Organ Pipe and Column Pipe
WAVES

172557 A cylindrical tube open at both ends has a fundamental frequency ' $f$ ' in air. The tube is dipped vertically in water so that half of it is in water. The new fundamental frequency is

1 $\mathrm{f}$
2 $\frac{\mathrm{f}}{2}$
3 $2 \mathrm{f}$
4 $4 \mathrm{f}$
WAVES

172558 An open air pipe of length \(80 \mathrm{~cm}\) has the second harmonic frequency equal to the fundamental frequency of a closed organ air pipe. The length of the closed pipe is-

1 \(20 \mathrm{~cm}\)
2 \(40 \mathrm{~cm}\)
3 \(60 \mathrm{~cm}\)
4 \(10 \mathrm{~cm}\)
WAVES

172559 If $\lambda_{1}, \lambda_{2}, \lambda_{3}$ are the wavelengths of the waves giving resonance with the fundamental, first, second overtones respectively of a closed organ pipe, then the ratio $\lambda_{1}: \lambda_{2}: \lambda_{3}=$

1 $1: 3: 5$
2 $1: 2: 3$
3 $5: 3: 1$
4 $15: 5: 3$
WAVES

172560 The frequency of a tuning fork is $220 \mathrm{~Hz}$ and the velocity of sound in air is $330 \mathrm{~m} / \mathrm{s}$. When the tuning fork completes 80 vibrations, the distance travelled by the

1 $120 \mathrm{~m}$
2 $60 \mathrm{~m}$
3 $53 \mathrm{~m}$
4 $100 \mathrm{~m}$
WAVES

172561 An organ pipe with both ends open has a length $L=25 \mathrm{~cm}$. An extra hole is created at position $\frac{L}{2}$. The lowest frequency of sound produced is (assume, speed of sound $=\mathbf{3 4 0} \mathrm{m} / \mathrm{s}$ )

1 $680 \mathrm{~Hz}$
2 $340 \mathrm{~Hz}$
3 $1360 \mathrm{~Hz}$
4 $4352 \mathrm{~Hz}$
WAVES

172557 A cylindrical tube open at both ends has a fundamental frequency ' $f$ ' in air. The tube is dipped vertically in water so that half of it is in water. The new fundamental frequency is

1 $\mathrm{f}$
2 $\frac{\mathrm{f}}{2}$
3 $2 \mathrm{f}$
4 $4 \mathrm{f}$
WAVES

172558 An open air pipe of length \(80 \mathrm{~cm}\) has the second harmonic frequency equal to the fundamental frequency of a closed organ air pipe. The length of the closed pipe is-

1 \(20 \mathrm{~cm}\)
2 \(40 \mathrm{~cm}\)
3 \(60 \mathrm{~cm}\)
4 \(10 \mathrm{~cm}\)
WAVES

172559 If $\lambda_{1}, \lambda_{2}, \lambda_{3}$ are the wavelengths of the waves giving resonance with the fundamental, first, second overtones respectively of a closed organ pipe, then the ratio $\lambda_{1}: \lambda_{2}: \lambda_{3}=$

1 $1: 3: 5$
2 $1: 2: 3$
3 $5: 3: 1$
4 $15: 5: 3$
WAVES

172560 The frequency of a tuning fork is $220 \mathrm{~Hz}$ and the velocity of sound in air is $330 \mathrm{~m} / \mathrm{s}$. When the tuning fork completes 80 vibrations, the distance travelled by the

1 $120 \mathrm{~m}$
2 $60 \mathrm{~m}$
3 $53 \mathrm{~m}$
4 $100 \mathrm{~m}$
WAVES

172561 An organ pipe with both ends open has a length $L=25 \mathrm{~cm}$. An extra hole is created at position $\frac{L}{2}$. The lowest frequency of sound produced is (assume, speed of sound $=\mathbf{3 4 0} \mathrm{m} / \mathrm{s}$ )

1 $680 \mathrm{~Hz}$
2 $340 \mathrm{~Hz}$
3 $1360 \mathrm{~Hz}$
4 $4352 \mathrm{~Hz}$
WAVES

172557 A cylindrical tube open at both ends has a fundamental frequency ' $f$ ' in air. The tube is dipped vertically in water so that half of it is in water. The new fundamental frequency is

1 $\mathrm{f}$
2 $\frac{\mathrm{f}}{2}$
3 $2 \mathrm{f}$
4 $4 \mathrm{f}$
WAVES

172558 An open air pipe of length \(80 \mathrm{~cm}\) has the second harmonic frequency equal to the fundamental frequency of a closed organ air pipe. The length of the closed pipe is-

1 \(20 \mathrm{~cm}\)
2 \(40 \mathrm{~cm}\)
3 \(60 \mathrm{~cm}\)
4 \(10 \mathrm{~cm}\)
WAVES

172559 If $\lambda_{1}, \lambda_{2}, \lambda_{3}$ are the wavelengths of the waves giving resonance with the fundamental, first, second overtones respectively of a closed organ pipe, then the ratio $\lambda_{1}: \lambda_{2}: \lambda_{3}=$

1 $1: 3: 5$
2 $1: 2: 3$
3 $5: 3: 1$
4 $15: 5: 3$
WAVES

172560 The frequency of a tuning fork is $220 \mathrm{~Hz}$ and the velocity of sound in air is $330 \mathrm{~m} / \mathrm{s}$. When the tuning fork completes 80 vibrations, the distance travelled by the

1 $120 \mathrm{~m}$
2 $60 \mathrm{~m}$
3 $53 \mathrm{~m}$
4 $100 \mathrm{~m}$
WAVES

172561 An organ pipe with both ends open has a length $L=25 \mathrm{~cm}$. An extra hole is created at position $\frac{L}{2}$. The lowest frequency of sound produced is (assume, speed of sound $=\mathbf{3 4 0} \mathrm{m} / \mathrm{s}$ )

1 $680 \mathrm{~Hz}$
2 $340 \mathrm{~Hz}$
3 $1360 \mathrm{~Hz}$
4 $4352 \mathrm{~Hz}$
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WAVES

172557 A cylindrical tube open at both ends has a fundamental frequency ' $f$ ' in air. The tube is dipped vertically in water so that half of it is in water. The new fundamental frequency is

1 $\mathrm{f}$
2 $\frac{\mathrm{f}}{2}$
3 $2 \mathrm{f}$
4 $4 \mathrm{f}$
WAVES

172558 An open air pipe of length \(80 \mathrm{~cm}\) has the second harmonic frequency equal to the fundamental frequency of a closed organ air pipe. The length of the closed pipe is-

1 \(20 \mathrm{~cm}\)
2 \(40 \mathrm{~cm}\)
3 \(60 \mathrm{~cm}\)
4 \(10 \mathrm{~cm}\)
WAVES

172559 If $\lambda_{1}, \lambda_{2}, \lambda_{3}$ are the wavelengths of the waves giving resonance with the fundamental, first, second overtones respectively of a closed organ pipe, then the ratio $\lambda_{1}: \lambda_{2}: \lambda_{3}=$

1 $1: 3: 5$
2 $1: 2: 3$
3 $5: 3: 1$
4 $15: 5: 3$
WAVES

172560 The frequency of a tuning fork is $220 \mathrm{~Hz}$ and the velocity of sound in air is $330 \mathrm{~m} / \mathrm{s}$. When the tuning fork completes 80 vibrations, the distance travelled by the

1 $120 \mathrm{~m}$
2 $60 \mathrm{~m}$
3 $53 \mathrm{~m}$
4 $100 \mathrm{~m}$
WAVES

172561 An organ pipe with both ends open has a length $L=25 \mathrm{~cm}$. An extra hole is created at position $\frac{L}{2}$. The lowest frequency of sound produced is (assume, speed of sound $=\mathbf{3 4 0} \mathrm{m} / \mathrm{s}$ )

1 $680 \mathrm{~Hz}$
2 $340 \mathrm{~Hz}$
3 $1360 \mathrm{~Hz}$
4 $4352 \mathrm{~Hz}$
WAVES

172557 A cylindrical tube open at both ends has a fundamental frequency ' $f$ ' in air. The tube is dipped vertically in water so that half of it is in water. The new fundamental frequency is

1 $\mathrm{f}$
2 $\frac{\mathrm{f}}{2}$
3 $2 \mathrm{f}$
4 $4 \mathrm{f}$
WAVES

172558 An open air pipe of length \(80 \mathrm{~cm}\) has the second harmonic frequency equal to the fundamental frequency of a closed organ air pipe. The length of the closed pipe is-

1 \(20 \mathrm{~cm}\)
2 \(40 \mathrm{~cm}\)
3 \(60 \mathrm{~cm}\)
4 \(10 \mathrm{~cm}\)
WAVES

172559 If $\lambda_{1}, \lambda_{2}, \lambda_{3}$ are the wavelengths of the waves giving resonance with the fundamental, first, second overtones respectively of a closed organ pipe, then the ratio $\lambda_{1}: \lambda_{2}: \lambda_{3}=$

1 $1: 3: 5$
2 $1: 2: 3$
3 $5: 3: 1$
4 $15: 5: 3$
WAVES

172560 The frequency of a tuning fork is $220 \mathrm{~Hz}$ and the velocity of sound in air is $330 \mathrm{~m} / \mathrm{s}$. When the tuning fork completes 80 vibrations, the distance travelled by the

1 $120 \mathrm{~m}$
2 $60 \mathrm{~m}$
3 $53 \mathrm{~m}$
4 $100 \mathrm{~m}$
WAVES

172561 An organ pipe with both ends open has a length $L=25 \mathrm{~cm}$. An extra hole is created at position $\frac{L}{2}$. The lowest frequency of sound produced is (assume, speed of sound $=\mathbf{3 4 0} \mathrm{m} / \mathrm{s}$ )

1 $680 \mathrm{~Hz}$
2 $340 \mathrm{~Hz}$
3 $1360 \mathrm{~Hz}$
4 $4352 \mathrm{~Hz}$