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Wave momentum

  1. Dec 29, 2008 #1
    What is the momentum of a wave? I know that for a photon

    [tex]p=\frac{h}{\lambda}=\frac{hf}{c}=\frac {E}{c}[/tex]

    but what about a classical, mechanical wave? Is it also equal to the wave's energy divided by its speed, or is it more complicated than that?
  2. jcsd
  3. Dec 30, 2008 #2


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    For a classical EM wave, the h/lambda doesn't apply, but p=E/c still does.
  4. Dec 30, 2008 #3
    Yes, but what about mechanical waves, like sound waves or pulses on a string? There must be some formula for momentum in terms of density, elasticity, amplitude, etc.

    Vanadium 50, where are you?
    Last edited: Dec 30, 2008
  5. Dec 30, 2008 #4
    Vibration isn't really my area, so treat my comments with caution.

    Surely it's meaningless to talk about the momentum of a mechanical wave? You can talk about momentum for a photon because it is not actually a wave, but does display wave like properties (I'm sure something I just said there will upset 'real' physicists). Mechanical waves (flexural and longitudenal) are just vibrations - they are not 'things'. It's just a way to describe a type of movement. The waves themselves do not have a mass (a photon does... more gasps from physicists, I'm sure) so can't have momentum. If you look at the medium a mechanical wave is transmitted in, an element inside of it has a displacement (and the derivatives of displacement), a mass and forces acting on it, which vary with time (not the mass!). A single element therefore has time varying momentum. The whole structure does not.
  6. Dec 30, 2008 #5
  7. Dec 30, 2008 #6
    From that thread, I'd argue that it's not exactly the wave making the surfer go. The surfer is 'continuously falling' down a crest. That's gravity making the surfer move! It's just the geometry and movement of the wave that allows that to happen. Different parts of the wave making the surfer move have different amounts of potential and kinetic energy (and therefore momentum) at different times. Theres a continuous transfer between the two, but here we're not talking about the momentum of the wave, but the momentum of water particles, which increases and decreases.

    I don't even know how you would define a wave for the purpose of deriving momentum. I only consider it a type of motion.

    As I said, I'm no expert in this field. I'm sure Vanadium 50 can correct me.
  8. Dec 30, 2008 #7
    I was wrong. Here's an explanation and derivation for wave momentum:


    I don't think it disagrees so much with what I said, but it takes it a lot further and I learnt some new stuff too.

    The reference defines a momentum density, which corresponds to what I said about each individual 'elements' inside the medium having their own momentum. It takes it further by defining the momentum carried by a wave as been the integral of momentum density with respect to distance along the wave and time. It also shows the relationship between momentum density and energy flow. That energy carried by a wave is more obvious to see I think.

    I think it comes down to definitions. To say that a wave motion causes the medium it is in to carry momentum is obvious I think (see my first post). To then say that the wave has momentum is a bit more confusing, since I considered the wave to be the motion only.

    Enjoy the link :p
  9. Dec 30, 2008 #8

    Vanadium 50

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    By starting a new thread, you threw me off the scent.

    Clem is right: p = E/c is valid for mechanical waves. Note that c is the wave's velocity, not necessarily the speed of light.
  10. Dec 30, 2008 #9
    Really? I understood that wave momentum was a much more contentious and complicated issue than that. (An example paper is J.Fluid Mech. v106 p331 1981.)
  11. Dec 30, 2008 #10

    Vanadium 50

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    There is a complication with transverse waves, as one can show that setting up a transverse wave also sets up a longitudinal wave, and this carries the energy and momentum. One can make the situation more complicated still by introducing an non-uniform elasticity tensor. But the fact that there are ways of making things more complicated is not, in my mind, an excuse to toss out a model that is explanatory. (Just like I wouldn't stop people from understanding Newton's law of universal gravitation because it's not GR)

    It's an experimental fact (although it was disputed earlier) that one can lose energy and/or momentum to a mechanical wave, and one can gain energy and momentum from mechanical waves. Momentum and energy are conserved if one ascribes to the wave itself the energy and momentum being transferred. Some people say "it's not 'really' in the wave; it's in the medium that's oscillating", which is in my mind a quibble that replaces a useful simple concept with one that's so complicated as to be useless. It would be like saying, "there's not really any such thing as an electric current; it's all just the motion of individual electrons".

    For those who still don't believe that waves carry momentum, take a metal rod, and clamp it down at both ends and as many points in the middle as you'd like to insure it doesn't move. Place an object that's free to move at one end, touching the rod, and strike the other end of the rod with a hammer. The object takes off. Where did its momentum come from? And when the hammer stopped, where did its momentum go? Remember, the rod is stationary.
  12. Dec 31, 2008 #11
    Ah, Google Books! That saves me a trip to Durham, at least for Elmore and Heald. Thanks Chris. And thank you Vanadium 50 for returning to this topic :smile:.

    The relationship I was looking for is expressed in equation 1.11.12:

    (energy flux) = (speed)2 x (momentum density)

    which can be rearranged to make (momentum)=(energy)/(speed), just like Vanadium 50 said and just like with electromagnetic waves.

    I can't say I understand the derivation yet - it's pretty long and so far I've barely looked at it - but the text says that this relationship applies to all plane mechanical waves 'traveling in linear isotropic media', so perhaps it is the clue to the puzzle I posed in the 'a clue for de Broglie?' thread. I am also beginning to wonder if the two conditions behind the wave reflection/transmission equations (continuity and differentiabilty of waves at a boundary) do in fact imply conservation of momentum and kinetic energy, just in a subtle way. Hmm...(scratches head)
  13. Dec 31, 2008 #12
    I like this... You've convinced me with it. The concept of wave-momentum was a bit alien to me - I've only ever looked at forces at various support types due to waves, and for this you don't need to consider momentum.

    I hadn't realised this was the case, but now you say it, I can see that it would be true.
  14. Dec 31, 2008 #13
    Newton's cradle seems like a good example, too. Of course, these are both cases involving longitudinal waves. That a transverse wave of the same energy and speed carries just as much momentum is less obvious to me.
  15. Dec 31, 2008 #14
    A wave in a classical material (eg: water or air) has no overall momentum, but it does have instantaneous momentum. At any moment in time, there is momentum; at the onset of the wave a crest may be developing with a positive momentum. Later, as the wave passes, the momentum would reverse and portray a negative value. The summation of momentum over time is zero.

    A sound wave conveys compression of the air, followed by rarefraction. A water wave has a crest followed by a trough. As the crest is developing, the water molecules are actually moving foreward; later they retreat into the trailing trough. A sample molecule transcribes a circular motion as the wave passes by. (I am ignoring a different phenomenon of braking waves.)
  16. Dec 31, 2008 #15

    Vanadium 50

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    Would you like to explain why if a wave carries no "overall momentum" the rod-and-hammer apparatus performs as described?
  17. Jan 1, 2009 #16

    Re the rod-and-hammer, let's consider a segment within an elastic material rod.

    - That segment initially has zero momentum.
    - As the wave approaches the segment, the elastic structure compresses. A positive momentum can be calculated.
    - Later as the wave recedes, that same structure extends (rebounds). A negative momentum is calculated.
    - Summed over time, the segment has zero momentum.

    Quite simply, the rod does not translate (move) overall. With zero overall velocity, there is zero overall momentum within the rod. But what of the momentum introduced by the hammer? Well, it is carried off by the object on the opposite end of the rod (here I am considering, for example, the opposite end of the rod placed against a concrete wall that is being chipped away by the hammer and chisel mechanism).

    In contrast, if the rod were made of plastic (deformable) material, then *some energy would be lost to* the rod itself. Where steel is used in the rod, and stressed beyond its yield stress, then an elasto-plastic behaviour becomes manifested. Some of the energy is absorbed by the plastic deformation of the steel, while the remainder is imparted by the opposing medium (concrete wall in my example).
    Last edited: Jan 1, 2009
  18. Jan 1, 2009 #17
    Doesn't this imply that momentum was transported from one end of the rod to the other? In other words, that the compression wave carried the momentum along with it?
  19. Jan 1, 2009 #18


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    Here's a simpler derivation for one dimensional transverse waves on a string based on Lagrangian mechanics. Let [tex] \phi(x) [/tex] be the displacement of the string at x. The kinetic energy of the string (in appropriate units) is [itex] \int (1/2)(\partial{\phi}/\partial{t})^2 [/itex], and the potential energy of the string is [itex] \int (c^2/2)(\partial{\phi}/\partial{x})^2 [/itex]. For a right moving wave of the form [itex] \phi(x) = F(x - ct) [/itex], the energy is T + U = [itex] E = \int c^2 (dF/dx)^2 dx [/itex]. The linear momentum of the wave is the Noether charge of space translation symmetry (you can check that the Lagrangian T-U is invariant under space translations). An infinitesimal space translation has the form [itex] \phi(x) \longrightarrow \phi(x) - (\partial{\phi}/\partial{x}) \epsilon [/itex]. The charge of this symmetry is

    [tex] -\int \Pi_{\phi}(x) \phi(x) dx = -\int (\partial{\phi}/\partial{t})(\partial{\phi}/\partial{x}) dx = \int c(dF/dx)^2 dx[/tex]

    which is just E/c, so E = cP.
    Last edited: Jan 1, 2009
  20. Jan 1, 2009 #19

    Vanadium 50

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    Of course the rod doesn't move - by construction. But how does the momentum get from one end of the rod to the other if it is not carried by a wave?
  21. Jan 1, 2009 #20
    dx, I think you have just given us the golden key.

    I have three questions:

    1. what is [tex] \Pi_{ \phi }(x)[/tex]?
    2. this proof seems to imply that longitudinal displacement is not even necessary for wave momentum - is this correct?
    3. do you have any thoughts about this:



    Thank you very much, by the way.
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