
The fundamental frequency of a closed end organ pipe is n. Its length is doubled and radius is halved. Its frequency will become nearly:
A. \[\dfrac{n}{2} \\ \]
B. \[\dfrac{n}{3} \\ \]
C. \[n\]
D. \[2n\]
Answer
233.1k+ views
Hint: In the closed organ pipe, the node is formed at the end. For this question we need to use the relation between the fundamental frequency, speed and wavelength with end correction. When the length or radius is changed, the speed of the sound remains unchanged.
Formula used:
\[{\nu _0} = \dfrac{v}{{4\left( {l + 0.6r} \right)}}\]
where v is the speed of sound wave, l is the length of the organ pipe and r is the radius of the organ pipe.
Complete step by step solution:
Taking end correction into consideration, the fundamental frequency of the closed end organ pipe is given as,
\[{\nu _0} = \dfrac{v}{{4\left( {l + 0.6r} \right)}}\]
where v is the speed of sound wave, l is the length of the organ pipe and r is the radius of the organ pipe.
Let the initial length of the organ pipe is \[{l_1}\] and the radius of the end is \[{r_1}\]. Then the initial fundamental frequency is,
\[{\nu _{01}} = \dfrac{v}{{4\left( {{l_1} + 0.6{r_1}} \right)}}\]
It is given that the length is doubled and the radius is halved. So, the final length of the organ pipe will be \[{l_2} = 2{l_1}\] and the final radius of the end of the pipe will be,
\[{r_2} = \dfrac{{{r_1}}}{2}\]
Then the final fundamental frequency is,
\[{\nu _{02}} = \dfrac{v}{{4\left( {{l_2} + 0.6{r_2}} \right)}}\]
Taking ratio of both the fundamental frequencies, we get
\[\dfrac{{{\nu _{01}}}}{{{\nu _{02}}}} = \dfrac{{\dfrac{v}{{4\left( {{l_1} + 0.6{r_1}} \right)}}}}{{\dfrac{v}{{4\left( {{l_2} + 0.6{r_2}} \right)}}}}\]
On simplifying, we get
\[\dfrac{{{\nu _{01}}}}{{{\nu _{02}}}} = \dfrac{{\left( {{l_2} + 0.6{r_2}} \right)}}{{\left( {{l_1} + 0.6{r_1}} \right)}} \\ \]
\[\Rightarrow \dfrac{{{\nu _{01}}}}{{{\nu _{02}}}} = \dfrac{{\left( {2{l_1} + 0.6 \times \left( {\dfrac{{{r_1}}}{2}} \right)} \right)}}{{\left( {{l_1} + 0.6{r_1}} \right)}} \\ \]
\[\Rightarrow \dfrac{{{\nu _{01}}}}{{{\nu _{02}}}} = \dfrac{{\left( {2 + 0.3\left( {\dfrac{{{r_1}}}{{{l_1}}}} \right)} \right)}}{{\left( {1 + 0.6\left( {\dfrac{{{r_1}}}{{{l_1}}}} \right)} \right)}} \\ \]
As for the organ pipe length is larger than the radius of the organ pipe,
\[\dfrac{{{\nu _{01}}}}{{{\nu _{02}}}} = 2 \\ \]
\[\therefore {\nu _{02}} = \dfrac{{{\nu _{01}}}}{2}\]
The initial fundamental frequency is given as n, so the final fundamental frequency will be,
\[{\nu _{02}} = \dfrac{n}{2}\].
Therefore, the correct option is A.
Note: If the radius of the organ pipe is comparable to the length of the organ pipe, then we can not ignore the value of the ratio of radius to the length. In that case we need to be given the relation between the radius and the length of the pipe.
Formula used:
\[{\nu _0} = \dfrac{v}{{4\left( {l + 0.6r} \right)}}\]
where v is the speed of sound wave, l is the length of the organ pipe and r is the radius of the organ pipe.
Complete step by step solution:
Taking end correction into consideration, the fundamental frequency of the closed end organ pipe is given as,
\[{\nu _0} = \dfrac{v}{{4\left( {l + 0.6r} \right)}}\]
where v is the speed of sound wave, l is the length of the organ pipe and r is the radius of the organ pipe.
Let the initial length of the organ pipe is \[{l_1}\] and the radius of the end is \[{r_1}\]. Then the initial fundamental frequency is,
\[{\nu _{01}} = \dfrac{v}{{4\left( {{l_1} + 0.6{r_1}} \right)}}\]
It is given that the length is doubled and the radius is halved. So, the final length of the organ pipe will be \[{l_2} = 2{l_1}\] and the final radius of the end of the pipe will be,
\[{r_2} = \dfrac{{{r_1}}}{2}\]
Then the final fundamental frequency is,
\[{\nu _{02}} = \dfrac{v}{{4\left( {{l_2} + 0.6{r_2}} \right)}}\]
Taking ratio of both the fundamental frequencies, we get
\[\dfrac{{{\nu _{01}}}}{{{\nu _{02}}}} = \dfrac{{\dfrac{v}{{4\left( {{l_1} + 0.6{r_1}} \right)}}}}{{\dfrac{v}{{4\left( {{l_2} + 0.6{r_2}} \right)}}}}\]
On simplifying, we get
\[\dfrac{{{\nu _{01}}}}{{{\nu _{02}}}} = \dfrac{{\left( {{l_2} + 0.6{r_2}} \right)}}{{\left( {{l_1} + 0.6{r_1}} \right)}} \\ \]
\[\Rightarrow \dfrac{{{\nu _{01}}}}{{{\nu _{02}}}} = \dfrac{{\left( {2{l_1} + 0.6 \times \left( {\dfrac{{{r_1}}}{2}} \right)} \right)}}{{\left( {{l_1} + 0.6{r_1}} \right)}} \\ \]
\[\Rightarrow \dfrac{{{\nu _{01}}}}{{{\nu _{02}}}} = \dfrac{{\left( {2 + 0.3\left( {\dfrac{{{r_1}}}{{{l_1}}}} \right)} \right)}}{{\left( {1 + 0.6\left( {\dfrac{{{r_1}}}{{{l_1}}}} \right)} \right)}} \\ \]
As for the organ pipe length is larger than the radius of the organ pipe,
\[\dfrac{{{\nu _{01}}}}{{{\nu _{02}}}} = 2 \\ \]
\[\therefore {\nu _{02}} = \dfrac{{{\nu _{01}}}}{2}\]
The initial fundamental frequency is given as n, so the final fundamental frequency will be,
\[{\nu _{02}} = \dfrac{n}{2}\].
Therefore, the correct option is A.
Note: If the radius of the organ pipe is comparable to the length of the organ pipe, then we can not ignore the value of the ratio of radius to the length. In that case we need to be given the relation between the radius and the length of the pipe.
Recently Updated Pages
JEE Main 2023 April 6 Shift 1 Question Paper with Answer Key

JEE Main 2023 April 6 Shift 2 Question Paper with Answer Key

JEE Main 2023 (January 31 Evening Shift) Question Paper with Solutions [PDF]

JEE Main 2023 January 30 Shift 2 Question Paper with Answer Key

JEE Main 2023 January 25 Shift 1 Question Paper with Answer Key

JEE Main 2023 January 24 Shift 2 Question Paper with Answer Key

Trending doubts
JEE Main 2026: Session 2 Registration Open, City Intimation Slip, Exam Dates, Syllabus & Eligibility

JEE Main 2026 Application Login: Direct Link, Registration, Form Fill, and Steps

JEE Main Marking Scheme 2026- Paper-Wise Marks Distribution and Negative Marking Details

Understanding the Angle of Deviation in a Prism

Hybridisation in Chemistry – Concept, Types & Applications

How to Convert a Galvanometer into an Ammeter or Voltmeter

Other Pages
JEE Advanced Marks vs Ranks 2025: Understanding Category-wise Qualifying Marks and Previous Year Cut-offs

Laws of Motion Class 11 Physics Chapter 4 CBSE Notes - 2025-26

Waves Class 11 Physics Chapter 14 CBSE Notes - 2025-26

Mechanical Properties of Fluids Class 11 Physics Chapter 9 CBSE Notes - 2025-26

Thermodynamics Class 11 Physics Chapter 11 CBSE Notes - 2025-26

Units And Measurements Class 11 Physics Chapter 1 CBSE Notes - 2025-26

