SHM Flashcards
SHM of a spring equation
mẍ = -kx
(force = spring force)
general SHM equation and solution
equation:
ẍ = -ω²x
solution:
x(t) = A*cos(ωt + ϕ)
ϕ: phase angle
equation for the total energy of an oscillating spring
E= ½kA²
E: total energy
k: spring constant
A: amplitude
equation for damped harmonic motion of a spring
mẍ + bẋ + kx= 0
k: spring constant
b: friction factor
general damped harmonic motion equation
mẍ + γẋ + ω₀²x= 0
γ: the damping factor (Gamma symbol)
γ = b/m
ω₀ = (k/m)^½
general displacement equations for the 3 types of damped oscillation
light: (ω₀ > γ/2)
x(t) = A* e^(-γ/2 * t) * cos(ωt +ϕ)
heavy: (ω₀ < γ/2)
x(t)= e^(-γ/2 * t) * [ Ae^(αt) + Be^(-αt) ]
α² = γ²/4 - ω₀²
critical: (ω₀ = γ/2)
x(t) = e^(-γ/2 * t) * (A+Bt)
A and B are unknowns based on the initial conditions
quality factor equation
Q = ω₀/γ
energy equation for very light damping
E = E₀ * e^(-γt)
general equation for forced damped motion
mẍ + bẋ + kx= F₀*cos(ωt)
F₀*cos(ωt) is the driving force
displacement equation for a forced oscillation
x = A*cos(ωt - δ)
ω: the driving frequency
where:
tan(δ) = γω/ (ω₀²-ω²)
A = F₀ / m[ (ω₀²-ω²)² + ω²γ² ]^½
how does resonance work for a damped and undamped forced oscillator
undamped:
as ω –> ω₀, A –> ∞
damped:
resonance at ω = ω₀
δ = π/2 at resonance
δ transitions between 0 and π as ω increases
equation of oscillation for an RLC circuit
Lq(..) + Rq(.) + 1/C q = V₀ * e^(iωt)
L: inductance
R: resistance
C: capacitance
q: charge
this gives
I = I₀ * e^(iωt)
I: current