Elastic collision between pool balls

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Homework Help Overview

The discussion revolves around an elastic collision between a super cue ball and a target ball on a frictionless table. The cue ball is larger than the target ball, and the problem involves determining the velocities and directions of both balls after the collision, as well as the target ball's direction in the center of mass frame.

Discussion Character

  • Exploratory, Assumption checking, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss the use of conservation of linear momentum and kinetic energy to set up equations for the collision. There are attempts to express the masses of the balls based on their volumes and densities. Some participants express confusion about how to start solving the problem due to the presence of vector equations.

Discussion Status

There is ongoing exploration of the equations related to momentum and energy conservation. Some participants have provided partial equations and are questioning the correctness of their expressions. Guidance has been offered regarding the interpretation of vector equations as scalar equations for momentum components.

Contextual Notes

Participants note the importance of the angle between the velocities after the collision and the need to account for the direction of the cue ball's velocity post-collision. There is mention of a figure that aids in visualizing the problem, which was initially missing.

John004
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Homework Statement


A super cue ball is made of the same material with the target ball (radius r) but slightly larger: rc = (3)^(1/3)*r The cue ball collides with the target ball on a frictionless table, as shown below, with initial speed of v0. The collision is not head-on, as shown below.

a) What are the velocities of the two balls after the collision? You need to determine both the speeds and directions!

b) In the CM frame, what is the target ball’s direction, relative to the x-axis?

Homework Equations


ρ = m/V
ρ = 4/3 π r3

The Attempt at a Solution


[/B]
so for the masses,

m1 = ρV1 , m2 = ρV2

taking the ratio of those guys gives m1 = 3 m2

if i use conservation of linear momentum and kinetic energy conservation, i end up with two sets of equations but one is a vector equation and the other is not, so i don't know how to even start this problem
 

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John004 said:

Homework Statement


A super cue ball is made of the same material with the target ball (radius r) but slightly larger: rc = (3)^(1/3)*r The cue ball collides with the target ball on a frictionless table, as shown below, with initial speed of v0. The collision is not head-on, as shown below.

a) What are the velocities of the two balls after the collision? You need to determine both the speeds and directions!

b) In the CM frame, what is the target ball’s direction, relative to the x-axis?

Homework Equations


ρ = m/V
ρ = 4/3 π r3

The Attempt at a Solution


[/B]
so for the masses,

m1 = ρV1 , m2 = ρV2

taking the ratio of those guys gives m1 = 3 m2

if i use conservation of linear momentum and kinetic energy conservation, i end up with two sets of equations but one is a vector equation and the other is not, so i don't know how to even start this problem
There should be a figure to the problem. Attach it please!
The vector equation can be written as two scalar equations for the components of the linear momentum. So you have three equations.
 
ehild said:
There should be a figure to the problem. Attach it please!
The vector equation can be written as two scalar equations for the components of the linear momentum. So you have three equations.
Oh right! its there now.
 
John004 said:
Oh right! its there now.
OK. So the velocity of the target ball encloses the angle pi/3 with the original velocity of the cue ball after the collision. The direction of velocity of the cue ball is unknown after collision. And energy is conserved. Write the equations for the components of the momenta, and also for the conservation of energy.
 
ehild said:
OK. So the velocity of the target ball encloses the angle pi/3 with the original velocity of the cue ball after the collision. The direction of velocity of the cue ball is unknown after collision. And energy is conserved. Write the equations for the components of the momenta, and also for the conservation of energy.
Ok so this is what I've done so far

m1<u1x,u1y> = m1<v1x, v1y> + m2<v2x, v2y>

where u1 is the velocity of mass 1 before the collision, v1 is the velocity of mass 1 afterwards, and similarly for mass 2.

I end up with

(√3)/6 v2 + v1cos(φ) = v0 where v0 = u1x these are the magnitudes of the velocities

v2 = -(6/√3)v1sin(φ)

and then the energy conservation expression

3v02 = 3v12 + v22

does this look ok so far?
 
John004 said:
I end up with

(√3)/6 v2 + v1cos(φ) = v0 where v0 = u1x these are the magnitudes of the velocities

v2 = -(6/√3)v1sin(φ)
Check the equations, there are mistakes in both.
John004 said:
and then the energy conservation expression

3v02 = 3v12 + v22

does this look ok so far?
The energy equation is OK.
 
ehild said:
Check the equations, there are mistakes in both.

The energy equation is OK.

m1<u1x, 0> = m1<v1x, v1y> + m2<v2x, v2y>

<m1u1x, 0> = <m1v1x, m1v1y> + <m2v2x, m2v2y>

<m1u1x, 0> = < m1v1x + m2v2x, m1v1y + m2v2y>

therefore,

m1v1x + m2v2x = m1v0

m1v1y = -m2v2y

3v1cos(φ) + ½v2 = 3v0

v2 = -(6/√3)v1sin(φ) still got the same thing for this one
 
John004 said:
3v1cos(φ) + ½v2 = 3v0

v2 = -(6/√3)v1sin(φ) still got the same thing for this one
It is OK. But do not forget, that you get negative angle φ. The cue ball moves under the x-axis after collision.
Isolate cos(φ) and sin(φ), square and add the equations, so as φ eliminates.
 

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