Oscillations: Question 8

Syllabus 17.1, 17.2

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]

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Worked solution

Part (a): Show that ω = 9.49 rad s⁻¹

For a mass on a spring, the angular frequency is: ω=km=180.200=90\omega=\sqrt{\frac{k}{m}}=\sqrt{\frac{18}{0.200}}=\sqrt{90}

Recompute as a check, evaluating the division first in a different way: 18÷0.200=90.018\div0.200=90.0 exactly, and 90=9.4868\sqrt{90}=9.4868.

So ω=9.49 rad s1\omega=9.49\text{ rad s}^{-1} (3 s.f.), as required to show. This exact value ω2=90 rad2 s2\omega^2=90\text{ rad}^2\text{ s}^{-2} is carried forward for accuracy.

Part (b): Total energy

The total (constant) energy of an SHM oscillation is: E=12mω2x02E=\tfrac12m\omega^2x_0^2

Substituting m=0.200 kgm=0.200\text{ kg}, ω2=90 rad2 s2\omega^2=90\text{ rad}^2\text{ s}^{-2}, x0=0.050 mx_0=0.050\text{ m}: E=12×0.200×90×(0.050)2=0.100×90×0.0025E=\tfrac12\times0.200\times90\times(0.050)^2=0.100\times90\times0.0025

Working step by step: 0.100×90=9.000.100\times90=9.00; then 9.00×0.0025=0.0225 J9.00\times0.0025=0.0225\text{ J}.

Recompute in a different grouping as a check: (0.050)2×90=0.0025×90=0.225(0.050)^2\times90=0.0025\times90=0.225; then 0.100×0.225=0.0225 J0.100\times0.225=0.0225\text{ J}, the same result.

So E=2.25×102 JE=\boxed{2.25\times10^{-2}}\text{ J}, i.e. 22.5 mJ22.5\text{ mJ}.

Part (c): Show that x = 2.89 × 10⁻² m when KE = 2PE

At any displacement, KE+PE=EKE+PE=E (total energy is constant). If KE=2PEKE=2PE, then: 2PE+PE=E    3PE=E    PE=E32PE+PE=E \implies 3PE=E \implies PE=\frac{E}{3}

Since PE=12mω2x2PE=\tfrac12m\omega^2x^2 and E=12mω2x02E=\tfrac12m\omega^2x_0^2: 12mω2x2=12mω2x023    x2=x023    x=x03\tfrac12m\omega^2x^2=\frac{\tfrac12m\omega^2x_0^2}{3} \implies x^2=\frac{x_0^2}{3} \implies x=\frac{x_0}{\sqrt3}

Substituting x0=0.050 mx_0=0.050\text{ m}: x=0.0503=0.0501.7321=0.028868 mx=\frac{0.050}{\sqrt3}=\frac{0.050}{1.7321}=0.028868\text{ m}

Recompute as a check, working directly in energy terms: PE=E/3=0.0225/3=0.00750 JPE=E/3=0.0225/3=0.00750\text{ J}. Then x2=2PEmω2=2×0.007500.200×90=0.015018.0=8.333×104 m2x^2=\dfrac{2PE}{m\omega^2}=\dfrac{2\times0.00750}{0.200\times90}=\dfrac{0.0150}{18.0}=8.333\times10^{-4}\text{ m}^2, so x=8.333×104=0.028868 mx=\sqrt{8.333\times10^{-4}}=0.028868\text{ m}, the same value, confirming the result.

So x=2.89×102 mx=\boxed{2.89\times10^{-2}}\text{ m} (3 s.f.), as required to show.

Part (d): Speed at this displacement

v=ωx02x2v=\omega\sqrt{x_0^2-x^2}

Substituting x02=(0.050)2=0.0025 m2x_0^2=(0.050)^2=0.0025\text{ m}^2 and x2=x02/3=8.333×104 m2x^2=x_0^2/3=8.333\times10^{-4}\text{ m}^2: x02x2=0.00250.0008333=0.0016667 m2x_0^2-x^2=0.0025-0.0008333=0.0016667\text{ m}^2 0.0016667=0.040825 m\sqrt{0.0016667}=0.040825\text{ m} v=9.4868×0.040825=0.38730 m s1v=9.4868\times0.040825=0.38730\text{ m s}^{-1}

Recompute as a check, using KE=12mv2KE=\tfrac12mv^2 directly: since KE=2E/3=2×0.0225/3=0.0150 JKE=2E/3=2\times0.0225/3=0.0150\text{ J}, then v2=2×KEm=2×0.01500.200=0.150 m2s2v^2=\dfrac{2\times KE}{m}=\dfrac{2\times0.0150}{0.200}=0.150\text{ m}^2\text{s}^{-2}, so v=0.150=0.3873 m s1v=\sqrt{0.150}=0.3873\text{ m s}^{-1}, the same value, confirming the result.

So v=0.387 m s1v=\boxed{0.387}\text{ m s}^{-1} (3 s.f.).

Final answers

  • (a) ω=9.49 rad s1\omega=\boxed{9.49}\text{ rad s}^{-1}
  • (b) E=2.25×102 JE=\boxed{2.25\times10^{-2}}\text{ J}
  • (c) x=2.89×102 mx=\boxed{2.89\times10^{-2}}\text{ m}
  • (d) v=0.387 m s1v=\boxed{0.387}\text{ m s}^{-1}