2D conservation of Energy and Momentum with *Three* unknowns

In summary: Please don't ignore my suggestion that you pay attention to what I wrote about the geometry of the situation.In summary, the problem involves two identical balls colliding elastically, with one ball moving at a speed of 3.0 m/s and the other stationary. After the collision, the first ball moves away at an angle of 30 degrees to its original path. The goal is to determine the speed and direction of both balls after the collision. The equations used are the conservation of momentum and conservation of energy, and the law of cosines is applied to find the angle between the momentum vectors of the two balls after the collision.
  • #1
Sjoyes
10
0

Homework Statement


A 2.0 kg ball moving with a speed of 3.0 m/s hits, elastically, an identical

stationary ball as shown. If the first ball moves away with angle 30 ° to the

original path, determine

a. the speed of the first ball after the collision.

b. the speed and direction of the second ball after the collision.

Homework Equations


m1v1 + m2v2 = m1v1' + m2v2'

1/2m1v1^2 + 1/2m2v2^2 = 1/2m1v1'^2 + 1/2m2v2'^2

The Attempt at a Solution


[/B]
m1 = m2 = 2.0kg
v1 = 3.0m/s
v2 = 0m/s
theta1 = 30

In the x direction

m1v1 + m2v2 = m1v1'cos30 + m2v2'cos(theta2)
(2.0)(3.0) + (2.0)(0) = (2.0)v1'cos30 + (2.0)v2'cos(theta2)
masses cancel out to leave;
3.0 = v1'cos30 + v2'cos(theta2)

In the y direction

m1(0) + m2(0) = m1v1'sin30 + m2v2'sin(theta2)
masses cancel to leave:
-v1'sin30 = v2'sin(theta2)

Now here is where I am getting stuck. I know that I have to somehow combine the x and y equations as well as the conservation of NRG eqn to find the three unknowns, but I am lost as to how the algebra will work out. I think I have to square them somehow to eventually get cos^2(theta2) + sin^2(theta2) = 1 to get around the unknown theta... but everytime I have tried, it doesn't work out. Please help!
 
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  • #2
The balls each have a momentum vector after the collision and you can visualize those vectors as two sides of a triangle, with the third side being their sum. Conservation of energy says that the sum of the squares of the the magnitudes of the two momentum vectors is the square of the magnitude of the third side. So the triangle is a right triangle.

To show this by algebra, you could argue from the law of cosines C^2 = A^2 + B^2 - 2 AB Cos(theta) that the term 2 AB cos(theta) is zero.
 
  • #3
So are you saying that:

v1^2 = v1'^2 + v2'^2 - 2(v1')(v2')cos(theta) ??

then would v1' and v2' just be the rearrangement of the x and y components of the momentum eqns in the Pythagorean theorem?
i.e. v1' = sqrt(((v1 - v2'cos(theta))/cos30)^2 + ((v2'sin(theta))/sin30)^2)
and v2' = sqrt(((v1-v1'cos30)/cos(theta))^2 +((v1'sin30)/sin(theta))^2) ?
 
  • #4
Sjoyes said:
So are you saying that:

v1^2 = v1'^2 + v2'^2 - 2(v1')(v2')cos(theta) ??

No, not as I understand your notation. You aren't using "theta" for the angle between the two momentum vectors after the collision.

I'm talking about the magnitudes of 3 vectors. If A,B,C are vectors with C = A + B then |C|^2 =|A|^2 + |B|^2 - 2|A||B| cos( alpha) where alpha is the angle between A and B and |V | denotes the magnitude of a vector V.

In your notation, I think alpha = theta2 + 30 deg.

then would v1' and v2' just be the rearrangement of the x and y components of the momentum eqns in the Pythagorean theorem?

That isn't a clear question.

The magnitudes of the vectors can be computed from the magnitudes of their orthogonal components by using the Pythagorean theorem, but in this problem you can tell the magnitudes just by thinking of "the unit circle".

For example one ball leaves the collision with a magnitude vector whose components are (m1 v'1 cos(30 deg), m1 v'1 sin(30 deg)) The magnitude of this vector is the absolute value of m1v'1.
 
  • #5
I am so very lost.

I don't think I understand where you are trying to hint me towards using the law of cosines. Is it for the whole system, or just one isolated vector? i.e. C = v1 or am I just using it to find v1' and A and B will be the x and y component of v1'?

Stephen Tashi said:
The balls each have a momentum vector after the collision and you can visualize those vectors as two sides of a triangle, with the third side being their sum. Conservation of energy says that the sum of the squares of the the magnitudes of the two momentum vectors is the square of the magnitude of the third side. So the triangle is a right triangle.
Also is this referring to the momentum vectors of one ball, or the whole system?

If it was for one ball, would it be

v1'^2 = (m1v1'cos30)^2 + (m1v1'sin30)^2

or using momentum;

v1'^2 = ((v1-v2'cos(theta))/cos30)^2 + ((v2'sin(theta))/sin30)^2

If it was for the system, would it look like this;

v1^2 = v1'^2 + v2'^2
v1^2 = (sqrt((m1v1'cos30)^2+(m1v1'sin30)^2))^2 + (sqrt((m2v2'cos(theta))^2 +(m2v2'sin(theta))^2))^2

or if using the conservation on momentum eqns in x and y;

v1^2 = (((v1 - v2'cos(theta))/cos30)^2 + ((v2'sin(theta))/sin30)^2)^2 +(((v1-v1'cos30)/cos(theta))^2 +((v1'sin30)/sin(theta))^2)^2

Oh dear... as you can see, I am very lost as to what to use where... is any of this right?
 
  • #6
Sjoyes said:
I don't think I understand where you are trying to hint me towards using the law of cosines. Is it for the whole system, or just one isolated vector? i.e. C = v1 or am I just using it to find v1' and A and B will be the x and y component of v1'?

C is the vector sum of the momentum vectors of the two balls after the collision. A is the vector of momentum of one ball after the collisionl, B is the vector of momentum for the other ball. [Remember that momentum is a vector quantity, not a scalar quantity.] You haven't defined your variables. You seem to be using v1 to mean both a vector and the magnitude of a vector. That isn't good notation.

Because of conservation of momentum C is also equal to the momentum vector of the first ball before the collision.

To apply the law of cosines you must have a variable or an expression that represents the angle between the momentum vectors of the two balls after the collision.

You wrote several equations that have velocity on the left hand side and momentum on the right hand side, so they don't make sense.
 
  • #7
OK, I think I understand a little better now?
Just like in kinematics, adding vectors A and B tip to tail, will be equal to vector C, and like you said, C will be equal to the vector of the first ball because of conservation of momentum.

So in the x direction

(v1i)^2 = (v1fcos30)^2 + (v2fcos(alpha))^2 - (2(v1fcos30)(v2fcos(alpha)) cos theta)

and in the y direction

0 = (v1fsin30)^2 + (v2fsin(alpha))^2 - (2(v1fsin30)(v2fsin(alpha)) cos theta)

(where alpha is the angle between v2f and the horizontal and theta is the angle between v1f and v2f)

Stephen Tashi said:
To apply the law of cosines you must have a variable or an expression that represents the angle between the momentum vectors of the two balls after the collision.

so would this become something like theta= alpha + 30?
 
  • #8
Sjoyes said:
OK, I think I understand a little better now?
Just like in kinematics, adding vectors A and B tip to tail, will be equal to vector C, and like you said, C will be equal to the vector of the first ball because of conservation of momentum.

Yes, but you are still thinking of things component-by-component instead of acknowledging that the magnitude of a 2-D vector involves two components.

Write both components of the vectors.

|(0, mv1)|^2 = |(m v'1 cos(30 deg), mv'1 sin(30 deg) )| ^2 + |(mv'2 cos (alpha), mv'2 sin(alpha)|^2 - 2 |(m v'1 cos(theta), mv'1 sin(theta) )| |(mv'2 cos (alpha), mv'2 sin(alpha)| cos(30 deg + alpha))

This give you one equation , not two equations.

You know the formula for the magnitude of a vector V = (a,b) in terms of it's components - yes ?
 
  • #9
Stephen Tashi said:
You know the formula for the magnitude of a vector V = (a,b) in terms of it's components - yes ?
That would be Pythagorean theorem... c^2 = a^2 + b^2
so the first term (on the right) would become

|sgrt((mv'1cos(30deg))^2 + (mv'1sin(30deg))^2)|^2... and so on...

also in the second half of your equation (the -2AB...), is the theta referring to the 30 deg? or the 30 deg +alpha?
 
  • #10
Sjoyes said:
That would be Pythagorean theorem... c^2 = a^2 + b^2
so the first term (on the right) would become

|sgrt((mv'1cos(30deg))^2 + (mv'1sin(30deg))^2)|^2... and so on...

Yes. It comes out to be (mv'1)^2 since sin^2(angle) + cos^2(angle) = 1.

also in the second half of your equation (the -2AB...), is the theta referring to the 30 deg? or the 30 deg +alpha?
[/QUOTE}

Yes. I should have used 30 deg for theta.
 
  • #11
OK,
so since sin^2(angle) + cos^2(angle) =1 is in both A and B terms, then everything would simplify to:

mv1^2 = mv'1^2 + mv'2^2 - 2(mv'1)(mv'2) cos (30deg +theta)
 
  • #12
Sjoyes said:
OK,
so since sin^2(angle) + cos^2(angle) =1 is in both A and B terms, then everything would simplify to:

mv1^2 = mv'1^2 + mv'2^2 - 2(mv'1)(mv'2) cos (30deg +theta)

Yes. Then you can apply conservation of energy to show the last term must be zero.
 
  • #13
mv1^2 = mv'1^2 + mv'2^2 - 2(mv'1)(mv'2) cos (30deg +alpha)

In my notation the angle is 30 deg + alpha.
 
  • #14
Stephen Tashi said:
mv1^2 = mv'1^2 + mv'2^2 - 2(mv'1)(mv'2) cos (30deg +alpha)

In my notation the angle is 30 deg + alpha.

Yes, sorry, just a typo.

So since the 2(mv'1)(mv'2) cos (30deg + alpha) is 0... then that just leaves me with mv1^2 = mv'1^2 + mv'2^2... but then I still have two unknowns. So I would need another equation to substitute into that to figure out one of the unknowns.

Now I am confused again... what can I possibly use to figure this out?
 
  • #15
Sjoyes said:
Yes, sorry, just a typo.

So since the 2(mv'1)(mv'2) cos (30deg + alpha) is 0... then that just leaves me with mv1^2 = mv'1^2 + mv'2^2... but then I still have two unknowns. So I would need another equation to substitute into that to figure out one of the unknowns.

Now I am confused again... what can I possibly use to figure this out?

Don't forget to explain why 2(mv'1)(mv'2) cos (30 deg + alpha) = 0 in your work.

2(mv'1)(mv'2) cos (30 deg + alpha) = 0 should tell you something about the possibilities for alpha
 
  • #16
Stephen Tashi said:
Don't forget to explain why 2(mv'1)(mv'2) cos (30 deg + alpha) = 0 in your work.

2(mv'1)(mv'2) cos (30 deg + alpha) = 0 should tell you something about the possibilities for alpha

Well I was thinking that the 2ABcos(angle) term had to be 0 because the rest of the equation (C^2 = A^2 + B^2) is analogous to the conservation of NRG eqn ( (1/2)mv1^2 + (1/2)mv2^2 = (1/2)mv'1^2 + (1/2) mv'2^2 ) and because of that, 2ABcos(angle) had to be zero.

But the only for sure way that 2ABcos(angle) could be 0 is if the cos(angle) term is 0, which would mean that alpha is 60deg?
 
  • #17
Sjoyes said:
Well I was thinking that the 2ABcos(angle) term had to be 0 because the rest of the equation (C^2 = A^2 + B^2) is analogous to the conservation of NRG eqn ( (1/2)mv1^2 + (1/2)mv2^2 = (1/2)mv'1^2 + (1/2) mv'2^2 ) and because of that, 2ABcos(angle) had to be zero.
That's correct reasoning. You can show it by algebra if you write the conservation of kinetic energy equation , multiply it by 2 and subtract that equation from the above equation.

But the only for sure way that 2ABcos(angle) could be 0 is if the cos(angle) term is 0, which would mean that alpha is 60deg?
Yes, if after the collision we draw the first balls momentum vector in the first quadrant and the second ball's momentum vector in the fourth quadrant, the angle of the second balls momentum vector measured counter clockwise to the x-axis is 60 deg. You would call the angle of the second ball's momentum vector -60 deg or 300 deg when describing it in the conventional way as an angle in the fourth quadrant.

cos(angle) = 0 when angle = 90 deg or angle = 270 deg. You can say the 270 deg solution won't solve the problem since the second ball's momentum vector must be in the fourth quadrant in order to conserve y-momentum.
 
  • #18
OK, now that I have the angle of v'2, I think I know how to figure out v'1 and v'2;
Using conservation of momentum...

In the x direction
m1v1 + m2v2 = m1v'1 + m2v'2
(2)(3) + (2)(0) = (2)v'1cos(30) + (2)v'2cos(60)
3 = v'1cos(30) + v'2cos(60)

In the y direction
m1v1 + m2v2 = m1v'1 + m2v'2
(2)(0) + (2)(0) = (2)v'1sin(30) + (2)v'2sin(60)
v'1sin(30) = v'2sin(60)
v'1 = (v'2sin(60))/sin(30)

Sub y eqn into x eqn

3 = ((v'2sin(60))/sin(30))cos(30) + v'2cos(60)
3 = v'2(1.5) + v'2(0.5)
3 = 2v'2
v'2 = 1.5

Sub v'2 in y eqn

v'1sin(30) = (1.5)sin(60)
v'1 = 2.6

So v'1 = 2.6m/s and v'2 = 1.5m/s

Thank you so much for taking some of your time to help another having serious struggles! You are a champ for being patient with someone not so fluent in physics.
Thanks again. :)
 
  • #19
Sjoyes said:
In the y direction
m1v1 + m2v2 = m1v'1 + m2v'2
(2)(0) + (2)(0) = (2)v'1sin(30) + (2)v'2sin(60)

You need to subtract 2v'2 sin(60) or treat the angle as -60 deg, which will have the same effect. The y-components point in the opposite directions.
 
  • #20
Right! Missed that!

Thanks again for all your help.
 

FAQ: 2D conservation of Energy and Momentum with *Three* unknowns

What is the conservation of energy in 2D?

The conservation of energy in 2D refers to the principle that the total energy of a system remains constant in a two-dimensional space, even as energy is transferred or transformed between different forms. This means that the sum of all potential and kinetic energies within the system remains the same, regardless of any changes that may occur.

What is the conservation of momentum in 2D?

The conservation of momentum in 2D states that the total momentum of a system in two-dimensional space remains constant, as long as there are no external forces acting on the system. This means that the total mass and velocity of all objects within the system will remain the same, even if individual objects may experience changes in velocity.

What are the three unknowns in 2D conservation of energy and momentum?

The three unknowns in 2D conservation of energy and momentum are the initial and final velocities and positions of the objects within the system. These variables are typically represented by the letters u (initial velocity), v (final velocity), x (initial position), and y (final position).

How is 2D conservation of energy and momentum applied in real world scenarios?

2D conservation of energy and momentum is applied in various real-world scenarios, such as collisions between objects in two-dimensional space. By applying the principles of conservation of energy and momentum, scientists and engineers can predict the outcomes of these interactions and design systems that maximize energy and momentum conservation.

What are some limitations of 2D conservation of energy and momentum?

One limitation of 2D conservation of energy and momentum is that it assumes there are no external forces acting on the system. In reality, external forces such as friction and air resistance can affect the outcome of a system and may not be accounted for in the conservation equations. Additionally, the equations may become more complex when dealing with multiple objects or when considering energy and momentum loss due to factors such as heat and sound.

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