think accelerating more quickly/slowly has much to do with the magnitude of v, and in that case, my answer above would be wrong too.

You started off with an answer that said: B&D, then A&C, then E&F.

Let's start again. Why don't you give your revised answer and why.
 
JessicaHelena said:
when you say "On the downslope a sphere accelerates more slowly if it rolls (instead of slips)." It would certainly have less v_trans, but I don't think accelerating more quickly/slowly has much to do with the magnitude of v,
You are right that a reduced acceleration does not obviously lead to a lower speed since it will accelerate for longer. Indeed, for two balls rolling down different ramps of the same height the gentler ramp will produce less acceleration, but the speed will be the same at the bottom.
If you want to analyse it in terms of forces rather than energy then you will need to get into the actual equations.

I consider the question flawed. The box also has rotational inertia, and making it small does not circumvent that. As it goes through the curve at the bottom some energy will become rotational. What happens to that as the track straightens again? Seems to me the options do not encompass the true answer.
 
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