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Page 1: Measuring Acoustic Wavelength and Velocity Diva, Tama & Hafiz.

S

Measuring Acoustic Wavelength and

VelocityDiva, Tama & Hafiz

Page 2: Measuring Acoustic Wavelength and Velocity Diva, Tama & Hafiz.

Introduction

Wave properties:

Wavelength (λ): parallel displacement in one cycle.

Amplitude (a): maximum perpendicular displacement.

Period (t): time taken for one cycle.

Frequency (f): cycles undergone per unit time.

Velocity (v): linear displacement per unit time.

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Resonance principle

Every half a cycle, a wave reaches its amplitude.

When the amplitude of a sound wave makes

contact with a physical barrier (e.g. the inside of a

tube), it amplifies the sound’s intensity. This effect

is called resonance.

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Hypothesis

The relationship between velocity, wavelength and frequency is defined as v = λf

By generating a sound wave with a constant frequency and finding its wavelength through the points of resonance, we might be able to find the speed of sound through a medium using a derivative of the above formula.

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Materials

Biuret

Tuning forks (216 Hz, 288 Hz, 512 Hz)

Bucket

Retort stand

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Procedure

1. Fill the biuret to the brim with tap water.

2. Tap the tuning fork on a hard surface and listen to its vibration as closely to the surface as possible.

3. Open the biuret and let the water flow out. When the water level reaches a point of resonance, the note should be momentarily amplified.

4. Rinse and repeat until no further resonance is heard.

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Assuming that the sound wave experiences resonance every half a cycle,

l2 – l1 = λ/2

Where l = distance of a given resonance point from the surface.

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Sources of error

Irregular water flow

External disturbances

Tuning fork vibration frequency not necessarily the same as the sound wave generated

Human error False positives Mistiming Zero error/parallax

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Results

216 HzNo

distance from opening (cm)

Test 1 Test 2

1 10.2 6.0

2 12.3 9.5

3 15.0 12.6

4 17.1 16.5

5 22.2 20.2

6 23.1

7 24.6

l2 – l1 = 2.1 cm, 3.5 cmCalculated length: 4.2 cm, 7.0 cmMean result: 5.6 cmCalculated velocity: 12.096 ms-1

  Average difference: 3.0 cm, 3.1 cmAvg. calculated length: 6.0 cm, 6.2 cmMean result: 6.1 cmCalculated velocity: 13.176 ms-1

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288 Hz

No

distance from opening (cm)

Test 1 Test 2

1 3.0 7.6

2 6.1 10.3

3 8.5 14.6

4 11.2 17.9

5 13.1 20.7

6 14.5 24.4

7 19.5 26.2

8 23.7

9 28.8

l2 – l1 = 3.1 cm, 2.7 cmCalculated length: 6.2 cm, 5.4 cmMean result: 5.8 cmCalculated velocity: 16.704 ms-1

  Average difference: 3.7 cm, 3.1 cmAvg. calculated length: 7.4 cm, 6.2 cmMean result: 6.8 cmCalculated velocity: 19.584 ms-1

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512 Hz

No

distance from opening (cm)

Test 1 Test 2

1 5.9 16.6

2 10.5 22.3

3 13.0 28.7

4 15.0 31.6

5 21.0 34.0

6 23.0 43.7

7 26.0

8 28.3

l2 – l1 = 4.6 cm, 5.7 cmCalculated length: 9.2 cm, 11.4 cmMean result: 10.3 cmCalculated velocity: 52.736 ms-1

  Average difference: 3.2 cm, 5.4 cmAvg. calculated length: 6.4 cm, 10.8 cmMean result: 8.1 cmCalculated velocity: 41.472 ms-1

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Observation

The values calculated were much lower than the

known speed of sound in air (334.2 m/s)

This might be due to the experiment method,

which depends on human hearing to take readings

and is therefore prone to human error.

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Conclusion

Though the concept is sound, a more reliable method of measurement is required to achieve proper results.

Hence, this lab session is inconclusive.

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References

Brian Arnold et al. International A/AS-Level Physics. London: Hodder Education, 2008.

“Sound Waves”. Rice University Web Services. Rice University, n.d.