How to determine the direction of propgation of a plane wave?

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Discussion Overview

The discussion revolves around determining the direction of propagation of a plane wave represented by the equation u=exp(-i k x). Participants explore various aspects of wave propagation, including mathematical representations, physical interpretations, and the role of time dependence in wave behavior.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • Some participants suggest that the wavevector k indicates the direction of the wave, with the positive sign corresponding to movement to the right and the negative sign to the left.
  • Others argue that the Poynting vector, calculated as P = E x H, provides a clearer indication of the direction of power flow for electromagnetic waves.
  • A participant emphasizes the necessity of including time dependence in the wave equation to accurately determine the direction of propagation.
  • Another participant points out that a wave described solely by spatial dependence does not imply movement, and that a moving wave requires a specific time-dependent form.
  • Some contributions highlight that in quantum mechanics, the direction associated with the wavevector is more of a convention in time-independent cases.
  • There is a discussion about the implications of superposition of waves with different directions and how the Poynting vector can clarify the overall direction of propagation in such cases.

Areas of Agreement / Disagreement

Participants express differing views on how to determine the direction of wave propagation, with no consensus reached on the best approach. Some focus on the wavevector, while others emphasize the importance of time dependence and the Poynting vector.

Contextual Notes

Limitations include the absence of time dependence in some contributions, which may affect the interpretation of the wave's behavior. Additionally, the discussion does not resolve the complexities introduced by superposition of waves with varying characteristics.

Rex_chaos
hi all,
Suppose there is a plane wave u=exp(-i k x), where k is a wavenumber. How to determine it's moving direction?
 
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In general, you can find the direction of the power flow of an EM wave by calculating the Poynting vector:

P = E x H.

Anyway, for this case (the case of a TEM plane wave), the electric field may be expressed as:

E(R) = E0 exp(-ik dot R).

The corresponding magnetic field may be expressed as:

H(R) = (1/eta) an x E(R).

Here, eta is the intrinsic impedance of the medium.

I will assume that your wave is linearly polarized which makes

E0= ay E0 cos(2[pi]f t)

and

H0 = az (E0 / eta) cos(2[pi]f t).

You should be able to prove to yourself that the power flow is in the +x direction.

eNtRopY
 
Last edited by a moderator:
Perhaps i missed something during my physics classes but the k in this equation is the wavevector which gives you the direction. In general the solution to a 1D wave equation will be of the form:

Aexp(ikx)+Bexp(-ikx)

Where the plus is for moving to the right en the minus for moving to the left. In higher dimensions the k is a vector pointing in the direction of travel...
 
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Aexp(ikx)+Bexp(-ikx)

Where the plus is for moving to the right en the minus for moving to the left...

Yes, I know the result. However, how to prove that +k corresponding to a wave moving to the right?
 
This wave does not move...
It has a definite value at each point in space which is fixed in time.
Only if you have :

Aexp(i(kx-wt)) + Bexp(-i(kx+wt))

you can have a moving wave. Note the difference of the sign in front of w.
To show in which direction it moves it suffices to study the argument being zero:

kx-wt=0 --> x=ct moving to +x
kx+wt=0--> x=-ct moving to -x

where c=w/k the velocity of the wave.
 
To determine in which direction the wave propagates you need to specity the time dependence as well as the space dependance. You've only given the spatial dependence of the phasor. There are two choices of a time dependence corresponding to two choices of the sign of "wt".

Pete
 
If you're talking QM in the time-independent case, then it's just convention that the + waves goes right and the - goes left. It's actually erroneous to say they're going anywhere; "time-independent" scattering is a sort of vague approximation they teach you in beginning classes -- but of course they never explain why it works. :)
 
Originally posted by heumpje
Perhaps i missed something during my physics classes but the k...

It is true that in the trivial case which has the form E ~ exp(-kx) the wavevector gives the direction of the traveling wave. However, examine a case with superpositioned wave patterns having unequal direction, orientation and magnitude. You will see that calculating the Poynting vector gives the most straight-forward method for determining the direction of an EM wave.

eNtRopY
 
Last edited by a moderator:
Originally posted by pmb
To determine in which direction the wave propagates you need to specity the time dependence as well as the space dependance. You've only given the spatial dependence of the phasor. There are two choices of a time dependence corresponding to two choices of the sign of "wt".

Pete

It is common practice to absorb the time dependence in the magnitude coefficient as I shown above. I assume Rex_chaos meant:

u [pro] exp(-i k x)

rather than

u = exp(-i k x).

Otherwise, his problem is too trivial.

eNtRopY
 
  • #10
re - "It is common practice to absorb the time dependence in the magnitude coefficient as I shown above. I assume Rex_chaos meant:"

Sometimes that's true. But to determine the direction you have to know what it was that was absorbed.

Pete
 

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