Springs & pendulums
- Mass on a spring
- T = 2π·√(m/k)
- Pendulum
- T = 2π·√(L/g)
- Angular frequency
- ω = √(k/m) = 2π/T
- Maximum speed and acceleration
- vmax = A·ω, amax = A·ω²
- Energy
- E = ½·k·A²
Waves and Optics: cram pack
Formula sheets, the key method steps for every topic and 4 practice problems, with full solutions at the back.
1Formulas and methods
Waves, sound & optics
- Wave speed
- v = fλ, T = 1/f
- String
- v = √(T/μ), μ = m/L
- Sound level
- β = 10·log10(I/I0), I0 = 10⁻¹² W/m²
- Point source
- I = P/(4πr²)
- Standing waves
- string or open pipe fn = n·v/(2L); closed pipe fn = n·v/(4L), n odd
- Doppler effect
- f′ = f·(v ± vo)/(v ∓ vs)
- Refractive index
- n = c/v, λ = λ0/n
- Snell’s law
- n1sin θ1 = n2sin θ2
- Critical angle
- sin θc = n2/n1
- Optical fibre
- NA = sin θa = √(n1² − n2²)
- Lenses and mirrors
- 1/f = 1/do + 1/di, m = −di/do, mirror f = R/2
- Double slit
- d·sin θ = mλ, ym = mλL/d
- Grating
- d = 1/N, d·sin θ = mλ, mmax ≤ d/λ
- Single slit
- a·sin θ = mλ (dark), w = 2λL/a
Method
- Identify the kind of problem: wave speed, sound level, standing wave, Doppler, refraction, lens or mirror, or interference.
- Write the relation first: v = fλ, β = 10·log(I/I₀), fₙ = n·v/(2L) or n·v/(4L), f′ = f(v ± vo)/(v ∓ vs), n₁sin θ₁ = n₂sin θ₂, 1/f = 1/d₀ + 1/dᵢ, d·sin θ = mλ.
- Convert units: nm, mm and cm to m, and check whether angles are measured from the normal.
- Check signs and plausibility: a virtual image has dᵢ < 0, an approaching source sounds higher, a closed pipe has only odd harmonics.
2Practice problems
1.Springs & pendulumsMedium
A 0.4 kg mass on a spring with k = 230 N/m is pulled 9 cm in the positive direction and released from rest at t = 0. Find its velocity v at t = 1.35 s (with sign).
m = 0.4 kgk = 230 N/mA = 9 cmt = 1.35 s
v = m/s
2.Springs & pendulumsHard
A 4 kg mass on a spring with k = 80 N/m is pulled 7 cm from equilibrium and released. Find the total energy E of the oscillation.
m = 4 kgk = 80 N/mA = 7 cm
E = J
3.Waves, sound & opticsMedium
An observer moves at 10 m/s away from a stationary source of 1000 Hz. The speed of sound is 343 m/s. Find the frequency f′ that the observer hears.
f = 1000 Hzv = 343 m/svo = 10 m/s
f′ = Hz
4.Waves, sound & opticsHard
Light of wavelength 600 nm falls at right angles on a grating with 600 lines per millimetre. Find the angle θ1 of the order-1 maximum.
N = 600 mm⁻¹λ = 600 nmm = 1
θ1 = °
3Solutions
1.Springs & pendulums
Answer: v = −1.763 m/s
Simple harmonic motion: a mass m on a spring of stiffness k oscillates with angular frequency ω = √(k/m) and period T = 2π/ω = 2π·√(m/k). A simple pendulum of length L has T = 2π·√(L/g). With amplitude A, the largest speed is A·ω, the largest acceleration A·ω² and the energy ½·k·A².
Angular frequency
ω = √(230/0.4) = 23.98 rad/s
ω·t = 23.98·1.35 = 32.37 rad
Velocity
v = −A·ω·sin(ω·t) = −0.09·23.98·sin(32.37) = −1.763 m/s
Answer
v = −1.763 m/s
2.Springs & pendulums
Answer: E = 0.196 J
Simple harmonic motion: a mass m on a spring of stiffness k oscillates with angular frequency ω = √(k/m) and period T = 2π/ω = 2π·√(m/k). A simple pendulum of length L has T = 2π·√(L/g). With amplitude A, the largest speed is A·ω, the largest acceleration A·ω² and the energy ½·k·A².
Angular frequency
ω = √(80/4) = 4.472 rad/s
Energy
E = ½·k·A² = ½·80·0.07² = 0.196 J
Answer
E = 0.196 J
3.Waves, sound & optics
Answer: f′ = 970.8 Hz
Standing waves and the Doppler effect: a string fixed at both ends, or a pipe open at both ends, fits whole half-wavelengths: L = nλ/2, fn = n·v/(2L), n = 1, 2, 3, … A pipe closed at one end has a node at the closed end and an antinode at the open end: L = nλ/4 with odd n only, fn = n·v/(4L). When source or observer move along the line between them, f′ = f·(v ± vo)/(v ∓ vs): use the upper signs for motion towards each other. Two waves of nearly equal frequency beat at |f₁ − f₂|.
Doppler formula
f′ = f·(v − vo)/(v + vs) = 1000·(343 − 10)/(343 + 0)
f′ = 970.8 Hz
Answer
f′ = 970.8 Hz
4.Waves, sound & optics
Answer: θ1 = 21.1 °
Interference and diffraction: light from two slits a distance d apart reaches a point on the screen with a path difference d·sin θ. Bright fringes appear where d·sin θ = mλ (m = 0, ±1, ±2, …). For a screen at distance L ≫ d, the m-th bright fringe is at y = mλL/d and the fringe spacing is Δy = λL/d. A grating with N lines per millimetre has d = 1/N and sharp maxima at d·sin θ = mλ; since sin θ ≤ 1, the highest order is the largest whole number m ≤ d/λ. A single slit of width a has dark fringes at a·sin θ = mλ, m = ±1, ±2, …
Line spacing
d = 1/600 mm = 1.667 × 10⁻⁶ m
Grating equation
sin θ = mλ/d = 1·600 × 10⁻⁹/(1.667 × 10⁻⁶) = 0.36
θ = 21.1°
Answer
θ1 = 21.1°
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