First (Fundamental); No
Length of the pipe, \(l\) = \(20 \;cm\) = \(0.2 \;m\)
Source frequency = \(n^{th}\) normal mode of frequency is \(V_n\) = \(430 \;Hz\)
Speed of sound, \(v\) = \(340 \;m/s\)
In a closed pipe, the \(n^{th}\) normal mode of frequency is given by the relation:
\(v_n\) = \((2n-1)\frac{v}{4l}\) ; \(n\) is an interger = \(0,1,2,3,4\)
\(430\) = \((2n-1)\frac{340}{4\times 0.2}\)
\(2n-1\)= \(\frac{430\times 4\times 0.2}{340}\) = \(1.01\)
\(2n\) = \(2.01\)
\(n∼1\)
Hence, the first mode of vibration frequency is resonantly excited by the given source.
In a pipe open at both ends, the nth mode of vibration frequency is given by the relation
\(v_n\) = \(\frac{nv}{2l}\)
\(n\) = \(\frac{2lV_n}{v}\)
= \(\frac{2×0.2×430}{340}\) = \(0.5\)
Since the number of the mode of vibration (\(n\)) has to be an integer, the given source does not produce a resonant vibration in an open pipe.
You have learnt that a travelling wave in one dimension is represented by a function y = f (x, t) where x and t must appear in the combination x – v t or x + v t, i.e. y = f (x ± v t). Is the converse true? Examine if the following functions for y can possibly represent a travelling wave :
(a) (x – vt )2
(b) log \([\frac{x + vt}{x_0} ] \)
(c) \(\frac{1}{(x + vt)}\)
The transverse displacement of a string (clamped at its both ends) is given by
y(x, t) = 0.06 sin \((\frac{2π}{3 }x)\) cos (120 πt)
where x and y are in m and t in s. The length of the string is 1.5 m and its mass is 3.0 ×10–2 kg.
Answer the following :
(a) Does the function represent a travelling wave or a stationary wave?
(b) Interpret the wave as a superposition of two waves travelling in opposite directions. What is the wavelength, frequency, and speed of each wave?
(c) Determine the tension in the string
Given below are some functions of x and t to represent the displacement (transverse or longitudinal) of an elastic wave. State which of these represent (i) a travelling wave, (ii) a stationary wave or (iii) none at all:
(a) y = 2 cos (3x) sin (10t)
(b) \(y=2\sqrt{x-vt}\)
(c) y = 3 sin (5x – 0.5t) + 4 cos (5x – 0.5t)
(d) y = cos x sin t + cos 2x sin 2t
Waves are a disturbance through which the energy travels from one point to another. Most acquainted are surface waves that tour on the water, but sound, mild, and the movement of subatomic particles all exhibit wavelike properties. inside the most effective waves, the disturbance oscillates periodically (see periodic movement) with a set frequency and wavelength.
Waves in which the medium moves at right angles to the direction of the wave.
Examples of transverse waves:
The high point of a transverse wave is a crest. The low part is a trough.
A longitudinal wave has the movement of the particles in the medium in the same dimension as the direction of movement of the wave.
Examples of longitudinal waves: