Waves in 2D Flashcards
What heppends in the simplest case when adding two components
y1 + y2 = 2A [cos {(w1-w2)/2 t - (k1-k2)/2 x}][cos {(w1+w2)/2 t - (k1+k2)/2 x}]
Waves in 2D restoring force
T𝛿y𝛿x ∂^2z/∂x^2 + T𝛿y𝛿x ∂^2z/∂y^2
=> T𝛿y𝛿x ∂^2z/∂x^2+ T𝛿y𝛿x ∂^2z/∂y^2 = ρ𝛿x𝛿y ∂^2z/∂t^2
For an infinite membrane
z = Aexp{i(ωt - k͟·r)}
For a finite membrane
z = Aexp{i(ωt - (kₓx + kᵧy)} + Bexp{i(ωt - (kₓx - kᵧy)}
z = 2Asin{ωt - kₓx}sin{nπy/b}
cut off frequency
fmin = ωmin/2π
where ωmin = πc/b
group velocity
vg = c √(1 - ωmin^2/ω^2)
time taken
t = x/vg
c =
√Y/ρ
fmax =
1/π √K/m
K =
YA/a
and for one atom per lattice point
K = a^2 Y/a
A 2D membrane diagram
see notes
How an equation for waves transmitted on the membrane can be determined.
1) boundary conditions
2) initial membrane conditions
boundary conditions will determine whether we need sin or cos functions for each dimension, including time
cut - off frequency
k^2 = kx^2 + ky^2
for a wave to propogate kx must be real
k = w/c and ky = pi/b
therefore wmin = pi c /b
2D Membrane stretched between two parallel supports diagram
for a finite membrane diagram