Standing wave in a tube -- multiple choice question

In summary: What do they have in common? When the length of the tube is ##L##, the wavelength of the first harmonic is ##L = \frac λ 2##. The original frequency of the first harmonic is then ##f_0 = \frac v λ = \frac v {2L}##Cutting the tube in half reduces the frequency by the same factor, so ##L_{new} = \frac L 2 = \frac λ 4##Then ##f_0 = \frac v λ = \frac v {4 L_{new}}## So now you have expressed the original frequency in terms of ##L_{new}##. You
  • #1
EF17xx
36
0

Homework Statement


Screen Shot 2018-03-27 at 16.19.22.png

The correct answer according to answer sheet is answer B.

Homework Equations


λn= 2L/n (both ends open)
λn = 4L/n (one end open one end closed)
c=λf

Speed of sound does not change. as it is still in air... (correct assumption? )

The Attempt at a Solution


f1= 500Hz
L = λ/2
f= v/2L

Tube cut in half means L/2 = λ/4
L(new)= λ/4
f= v/4L(new)

Lnew = L/2

Therefore

v/4(L/2) = f
f= v/2L
therefore f is still 500Hz

I am just wondering if my reasoning and assumptions are CORRECT could someone please confirm.
 

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  • #2
Yes - half-wavelength in the open tube, quarter-wavelength in the closed tube half as long - same wavelength and frequency.
 
  • #3
EF17xx said:

Homework Statement


View attachment 222833
The correct answer according to answer sheet is answer B.

Homework Equations


λn= 2L/n (both ends open)
λn = 4L/n (one end open one end closed)
c=λf

Speed of sound does not change. as it is still in air... (correct assumption? )

The Attempt at a Solution


f1= 500Hz
L = λ/2
f= v/2L

Tube cut in half means L/2 = λ/4
L(new)= λ/4
f= v/4L(new)

Lnew = L/2

Therefore

v/4(L/2) = f
f= v/2L
therefore f is still 500Hz

I am just wondering if my reasoning and assumptions are CORRECT could someone please confirm.

It appears that you have cut the tube in half twice and somehow ended up with the same frequency at the end. I think you might start by asking yourself, "What does cutting the tube in half do to the frequency?" and "What does closing the end do to the frequency?"

Part of what makes your reasoning difficult to follow is notation like v/4(L/2) = f. Does that mean ##\frac {vL}8## or ##\frac v{2L}##? Also, you have used variables Lnew and L(new). Do they mean the same thing or something different? Using clearer notation can help you and other people understand what you wrote. Take a look at the LaTeX guide.
 
  • #4
Lnew is the length of the tube after it has been cut in half expressed in terms of the original length of the tube (L) therefore L(new) = L/2

(v) / (4(L/2))

Therefore f= v/2L
 
  • #5
EF17xx said:
Lnew is the length of the tube after it has been cut in half expressed in terms of the original length of the tube (L) therefore L(new) = L/2

(v) / (4(L/2))

Therefore f= v/2L
OK, it looks like you mean that L(new) = Lnew = L/2. So your reasoning seems to go like this:

When the length of the tube is ##L##, the wavelength of the first harmonic is ##L = \frac λ 2##. The original frequency of the first harmonic is then
##f_0 = \frac v λ = \frac v {2L}##

Cutting the tube in half reduces the frequency by the same factor, so
##L_{new} = \frac L 2 = \frac λ 4##

Then ##f_0 = \frac v λ = \frac v {4 L_{new}}##

So now you have expressed the original frequency in terms of ##L_{new}##. You have not said anything about what happens to the frequency when you reduce the length of the tube.

Now you substitute ##\frac L 2## for ##L_{new}## and get back your original equation
##f_0 = \frac v λ##

You still have not said anything about what happens to the frequency when you reduce the size of the tube, and you have not considered what happens when you close the end of the tube.

I suggest that you try this:
1) Consider what happens to the wavelength when you shorten the tube. Write an equation for the new wavelength ##λ'## in terms of ##λ##.
2) Consider what happens to the wavelength when you close the end of the tube. Write an equation for this newer wavelength ##λ''## in terms of ##λ'##.
3) Compare ##λ''## with ##λ##.
 

What is a standing wave in a tube?

A standing wave in a tube is a type of sound wave that is produced when a sound source is placed at one end of a tube and the other end is closed off. This causes the sound waves to reflect back and forth between the two ends, creating a pattern of nodes (points of no vibration) and antinodes (points of maximum vibration) within the tube.

How is a standing wave in a tube different from other types of sound waves?

A standing wave in a tube is different from other types of sound waves because it does not travel through a medium. Instead, it is confined within the tube and does not propagate outward. It also has a specific pattern of nodes and antinodes, which is not present in other types of sound waves.

What factors affect the formation of a standing wave in a tube?

The formation of a standing wave in a tube is affected by several factors, including the length of the tube, the speed of sound in the medium, and the frequency of the sound source. These factors determine the distance between nodes and antinodes in the standing wave pattern.

How can the frequency of a standing wave in a tube be changed?

The frequency of a standing wave in a tube can be changed by altering the length of the tube or by changing the frequency of the sound source. As the length of the tube or the frequency of the sound source increases, the distance between nodes and antinodes also increases, resulting in a higher frequency standing wave.

What are some real-world applications of standing waves in tubes?

Standing waves in tubes have several practical applications, such as in musical instruments like flutes and organ pipes, where they produce different pitches depending on the length of the tube. They are also used in acoustic resonators, which amplify certain frequencies and cancel out others. In addition, standing waves in tubes can be used in industrial settings for measuring the speed of sound in different mediums.

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