The physics of billiards. (Describing the motion)

Click For Summary

Homework Help Overview

The discussion revolves around describing the motion of a cue ball on a billiard table, focusing on the transition between sliding and rolling motion. The original poster is constrained from using equations related to rotational motion or work and energy theorems, which shapes the nature of the inquiry.

Discussion Character

  • Exploratory, Assumption checking, Problem interpretation

Approaches and Questions Raised

  • The original poster attempts to reason through the motion of the cue ball, questioning whether it will slide or roll after being struck. They explore scenarios of pure sliding versus a combination of sliding and rolling. Participants raise questions about the forces acting on the ball and the nature of friction involved. There is also a focus on calculating the distance traveled before the ball begins to roll purely and the minimum force required for each scenario.

Discussion Status

Participants are actively engaging with the original poster's reasoning, offering insights into the forces at play and the relationships between them. Some guidance has been provided regarding the need for a free body diagram and the implications of different friction types. There is ongoing exploration of the equations governing the motion, with some participants questioning the consistency of signs used in calculations.

Contextual Notes

The original poster is working under specific constraints that limit the use of certain physics principles, which may affect the approaches discussed. There is also a noted confusion regarding the signs used in equations, which is being clarified through the discussion.

JuanC97
Messages
48
Reaction score
0
A. The problem: (If you want the short version just read the underlined statements)
I need to describe the motion of a cue ball over the cloth of a billiard table.
For rule, I can't use equations for rotational motion or 'Work and Energy theorems'
. I have some ideas but I'm not sure about the concepts and procedures. I'd appreciate it if you take a look to my reasoning and give me some pieces of advices (I'm just trying to describe traslation)

B. Relevant equations:
Friction force due to bearing (Rolling resistance): Frr = Crr* N
Crr is the Rotational resistance coefficient ; N is the Normal force.
Dynamic (Kinetic / Sliding) friction: Frd = μd * N

C. The attempt at a solution: (Reasoning)
See the first Image: The white ball is at rest. There are frictional forces.
The cue hits the ball in its center of mass and the force it's aplied parallel to the plane.
Because of the motion it will be a frictional force acting opposite the movement but...
Here's the problem: the ball will roll or it will slide ? (What kind of friction goes into the equations?)

I think these are the most probable situations:
1. The cue hits the ball and its motion is Pure sliding. A few meters later, the motion is pure rolling.
2. The cue hits the ball and its motion combines Sliding and rolling. Then, is just pure rolling.

D. The questions:
* In both cases I have to calculate the distance traveled before starting to roll purely. How?
* How can I find an expression of the minimum force needed to make each of those possiblities real?

It's my first question in PF.
I will appreciate every hint and piece of advice that you could give me. :)
 

Attachments

  • IMG 1.png
    IMG 1.png
    16.7 KB · Views: 669
Physics news on Phys.org
Draw the free body diagram. Supposing the initial (center of mass) motion is to the right, you need to answer the following questions:

1. Which forces are acting on the ball, and in which direction?
2. Where on the ball are these forces acting?

You should find that the rolling resistance and dynamic friction oppose each other. Which one is larger? It depends on whether ## C_r > \mu_d ## or vice versa; the two possibilities correspond to the two scenarios you described above.

To calculate the distance, use the fact that net torques cause angular acceleration (## \tau = I \alpha ##, and ##I = \frac{2}{5} M R^2## for a sphere) and the kinematic equations for rotational motion.
 
JuanC97 said:
1. The cue hits the ball and its motion is Pure sliding. A few meters later, the motion is pure rolling.
Pure sliding at first, yes. What is the nature of the motion between then and pure rolling?
JuanC97 said:
In both cases I have to calculate the distance traveled before starting to roll purely.
UVCatastrophe said:
you need to answer the following questions:

1. Which forces are acting on the ball, and in which direction?
2. Where on the ball are these forces acting?
Agreed.
UVCatastrophe said:
You should find that the rolling resistance and dynamic friction oppose each other.
Eh? The two will act in the same direction, and will be effectively indistinguishable until pure rolling is achieved, so might as well consider it all to be friction.
 
Ok, I'm working on the equations for rolling motion and traslation. (They're almost done but, I'll share them another day). Now I have this question:

I found on Internet that the time that the ball slips (before starting to roll at 100%) is: [tex]\Delta t = \frac{2}{7} \frac{V_o}{\mu g}[/tex]
But... When I try to deduce it I get another thing. Here's what I did:
[tex]\left[Eq. 1\right] \; \; \; I\Delta \omega = \tau \Delta t \; \longrightarrow \; I(\omega_f - \omega_o) = FR\Delta t \\<br /> \left[Eq. 2\right] \; \; \; m\Delta V = F\Delta t \; \longrightarrow \; m(V_f - V_o) = F\Delta t[/tex]
Since V=WR when the ball starts the pure rolling motion and W(0)=0, we can rewrite these equations.
[tex]\left[Eq. 1\right] \; \; \; I\omega_f = FR\Delta t \; \longrightarrow \: \omega_f=FR\Delta t / I<br /> \\<br /> \left[Eq. 2\right] \; \; \; m(\omega_f R - V_o) = F\Delta t \; \longrightarrow \; \frac{5\, m\, R^2 \, F \, \Delta t}{2\, m\, R^2} - mV_o = F\Delta t<br /> \\<br /> \left(\frac{5}{2} - 1\right)F\Delta t = mV_o \; \longrightarrow \; \frac{3}{2}F\Delta t = mV_o \; \longrightarrow \; \Delta t = \frac{2mV_o}{3F} = \frac{2mV_o}{3mg\mu} = \frac{2}{3}\frac{V_o}{g\mu}[/tex]
And this should be true if the ball moves along a plane with friction before starting the phase of pure rolling.
So... which of those " Δt " is the right time that takes the ball to start the pure rolling motion?
 
Last edited:
You're not being consistent with your signs. I can't point to a specific error unless you define which is the positive sense for forces, velocities, rotations... At the end you should have ##(\frac 52+1)##.
Btw, you can simplify it a little by considering conservation of angular momentum about a fixed point at ground level. The frictional force has no moment about such a point.
 
I use this convection:

Forces that goes in the same direction of the linear acceleration are positive.
Torques that goes in the clockwise sense are positive (Because these torques goes in the same direction of the angular acceleration)
 
JuanC97 said:
Forces that goes in the same direction of the linear acceleration are positive.
Then that's opposite to the direction of travel, right? So what sign are you using for velocities?
JuanC97 said:
Torques that goes in the clockwise sense are positive
That doesn't help me because there's no diagram. Do you mean the direction of angular acceleration is positive?
 
haruspex said:
what sign are you using for velocities?
I take both velocities as positive (The same for the accelerations). Then, these would be my equations:
[tex]-F_r = ma \\ FrR=I\alpha[/tex]
 

Attachments

  • image.png
    image.png
    5.6 KB · Views: 582
JuanC97 said:
I take both velocities as positive (The same for the accelerations). Then, these would be my equations:
[tex]-F_r = ma \\ FrR=I\alpha[/tex]
If all forces, accelerations, displacements and linear velocities are positive in the original direction of travel then F = ma. F takes a negative value, resulting in a negative acceleration. Conversely, this negative F will produce a positive angular acceleration, therefore FR = - Iα.
 
  • #10
Hmmm, that would explain a lot of things...
I'll remake some calcs, maybe that was the problem.
Thanks.
 

Similar threads

Replies
14
Views
3K
  • · Replies 60 ·
3
Replies
60
Views
5K
  • · Replies 16 ·
Replies
16
Views
2K
Replies
3
Views
3K
Replies
4
Views
2K
  • · Replies 4 ·
Replies
4
Views
5K
  • · Replies 8 ·
Replies
8
Views
5K
  • · Replies 5 ·
Replies
5
Views
3K
  • · Replies 8 ·
Replies
8
Views
4K
Replies
11
Views
2K