Is Conservation of Energy Always Applicable in Collisions?

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Discussion Overview

The discussion revolves around the applicability of conservation of energy in the context of collisions involving a movable inclined plane and a block. Participants explore whether mechanical energy is conserved when a block collides with the plane, considering various scenarios and assumptions about the nature of the collision and energy transformations.

Discussion Character

  • Exploratory
  • Debate/contested
  • Conceptual clarification
  • Mathematical reasoning

Main Points Raised

  • Some participants question whether the interaction between the block and the inclined plane constitutes a collision, particularly if the block passes through the plane.
  • There is a suggestion that if the interaction is a collision, it is not elastic, implying that total kinetic energy is not conserved.
  • One participant proposes using the conservation of mechanical energy to relate the initial and final states of the block, despite the uncertainty about energy conservation during the collision.
  • Another participant introduces the idea of considering the block and wedge together to apply conservation principles, raising questions about the correct approach to relate variables like velocity, height, and mass.
  • Some participants express differing views on the conservation of energy, with one emphasizing that energy is always conserved in a broader sense, while others argue that kinetic energy specifically is not conserved in inelastic collisions.
  • One participant presents a mathematical approach involving forces and the work-energy theorem to derive relationships between the variables involved in the collision.
  • There is a discussion about the clarity of language used when referring to energy conservation, with some advocating for more precise terminology to avoid confusion.

Areas of Agreement / Disagreement

Participants express differing views on the conservation of energy in collisions, with no consensus reached. Some agree that kinetic energy is not conserved in inelastic collisions, while others maintain that energy conservation applies in a broader context.

Contextual Notes

Participants note the importance of distinguishing between different forms of energy and the conditions under which conservation principles apply. There are unresolved questions about the assumptions made regarding the nature of the collision and the definitions of energy types involved.

ximath
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Dear All,

Suppose we have a movable inclined plane (initially at rest) which has height h (if we attach wheels, then it should be movable) and assume that there is no friction anywhere. If a block travels with speed V towards the plane and goes up to the distance h, I wonder ;

Is mechanical energy of the block alone is conserved ? (not kinetic energy!)

First of all, I would like to know whether it is a collision or not. If the block is going through the plane, are they colliding ?

And if they are colliding, then it certainly is not an elastic collision. So total kinetic energy must not be conserved. But would equation

mblock * g * hblock = 1/2 mblock * Vinitial^2 - 1/2 mblock * Vfinal^2

hold ? (I thought I could use conservation of momentum to calculate Vfinal ) PS: I didn't want to post it as homework question to the other forum because it isn't a homework, only a conceptual exercise that I have imagined but have been unable to come up with a reasoning.
 
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ximath said:
Suppose we have a movable inclined plane (initially at rest) which has height h (if we attach wheels, then it should be movable) and assume that there is no friction anywhere. If a block travels with speed V towards the plane and goes up to the distance h, I wonder ;

Is mechanical energy of the block alone is conserved ? (not kinetic energy!)

First of all, I would like to know whether it is a collision or not. If the block is going through the plane, are they colliding ?

Hi ximath! :smile:

Yes, it is a collision, and it's "sharp" (as opposed to gradual), so energy won't be conserved.
PS: I didn't want to post it as homework question to the other forum because it isn't a homework, only a conceptual exercise that I have imagined but have been unable to come up with a reasoning.
It's still "homework or coursework" … do use that forum in future. :smile:
 
Hi again!

What if we consider block and wedge together: then could we write U1 + K1 = U2 + K2 to relate V with h, g and masses ?

If we can't, what would be the correct approach to relate V with those quantities ?


tiny-tim said:
It's still "homework or coursework" … do use that forum in future.
I'll use that forum next time :)
 
tiny-tim said:
Yes, it is a collision, and it's "sharp" (as opposed to gradual), so energy won't be conserved.

...What?
 
Crazy Tosser said:
...What?

Most collisions are not elastic collisions and so energy is not conserved.

Good rule of thumb … if it makes a noise, then energy isn't conserved! :biggrin:
ximath said:
Hi again!

What if we consider block and wedge together: then could we write U1 + K1 = U2 + K2 to relate V with h, g and masses ?

If we can't, what would be the correct approach to relate V with those quantities ?

Hi ximath! :smile:

Let's examine this systematically, since it's obviously worrying you …

as you've worked out, you need two equations to solve a collision problem like this …

and you're thinking one of them is always conservation of momentum, but if the other one isn't conservation of energy, where do I get my second equation from? :cry:

The answer is that it will usually be a geometrical constraint …

for example, if a bullet embeds itself in a block, then v1 = v2, which is the second equation you need.

In this case, the geometrical constraint is that the block is obliged to stay on the slope … that gives you your one extra (slightly complicated! :rolleyes:) equation!

That gives you the "initial final speed" of the block, just as it starts up the slope. Obviously, you can use conservation of energy after that. :smile:
 
tiny-tim said:
In this case, the geometrical constraint is that the block is obliged to stay on the slope … that gives you your one extra (slightly complicated! :rolleyes:) equation!

That gives you the "initial final speed" of the block, just as it starts up the slope. Obviously, you can use conservation of energy after that. :smile:
I am not sure I understand... Could you give me an idea of how to derive that equation in that case ? And how can I use conservation of energy after that, if energy is not conserved ?
 
tiny-tim said:
Most collisions are not elastic collisions and so energy is not conserved.

Good rule of thumb … if it makes a noise, then energy isn't conserved! :biggrin:

Well, that's like your perception, man...

If you view it in this way, then I bet you that the total energy of the accelerated air molecules, emitted light, heated surface, and kinetic energy of molecules inside the blocks is conserved.

Next time, instead of using "energy is not conserved", use "kinetic energy of the blocks is not conserved" :P
 
Crazy Tosser said:
Next time, instead of using "energy is not conserved", use "kinetic energy of the blocks is not conserved" :P


Like most people, I'll continue to say "conservation of energy" when mechanical or kinetic energy is obviously implied.
ximath said:
And how can I use conservation of energy after that, if energy is not conserved ?

It's like a mid-air collision … you have to split the experiment into two parts … the collision itself, in which energy is not conserved … and then the aftermath, in which energy is conserved.
I am not sure I understand... Could you give me an idea of how to derive that equation in that case ?

Nooo! Have a go yourself! :smile:
 
Last edited:
Hi,

I guess I solved it.

My approach:

Suppose X is the distance wedge travels and n is the normal force acted by wedge to the
block, w is the weight of the block and M is the mass of the weight.

Then;

n sin(theta) * ( X + h/tan(theta) ) = Ki - Kf

and since w = n cos (theta) ;

w*tan(theta)*(X + h/than(theta)) = Ki - Kf

Vi^2 - Vf^2 = 2g(tan(theta)X + h)

and if we substitute Vi = (m + M) * Vf / m (conservation of momentum) to find an equation.

The other equation I have found was from the work-energy theorem for the wedge.

nsin(theta)*X = 1/2 M Vf^2 and thus Xtan(theta) = MVf^2 / 2mg

And solving these two equations give the result I expected.

Thanks a lot for that!
 
  • #10
tiny-tim said:
Like most people, I'll continue to say "conservation of energy" when mechanical or kinetic energy is obviously implied.





I’m not sure about “most people” but this is a physics forum and saying that “energy is not conserved” is at least very confusing and at most very wrong. Energy is ALWAYS conserved, and that is one of the most fundamental statements in all of physics. Maybe kinetic energy was “implied” and maybe it wasn’t, but why not take the extra precaution of specifically stating the type of energy involved to avoid any confusion? It just seems a reasonable approach.
 
  • #11
so sue me …

schroder said:
I’m not sure about “most people” …

Sorry, but I am!

Virtually everyone says "conservation of momentum" and "conservation of energy" (… "does or does not apply" in a particular case), without qualifying the word "energy" in any way.

Further or alternatively, m'luds, the context is almost always "in" something (usually "in a collision"), and so the conservation or non-conservation clearly falls to be interpreted as applying in that context.
… but this is a physics forum …

… and not a legal one! :biggrin:
 

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