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MHT-CET Physics · Superposition of Waves

Progressive Waves: the Wave Equation, Phase and Particle Velocity

A progressive wave y = A sin(ωt − kx) carries a disturbance at v = ω/k = fλ; two points Δx apart differ in phase by 2πΔx/λ, and each particle oscillates with a top speed Aω that is quite separate from the wave's speed.

Why this matters

34 PYQs, three HARD. Three shapes: reading ω, k, λ, v and the direction off a wave equation (and the speed on a string, √(T/μ)), converting between phase and path difference, and comparing the particles' maximum velocity with the wave velocity.

Concept 1 of 3: Reading the Wave Equation

Everything is in the two coefficients: the number multiplying t is ω, the one multiplying x is k. Their ratio is the speed, and the relative sign of the t and x terms gives the direction — opposite signs, the wave moves toward +x; same signs, toward −x.

Definition

  • y=Asin⁡(ωt−kx+ϕ)y = A\sin(\omega t - kx + \phi): f=ω2πf = \dfrac{\omega}{2\pi}, λ=2πk\lambda = \dfrac{2\pi}{k}, v=ωk=fλv = \dfrac{\omega}{k} = f\lambda. Opposite signs: along +x+x; same signs: along −x-x.
  • y=Asin⁡2π(tT−xλ)y = A\sin 2\pi\left(\dfrac{t}{T} - \dfrac{x}{\lambda}\right) reads off TT and λ\lambda directly.
  • Frequency is fixed by the source; entering a new medium changes vv and λ\lambda together.
  • String: v=Tμv = \sqrt{\dfrac{T}{\mu}}. Hanging rope with a load: tension, and so λ\lambda, grows toward the top.
  • Sound: v∝Tabsv \propto \sqrt{T_{\text{abs}}}. Reflection at a rigid wall: phase reverses (180∘180^\circ), speed unchanged.

Progressive wave

y=Asin⁡(ωt−kx),v=ωk=fλy = A\sin(\omega t - kx), \qquad v = \frac{\omega}{k} = f\lambda

Worked example

y=0.05sin⁡(200πt−4πx)y = 0.05\sin(200\pi t - 4\pi x) (SI). Frequency, wavelength, speed and direction?
Practice this conceptself-check · 3 quick reps

The same idea in a real exam question:

MHT-CET · 2024 · 10th May Shift 2 · Q49Easy

Example 1 · Superposition of Waves · Progressive Wave, Wave Equation, and Velocity

The equation of wave is Y=6sin⁡ ⁣(12πt−0.02πx+π3)Y=6\sin\!\left(12\pi t-0.02\pi x+\frac{\pi}{3}\right) where 'xx' is in m and 'tt' in s. The velocity of the wave is

Leaving π in the wave number

In 12πt−0.02πx12\pi t - 0.02\pi x, k=0.02πk = 0.02\pi, so v=600v = 600 m/s. Reading k=0.02k = 0.02 gives 600π600\pi — watch whether the π\pi is attached to x.

Concept 2 of 3: Phase Difference and Path Difference

One wavelength of distance is one full cycle of phase, 2π. So any separation along the wave converts to phase by the fraction of a wavelength it covers — 60° is a sixth of a wavelength.

Definition

  • Δϕ=2πλΔx\Delta\phi = \dfrac{2\pi}{\lambda}\Delta x, Δx=λ2πΔϕ\Delta x = \dfrac{\lambda}{2\pi}\Delta\phi.
  • Points 60∘60^\circ apart: λ6\dfrac{\lambda}{6}; 90∘90^\circ: λ4\dfrac{\lambda}{4}.
  • Two waves at a point (x,t)(x, t): phase difference = difference of their full phases, e.g. (25x−40t)−(20x−30t)(25x - 40t) - (20x - 30t).
  • acos⁡(θ)a\cos(\theta) leads asin⁡(θ)a\sin(\theta) by π2\dfrac{\pi}{2}, so a sine and a cosine wave with an extra ϕ\phi differ by ϕ+π2\phi + \dfrac{\pi}{2}.
  • Points in the same state of vibration are a whole number of wavelengths apart.

Phase and path

Δϕ=2πλ Δx\Delta\phi = \frac{2\pi}{\lambda}\,\Delta x

Worked example

Sound of 680 Hz in air at 340 m/s. How far apart are two points 60∘60^\circ out of phase?
Practice this conceptself-check · 2 quick reps

The same idea in a real exam question:

MHT-CET · 2023 · 4th May Shift 2 · Q19Easy

Example 2 · Superposition of Waves · Progressive Wave, Wave Equation, and Velocity

A transverse wave travelling along a stretched string has a speed of 30 m/s and a frequency of 250 Hz. The phase difference between two points on the string 10 cm apart at the same instant is

Mixing degrees and radians

Δx=λ2πΔϕ\Delta x = \frac{\lambda}{2\pi}\Delta\phi needs Δϕ\Delta\phi in radians; in degrees use Δϕ360∘λ\frac{\Delta\phi}{360^\circ}\lambda. Plugging 60 into the radian form is the classic slip.

Concept 3 of 3: Particle Velocity Against Wave Velocity

The wave moves along x at ω/k; each particle just bobs up and down, fastest as it passes the middle, at Aω. Their ratio, Aω ÷ (ω/k) = Ak, depends only on the amplitude and the wavelength.

Definition

  • Particle: vp,max⁡=Aωv_{p,\max} = A\omega, amax⁡=Aω2a_{\max} = A\omega^2. Wave: v=ωkv = \dfrac{\omega}{k}.
  • vp,max⁡v=Ak=2πAλ\dfrac{v_{p,\max}}{v} = Ak = \dfrac{2\pi A}{\lambda}.
  • y=asin⁡2π(bt−cx)y = a\sin 2\pi(bt - cx): v=bcv = \dfrac{b}{c}, vp,max⁡=2πabv_{p,\max} = 2\pi ab.
  • y=Asin⁡2(ωt−kx)y = A\sin^2(\omega t - kx) is a wave of amplitude A2\dfrac{A}{2} at 2ω2\omega and 2k2k: vp,max⁡=Aωv_{p,\max} = A\omega, wavelength πk\dfrac{\pi}{k}.
  • Energy of a wave ∝n2A2\propto n^2A^2.

Speed ratio

vp,max⁡vwave=Ak=2πAλ\frac{v_{p,\max}}{v_{\text{wave}}} = Ak = \frac{2\pi A}{\lambda}

Worked example

y=0.02sin⁡(100t−5x)y = 0.02\sin(100t - 5x) (SI). Maximum particle speed, wave speed and their ratio?
Practice this conceptself-check · 2 quick reps

The same idea in a real exam question:

MHT-CET · 2024 · 13th May Shift 2 · Q45Moderate

Example 3 · Superposition of Waves · Progressive Wave, Wave Equation, and Velocity

The equation of a progressive wave is Y=asin⁡2π ⁣(nt−x5)Y=a\sin 2\pi\!\left(nt-\frac{x}{5}\right). The ratio of maximum particle velocity to wave velocity is

Treating a sin² wave like a sine wave

Asin⁡2θ=A2(1−cos⁡2θ)A\sin^2\theta = \frac{A}{2}(1 - \cos 2\theta): the oscillation has amplitude A2\frac{A}{2} at twice the frequency, so the particles peak at AωA\omega, not 2Aω2A\omega — and the wavelength is πk\frac{\pi}{k}.

Summary — formulas & gotchas at a glance

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Formulas (3)

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Test yourself on Superposition of Waves

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