2. Consider a rope fixed at both ends under tension so that it is horizontal (i.e. assume the rope is along x-axis, with gravity acting along z-axis). Now the right end is continually oscillated at high frequency v (say v=100 Hz) horizontally and in a direction along the rope; amplitude of oscillation is negligible. The oscillation travells along the rope and is reflected at the left end. Let the total length of rope be l, total mass be m and the acceleration due to gravity be g. After initial phase (say a mintue or so), the (BLANK-2) in nature. It results from superposition of left travelling and right travelling(BLANK-3)_waves. This resulting wave has a frequency that of oscillation frequency nu. Simple dimensional analysis indicates that the frequency of can be of the form: rope has (BLANK-1)_ wave, which is (BLANK-4) (BLANK-5). (A) BLANK-1: travelling, oscillating, stationary,regular (B) BLANK-2dransverse, longitudinal, regular, irregular (C) BLANK-3:ransverse, longitudinal regular, irregular (D) BLANK-4:equal to, half, double, independent from (E) BLANK-5: qrt (g/T, sqrt ( mg ), sqrt ( m gl ), sqrt ( 1/ g )
2. Consider a rope fixed at both ends under tension so that it is horizontal (i.e. assume the rope is along x-axis, with gravity acting along z-axis). Now the right end is continually oscillated at high frequency v (say v=100 Hz) horizontally and in a direction along the rope; amplitude of oscillation is negligible. The oscillation travells along the rope and is reflected at the left end. Let the total length of rope be l, total mass be m and the acceleration due to gravity be g. After initial phase (say a mintue or so), the (BLANK-2) in nature. It results from superposition of left travelling and right travelling(BLANK-3)_waves. This resulting wave has a frequency that of oscillation frequency nu. Simple dimensional analysis indicates that the frequency of can be of the form: rope has (BLANK-1)_ wave, which is (BLANK-4) (BLANK-5). (A) BLANK-1: travelling, oscillating, stationary,regular (B) BLANK-2dransverse, longitudinal, regular, irregular (C) BLANK-3:ransverse, longitudinal regular, irregular (D) BLANK-4:equal to, half, double, independent from (E) BLANK-5: qrt (g/T, sqrt ( mg ), sqrt ( m gl ), sqrt ( 1/ g )
Related questions
Question
100%
Kindly give the answer
Transcribed Image Text:2. Consider a rope fixed at both ends under tension so that it is horizontal (i.e. assume the rope
is along x-axis, with gravity acting along z-axis). Now the right end is continually oscillated
at high frequency v (say v=100 Hz) horizontally and in a direction along the rope; amplitude
of oscillation is negligible. The oscillation travells along the rope and is reflected at the left
end.
Let the total length of rope be l, total mass be m and the acceleration due to gravity
be
g.
After initial phase (say a mintue or so), the
(BLANK-2) in nature. It results from superposition of left travelling and right
travelling(BLANK-3)
that of oscillation frequency nu. Simple dimensional analysis indicates that the frequency of
can be of the form:
горе
has(BLANK-1)_ wave, which is
waves. This resulting wave has a frequency
(BLANK-4)
(BLANK-5)
(A) BLANK-1: travelling, oscillating, Stationary,regular
(B) BLANK-2zfransverse, longitudinal, regular, irregular
(C) BLANK-3:gránsverse, longitudinal regular, irregular
(D) BLANK-4: equal to, half, double, independent from
(E) BLANK-5: sqrt (g/T), sqrt ( mg ), sqrt ( m gl ), sqrt (1/g)
Expert Solution
This question has been solved!
Explore an expertly crafted, step-by-step solution for a thorough understanding of key concepts.
This is a popular solution!
Trending now
This is a popular solution!
Step by step
Solved in 3 steps
