A uniform rope having mass m hangs vertically from rigid support. A transverse wave pulse is produced at the lower end. The frequency of wave pulse varies with x from the lower ends as
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Let a uniform rope of length L and mass m is given as shown in figure .
we cut an elementary length of dx form the lower end of rope.
so, mass of element =
Tension on elementary part = mg.dx/L
Now, formula of velocity is
Where T is tension in string e.g., T = mg.dx/L
μ is mass per unit length e.g., mass per unit length ( μ ) =( m.dx/L)/x = m.dx/Lx
∴ velocity of wave at x from the lower point =
=
but we know, velocity of wave = wavelength × frequency
so, frequency = velocity of wave/wavelength
e.g., frequency is directly proportional to velocity of wave if wavelength remains constant.
so, frequency,
hence, graph between frequency and x will be parabolic as shown in figure.
we cut an elementary length of dx form the lower end of rope.
so, mass of element =
Tension on elementary part = mg.dx/L
Now, formula of velocity is
Where T is tension in string e.g., T = mg.dx/L
μ is mass per unit length e.g., mass per unit length ( μ ) =( m.dx/L)/x = m.dx/Lx
∴ velocity of wave at x from the lower point =
=
but we know, velocity of wave = wavelength × frequency
so, frequency = velocity of wave/wavelength
e.g., frequency is directly proportional to velocity of wave if wavelength remains constant.
so, frequency,
hence, graph between frequency and x will be parabolic as shown in figure.
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