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, and v = √(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)
0.151.47500.36181.21
0.201.46500.40201.20
0.252.45500.52261.55

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 as μ = 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)
15000.23345
17000.216367.2
20000.18360

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.

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