Energy, Force, and Inertia Problem. Ball down ramp to loop to loop

In summary: IαThis is correct.In summary, a sphere of mass m and radius r rolls without slipping along the track shown below. It starts from rest with the lowest point of the sphere at height h above the bottom of the loop of radius R, much larger than r. The force components on the sphere at the point P are mg(3R)Fx and mg(3R)Fy, where Fx is the centripetal acceleration and Fy is the force of gravity.
  • #1
rschaefer2
12
0

Homework Statement


A solid sphere of mass m and radius r rolls without slipping along the track shown below. It starts from rest with the lowest point of the sphere at height h above the bottom of the loop of radius R, much larger than r. (Consider up and to the right to be the positive directions for y and x respectively)What are the force components on the sphere at the point P if h = 3R? (Use any variable or symbol stated above along with the following as necessary: g for the acceleration of gravity.)

Homework Equations


Isphere=(2/5)mr2
K=.5mv2
K=.5Iω2
PE=mgh
ac=v2/R

The Attempt at a Solution


Fx
First, solving for v2
mg(3R)=.5mv2+(.5)(2/5)(mr2)(v2/r2)
mg2R=.7mv2+mgR
v2=20gR/7

Centripetal acceleration is the acceleration in the x direction
a=v2/R=20gR/7R
Fx=ma=-20mg/7 <=== Correct!

Fy
Force in y direction is only the force from gravity
F=ma
Fy=-mg <=== Wrong!

please help! What am I missing?
 

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  • #2
Hello, and welcome!

Note that you are measuring heights from the "floor". Does point P have a height?

EDIT:
rschaefer2 said:
mg(3R)=.5mv2+(.5)(2/5)(mr2)(v2/r2)
mg2R=.7mv2
v2=20gR/7

OK, I saw that you left out the potential energy at P in the first equation, but it looks like you took care of it in the second equation.
 
  • #3
I don't see anything wrong with your answer for Fy. Wait! Is the force of gravity the only force with a y component acting on the ball at P?
 
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  • #4
Well, i guess there is friction to? But there wasn't any coefficients given for kinetic friction
 
  • #5
Right. Is the friction kinetic or static?
 
  • #6
Actually, static correct? Because the object is rolling.
 
  • #7
That's right- rolling without slipping. So, even if they did give you a coefficient of static friction it wouldn't be of much help. The static coefficient only let's you find the maximum force of static friction, and there is no reason why the static friction would need to be at its maximum value at P.

So, you'll need to find the friction force some other way. Will the ball have any angular acceleration at P?
 
  • #8
The ball itself? Well angular acceleration will be the derivative of ω with respect to s? EDIT: s as in seconds, from g
 
  • #9
That's a correct statement if s denotes time. [Edit: Ah, I see that you are using s for time!] But it's not of much help.

Do you think the ball will be speeding up or slowing down at P?
 
  • #10
Definitely slowing down, because v will be decreasing
 
  • #11
Will ω also be decreasing?
 
  • #12
Yes, because v=ωr
 
  • #13
Good. So, looks like you have an unknown y-component of acceleration, an unknown angular acceleration, and an unknown friction force. You'll need three independent equations that relate these unknowns. How many equations can you think of?
 
  • #14
1) [itex]\sumτ[/itex]=I(alpha)
2)v=ωr
3)fs=μFn
4) alpha=aT/r
5)aT=(-mg-fs)m
Fn= -20mg/7
I=2/5mv2/r2

I can't seem to relate it using these, I'm probably missing one of the equations.
 
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  • #15
Oooo. Shotgun approach. Need to narrow the field. Eq. #1 looks like a keeper. #4 is also good except the subscipt T is suspicious. What does aT stand for?

Finally, you'll need another equation that relates at least two of the three unknowns: ay, [itex]\alpha[/itex], and the friction force. (Hint: We don't want to upset Newton - which is easy to do.)
[EDIT: your #5 equation looks like it might be the third equation. Not sure the signs are correct though and there appears to be another mistake in it also.]
 
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  • #16
at=ay

Okay, thanks! I'll try to work them out.
 
  • #17
Ok, good. (I was going to have to quit for now anyway - it's late and I need my beauty rest.)
 
  • #18
My attempt:

Equation 1 expands to:
mg+fs=(2/5)mr2(ay/r)

plugging the right side of this equation into equation 3:

ay=(2/5)mray/m

and this is where i get stuck, because the acceleration terms cancel out.
 
  • #19
rschaefer2 said:
Equation 1 expands to:
mg+fs=(2/5)mr2(ay/r)
What you have written on left side doesn't represent the type of quantity you wrote earlier on the left side of equation 1. (The dimensions of what you have on the left don't match the dimensions you have on the right.)

Also, it might help to think about the direction of the friction force. If the angular speed of the ball is slowing down at P, what must be the direction of the net torque on the ball (clockwise or counterclockwise)? What direction does the friction force need to act in order to produce that direction of torque about the center of the ball?
 
  • #20
EDIT: From previous, I've changed torque to only static friction in the positive direction, as mg acts through the axis. Also, the friction force needs to counteract the clockwise movement, therefore needing to be positive (counterclockwise).

So I'm pretty sure I've worked this out correctly. I just want to double check, as this is my last attempt for points. Thanks!

Equations:
1) [itex]\sum[/itex]τ=Iα
fsr=Iα
α=fsr/I

2)α=ay/r
fsr/I=ay/r
ay=fsr2/I

3)may=(-mg+fs)
mfsr2/((2/5)mr2)=-mg+fs
5/2fs-fs=-mg
3/2fs=-mg
fs=-2/3mg

Plug back into 1)
α=(-2/3)mgr/I
α=(-10g/6r)

Plug into 2)
(-10g/6r)=ayr
ay=(-10g/6)

Fy=may
Fy=(-10mg/6)
 
  • #21
rschaefer2 said:
1) [itex]\sum[/itex]τ=Iα
fsr=Iα

2)α=ay/r

3)may=(-mg+fs)

Your equation (1) indicates that you are choosing the positive direction for rotation to be the direction of the torque produced by fs. Is that clockwise or counterclockwise?

Your equation (3) indicates that you are choosing positive y in the upward direction.

Now, if ay is positive, is the angular acceleration α positive or negative according to your conventions adopted in (1)?
Equation (2) implies that α is positive when ay is positive. Is that correct?

Dang signs :frown:
 
  • #22
Rolling up the ramp, the ball is rotating clockwise. Since ω is decreasing, the torque acting on the sphere must be in the opposite direction, counter clockwise.

So the positive direction of rotation is counterclockwise

If ay is positive, then the angular speed should also increase, therefore it should rotate clockwise quicker. So equation two should be ay=-αr?
 
  • #23
rschaefer2 said:
Rolling up the ramp, the ball is rotating clockwise. Since ω is decreasing, the torque acting on the sphere must be in the opposite direction, counter clockwise.

So the positive direction of rotation is counterclockwise

If ay is positive, then the angular speed should also increase, therefore it should rotate clockwise quicker. So equation two should be ay=-αr?

Yes, I believe so. Note that you got a negative value of fs which would indicate that the friction force is downward. But you know that it is upward. So, see how it works out with ay=-αr :smile:
 
  • #24
Awesome, thank you! my new answer is (-10/14)mg, with the correct signs. Any confirmation?
 
  • #25
That's what I got, too. You might want to reduce the fraction. Good! :smile:
 

FAQ: Energy, Force, and Inertia Problem. Ball down ramp to loop to loop

What is energy?

Energy is the ability to do work or cause change. It comes in many forms, including kinetic energy (energy of motion), potential energy (stored energy), thermal energy (heat), and electrical energy.

What is force?

Force is a push or pull that causes an object to accelerate, change direction, or stop. It is measured in units of Newtons (N) and can be described by its magnitude (strength) and direction.

What is inertia?

Inertia is the tendency of an object to resist changes in its state of motion. The greater an object's mass, the greater its inertia. This means that it will require more force to accelerate or decelerate a heavier object than a lighter one.

How does a ball roll down a ramp?

When a ball is placed at the top of a ramp, it has potential energy due to its position. As it rolls down the ramp, this potential energy is converted into kinetic energy, causing the ball to speed up. The force of gravity is what pulls the ball down the ramp, and the angle of the ramp determines how much of the force is directed in the direction of motion.

What happens when a ball goes through a loop on a ramp?

When a ball goes through a loop on a ramp, it experiences a change in direction due to the centripetal force. This force is directed toward the center of the loop and keeps the ball moving in a circular motion. The ball also gains kinetic energy as it goes through the loop, as its speed increases due to the force of gravity pulling it down the ramp.

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