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A laboratory experiment conducted at brooklyn college to investigate resonance conditions and the dependence of wavelength on tension and linear mass density of a vibrating string. The theory behind standing waves on a string is explained, along with the procedure for setting up the apparatus and making observations. Students are asked to make resonances of different modes by adjusting the length and tension of two strings and measure the distance between nodes and antinodes to determine the wavelength.
Typology: Lecture notes
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Purpose
a. To investigate resonance conditions for a vibrating string. b. To study dependence of wavelength on the tension and linear mass density of the string.
Theory
where v is the velocity of the propagation of the wave. The velocity, v of a wave on a stretched string depends on the tension, T, in the string and the mass per unit of the string ,, and is given by
If a stretched and vibrating string is clamped at both ends, like a guitar string, the wave reflects from the fixed ends and waves travel in both directions. The incident and reflected waves will combine according to superposition principle. When a proper amount of tension is applied along the string for a given length of the string, the waves travelling in opposite directions resonate and form a standing wave. Figure 1 shows two of the many possible modes of making standing waves on a string. In the figures, N indicates the locations the string is stationary, called nodes, and A indicates the locations the string is vibrating with maximum amplitude, called antinodes. Standing waves are discrete phenomena, meaning that they only occur at specific values of wavelength.
The distance from a node to an adjacent node (or from an antinode to adjacent antinode) is half of the wavelength. In order to form a standing wave a resonance condition has to be satisfied:
where L is the length of the string and n is an integer. For the standing wave in Figure 1a, the value of n is 1, and the wave pattern is called the fundamental or first harmonic. For Figure 1b, the value of n is 3, and the wave pattern is called the third harmonic.
In this experiment you will use a vibrator of constant frequency to vibrate the string. Your investigations involve making resonances of different modes by adjusting the length and tension in two different strings.
Apparatus
Two strings (about 2 m length), 120-cycle electric vibrator and C-clamp; weight hanger, one 50 gram slotted weight, twelve 100 gram slotted weights, hand stroboscope, and triple-beam balance.
Figure 1a. A first harmonic standing wave. harmonic.
Figure 1b. A third harmonic standing wave.
Description of Apparatus
You will use a vibrator that consists of an electromagnet which causes a steel bar to vibrate at a fixed frequency of 120 Hz as shown in Figure 2a. The vibrator is clamped on a lab table. One end of the string is tied to the vibrating bar. The string is then passed over a light pulley wheel, and a weight hanger is attached to the other end. The weight on the hanger provides the tension in the string. You can slide the vibrator along the table, thus varying the length ( L ) of vibrating string. You will change the weight to change the tension in the string. A typical set up of this lab is shown in Figure 2b.
When L is adjusted to approximately equal to a whole number of half-wavelengths, a resonant condition is set up in the string, and standing waves will be observed as shown in Figure 2. The distance D between adjacent nodes of the standing waves can be observed and measured, and is equal to one-half of the wavelength, λ.
2
D
Procedure
Figure 2a. Vibrator vibrating a string.
Vibrator
Vibrating string Clamp
Figure 2b. Experimental set up.
Data Sheet
Date experiment performed:
Name of group members:
a. For heavier string
Mass of heavier string: Length of the heavier string:
Table 1.
Trial Draw Standing wave pattern below
Hanging mass, M (kg)
Number of nodes
Length (cm)
b. For lighter string
Mass of heavier string: Length of the heavier string:
Table 2.
Trial Draw Standing wave pattern below
Hanging mass, M (kg)
Number of nodes
Length (cm)