Impedance Matching Flashcards
Power in terms of Impedance
Pi = 1/2 Z₁A²ω²
Pr = 1/2Z₁A²ω²
Pt = 1/2Z₂A²ω²
When there is no mass at the boundary
B/A =
C/A =
B/A = (Z₁ - Z₂)/(Z₁ + Z₂)
C/A = 2Z₁/(Z₁ + Z₂)
All energy arriving at the boundary with the incident wave leaves with
the reflected and transmitted wave. Because energy is conserved
When there is no mass at the boundary
energy is conserved
The simple joined string shows
no reflection if Z2 = Z1
A sinusoidal wave incident on a fixed or free end gives
rise to a reflected wave, and that when the incident and reflected waves interact, we get standing waves
λn =
2π/kn = 2π/nπ/L
= 2L/n
fn =
c/λn
= n * c/2L
Each normal mode satisfies the
boundary condition of the string being fixed at each end
The n=1 mode is called the
fundamental mode or the 1st harmonic
When do you get perfect nodes
if incident and reflected waves have identical amplitudes, this happens only if the incident and reflected wave energies are the same. In which case no energy is lost at the boundaries and so the total net energy flux is 0.
plucked strings are
pulled aside and released with zero velocity
consider two different strings joined at x = 0 their yi , yr and yt can be defined as
yi = Aoe^(i{wt-k1x})
yr = Aoe^(i{wt+k1x})
yt = A2e^(i{wt-k2x})
To solve two different strings joined at x = 0 with a mass M
1) yi+yr = yt
2) Apply boundary conditions for
a) yi+yr = yt x = 0
2) Consider the forces acting on the mass M at x = 0
T d(yi+yr)/dx - Td(yt)/dx = M d^2(yt)/dx^2
3) substitute progressive transverse wave into 2)
simplify and solve
for a progressive transverse wave y(x,t) =
y(x ± ct)
dy/dt = ± c dy/dx
dy/dx = 1/c dy/dt