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Question: A harmonic mode of a closed pipe of length 22 cm resonates when excited by a source frequency of 187...

A harmonic mode of a closed pipe of length 22 cm resonates when excited by a source frequency of 1875 Hz. Find the harmonic mode that resonates and the number of nodes present in it. (Velocity of sound in air is 330 m/s).
a) first harmonic, 1 node
b) third harmonic, 1 node
c) third harmonic, 2 nodes
d) fifth harmonic, 4 nodes
e) fifth harmonic, 3 nodes

Explanation

Solution

A harmonic mode is said to resonate with a certain source frequency. This implies that the frequency of that particular harmonic node will be equal to the source frequency. Only odd harmonics will be present in a closed pipe.

Formula Used:
The natural frequencies of a closed pipe are given by, νn=(n+12)v2l{\nu _n} = \left( {n + \dfrac{1}{2}} \right)\dfrac{v}{{2l}} where vv is the velocity of sound in air, n=012,....n = 0{\text{, }}1{\text{, }}2{\text{,}}.... is the number of the harmonics and ll is the length of the pipe.

Complete step by step answer:
Step 1: List the parameters that are known from the question.
The length of the closed pipe is l=22cml = 22{\text{cm}} .
A particular harmonic resonates with an external source of frequency νs=1875Hz{\nu _s} = 1875{\text{Hz}} .
The velocity of sound in air is v=330m/sv = 330{\text{m/s}} .
Step 2: Find the harmonic that resonates with the external source.
The natural frequencies of a closed pipe are given by, νn=(n+12)v2l{\nu _n} = \left( {n + \dfrac{1}{2}} \right)\dfrac{v}{{2l}} -------- (1)
where vv is the velocity of sound in air, n=012,....n = 0{\text{, }}1{\text{, }}2{\text{,}}.... is the number of the harmonics and ll is the length of the pipe.
The required harmonic can be found by calculating the natural frequency of each harmonic using equation (1).
Substituting for n=0n = 0 in equation (1) we get the fundamental mode as ν0=v4l{\nu _0} = \dfrac{v}{{4l}} ------- (2)
Now, substitute the values for v=330m/sv = 330{\text{m/s}} and l=22cml = 22{\text{cm}} in the above relation.
Then the fundamental frequency is ν0=3304×22×102=375Hz{\nu _0} = \dfrac{{330}}{{4 \times 22 \times {{10}^{ - 2}}}} = 375{\text{Hz}}
Now, ν0νs{\nu _0} \ne {\nu _s} and thus the first harmonic does not resonate with the source.
Substituting for n=1n = 1 in equation (1) we get the third harmonic ν3=3v4l{\nu _3} = \dfrac{{3v}}{{4l}}
Now, substitute the values for v=330m/sv = 330{\text{m/s}} and l=22cml = 22{\text{cm}} in the above relation.
Then the third harmonic is ν3=3×3304×22×102=1125Hz{\nu _3} = \dfrac{{3 \times 330}}{{4 \times 22 \times {{10}^{ - 2}}}} = 1125{\text{Hz}}
Now, ν3νs{\nu _3} \ne {\nu _s} and thus the third harmonic does not resonate with the source.
Substituting for n=2n = 2 in equation (1) we get the fifth harmonic ν5=5v4l{\nu _5} = \dfrac{{5v}}{{4l}}
Now, substitute the values for v=330m/sv = 330{\text{m/s}} and l=22cml = 22{\text{cm}} in the above relation.
Then the fifth harmonic is ν5=5×3304×22×102=1875Hz{\nu _5} = \dfrac{{5 \times 330}}{{4 \times 22 \times {{10}^{ - 2}}}} = 1875{\text{Hz}}
Now, ν5=νs=1875Hz{\nu _5} = {\nu _s} = 1875{\text{Hz}}
Thus the fifth harmonic resonates with the source.
The number of nodes present will be 3(including the one at the end).
Therefore the correct option is e.

Note: Alternate method
The third and fifth harmonics can also be expressed in terms of the first harmonic as 3ν03{\nu _0} and 5ν05{\nu _0} respectively.
Substituting the value for the fundamental frequency ν0=375Hz{\nu _0} = 375{\text{Hz}} we get, third harmonic 3ν0=3×375=1125Hz3{\nu _0} = 3 \times 375 = 1125{\text{Hz}} and fifth harmonic 5ν0=5×375=1875Hz5{\nu _0} = 5 \times 375 = 1875{\text{Hz}}
Also, when substituting the value for length in equation (1) a unit conversion from cm to m must be done.