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Density
ρ = m/v
Pressure
P = F/A
Pressure at a depth in a fluid
P = P0 + ρgh
Pascal’s Law
P = F1/A1 = F2/A2
Force at a depth
F = ½ ρgwh2
Continuity equation of a fluid
A1v1 = A2v2
Volume flow rate
dV/dt = (Δx A)/Δt = Av
Incompressible fluid
m1=m2
P1 + ρgy1 + ½ ρv12 = P2 + ρgy2 + ½ ρv22
Frequency
f = N(1/t)
Angular frequency or oscillation
ω = 2πf = sqrt(k/m) = sqrt(mgd/i)
Period of motion
T = 2π/ω
Acceleration and angular frequency
a = -ωx
Spring constant
k = mg/x
Energy
E = ½ mv² + ½ kx² = ½ kA²
Oscillations - position
x(t) = Acos(ωt + φ)
Oscillations - velocity
v(t) = -Aωsin(ωt+φ)
Oscillations - acceleration
a(t) = -Aω²cos(ωt+φ)
Torsion constant
T = 2πsqrt(i/κ) = iω²
Speed of propagation (velocity for wave/oscillation problems)
v = λ/T = λf = ω/k
Traveling sinusoidal wave
y(x,t) = Asin(k(x-vt)) = Asin(kx-ωt)
What direction is wave motion in if the sin wave is (kx + ωt)?
-x direction
What direction is wave motion in if the sin wave is (kx - ωt)?
+x direction
Wave number
k = 2π/λ
Period
T = 2π/ω
Wave functions that move in -x direction
y(x,t) = Asin(-kx - ωt)
y(x,t) = Asin(kx + ωt)
y(x,t) = Acos(kx + ωt)
Wave speed on a rope
v2 = T/κ = β/ρ = S/ρ = Y/ρ
(bulk modulus, shear modulus, young’s modulus)
Different speeds for waves/oscillations
Wave propagates at v = ω/k = λf = λ/T = sqrt(T/μ)
Medium oscillates at vy = ωAsin(kx - ωt)
Energy of a small section of sinusoidally vibrating string section
(harmonic oscillator)
dE = ½ (dm)vy2 + ½ (dm) ω²y²
Power for a sinusoidally vibrating string
P = ½ μvω²A²
Intensity and distance
I1r12 = I2r22
Intensity and power
I = P/(4πr²)
Incident wave
y1(x,t) = Acos(kx - ωt)
Reflected wave
y2(x,t) = Bcos(kx + ωt)
Is a reflected wave on a fixed end inverted or the same?
The reflected wave for a fixed end is inverted
Is the reflected wave on a free end inverted or the same?
The reflected wave for a free end is the same