Waves - NEET Physics Questions
Question 11: moderate

In the given progressive wave equation y = 0.5 sin (10πt – 5x); where x, y in cm and t in second. The maximum velocity of the particle is

1. 5 cm /sec
2. 5π cm /sec
3. 10 cm /sec
4. 10.5 cm /sec
View Answer
Question 12: moderate

The path difference between the two waves

\[ y_{1}= a_{1} sin \left( \omega t -\frac{2\Pi x}{\lambda} \right) \]

and

\[ y_{2}= a_{2} cos \left( \omega t -\frac{2\Pi x}{\lambda} + \varphi \right) \]

is

1. \[ \frac{\lambda}{2\Pi}\phi \]
2. \[ \frac{\lambda}{2\Pi}(\phi +\frac{\Pi}{2}) \]
3. \[ \frac{\lambda}{2\Pi}(\phi - \frac{\Pi}{2}) \]
4. \[ \frac{2\Pi}{\lambda}\phi  \]
View Answer
Question 13: moderate

The \(4^{\text{th}}\) overtone of a closed organ pipe is same as that of \(3^{\text{th}}\) overtone of an open pipe. The ratio of the length of the closed pipe to the length of the open pipe is:

1. 9 : 8
2. 7 : 9
3. 8 : 9
4. 9 : 7
View Answer

The frequency of the \(4^{\text{th}}\) overtone (9th harmonic) of a closed pipe is \(f_c = \frac{9v}{4L_c}\). The frequency of the \(3^{\text{rd}}\) overtone (4th harmonic) of an open pipe is \(f_o = \frac{4v}{2L_o} = \frac{2v}{L_o}\). Equating the two, \(\frac{9v}{4L_c} = \frac{2v}{L_o} ⇒ \frac{L_c}{L_o} = \frac{9}{8}\).

Question 14: moderate

A person hums in a well and finds strong resonance at frequencies \(180\text{ Hz}\), \(300\text{ Hz}\) and \(420\text{ Hz}\). The fundamental frequency of the well is (velocity of sound = \(335\text{ m/s}\))

1. \(180\text{ Hz}\)
2. \(100\text{ Hz}\)
3. \(60\text{ Hz}\)
4. \(120\text{ Hz}\)
View Answer

The resonance frequencies form an odd-harmonic progression for a closed-end pipe: \((2n-1)f_0\). The difference between consecutive harmonics is \(2f_0 = 300 - 180 = 120\text{ Hz}\) which gives \(f_0 = 60\text{ Hz}\).

Question 15: moderate

The \(4^{\text{th}}\) overtone of a closed organ pipe is same as that of \(3^{\text{rd}}\) overtone of an open pipe. The ratio of the length of the closed pipe to the length of the open pipe is:

1. 9 : 8
2. 7 : 9
3. 8 : 9
4. 9 : 7
View Answer

For a closed pipe, \(f_c = \frac{9v}{4L_c}\). For an open pipe, \(f_o = \frac{4v}{2L_o}\). Since \(f_c = f_o\), we have \(\frac{9v}{4L_c} = \frac{4v}{2L_o} ⇒\frac{L_c}{L_o} = \frac{9}{8}\).

Question 16: moderate

Velocity of sound in air is \(320\text{ m/s}\). If frequency of \(1^{\text{st}}\) overtone of a closed organ pipe is \(480\text{ Hz}\), then the length of the organ pipe is

1. \(100\text{ cm}\)
2. \(25\text{ cm}\)
3. \(75\text{ cm}\)
4. \(50\text{ cm}\)
View Answer

The frequency of the \(1^{\text{st}}\) overtone (third harmonic) of a closed organ pipe is given by \(f = \frac{3v}{4L}\). Given \(f = 480\text{ Hz}\) and \(v = 320\text{ m/s}\), we have \(480 = \frac{3 \times 320}{4L} ⇒ L = \frac{960}{1920} = 0.5\text{ m} = 50\text{ cm}\).

Question 17: moderate

The fifth overtone of a closed pipe is observed to be unison with third overtone of an open pipe. The ratio of the lengths of the pipes is

1. 9 : 7
2. 11 : 8
3. 12 : 9
4. 13 : 10
View Answer

For the fifth overtone of a closed pipe, \(f_c = 11 \left(\frac{v}{4L_c}\right)\). For the third overtone of an open pipe, \(f_o = 4 \left(\frac{v}{2L_o}\right)\). Equating \(f_c = f_o\) yields \(\frac{L_c}{L_o} = \frac{11}{8}\).

Question 18: moderate

The two nearest harmonics of an open organ pipe are 300 Hz and 450 Hz. If speed of sound in the pipe is 300 m/s, then length of the pipe is

1. 500 cm
2. 75 cm
3. 150 cm
4. 100 cm
View Answer

For an open organ pipe, successive harmonics differ by the fundamental frequency: \( f_1 = 450 - 300 = 150\text{ Hz} \). Using \( f_1 = \frac{v}{2L} \), we get \( 150 = \frac{300}{2L} \implies L = 1\text{ m} = 100\text{ cm} \).

Question 19: moderate

In a resonance tube at room temperature two successive resonance lengths of air column are \(25\text{ cm}\) and \(80\text{ cm}\). If the frequency of tuning fork is \(340\text{ Hz}\) then the speed of sound at that temperature is

1. 354 m/s
2. 340 m/s
3. 374 m/s
4. 350 m/s
View Answer

The speed of sound in a resonance tube is given by \(v = 2 f (l_2 - l_1)\). Substituting \(f = 340\text{ Hz}\), \(l_1 = 0.25\text{ m}\), and \(l_2 = 0.80\text{ m}\), we get \(v = 2(340)(0.80 - 0.25) = 374\text{ m/s}\).