Standing waves and resonance in a glass tube

In summary, the length of the air column in a closed glass tube can be varied between 0.50m and 1.50m. When a tuning fork of frequency 306 Hz is sounded at the top of the tube, resonance will occur at lengths of 1.084 m, 2.168 m, or 3.252 m. This can be determined by using the equation L = (n*v)/f, where n is the harmonic number, v is the speed of sound (330 ms-1), and f is the frequency of the standing wave.
  • #1
kapitan90
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Homework Statement


A glass tube is closed at one end. The air column it contains has a length that can be varied
between 0.50m and 1.50 m. If a tuning fork of frequency 306 Hz is sounded at the top of
the tube, at which lengths of the air column would resonance occur? (Take the speed of
sound to be 330 ms-1.)

Homework Equations


When we want to check where resonance occurs, how do we know whether the standing wave created is first, second or third harmonic?
 
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  • #2
The Attempt at a SolutionIn this case, the fundamental frequency (f1) of the standing wave is equal to the frequency of the tuning fork, which is 306 Hz. The first harmonic (f2) is twice the fundamental frequency (2f1=612Hz), the second harmonic (f3) is three times the fundamental frequency (3f1=918Hz) and the third harmonic (f4) is four times the fundamental frequency (4f1=1224Hz). To find the length of the air column at which resonance occurs, we can use the equation: L= (n*v)/f where L is the length of the air column, n is the harmonic number (1,2,3,4, etc.), v is the speed of sound (330 ms-1) and f is the frequency of the standing wave. Therefore, for the first harmonic, the length of the air column at which resonance occurs is:L1= (1*330)/306 = 1.084 m For the second harmonic, the length of the air column at which resonance occurs is:L2= (2*330)/306 = 2.168 m For the third harmonic, the length of the air column at which resonance occurs is:L3= (3*330)/306 = 3.252 m Therefore, resonance will occur when the length of the air column is 1.084 m, 2.168 m or 3.252 m.
 

1. What are standing waves and resonance in a glass tube?

Standing waves are a type of wave that occurs when two waves with the same frequency and amplitude traveling in opposite directions interfere with each other. Resonance is the phenomenon where an object vibrates at its natural frequency when exposed to an external force.

2. How do standing waves and resonance occur in a glass tube?

In a glass tube, standing waves and resonance occur when sound waves are produced at one end of the tube and travel to the other end, reflecting back and forth. The waves interfere with each other and create nodes and antinodes, resulting in standing waves. When the frequency of the sound waves matches the natural frequency of the glass tube, resonance occurs.

3. What factors affect standing waves and resonance in a glass tube?

The factors that affect standing waves and resonance in a glass tube include the length and diameter of the tube, the speed of sound in the tube, and the material and thickness of the tube’s walls. These factors determine the natural frequency of the tube and the wavelengths of the standing waves.

4. What are some real-world applications of standing waves and resonance in a glass tube?

Standing waves and resonance in a glass tube have various practical applications, such as in musical instruments like flutes and organs, where the air column inside the tube acts as a resonator. They are also used in industrial settings for ultrasonic cleaning and non-destructive testing, as well as in medical equipment like ultrasound machines.

5. How can standing waves and resonance be manipulated in a glass tube?

The natural frequency and wavelength of standing waves and resonance in a glass tube can be altered by changing the length, diameter, and material of the tube. By manipulating these factors, scientists and engineers can create specific resonant frequencies for different applications, such as in musical instruments or industrial equipment.

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