2020 A/L Physics Past Paper · Question 16 (English Medium)

Simple harmonic motion: angular frequency from the largest velocity and acceleration

A particle of mass mm performs simple harmonic motion. If the largest speed and the largest acceleration of the particle are VV and aa respectively, the angular frequency (ω)(\omega) of the particle is given by

  1. (1) Vma\dfrac{V}{ma}
  2. (2) 2πVa\dfrac{2\pi V}{a}
  3. (3) 2πaV\dfrac{2\pi a}{V}
  4. (4) aV\dfrac{a}{V}
  5. (5) Va\dfrac{V}{a}
Answer and explanation

Answer: (4) aV\dfrac{a}{V}

What the question asks

We want: the angular frequency ω\omega from the largest velocity VV and the largest acceleration aa — an expression in VV, aa (and mm if needed).

Relevant theory

v = ±w√( ( A² − x² ) ), where w = √(k/m)

a = −ω²x

Required equations

v=ωr2−x2v = \omega\sqrt{r^2 - x^2}

V=ωrV = \omega r

ax=−ω2xa_x = -\omega^2 x

a=ω2ra = \omega^2 r

Reasoning and calculation

Symbols: rr — amplitude; ω\omega — angular frequency; xx — displacement from the centre; VV — largest speed (at the centre); aa — largest acceleration (at an end); mm — mass.

Eliminate the awkward amplitude rr: dividing a=ω2ra = \omega^2 r by V=ωrV = \omega r cancels rr.

aV=ω2rωr\frac{a}{V} = \frac{\omega^2 r}{\omega r}

ω=aV\omega = \frac{a}{V}

Reading the options

Matching the form: ω=aV\omega = \dfrac{a}{V} — option (4).

In (2), 2πω=T\dfrac{2\pi}{\omega} = T.

In (3), an extra 2π2\pi.

(5) is inverted.

(1) brings in an unneeded mm.

T = 2π/ω

Checks

Dimension check: [aV]=LT−2LT−1=T−1\left[\dfrac{a}{V}\right] = \dfrac{LT^{-2}}{LT^{-1}} = T^{-1} — matches the angular frequency. [Vma]=M−1T\left[\dfrac{V}{ma}\right] = M^{-1}T ✗, [Va]=T\left[\dfrac{V}{a}\right] = T ✗.

Does it make sense? Doubling the amplitude rr doubles both VV and aa; ω=a/V\omega = a/V stays the same — matching the fact that SHM frequency does not depend on amplitude. With numbers: r=0.1r = 0.1 m, ω=4 rad s−1\omega = 4\ \text{rad s}^{-1} gives V=0.4V = 0.4, a=1.6a = 1.6, a/V=4a/V = 4 ✓.

a/Va / V

Conclusion

ω=aV\omega = \frac{a}{V}

V=ωrV = \omega r, a=ω2ra = \omega^2 r ⇒ ω=aV\omega = \dfrac{a}{V} — the answer is (4).

Extra data like mm may be given just to test you; in mechanics questions, check with dimensions whether it is actually needed.

Exam tip

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