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

Click For Summary
SUMMARY

The direction of propagation of a plane wave, represented as u=exp(-i k x), can be determined using the wavevector k, which indicates the direction of travel. The Poynting vector, calculated as P = E x H, provides a straightforward method for identifying the power flow direction of electromagnetic (EM) waves. For a linearly polarized TEM plane wave, the electric field E(R) and magnetic field H(R) can be expressed in terms of their respective amplitudes and the intrinsic impedance of the medium. The analysis confirms that a positive k corresponds to a wave moving in the +x direction, while the time dependence of the wave is crucial for understanding its propagation.

PREREQUISITES
  • Understanding of plane wave equations and wavevectors
  • Familiarity with electromagnetic theory, specifically the Poynting vector
  • Knowledge of time-dependent wave functions in physics
  • Basic concepts of linear polarization in electromagnetic waves
NEXT STEPS
  • Study the derivation and implications of the Poynting vector in electromagnetic theory
  • Learn about the relationship between wavevector k and wave propagation direction in various media
  • Explore time-dependent wave functions and their significance in wave mechanics
  • Investigate the effects of superposition in wave patterns and their directional properties
USEFUL FOR

Physics students, electrical engineers, and researchers in electromagnetic theory who seek to deepen their understanding of wave propagation and the mathematical tools used to analyze it.

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?
 
Physics news on Phys.org
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...
 
Last edited:
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
 

Similar threads

  • · Replies 17 ·
Replies
17
Views
2K
  • · Replies 3 ·
Replies
3
Views
5K
  • · Replies 11 ·
Replies
11
Views
4K
  • · Replies 7 ·
Replies
7
Views
3K
  • · Replies 21 ·
Replies
21
Views
2K
  • · Replies 5 ·
Replies
5
Views
3K
Replies
8
Views
1K
Replies
2
Views
2K
  • · Replies 6 ·
Replies
6
Views
1K
  • · Replies 11 ·
Replies
11
Views
2K