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Standing Waves in Strings and Organ Pipes, Fundamental Mode and Harmonics, Beats NEET Questions
NEET SYLLABUS
Physics - Oscillations and Waves
Oscillations and Periodic Motion, Periodic Functions,Simple Harmonic Motion and its Equation, Kinetic and potential Energies
Simple Pendulum - Derivation of Expression for its Time Period
Wave Motion
Displacement Relation for a Progressive Wave
Principle of Superposition of Waves and Reflection of Waves
Longitudinal and Transverse Waves
Speed of Travelling Wave
Standing Waves in Strings and Organ Pipes, Fundamental Mode and Harmonics, Beats
Standing Waves in Strings and Organ Pipes, Fundamental Mode and Harmonics, Beats MCQ Questions
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7.
In a standing wave, particles on OPPOSITE sides of a node are:
A.
Phase difference of Ļ/2
B.
Exactly in phase
C.
No fixed phase relationship
D.
Exactly out of phase ā they always move in opposite directions (phase difference = Ļ)
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ANSWER
:
D. Exactly out of phase ā they always move in opposite directions (phase difference = Ļ)
8.
The energy in a standing wave compared to two constituent progressive waves is:
A.
Half ā destructive interference destroys half the energy
B.
Equal ā total energy is conserved; energy is redistributed (concentrated near antinodes, zero near nodes) but total is preserved
C.
Zero ā standing waves carry no energy
D.
Double ā energy is created by constructive interference
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B. Equal ā total energy is conserved; energy is redistributed (concentrated near antinodes, zero near nodes) but total is preserved
9.
A string of length L is fixed at both ends. The boundary conditions require:
A.
No restriction on wavelength ā any wavelength is possible
B.
A node at one end and antinode at the other
C.
Nodes at both fixed ends (x = 0 and x = L), so L must equal an integer number of half-wavelengths: L = nĪ»/2
D.
Antinodes at both fixed ends
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C. Nodes at both fixed ends (x = 0 and x = L), so L must equal an integer number of half-wavelengths: L = nĪ»/2
10.
The allowed wavelengths for standing waves in a string of length L fixed at both ends are:
A.
Any wavelength Ī» such that Ī» < 2L
B.
λ_n = 2L/n for n = 1, 2, 3,⦠(wavelength must fit an integer number of half-wavelengths in L)
C.
Ī»_n = 4L/n for n = 1, 2, 3,ā¦
D.
Ī»_n = 4L/(2nā1) for n = 1, 2, 3,ā¦
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B. λ_n = 2L/n for n = 1, 2, 3,⦠(wavelength must fit an integer number of half-wavelengths in L)
11.
The allowed frequencies (normal modes) for a string of length L fixed at both ends with wave speed v are:
A.
ν_n = nv/(4L) for n = 1, 2, 3,ā¦
B.
ν_n = (2nā1)v/(4L) for n = 1, 2, 3,⦠ā only ODD harmonics
C.
ν_n = nv/(2L) for n = 1, 2, 3,⦠ā ALL harmonics (both odd and even)
D.
Only one frequency νā = v/(2L) is possible
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C. ν_n = nv/(2L) for n = 1, 2, 3,⦠ā ALL harmonics (both odd and even)
12.
The FUNDAMENTAL MODE (first harmonic) of a string fixed at both ends has:
A.
Nodes at ends and centre; wavelength Ī»ā = 2L/3
B.
One antinode at each end and node at centre; wavelength Ī»ā = L
C.
One antinode at the centre; two nodes at the ends; wavelength Ī»ā = 2L; frequency νā = v/(2L)
D.
Two antinodes and one node at the centre; wavelength Ī»ā = L
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ANSWER
:
C. One antinode at the centre; two nodes at the ends; wavelength Ī»ā = 2L; frequency νā = v/(2L)
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