The fundamental frequency of a closed organ pipe is equal to the first overtone frequency of an open organ pipe. If the length of the open pipe is , the length of the closed pipe will be:
- A
- B
- C
- D
The fundamental frequency of a closed organ pipe is equal to the first overtone frequency of an open organ pipe. If the length of the open pipe is , the length of the closed pipe will be:
Correct answer:D
Standard Method
Given: The fundamental frequency of a closed organ pipe is equal to the first overtone frequency of an open organ pipe. The length of the open pipe is .
Find: The length of the closed pipe.
For a closed organ pipe, the fundamental frequency is
For an open organ pipe, the first overtone is the second harmonic, so its frequency is
According to the question,
Therefore,
Cancelling from both sides,
So,
Substituting ,
Therefore, the length of the closed pipe is . The correct option is D.
Wavelength Relation Method
Given: The fundamental frequency of a closed organ pipe equals the first overtone frequency of an open organ pipe. Let the closed pipe length be and the open pipe length be .
Find: .
For the fundamental mode of a closed organ pipe,
For the first overtone of an open organ pipe, the pipe contains one full wavelength, so
Using and the fact that the frequencies are equal, both pipes correspond to the same wavelength relation for the stated modes. Hence,
Now substitute ,
Therefore, the length of the closed pipe is , so the correct option is D.
Using the formula for the fundamental frequency of an open pipe instead of its first overtone. This is wrong because the first overtone of an open pipe is the second harmonic, not the fundamental. Use for the first overtone of an open pipe.
Using for the closed pipe. This is wrong because the fundamental mode of a closed organ pipe has a quarter-wavelength in the pipe. Use instead.
Equating wavelengths directly without identifying the correct mode pattern. This can lead to an incorrect length relation. First write the frequency expressions for the specified modes, then equate them carefully.
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