Wave Velocity Dynamics: String Tension and Sound Propagation
Classified in Physics
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Standing Waves & Speed of Sound: Experimental Analysis
Purpose of the Experiment
- To investigate the relationship between the frequency of vibration and tension in waves on a vibrating string.
- To measure the speed of sound experimentally.
Part 1: Standing Waves on a Vibrating String
Procedure for Part 1
- Vary the tension on the string by hanging different weights at its ends. Use 150g, 200g, and 250g.
- Once a standing wave is achieved, record the following information in a table: mass, weight (tension) on the string, frequency, wavelength, wave speed, and the square root of the tension.
- Relevant formulas:
λ = 2L / n
,f = 1 / T
(where T is the period),v = λf
, andv = √(T / μ)
. - Create a graph of wave speed (v) versus the square root of the tension (
√T
) using a computer. - Apply a linear fit to the graph and analyze what the slope of this line represents.
Data and Analysis (Part 1)
Experimental Data Table
MASS (kg) | TENSION (N) | f (Hz) | λ (m) | V (m/s) | √Tension (N1/2) |
---|---|---|---|---|---|
0.15 | 1.47 | 50 | 0.36 | 18 | 1.21 |
0.20 | 1.46 | 50 | 0.40 | 20 | 1.20 |
0.25 | 2.45 | 50 | 0.52 | 26 | 1.55 |
Interpretation of Results
- The linear fit of the graph (wave speed vs. square root of tension) yielded a slope (m) of 23.59. Theoretically, this slope represents the inverse of the square root of the string's linear mass density (
1/√μ
). - Conclusion on Wave Speed: As the tension in the string increases, the wave speed also increases. This relationship is clearly demonstrated by the formula
v = √(T / μ)
. - The determined value for the linear mass density (
μ
) of the string is 0.0045 kg/m.
Conclusion for Part 1
- In a string where a standing wave is produced by applying a frequency, increasing the tension leads to a noticeable increase in wave speed. This dependency is clearly shown in the wave speed formula.
- The slope of the
v
vs√T
graph represents the inverse of the square root of the linear mass density of the string (m = 1 / √μ
). Therefore, the linear mass density (μ
) can be theoretically calculated asμ = 1 / m²
. - Wave velocity of the string increases with increasing tension.
- The wavelength increases with increasing tension while maintaining a constant frequency, which implies that the wave velocity of the string increases (
v = λf
).
Part 2: Measuring the Speed of Sound
Procedure for Part 2
- Choose three different frequencies of sound waves from the wave generator to measure the speed of sound.
- For each frequency, locate two consecutive resonance points by moving the rod carrying the microphone inside the tube.
- Measure the distance between these two consecutive resonance points.
- Determine the wavelength (
λ
) by multiplying the measured distance by 2. - Calculate the value of the speed of sound (
v
) for each set frequency using the formula:v = λf
.
Data and Analysis (Part 2)
Experimental Data Table
F (Hz) | λ (m) | v = λf (m/s) |
---|---|---|
1500 | 0.23 | 345 |
1700 | 0.216 | 367.2 |
2000 | 0.18 | 360 |
Average Speed of Sound
- The average experimental speed of sound calculated is 357.4 m/s.
Conclusion for Part 2
- The average speed of sound determined in the laboratory (357.4 m/s) is a reasonably good value when compared to the accepted literature value (approximately 343 m/s at 20°C).
- While the experimental value is close, small variations in readings and measurement precision may account for the observed difference. This experiment provides a practical understanding of how these variables are calculated and measured.