Investigating Resonance and Wavelength in a Vibrating String Experiment, Lecture notes of Particle Physics

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.

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Brooklyn College 1
STANDING WAVES ON A STRING
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
In any wave motion, wavelength (
) and frequency (f) of the wave is related by
f
v
(1)
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
T
v
(2)
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:
2
n
L
(3)
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.
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STANDING WAVES ON A STRING

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

In any wave motion, wavelength ( ) and frequency ( f ) of the wave is related by

f

v

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

v ^ T

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:

n 

L  (3)

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

  1. Set the distance between the vibrating bar and the pulley to about 1 meter and clamp it loosely.
  2. Tie one end of the heavier string to the vibrating bar and the other end to the weight hanger. Add slotted weights to give a total hanging mass of 600 grams.
  3. Plug in the vibrator, loosen the clamp, and slowly slide the vibrator along the table (i.e., vary L ) until a set of standing waves is formed. Note any change in the sound from the string as you near resonance. When a clear resonance pattern is observed with stable nodes and antinodes, clamp the vibrator to the table.
  4. Count the number of nodes and draw the wave pattern (not including the ends of the string at the pulley and vibrating bar. They are not truly nodes) that appear along the string. Measure the distance between the first and last of these nodes. Divide this distance by the number of half- wavelengths observed to get your best estimate for D. Estimate the uncertainty in D.
  5. In order to check whether your measurement of D is independent of the number of standing waves on the string, loosen the clamp and slide the vibrator until another resonant length is found. Repeat Step 4. Do you get the same D , within your estimated uncertainty?
  6. Change the hanging weight, and repeat Steps 3 and 4. (You do not have to repeat Step 5 for each weight.) Use total masses ( M ) of 200 grams, 400 grams, 800 grams 1000 grams, and 1200 grams for this string and find D for each load.
  7. Unplug the vibrator, untie the heavier string, and weigh it on the balance. Then measure its length. Pay close attention to evaluating the uncertainty in these measurements. Compute μ from your measurements, and estimate its uncertainty.

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)

D (cm) meas = 2D  calc

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)

D (cm) meas = 2D calc