Traveling plane wave

From testwiki
Jump to navigation Jump to search

Template:Short description

The wavefronts of a traveling plane wave in three-dimensional space.

In mathematics and physics, a traveling plane wave[1] is a special case of plane wave, namely a field whose evolution in time can be described as simple translation of its values at a constant wave speed c, along a fixed direction of propagation n→.

Such a field can be written as

F(x→,t)=G(x→⋅n→−ct)

where G(u) is a function of a single real parameter u=d−ct. The function G describes the profile of the wave, namely the value of the field at time t=0, for each displacement d=x→⋅n→. For each displacement d, the moving plane perpendicular to n→ at distance d+ct from the origin is called a wavefront. This plane too travels along the direction of propagation n→ with velocity c; and the value of the field is then the same, and constant in time, at every one of its points.

The wave F may be a scalar or vector field; its values are the values of G.

A sinusoidal plane wave is a special case, when G(u) is a sinusoidal function of u.

Properties

A traveling plane wave can be studied by ignoring the dimensions of space perpendicular to the vector n→; that is, by considering the wave F(zn→,t)=G(z−ct) on a one-dimensional medium, with a single position coordinate z.

For a scalar traveling plane wave in two or three dimensions, the gradient of the field is always collinear with the direction n→; specifically, ∇F(x→,t)=n→G′(x→⋅n→−ct), where G′ is the derivative of G. Moreover, a traveling plane wave F of any shape satisfies the partial differential equation

∇F=−n→c∂F∂t

Plane traveling waves are also special solutions of the wave equation in an homogeneous medium.

See also

References

Template:Reflist

Template:Math-physics-stub