2020 A/L Physics Past Paper · Question 21 (English Medium)

A warmed open pipe — beats

Two identical resonance tubes, each 50 cm50\ \text{cm} long and open at both ends, sound their fundamental notes at 15∘C15^\circ\text{C}. The speed of sound in air v (m s−1)v\ (\text{m s}^{-1}) varies with temperature as v=331+0.6θv = 331 + 0.6\theta, where θ\theta is in ∘C^\circ\text{C}. If the temperature of one tube is raised to 30∘C30^\circ\text{C}, how many beats are produced in one second?

  1. (1) 44
  2. (2) 66
  3. (3) 99
  4. (4) 1212
  5. (5) 1414
Answer and explanation

Answer: (3) 99

Given information

We know:

Pipe length L=50 cm=0.50L = 50\ \text{cm} = 0.50 m, open at both ends.

Starting temperature 15∘C15^\circ\text{C}; one pipe is raised to 30∘C30^\circ\text{C}.

v=331+0.6θv = 331 + 0.6\theta; both pipes sound their fundamental notes.

What the question asks

We want: the beats per second fbf_b when the two pipes sound together.

Relevant theory

The relationship among the wave velocity v, frequency f and the wavelength λ, can be written in the form of v = f λ.

The number of times the sound reaches maximum in one second is called beat frequency,

Required equations

λ1=2L\lambda_1 = 2L

f=vλ1=v2Lf = \frac{v}{\lambda_1} = \frac{v}{2L}

fb=∣f1−f2∣f_b = |f_1 - f_2|

Applying it to this question

Plan:

Find the speed of sound at both temperatures.

Find each pipe’s fundamental note v/2Lv/2L.

Their difference is the beats.

The end correction ee is not given, so it is neglected.

Reasoning and calculation

340340

v1=331+0.6×15v_1 = 331 + 0.6 \times 15

349349

v2=331+0.6×30v_2 = 331 + 0.6 \times 30

f1=3402×0.50f_1 = \frac{340}{2 \times 0.50}

f2=3492×0.50f_2 = \frac{349}{2 \times 0.50}

99

fb=349−340f_b = 349 - 340

Checks

Units: m s−1m=s−1=Hz\dfrac{\text{m s}^{-1}}{\text{m}} = \text{s}^{-1} = \text{Hz}; beats are also per second ✓.

Does it make sense? Since 2L=12L = 1 m, every 1 m s−11\ \text{m s}^{-1} change in speed is 11 Hz; 0.6×15=9 m s−10.6 \times 15 = 9\ \text{m s}^{-1} ⇒ 99 beats. Nine beats per second is something an ear could count ✓.

0.6∗(t2−t1)/(2∗L)0.6 * (t2 - t1) / (2 * L)

Conclusion

fb=349−340=9 s−1f_b = 349 - 340 = 9\ \text{s}^{-1}

f1=340f_1 = 340 Hz, f2=349f_2 = 349 Hz; fb=9f_b = 9 — the answer is (3).

Using the closed-pipe formula f=v4Lf = \dfrac{v}{4L} for an open pipe.

Both ends are open; the fundamental has an antinode at each end: λ=2L\lambda = 2L.

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