Standing Wave in String and Organ Pipe - NEET Physics Chapterwise MCQs & PYQs
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NEET Standing Wave in String and Organ Pipe MCQs & PYQs
Practice NEET Standing Wave in String and Organ Pipe Questions
Question 51:
moderate
The two nearest harmonics of a tube closed at one end and open at other end are $220 \text{ Hz}$ and $260 \text{ Hz}$. What is the fundamental frequency of the system?
(2017-Delhi)
For a closed pipe, frequencies are odd multiples of fundamental $f_0$. Difference between successive harmonics is $2f_0 = 260 - 220 = 40 \text{ Hz}$. Thus, $f_0 = 20 \text{ Hz}$.
The second overtone of an open organ pipe has the same frequency as the first overtone of a closed pipe $L$ meter long. The length of the open pipe will be:
(2016-II)
2nd overtone of open pipe = $3 \times (v / 2L_{\text{open}})$. 1st overtone of closed pipe = $3 \times (v / 4L)$. Equating them: $3v / 2L_{\text{open}} = 3v / 4L \Rightarrow L_{\text{open}} = 2L$.
If we study the vibration of a pipe open at both ends, then the following statement is not true:
(2013)
In an open organ pipe, the open ends act as displacement antinodes and pressure nodes. Therefore, the pressure change is minimum (zero) at both ends, making statement 'a' incorrect.
If the tension and diameter of a sonometer wire of fundamental frequency $n$ is doubled and density is halved then its fundamental frequency will become:
(2001)
Fundamental frequency $n = \frac{1}{lD} \sqrt{\frac{T}{\pi \rho}}$. With new values $T' = 2T$, $D' = 2D$, and $\rho' = \rho/2$, the new frequency $n' = \frac{1}{2D} \sqrt{\frac{2T}{\pi (\rho/2)}} = \frac{1}{2D} \sqrt{\frac{4T}{\pi \rho}} = n$.
A string is cut into three parts, having fundamental frequencies $n_1$, $n_2$ and $n_3$ respectively. Then original fundamental frequency ‘$n$’ related by the expression as:
(2000)
For a given string, fundamental frequency $n \propto 1/l$. For the cut segments, $l = l_1 + l_2 + l_3$. Substituting $l = k/n$, we get $\frac{1}{n} = \frac{1}{n_1} + \frac{1}{n_2} + \frac{1}{n_3}$.
A standing wave having 3 nodes and 2 antinodes is formed between $1.21 \text{ \AA}$ distance then the wavelength is:
(1998)
A standing wave with 3 nodes and 2 antinodes corresponds to 2 full loops. The length of one loop is $\lambda/2$. Total distance $L = 2 \times (\lambda/2) = \lambda$. Therefore, the wavelength $\lambda = 1.21 \text{ \AA}$.
The length of a sonometer wire AB is $110 \text{ cm}$. Where should the two bridges be placed from A to divide the wire in 3 segments whose fundamental frequencies are in the ratio of $1:2:3$?
(1995)
Since frequency $f \propto 1/l$, the lengths will be in the ratio $1/1 : 1/2 : 1/3 = 6:3:2$. The sum of the ratios is 11. Lengths are $60 \text{ cm}$, $30 \text{ cm}$, and $20 \text{ cm}$. The bridges should be placed at $60 \text{ cm}$ and $60 + 30 = 90 \text{ cm}$ from A.
A stretched string resonates with tuning fork frequency $512 \text{ Hz}$ when length of the string is $0.5 \text{ m}$. The length of the string required to vibrate resonantly with a tuning fork of frequency $256 \text{ Hz}$ would be:
(1993)
By the law of length for strings, $f_1 L_1 = f_2 L_2$. Substituting the values, $512 \times 0.5 = 256 \times L_2$. Solving for $L_2$ yields $1 \text{ m}$.
A closed organ pipe (closed at one end) is excited to support the third overtone. It is found that air in the pipe has:
(1991)
For a closed pipe, the overtone sequence follows odd harmonics ($1, 3, 5, 7$). The third overtone corresponds to the 7th harmonic. It has 4 nodes and 4 antinodes (number of nodes = number of antinodes = overtone + 1).