Oscillations: Physics 9702 (Cambridge International AS & A Level)

Syllabus 17.1, 17.2, 17.3 · Strand 5 Fields and Oscillations

Questions
10
Total marks
56
Tier mix
10 Core

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Syllabus coverage

  • 17.1 8 questions
  • 17.2 2 questions
  • 17.3 2 questions

Oscillations (syllabus ref 17.1 to 17.3) studies repetitive motion about a fixed point, defined by displacement, amplitude, period, frequency, angular frequency ω\omega and phase difference. A system undergoes simple harmonic motion (SHM) whenever its acceleration is proportional to displacement from a fixed point but directed back toward it, a=ω2xa = -\omega^2 x; this differential relationship has the solutions x=x0sinωtx = x_0\sin\omega t and v=±ωx02x2v = \pm\omega\sqrt{x_0^2 - x^2}, letting displacement, velocity and acceleration all be tracked, sketched and interpreted as functions of time or of each other.

During SHM, energy continuously interchanges between kinetic and potential stores while the total mechanical energy stays constant at E=12mω2x02E = \tfrac12 m\omega^2 x_0^2. Real oscillators, however, lose energy to resistive forces (a process called damping, classified as light (many oscillations, gradually decaying amplitude), critical (fastest return to rest with no oscillation) or heavy (slow return, no oscillation). When an external periodic driving force acts on a system, the amplitude of oscillation becomes strongly dependent on driving frequency, reaching a maximum) resonance. When the system is driven at its own natural frequency.

Original worked examples below apply the SHM equations, energy formula and damping/resonance ideas with full solutions.

Question 1

Multiple choice A2 1 mark

A small ball attached to a horizontal spring oscillates with simple harmonic motion of amplitude x0=4.5 cmx_0 = 4.5\text{ cm} and frequency f=3.0 Hzf = 3.0\text{ Hz}.

What is the maximum speed of the ball during the oscillation?

Question 2

Structured A2 8 marks

A mass of m=0.250 kgm = 0.250\text{ kg} is attached to the end of a spring of force constant k=40 N m1k = 40\text{ N m}^{-1} and hangs in equilibrium. The mass is then pulled down a further 6.0 cm6.0\text{ cm} from its equilibrium position and released from rest at time t=0t=0, so that it oscillates with simple harmonic motion of amplitude x0=0.060 mx_0 = 0.060\text{ m}.

(a) State the equation for the displacement xx of the mass at time tt after release, and describe the shape of the graph of xx against tt that this equation represents over one complete oscillation. [2]

(b) Show that the angular frequency ω\omega of the oscillation is 12.6 rad s112.6\text{ rad s}^{-1}. [2]

(c) Calculate the maximum speed of the mass during the oscillation. [2]

(d) Calculate the maximum magnitude of the acceleration of the mass during the oscillation. [2]

Question 3

Structured A2 9 marks

A simple pendulum consists of a small bob of mass m=0.120 kgm = 0.120\text{ kg} on a light string of length L=0.900 mL = 0.900\text{ m}. The bob is displaced sideways to give an amplitude of x0=5.0 cmx_0 = 5.0\text{ cm} and released from rest, so that it swings with simple harmonic motion. Take g=9.81 m s2g = 9.81\text{ m s}^{-2}.

(a) Show that the period of oscillation is 1.90 s1.90\text{ s}. [2]

(b) Calculate the angular frequency ω\omega of the oscillation. [2]

(c) Calculate the total energy of the oscillation. [2]

(d) Calculate the kinetic energy and the potential energy of the bob at the instant its displacement from the equilibrium position is 3.0 cm3.0\text{ cm}. [3]

Question 4

Structured A2 8 marks

An engineering student sets up a demonstration rig: a metal block hangs from a vertical spring, with the block partly submerged in a cylinder of oil so that its oscillations can be damped by varying the oil's viscosity. In each case below, the block is pulled down by the same amount and released from rest.

(a) With no oil in the cylinder, the block oscillates with negligible damping. State what is meant by damping in an oscillating system, and describe how adding light damping would change the displacement-time graph of the block compared with this undamped case. [3]

(b) Oil is added so that the block returns to its equilibrium position in the shortest possible time, without overshooting and oscillating about it. State the name given to this particular case of damping, and describe how heavy damping would differ from it. [3]

(c) A small motor is later attached to the top of the spring, shaking the support up and down at an adjustable frequency. Explain what is meant by resonance, and state the condition on the driving frequency required for resonance to occur in this system. [2]

Question 5

Multiple choice A2 1 mark

A particle oscillates with simple harmonic motion of amplitude x0=0.12 mx_0 = 0.12\text{ m} and period T=0.50 sT = 0.50\text{ s}.

What is the speed of the particle at the instant its displacement from the centre of the oscillation is x=0.072 mx = 0.072\text{ m}?

Question 6

Multiple choice A2 1 mark

The cone of a small loudspeaker oscillates with simple harmonic motion of amplitude x0=1.5 mmx_0 = 1.5\text{ mm} and frequency f=200 Hzf = 200\text{ Hz}.

What is the magnitude of the maximum acceleration of the cone during the oscillation?

Question 7

Structured A2 9 marks

A prong of a vibrating tuning fork oscillates with simple harmonic motion of amplitude x0=0.80 mmx_0 = 0.80\text{ mm} and frequency f=256 Hzf = 256\text{ Hz}. At time t=0t=0, the tip of the prong passes through the centre of its oscillation moving with its maximum speed.

(a) State the appropriate equation for the displacement xx of the prong tip at time tt, and explain why this form (rather than a cosine equation) applies here. [2]

(b) Calculate the angular frequency ω\omega of the oscillation. [2]

(c) Calculate the displacement and the velocity of the prong tip at t=2.0×104 st = 2.0\times10^{-4}\text{ s}. [3]

(d) Use a=ω2xa=-\omega^2x to calculate the magnitude of the acceleration of the prong tip at this same instant, and state the direction of this acceleration relative to the displacement found in (c). [2]

Question 8

Structured A2 9 marks

A block of mass m=0.200 kgm = 0.200\text{ kg} rests on a frictionless horizontal surface and is attached to a light spring of force constant k=18 N m1k = 18\text{ N m}^{-1}. The block is pulled aside by x0=5.0 cmx_0 = 5.0\text{ cm} from its equilibrium position and released from rest, so that it oscillates with simple harmonic motion of amplitude x0=0.050 mx_0 = 0.050\text{ m}.

(a) Show that the angular frequency of the oscillation is ω=9.49 rad s1\omega = 9.49\text{ rad s}^{-1}. [2]

(b) Calculate the total energy of the oscillation. [2]

(c) Show that the displacement at which the kinetic energy of the block is exactly twice its potential energy is x=2.89×102 mx = 2.89\times10^{-2}\text{ m}. [3]

(d) Calculate the speed of the block at this displacement. [2]

Question 9

Multiple choice A2 1 mark

A displacement-time graph for a lightly damped oscillating system shows the amplitude of successive oscillations gradually decreasing over time.

Which one of the following statements about this system is correct?

Question 10

Structured A2 9 marks

A particle P moves with simple harmonic motion such that its displacement is x=x0cosωtx=x_0\cos\omega t, where x0=5.0 cmx_0 = 5.0\text{ cm} and ω=4.0 rad s1\omega = 4.0\text{ rad s}^{-1}.

(a) Calculate the period TT of the motion, and state the values of the displacement xx, velocity vv and acceleration aa of P at t=0t=0. [2]

(b) Calculate the values of xx, vv and aa of P at t=T/4t=T/4. [2]

(c) Calculate the values of xx, vv and aa of P at t=T/2t=T/2. [2]

(d) Using your answers to (a)-(c), describe the phase relationship of the velocity-time graph relative to the displacement-time graph, and of the acceleration-time graph relative to the displacement-time graph. [3]