What does p = mv (momentum) really mean?

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The equation p = mv defines momentum as the product of mass and velocity, highlighting its significance as a conserved quantity in physics. This conservation is rooted in Noether's theorem, which connects symmetries in physical systems to conservation laws. Momentum is not a tangible entity but a mathematical construct that effectively describes motion and behavior in physical interactions. The relationship between mass and velocity in this context illustrates how changes in either variable affect momentum, reinforcing its practical utility in understanding dynamics. Ultimately, momentum's definition and conservation underpins its importance in classical mechanics.
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What does p = mv really mean? For example, why is there a physical law based upon the product of mass and velocity? Why does a human made operation, multiplication, give a quantity called momentum? If we define momentum as the product of m and v, why can't we define by some other operation, like division? For example, if m = 5, and v = 3, what is it about adding 5 to itself three times that gives this quantity called momentum in 15 kg m/s?
 
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Momentum is significant because it (firstly) is a conserved quantity. This is not just true of linear momentum, but angular momentum as well. Noether's theorem shows that if a system is symmetric under a certain transformation, there is a corresponding conservation law. In the case of ##\mathbf{p} = m \mathbf{v}## (which I may add is a classical approximation), it turns out that the sum of total momenta a isolated closed system does not change in time.

I would highly recommend reading more about Noether's theorem. I think it will satisfy many of your curiosities and it happens to be quite elegant!
 
Mr Davis 97 said:
What does p = mv really mean?

It means, mathematically, that if you increase m or increase v, then you will increase p. If v is negative, you are going in the opposite direction. This information might be important in certain problems.

For example, why is there a physical law based upon the product of mass and velocity? Why does a human made operation, multiplication, give a quantity called momentum?

You will have an easier time with this stuff if you realize that momentum isn't a "thing" that exists, but a quantity that was invented, and defined mathematically, to describe how things behave. (People also have this problem when it comes to "energy" which is just a mathematical quantity, not some stuff that's floating around).

If we define momentum as the product of m and v, why can't we define by some other operation, like division? For example, if m = 5, and v = 3, what is it about adding 5 to itself three times that gives this quantity called momentum in 15 kg m/s?

Classical physics attempts to use mathematics in a way that describes the behavior. Think about when you roll your shopping cart through the parking lot, or start riding around on it(I totally do this). You will have "more momentum" if there's more stuff (or you) on the basket, or if you are going faster. So that equation describes what's going on very well.


-Dave K
 
Mr Davis 97 said:
What does p = mv really mean? For example, why is there a physical law based upon the product of mass and velocity? Why does a human made operation, multiplication, give a quantity called momentum? If we define momentum as the product of m and v, why can't we define by some other operation, like division? For example, if m = 5, and v = 3, what is it about adding 5 to itself three times that gives this quantity called momentum in 15 kg m/s?
Welcome to PF Mr. Davis 97!

We can certainly define some other operation, such as division, and say p = m/j where j is the rate of change of time relative to position. It is just easier for humans to think in terms of velocity (v) which is the rate of change of position with time.

As others have said, physicists are interested in describing the physical world so the quantities that we are interested in must describe something that has some physical significance. Newton observed that the same force applied for same time to objects of different mass resulted in the same change in the quantity of motion for each. 'Quantity of motion' was the term Newton used for the product of velocity and mass. So, Newton concluded that keeping track of this quantity of motion, which we now call p = mv would be very useful.

AM
 
You ask about p := mv
or any definitions?
 
Mr Davis 97 said:
What does p = mv really mean? For example, why is there a physical law based upon the product of mass and velocity? Why does a human made operation, multiplication, give a quantity called momentum? If we define momentum as the product of m and v, why can't we define by some other operation, like division?
There is certainly no reason that you couldn't. We have already used the term "momentum" to refer to the product of mass and velocity, so you would need another word. But if you wish you could define "flubnubitz" as the ratio of mass to velocity.

We have found momentum to be a very useful quantity, for the reasons outlined above, but as far as I know flubnubitz is not a useful quantity.
 
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There are arguments that Momentum is at least as fundamental a concept as mass, velocity or energy etc.. Those things are all related by some handy mathematical operations.
If we happened to live in the absence of significant gravity, we might well be more concerned with momentum than with mass (giving weight force) and we could have started on our study of mechanics with momentum being much higher up our list of familiarity.
 
Questions such as "What really is momentum?" or "What really is mass?" etc. are utterly useless as far as the science is concerned. Answering them adds nothing to the predictive or explanatory power of the theories they derive from. All you have to know is that momentum is well-defined both mathematically and operationally. Anything else that might be said about them is simply philosophical sophistry.
 
MrRobotoToo said:
Questions such as "What really is momentum?" or "What really is mass?" etc. are utterly useless as far as the science is concerned. Answering them adds nothing to the predictive or explanatory power of the theories they derive from. All you have to know is that momentum is well-defined both mathematically and operationally. Anything else that might be said about them is simply philosophical sophistry.

Very true. Once you try to add a verbal /mechanical description to a quantity, you can end up limiting your understanding and can lose the more general meaning. It's a trait that many people follow, who do not want to get into the Maths. Whether you understand the Maths fully or not (I don't) you need to accept that it is by far the best language we have for this stuff.
 
  • #10
Well, but operating something not defined looks like little bit Crazy, or?
 
  • #11
Where did anyone say anything about "not defined"?
 
  • #12
vjacheslav said:
Well, but operating something not defined looks like little bit Crazy, or?

Using the Maths of the relationship between one quantity and others is miles better than describing it a 'a sort of pushing thing you get when it bumps into you'. That's extreme, I know but many people do seem to want something like it. It can never be very satisfactory - if you want to take it further and relate it to other things.
 
  • #13
MrRobotoToo said:
momentum is well-defined both mathematically and operationally.
vjacheslav said:
operating something not defined looks like little bit Crazy
?

This is an odd comment, vjacheslav.
 
  • #14
sophiecentaur said:
Very true. Once you try to add a verbal /mechanical description to a quantity, you can end up limiting your understanding and can lose the more general meaning. It's a trait that many people follow, who do not want to get into the Maths. Whether you understand the Maths fully or not (I don't) you need to accept that it is by far the best language we have for this stuff.

True, but I think you can get an intuitive understanding of these classical concepts thru experience: if you've played football you know there's a difference in tackling a 250 pounder running at you compared to a 135er just standing there. Or, if you have spent the day carrying shingles up to the roof, you know why work is force x distance.

Other concepts, say entropy or electron spin, not so much.
 
  • #15
MrRobotoToo said:
Questions such as "What really is momentum?" or "What really is mass?" etc. are utterly useless as far as the science is concerned. Answering them adds nothing to the predictive or explanatory power of the theories they derive from. All you have to know is that momentum is well-defined both mathematically and operationally. Anything else that might be said about them is simply philosophical sophistry.
Where would physics be if Galileo and Newton and Einstein had not tried to explain what mass is? It might be philosophy (or philosophia naturali as Newton called it) but it is the desire to understand that drives human beings.

Momentum is defined this way because of an underlying physical significance. So to fully understand the physics one has to understand both the definition and why it is defined that way.

AM
 
  • #16
Andrew Mason said:
Momentum is defined this way because of an underlying physical significance.
It's only significance is its conservation under certain conditions. That's the only reason why it is defined this way.
 
  • #17
Talk to someone with no idea of the Maths involved in Physics and you usually hear a pretty poor model of the World. Maths is so crucial to understanding at any but the very superficial level. Imagine trying to have a conversation about Finances without a common knowledge of the Arithmetic of Interest and Profit. The consequence of not using appropriate Maths is constantly being demonstrated by how people are regularly conned into bad deals. The numbers (and the Algebra) always count.
I think many of the preceding comments have been made by people who do, in fact, have an appreciation of the Maths but it is so familiar to them that they are hardly aware of it.
 
  • #18
The word "momentum" is not particularly illuminating. Newton (following Descartes, but not exactly) used the term "quantity of motion", which survives as a standard term for the concept in some languages.

As a "quantity of motion", the product of mass and velocity makes perfect sense. It is clear intuitively that greater velocity means "more motion". Greater (moving) mass equally conveys "more motion".
 
  • #19
voko said:
The word "momentum" is not particularly illuminating. Newton (following Descartes, but not exactly) used the term "quantity of motion", which survives as a standard term for the concept in some languages.

As a "quantity of motion", the product of mass and velocity makes perfect sense. It is clear intuitively that greater velocity means "more motion". Greater (moving) mass equally conveys "more motion".

Also, without using the formal definition, Momentum can easily be confused with Kinetic Energy. Both quantities give an indication of, for instance, the result (damage etc.) of a collision. Of course, it's very useful to have the Maths with a verbal accompaniment but what are we even considering doing without the Maths? Going back to what Galileo was doing with the quantity is a bit pointless, except for historical interest, and you can always go far enough back in history to find 'Science' that's acceptable to any level of appreciation. We have moved on.
 
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  • #20
A.T. said:
It's only significance is its conservation under certain conditions. That's the only reason why it is defined this way.
Momentum is conserved under all conditions that we know of. That is rather significant. The fact that momentum is a quantity that is always conserved in all physical interactions is one reason we are interested in it.

The simple fact that a certain force applied for a certain time interval results in the same change in this quantity for all matter is important too, at least in non-relativistic physics. That is just the consequence of Newton's second law.

AM
 
  • #21
sophiecentaur said:
Talk to someone with no idea of the Maths involved in Physics and you usually hear a pretty poor model of the World. Maths is so crucial to understanding at any but the very superficial level. Imagine trying to have a conversation about Finances without a common knowledge of the Arithmetic of Interest and Profit. The consequence of not using appropriate Maths is constantly being demonstrated by how people are regularly conned into bad deals. The numbers (and the Algebra) always count.
I think many of the preceding comments have been made by people who do, in fact, have an appreciation of the Maths but it is so familiar to them that they are hardly aware of it.
I would not disagree with what you have said, but physics is obviously more than math, just like economics is more than just finances. In physics and economics we need to have a conceptual model to help us understand what is happening in the real world, in addition to just understanding the math.

AM
 
  • #22
I would say that the math is the conceptual model. You need the math and you need the mapping between the math and experimental measurements, but you don't need a map between the math and any other non mathematical concepts.
 
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  • #23
All in all, physik are badly need of conserving quantity, in order to obtain little bit equation :)
 
  • #24
Andrew Mason said:
The fact that momentum is a quantity that is always conserved in all physical interactions is one reason we are interested in it.
It's the only reason.
 
  • #25
A.T. said:
It's the only reason.

Interesting. Do you accept that a non-conserved quantity can be of importance? E.g., position, velocity, acceleration?
 
  • #26
voko said:
Interesting. Do you accept that a non-conserved quantity can be of importance? E.g., position, velocity, acceleration?

No. I only care about my momentum. Look out, here I come! :eek: (I'm not sure where I am or what the time is, so I might miss you completely).
 
  • #27
Us as well. Try to compare definition in differ theories
Classic and Quantum
for instance.
 
  • #28
voko said:
Do you accept that a non-conserved quantity can be of importance?
Sure.
 
  • #29
A.T. said:
Sure.

I cannot reconcile this with the earlier statements of yours. You admit that a non-conserved quantity such as velocity can be of importance, yet the "only significance" you allocate to momentum "is its conservation under certain conditions".

Do I understand you correctly that a statement like "the magnitude of the vehicle's velocity is X" is infinitely more significant than "the magnitude of the vehicle's momentum is Y", because the latter statement does not deal with conservation of momentum?
 
  • #30
voko said:
...yet the "only significance" you allocate to momentum "is its conservation under certain conditions"...
What application would momentum have if it wasn't conserved?
 
  • #31
A.T. said:
What application would momentum have if it wasn't conserved?

My question can only be answered with "yes" and "no", not with some other answer, and certainly not with a question. Can you just answer my question? Thank you.
 
  • #32
voko said:
Do I understand you correctly that a statement like "the magnitude of the vehicle's velocity is X" is infinitely more significant than "the magnitude of the vehicle's momentum is Y", because the latter statement does not deal with conservation of momentum?
No, you did not understand me correctly.
 
  • #33
Then one of the following must be true:

(1) A statement like "the magnitude of the vehicle's velocity is X" is infinitely more significant than "the magnitude of the vehicle's momentum is Y" because Z is true for some Z, where Z is not related to conservation of momentum.

(2) A statement like "the magnitude of the vehicle's velocity is X" is infinitely more significant than "the magnitude of the vehicle's momentum is Y" because Z is false for any Z.

Which one of the above is true?
 
  • #34
If you want to claim that there is more significance to momentum than its conservation, then it's up to you to point out what it is. Not for others to answer your convoluted questions.
 
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  • #35
A.T. said:
If you want to claim that there is more significance to momentum than its conservation, then it's up you to point out what it is. Not for others to answer your convoluted questions.

Michalos, Alex (1969). Principles of Logic. Englewood Cliffs: Prentice-Hall. p. 370. "usually one who makes an assertion must assume the responsibility of defending it. If this responsibility or burden of proof is shifted to a critic, the fallacy of appealing to ignorance is committed."

(quoted from http://en.wikipedia.org/wiki/Philosophic_burden_of_proof)

Shall I remind that it was a certain A.T. who asserted the following:

It's only significance is its conservation under certain conditions. That's the only reason why it is defined this way.

The afore-mentioned A.T. is now on the verge of committing the fallacy of appealing to ignorance.
 
  • #36
voko said:
Shall I remind that it was a certain A.T. who asserted the following:
It's only significance is its conservation under certain conditions. That's the only reason why it is defined this way.
Yep, and that claim can only be proven wrong, by pointing out another significance of momentum. Let me know when you have found one.
 
  • #37
A.T. said:
Yep, and that claim can only be proven wrong, by pointing out another significance of momentum. Let me know when you have found one.

I hope you realize that I could do so trivially by defining the term "significance" any way I see fit, exploiting yet another fallacy in your reasoning?
 
  • #38
voko said:
...defining the term "significance" any way I see fit...
Yes, you can play some semantic games with yourself, if that pleases you. Have fun.
 
  • #39
Voko, as a third party, I also think that your question is very convoluted. I wouldn't answer it either.

I don't think that I would go so far as to say that momentum is only significant due to its conservation, but I cannot think of a counter example. For example, in a pendulum problem the momentum of the pendulum is not conserved, and momentum is not used to solve pendulum problems.
 
  • #40
DaleSpam said:
I cannot think of a counter example.
I just thought of a counter-example. Momentum is used to find wavelength per deBroglie. That is a significance of momentum which could be important regardless of conservation.
 
  • #41
Would you to give any conditions of conserving momentum, please?
 
  • #42
A.T. said:
Yes, you can play some semantic games with yourself, if that pleases you. Have fun.

The semantic player here is you. You made a categorical statement involving an undefined notion. Your statement is not falsifiable as such. When confronted with critique, your required your critics to prove your statement wrong via a counter-example, which is impossible because it is not falsifiable. Your statement is fallacious, and your attitude, now that your fallacies have been demonstrated, is questionable.

Voko, as a third party, I also think that your question is very convoluted.

I think I made them - at the very least I was genuinely trying - to make them simple yes/no questions. The reason is that the original statement felt wrong to me, but at that point I had not really formulated to myself why it felt wrong, so I tried to use those questions to understand what was really meant and why that felt wrong to me. But we have moved on since then. The true reason is, the statement is meaningless. "Significance" is subjective. It means something to some person, and something different to another. It is entirely possible that A.T.'s perception of his statement is fully tautological: momentum's significance is in its conservation, period; that requires no proof and cannot be proven wrong; but that is quite possibly not true to anyone else.
 
  • #43
DaleSpam said:
I just thought of a counter-example. Momentum is used to find wavelength per deBroglie. That is a significance of momentum which could be important regardless of conservation.
Yes, that would be a counter-example, unless the derivation of the deBroglie equations depends on momentun conservation itself. I wasn't thinking about quantum mechanics in the context of this sub-forum.
 
  • #44
voko said:
It is entirely possible that A.T.'s perception of his statement is fully tautological: momentum's significance is in its conservation, period; that requires no proof and cannot be proven wrong; but that is quite possibly not true to anyone else.
Well, in the Newtonian viewpoint, momentum is the quantity which is conserved in inertial frames; you could call this somewhat tautological, since inertial frames are the ones in which momentum is conserved.

Nevertheless, it's a pretty profound concept that, having been given a name, "the thing which is conserved" follows the Second Law.
 
  • #45
olivermsun said:
Nevertheless, it's a pretty profound concept that, having been given a name, "the thing which is conserved" follows the Second Law.

In non-inertial frames of references momentum is not conserved but still follows the Second Law. Fictitious forces just violate the Third Law.
 
  • #46
So what you're saying is, if you posit additional, fictitious forces you can even make a non-inertial frame conserve momentum? :wink:
 
  • #47
olivermsun said:
So what you're saying is, if you posit additional, fictitious forces you can even make a non-inertial frame conserve momentum?

No. If the frame of reference conserves momentum it would be no longer non-inertial.
 
  • #48
You say the second law is still obeyed in a non-inertial (e.g., rotating) frame, but this is only because the (apparently spontaneous) change in momentum is explained by introducing a fictitious force.

Without the fictitious force, which doesn't obey the third law (and therefore does not obey conservation of momentum), motion in the rotating frame actually does not obey the 1st and 2nd laws.

Also, it's called fictitious because it doesn't conserve "facts."

So now I'm getting confused: what is actually being conserved, and what is not here? :biggrin:
 
  • #49
olivermsun said:
You say the second law is still obeyed in a non-inertial (e.g., rotating) frame, but this is only because the (apparently spontaneous) change in momentum is explained by introducing a fictitious force.

Fictitious forces result from the second law in non-inertial frames - not vice versa. Nothing needs to be explained or introduced here.

olivermsun said:
So now I'm getting confused: what is actually being conserved, and what is not here?

As fictitious forces violate the third law (that's why they are called fictitious) they do not conserve momentum.
 
  • #50
DrStupid said:
Fictitious forces result from the second law in non-inertial frames - not vice versa. Nothing needs to be explained or introduced here.
Now you're turning circular. Forces (fictitious or otherwise) don't "result" from the second law in any frame AFAIK. What would be "vice versa"—the second law resulting from fictitious forces in non-inertial frames?

As fictitious forces violate the third law (that's why they are called fictitious) they do not conserve momentum.

I always thought they are called fictitious (or pseudo-) because they don't arise from any interaction of bodies, but only from the "interaction" of reference frames.

But anyway this is getting silly. You must have missed all the smileys I put in my previous posts.

Let's let them carry on with the original inane discussion. :smile:
 
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