Plane-Wave Summary

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Plane-Wave Summary A two-dimensional plane wave may be expressed as − f(x; y; t) = Re A ei(kx+ly νt) = Re A eiθ (1) • x; y and t are independent variables (space and time). • k and l are the x and y wavenumbers (units: m−1). • A is the wave amplitude. • θ = kx + ly − νt is the wave phase angle. • The wave propagates normal to lines of constant phase angle. At any instant in time [t fixed; (x; y) varies]: Plot of θ as a function of (x,y) for fixed t. Plot of Re{exp(i θ)} as a function of (x,y) for fixed t. y y θ = 3π ∆ θ -1 θ = 2π 1 L θ = π θ = constant -1 HH θ = 0 1 L λ wave propagation X HH x x • θ = kx + ly + C; θ is a linear function of space. • θ is constant on lines of kx + ly. • eiθ = ei(θ + 2πn), where n is an integer, are lines of constant phase (e.g. highs and lows). • K~ = rθ = îk + ^jl is the wave vector; K = jK~ j is the wavenumber. 2π • λ = K is the wavelength: the distance between lines of constant phase. At any fixed point in space [(x; y) fixed; t varies]: Plot of q as a function of t for fixed (x,y). Plot of Re{exp(i q)} as a function of t for fixed (x,y). q -n q period t t • θ = C − νt; θ is a linear function of time. @θ • ν = − , is called the frequency: the rate that lines of constant phase pass a fixed point @t in space (units: s−1). Note that the figure above indicates ν < 0. This means that for fixed (x; y), such as the point marked \X" on the first figure, θ increases with time; this can only occur if phase lines move toward smaller x and y. 2π • The wave period is : length of time between points of constant phase (units: s). ν • The phase speed is the propagation speed of constant phase lines in the direction of K~ , ν 1 @θ c = = − (units: m s−1). K jrθj @t Special note on θ: iθ i(θr+iθi) iθr −θi ∗ iθr If θ has an imaginary part, θ = θr + iθi, then e = e = e e ≡ A e . θr is the wave phase angle as interpreted above, and A∗ = Ae−θi is a modified amplitude that depends on time and/or space. For example, if the frequency, ν, contributes the imaginary part, then the wave has time-dependent amplitude that grows or decays with time. Such waves are called unstable, to distinguish them from the neutral waves (A constant) that we discussed above..

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