Why is the Highlighted Statement True?

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Homework Help Overview

The discussion revolves around the principles of momentum and kinetic energy in the context of perfectly elastic collisions, specifically involving two equal masses. Participants are examining the validity of a highlighted statement related to these principles.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants explore the equations governing elastic collisions, questioning the assumptions about mass and the implications of conservation laws. They discuss the relationship between initial and final velocities and how these relate to kinetic energy and momentum conservation.

Discussion Status

The discussion is active, with participants providing insights and raising questions about the implications of their findings. Some have suggested combining momentum and energy conservation laws, while others are considering the effects of different mass scenarios. There is recognition of the need for further exploration of the topic.

Contextual Notes

Some participants note the potential for differing interpretations of the highlighted statement, particularly regarding its generality versus typicality. There are also mentions of constraints related to the context of collisions and the frames of reference involved.

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Homework Statement
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Relevant Equations
Please see below
Can someone please explain to me why the highlighted statement true?
1681971701932.png

Many thanks!
 
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Simple kinetics. Consider two equal masses head-on in a perfectly elastic collision. Can you write the equations for the resulting velocities?
 
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haruspex said:
Simple kinetics. Consider two equal masses head-on in a perfectly elastic collision. Can you write the equations for the resulting velocities?
Thank you for your reply @haruspex!

I guess it is reasonable assumption to assume that the molecules have the same mass.

##KE_i = KE_f## for perfectly elastic collision
##\frac{1}{2}mv^2_{1i} + \frac{1}{2}mv^2_{2i} = \frac{1}{2}mv^2_{1f} + \frac{1}{2}mv^2_{2f}##
##mv^2_{1i} + mv^2_{2i} = mv^2_{1f} +mv^2_{2f}##
##v^2_{1i} + v^2_{2i} = v^2_{1f} +v^2_{2f}##

Many thanks!
 
ChiralSuperfields said:
Thank you for your reply @haruspex!

I guess it is reasonable assumption to assume that the molecules have the same mass.

##KE_i = KE_f## for perfectly elastic collision
##\frac{1}{2}mv^2_{1i} + \frac{1}{2}mv^2_{2i} = \frac{1}{2}mv^2_{1f} + \frac{1}{2}mv^2_{2f}##
##mv^2_{1i} + mv^2_{2i} = mv^2_{1f} +mv^2_{2f}##
##v^2_{1i} + v^2_{2i} = v^2_{1f} +v^2_{2f}##

Many thanks!
and what about momentum conservation?
 
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Or, some down-to-earth comments.

Have you played or watched a game of pool or billiards?
Have you ever witnessed a car collision where a car hits a stopped car?

Is there any movement of the stopped object when it is hit?
 
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Tom.G said:
Or, some down-to-earth comments.

Have you played or watched a game of pool or billiards?
Have you ever witnessed a car collision where a car hits a stopped car?

Is there any movement of the stopped object when it is hit?

ok, except that the statement under consideration appears to claim it as general fact, not as merely typical.
 
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Thank you for your replies @haruspex and @Tom.G !

## mv_{1i}+ mv_{2i} = mv_{1f}+ mv_{2f} ##
## v_{1i}+ v_{2i} = v_{1f}+ v_{2f} ##
 
ChiralSuperfields said:
Thank you for your replies @haruspex and @Tom.G !

## mv_{1i}+ mv_{2i} = mv_{1f}+ mv_{2f} ##
## v_{1i}+ v_{2i} = v_{1f}+ v_{2f} ##
You should be able to combine the momentum and energy conservation laws to obtain: ##v_{1i}- v_{2i} = v_{2f} -v_{1f}##. (This is even if the masses differ, and is a very useful equation to remember. There's also a more general form involving coefficient of restitution.)
What does that allow you to deduce when the masses are the same?
 
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haruspex said:
You should be able to combine the momentum and energy conservation laws to obtain: ##v_{1i}- v_{2i} = v_{2f} -v_{1f}##. (This is even if the masses differ, and is a very useful equation to remember. There's also a more general form involving coefficient of restitution.)
What does that allow you to deduce when the masses are the same?
Thank you for your reply @haruspex!

That equation says that the relative velocities of the masses before the collision is equal to the relative velocities of the masses after the collision when all velocities are taken from the same frame of reference. If the masses are the same, then initial relative KE will equal to the finial relative KE.

##KE_{{rel}_{i}} = KE_{{rel}_{f}}##
##\frac{2m}{2}(v_{1i}- v_{2i})^2 = \frac{2m}{2}(v_{2f} -v_{1f})^2##
##m(v_{1i}- v_{2i})^2 =m(v_{2f} -v_{1f})^2##
##(v_{1i}- v_{2i})^2 =(v_{2f} -v_{1f})^2##

Do you please know whether that was what I was meant to get?

Many thanks!
 
  • #10
ChiralSuperfields said:
Do you please know whether that was what I was meant to get?
No.
We have ##v_{1i}- v_{2i} = v_{2f} -v_{1f}## and the momentum conservation equation ## m_1v_{1i}+ m_2v_{2i} = m_1v_{1f}+ m_2v_{2f} ##. For the special case of equal masses, the latter reduces to:
ChiralSuperfields said:
## v_{1i}+ v_{2i} = v_{1f}+ v_{2f} ##
What do those two equations that only involve velocities tell you?
 
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  • #11
## v_{1i}^2 + v_{2i}^2 = v_{1f}^2 + v_{2f}^2 ## (1)
## v_{1i} + v_{2i} = v_{1f} + v_{2f} ## (2)

You should be able to reforumulate eq. (1) using the conjugate rule in order to invoke eq. (2) to get the velocitiy-relation that haruspex wrote.
 
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  • #12
haruspex said:
ok, except that the statement under consideration appears to claim it as general fact, not as merely typical.
So? You also considered a special case, heads on collision.
 
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  • #13
malawi_glenn said:
So? You also considered a special case, heads on collision.
That was a first step. The generalisation to oblique collisions is easy: just take the velocity components in the line of centres.
More problematic may be differing masses.
 
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  • #14
haruspex said:
That was a first step. The generalisation to oblique collisions is easy: just take the velocity components in the line of centres.
More problematic may be differing masses.
But having one mass at rest initially is just to transform to its rest-frame
 
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  • #15
malawi_glenn said:
But having one mass at rest initially is just to transform to its rest-frame
The distribution of KE looks different in different inertial frames. Two observers may disagree on which started with the greater KE. Yes, they will agree that the roles swapped, but this is likely to make the argument unconvincing to some.
 
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  • #16
Thank you for your replies @haruspex and @malawi_glenn !

Sorry I will come back to this thread once the mid-term exams are over. I also don't want to waste your time on things I that are already in the textbook, so I think I will also finish learning momentum before replying.

Many thanks!
 
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