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Lab 10 - Transverse Standing Waves, Lab Reports of Physics

Purpose The purpose of this experiment is to verify the relationship among wave velocity, wavelength, and frequency of a transverse wave. A mechanical wave is the propagation through a medium of a disturbance of the medium. In this experiment, consider the string under tension and the string itself is the medium that carries the wave.

Typology: Lab Reports

2024/2025

Uploaded on 07/01/2025

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Transverse Standing Waves
Introduction
A mechanical wave is the propagation through a medium of a disturbance of the
medium. Consider the string under tension shown below. In this case, the string
itself is the medium that carries the wave.
Sketch
A continuous disturbance of the stretched string by the oscillator creates a train of
transverse waves that travels along the string. The waves are reflected at the pulley.
The leftward traveling reflected waves interfere with the rightward traveling incident
waves. The result under certain conditions is a standing wave pattern along the
length of the string.
The system resonates when the frequency of the oscillator matches a natural
frequency of the string under tension. Natural frequencies, in this case, are those
wave frequencies for which an integer number of half-wavelengths (segments) fit
along the string (which is "fixed" at both ends). Resonance corresponds to the
appearance of standing wave patterns.
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Transverse Standing Waves

Introduction A mechanical wave is the propagation through a medium of a disturbance of the medium. Consider the string under tension shown below. In this case, the string itself is the medium that carries the wave. Sketch A continuous disturbance of the stretched string by the oscillator creates a train of transverse waves that travels along the string. The waves are reflected at the pulley. The leftward traveling reflected waves interfere with the rightward traveling incident waves. The result under certain conditions is a standing wave pattern along the length of the string. The system resonates when the frequency of the oscillator matches a natural frequency of the string under tension. Natural frequencies, in this case, are those wave frequencies for which an integer number of half-wavelengths (segments) fit along the string (which is "fixed" at both ends). Resonance corresponds to the appearance of standing wave patterns.

To establish resonance, it is necessary and sufficient to adjust the length of the traveling waves until (1) where N is the number of segments in the standing wave pattern, each segment corresponding to a half-wavelength and l is the wavelength. Now, wavelength and wave frequency, f, are related by v = f l (2) where v is the velocity of propagation of the waves traveling along the string. The wave frequency is fixed - it is, in resonance, equal to the frequency of the oscillator, 120 Hz. According to Equation (2), the wavelength can by adjusted by adjusting v, which is done by changing the tension in the string. The relationship between v and FT, the tension in the string, is: (3) where μ is the linear mass density of the string. The tension in the string is created by hanging a mass, m, on the end of the string so therefore FT = mg. The purpose of this exercise is to verify Equation (3) for a string under tension. Using the value of μ given to you by your instructor, you will calculate values of v as a function of FT. Choose FT = 0, 1 N, 2 N, etc. up to 12 N. These values of v are your theoretical predictions. Compile your calculations in a table and graph v as a function of FT. Then you will experimentally determine the values of v as a function of the tension. The two sets of numbers can then be compared. Data Record the values for μ and the frequency given to you by your instructor. Measure and record the length, L, of the portion of the string free to oscillate – the distance from the oscillator to the top of the pulley.

L

N =

l

F T

v =