Level 3 — ProductionOscillations & Waves

Oscillations & Waves

45 minutes60 marksprintable — key stays hidden on paper

Level 3 Paper: Production (From-Scratch Derivations & Reasoning)

Time limit: 45 minutes Total marks: 60 Instructions: Show all derivations from first principles. State assumptions explicitly. Use ...... for mathematics. Calculators permitted; take g=9.81 m s2g = 9.81\ \text{m s}^{-2} and speed of sound in air =343 m s1= 343\ \text{m s}^{-1} unless told otherwise.


Question 1 — SHM & Energy from scratch (12 marks)

(a) Starting from the restoring force F=kxF = -kx and Newton's second law, derive the SHM differential equation and show that x=Acos(ωt+ϕ)x = A\cos(\omega t + \phi) is a solution. State the value of ω\omega in terms of kk and mm. (4)

(b) Derive the velocity expression v=±ωA2x2v = \pm\omega\sqrt{A^2 - x^2} from your solution, showing your working. (3)

(c) From the KE and PE expressions, prove that total mechanical energy is constant and equals 12kA2\tfrac{1}{2}kA^2. (3)

(d) A 0.25 kg0.25\ \text{kg} mass on a spring of stiffness k=100 N m1k = 100\ \text{N m}^{-1} oscillates with amplitude 0.04 m0.04\ \text{m}. Compute the maximum speed and total energy. (2)


Question 2 — Pendulum derivations (10 marks)

(a) Derive T=2πL/gT = 2\pi\sqrt{L/g} for a simple pendulum, stating clearly where and why the small-angle approximation is used. (4)

(b) For a physical (compound) pendulum of moment of inertia II about the pivot, mass MM, and pivot-to-centre-of-mass distance dd, derive T=2πI/(Mgd)T = 2\pi\sqrt{I/(Mgd)}. (4)

(c) A uniform rod of length LL pivoted at one end has I=13ML2I = \tfrac{1}{3}ML^2. Find its period as a multiple of the simple-pendulum period of length LL. (2)


Question 3 — Damping & Q factor (10 marks)

(a) Write the differential equation for a damped oscillator (mass mm, damping constant bb, stiffness kk). Define the three damping regimes (under-, critical, over-) in terms of the discriminant condition, explaining the physical behaviour of each in words. (5)

(b) The Q factor is Q=ω0m/bQ = \omega_0 m / b. Explain physically what a high Q means for (i) energy loss per cycle and (ii) resonance sharpness. (3)

(c) An underdamped oscillator has ω0=50 rad s1\omega_0 = 50\ \text{rad s}^{-1}, m=0.2 kgm = 0.2\ \text{kg}, b=0.4 kg s1b = 0.4\ \text{kg s}^{-1}. Compute QQ. (2)


Question 4 — Wave equation on a string (10 marks)

(a) By considering a small element of a stretched string under tension TT with linear mass density μ\mu, derive the wave equation 2yt2=Tμ2yx2\dfrac{\partial^2 y}{\partial t^2} = \dfrac{T}{\mu}\dfrac{\partial^2 y}{\partial x^2}. State your small-angle assumptions. (6)

(b) Hence write the wave speed and compute it for a string with T=80 NT = 80\ \text{N}, μ=5×103 kg m1\mu = 5\times10^{-3}\ \text{kg m}^{-1}. (2)

(c) This string is fixed at both ends, length 1.2 m1.2\ \text{m}. Find the fundamental frequency. (2)


Question 5 — Beats & Doppler reasoning (10 marks)

(a) By superposing two waves of nearly equal frequencies f1f_1 and f2f_2, derive the beat frequency fbeat=f1f2f_{\text{beat}} = |f_1 - f_2|. Show the amplitude-modulation envelope explicitly. (4)

(b) State the general Doppler formula for sound and explain out loud (in words) why the sign convention differs between a moving source and a moving observer. (3)

(c) A siren emits 600 Hz600\ \text{Hz}. It approaches a stationary observer at 30 m s130\ \text{m s}^{-1}. Find the observed frequency. (3)


Question 6 — Shock waves & intensity (8 marks)

(a) Define Mach number and derive the half-angle of the Mach cone, sinθ=1/M\sin\theta = 1/M, from the geometry of the wavefronts. (4)

(b) A rocket travels at Mach 2.5. Find the Mach cone half-angle. (2)

(c) Sound intensity rises from 106 W m210^{-6}\ \text{W m}^{-2} to 103 W m210^{-3}\ \text{W m}^{-2}. Find the increase in sound level in decibels. (2)

Answer keyMark scheme & solutions

Question 1

(a) [4 marks]

  • Newton: ma=F=kxmx¨=kxma = F = -kx \Rightarrow m\ddot{x} = -kx, so x¨+kmx=0\ddot{x} + \tfrac{k}{m}x = 0. (1)
  • Define ω2=k/m\omega^2 = k/m. (1)
  • Substitute trial x=Acos(ωt+ϕ)x = A\cos(\omega t+\phi): x¨=ω2Acos(ωt+ϕ)=ω2x\ddot{x} = -\omega^2 A\cos(\omega t+\phi) = -\omega^2 x. (1)
  • This satisfies x¨+ω2x=0\ddot{x}+\omega^2 x = 0, confirming solution; ω=k/m\omega = \sqrt{k/m}. (1)

(b) [3 marks]

  • x=Acosθx = A\cos\theta, v=x˙=Aωsin(ωt+ϕ)v=\dot x = -A\omega\sin(\omega t+\phi). (1)
  • sinθ=±1cos2θ=±1(x/A)2\sin\theta = \pm\sqrt{1-\cos^2\theta} = \pm\sqrt{1-(x/A)^2}. (1)
  • v=Aω(±1x2/A2)=±ωA2x2v = -A\omega(\pm\sqrt{1-x^2/A^2}) = \pm\omega\sqrt{A^2-x^2}. (1)

(c) [3 marks]

  • KE=12mv2=12mω2(A2x2)=12k(A2x2)KE = \tfrac12 m v^2 = \tfrac12 m\omega^2(A^2-x^2)= \tfrac12 k(A^2-x^2) (using mω2=km\omega^2=k). (1)
  • PE=12kx2PE = \tfrac12 kx^2. (1)
  • E=KE+PE=12kA2E = KE+PE = \tfrac12 k A^2, independent of xx ⇒ constant. (1)

(d) [2 marks]

  • ω=100/0.25=20 rad s1\omega=\sqrt{100/0.25}=20\ \text{rad s}^{-1}; vmax=ωA=20(0.04)=0.8 m s1v_{max}=\omega A = 20(0.04)=0.8\ \text{m s}^{-1}. (1)
  • E=12kA2=12(100)(0.04)2=0.08 JE=\tfrac12 kA^2 = \tfrac12(100)(0.04)^2 = 0.08\ \text{J}. (1)

Question 2

(a) [4 marks]

  • Restoring tangential force: F=mgsinθF = -mg\sin\theta. (1)
  • Torque/arc: mLθ¨=mgsinθmL\ddot\theta = -mg\sin\theta. (1)
  • Small angle: sinθθ\sin\theta\approx\theta (in radians) ⇒ θ¨+gLθ=0\ddot\theta + \tfrac{g}{L}\theta=0; needed to obtain linear SHM form. (1)
  • ω=g/L\omega=\sqrt{g/L}, T=2πL/gT=2\pi\sqrt{L/g}. (1)

(b) [4 marks]

  • Torque about pivot: τ=Mgdsinθ\tau = -Mgd\sin\theta. (1)
  • Iθ¨=MgdsinθI\ddot\theta = -Mgd\sin\theta. (1)
  • Small angle: θ¨+MgdIθ=0\ddot\theta + \tfrac{Mgd}{I}\theta=0ω=Mgd/I\omega=\sqrt{Mgd/I}. (1)
  • T=2πI/(Mgd)T=2\pi\sqrt{I/(Mgd)}. (1)

(c) [2 marks]

  • d=L/2d=L/2, I=13ML2I=\tfrac13 ML^2: T=2π13ML2/(MgL/2)=2π2L3gT=2\pi\sqrt{\tfrac13 ML^2/(Mg\cdot L/2)}=2\pi\sqrt{\tfrac{2L}{3g}}. (1)
  • Ratio to simple pendulum 2πL/g2\pi\sqrt{L/g}: factor 2/30.816\sqrt{2/3}\approx0.816. (1)

Question 3

(a) [5 marks]

  • mx¨+bx˙+kx=0m\ddot x + b\dot x + kx = 0. (2)
  • Discriminant of characteristic eqn via ω0=k/m\omega_0=\sqrt{k/m}, γ=b/2m\gamma=b/2m:
    • Underdamped: γ<ω0\gamma<\omega_0 — oscillates with decaying amplitude. (1)
    • Critical: γ=ω0\gamma=\omega_0 — returns to equilibrium fastest without oscillating. (1)
    • Overdamped: γ>ω0\gamma>\omega_0 — returns slowly, no oscillation. (1)

(b) [3 marks]

  • High Q ⇒ small energy loss per cycle (Q = 2π×2\pi\times energy stored / energy lost per cycle). (1.5)
  • High Q ⇒ narrow, sharp resonance peak (small bandwidth Δω=ω0/Q\Delta\omega=\omega_0/Q). (1.5)

(c) [2 marks]

  • Q=ω0m/b=50(0.2)/0.4=25Q=\omega_0 m/b = 50(0.2)/0.4 = 25. (2)

Question 4

(a) [6 marks]

  • Element from xx to x+dxx+dx, mass μdx\mu\,dx; tension TT acts along tangents at both ends. (1)
  • Net vertical force =Tsinθ2Tsinθ1=T\sin\theta_2 - T\sin\theta_1. (1)
  • Small angle: sinθtanθ=y/x\sin\theta\approx\tan\theta = \partial y/\partial x. (1)
  • Net force =T[(y/x)x+dx(y/x)x]=T2yx2dx= T[(\partial y/\partial x)_{x+dx}-(\partial y/\partial x)_x] = T\dfrac{\partial^2 y}{\partial x^2}dx. (1)
  • Newton: μdx2yt2=T2yx2dx\mu\,dx\,\dfrac{\partial^2 y}{\partial t^2}=T\dfrac{\partial^2 y}{\partial x^2}dx. (1)
  • 2yt2=Tμ2yx2\dfrac{\partial^2 y}{\partial t^2}=\dfrac{T}{\mu}\dfrac{\partial^2 y}{\partial x^2}. (1)

(b) [2 marks]

  • v=T/μ=80/0.005=16000=126.5 m s1v=\sqrt{T/\mu}=\sqrt{80/0.005}=\sqrt{16000}=126.5\ \text{m s}^{-1}. (2)

(c) [2 marks]

  • f1=v/(2L)=126.5/2.4=52.7 Hzf_1 = v/(2L)=126.5/2.4 = 52.7\ \text{Hz}. (2)

Question 5

(a) [4 marks]

  • y=Acos(2πf1t)+Acos(2πf2t)y=A\cos(2\pi f_1 t)+A\cos(2\pi f_2 t). (1)
  • Sum-to-product: =2Acos ⁣(2πf1f22t)cos ⁣(2πf1+f22t)=2A\cos\!\big(2\pi\tfrac{f_1-f_2}{2}t\big)\cos\!\big(2\pi\tfrac{f_1+f_2}{2}t\big). (1)
  • Envelope amplitude 2Acos(π(f1f2)t)2A\cos(\pi(f_1-f_2)t) modulates carrier. (1)
  • Intensity maxima occur twice per envelope period ⇒ fbeat=f1f2f_{beat}=|f_1-f_2|. (1)

(b) [3 marks]

  • f=fv±vovvsf' = f\dfrac{v\pm v_o}{v\mp v_s}. (1)
  • Observer motion changes the number of wavefronts encountered per second (relative speed of waves changes). (1)
  • Source motion compresses/stretches the wavelength itself (source chases its own waves), so it enters as a denominator; these are physically distinct mechanisms. (1)

(c) [3 marks]

  • Source approaching, observer stationary: f=fvvvs=60034334330f'=f\dfrac{v}{v-v_s}=600\dfrac{343}{343-30}. (1)
  • =600×343/313=600×1.0958=600\times343/313 = 600\times1.0958. (1)
  • =657.5 Hz=657.5\ \text{Hz}. (1)

Question 6

(a) [4 marks]

  • Mach number M=vsource/vsoundM = v_{source}/v_{sound}. (1)
  • In time tt: source travels vstv_s t, wavefront radius =vt= v\,t. (1)
  • Cone half-angle: sinθ=vtvst=vvs\sin\theta = \dfrac{v t}{v_s t} = \dfrac{v}{v_s}. (1)
  • =1/M=1/M. (1)

(b) [2 marks]

  • sinθ=1/2.5=0.4\sin\theta=1/2.5=0.4θ=arcsin0.4=23.6°\theta=\arcsin 0.4 = 23.6°. (2)

(c) [2 marks]

  • ΔL=10log10(I2/I1)=10log10(103/106)=10log10(1000)=30 dB\Delta L = 10\log_{10}(I_2/I_1)=10\log_{10}(10^{-3}/10^{-6})=10\log_{10}(1000)=30\ \text{dB}. (2)

[
  {"claim":"Q1d max speed 0.8 and energy 0.08 J","code":"import sympy as sp\nomega=sp.sqrt(100/sp.Rational(1,4))\nvmax=omega*sp.Rational(4,100)\nE=sp.Rational(1,2)*100*(sp.Rational(4,100))**2\nresult=(vmax==sp.Rational(8,10)) and (E==sp.Rational(8,100))"},
  {"claim":"Q3c Q factor equals 25","code":"Q=50*sp.Rational(2,10)/sp.Rational(4,10)\nresult=(Q==25)"},
  {"claim":"Q4 wave speed 126.5 and fundamental 52.7 Hz","code":"v=sp.sqrt(80/sp.Rational(5,1000))\nf1=v/sp.Rational(24,10)\nresult=(abs(float(v)-126.49)<0.1) and (abs(float(f1)-52.7)<0.1)"},
  {"claim":"Q5c Doppler observed freq approx 657.5 Hz","code":"fobs=600*343/(343-30)\nresult=abs(float(fobs)-657.5)<0.5"},
  {"claim":"Q6c decibel increase is 30 dB","code":"dL=10*sp.log(sp.Rational(10)**-3/sp.Rational(10)**-6,10)\nresult=(sp.simplify(dL)==30)"}
]