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Let us consider a one-dimensional chain of N identical particles, each of mass m, coupled together by a flexible massless string at equal distance l. The extreme ends of the string are held fixed at position x0 = 0 and xN+1 = ( N + 1)l. The position of pth particle from left (x0 = 0) is given by xP = pl. The initial tension in the string is T. We consider the transverse oscillations of the particles about their equilibrium positions. The amplitude of oscillations is assumed to be small so that any increase in the tension of the string as the particles oscillate is neglected. Transverse oscillations of such a linear array of coupled oscillators serve as a prototype – the results obtained here are valid also for the longitudinal oscillations of an equivalent system. Suppose at any instant of time t, displacement of pth particle is yp; the displacements of adjacent particles are yp – 1 and yp + 1 as shown in fig. The pth particle is acted upon the tensions T from two segments of the string – the resultant restoring force on it along y-axis is where and are the angles as shown in fig. For small displacement, y << l, angles are so that we take the approximation. The equation of motion of the pth particle, therefore, is where we have defined Note that there are p such equations, one for each of the N particles (p = 1 to N) with y0 = 0 and yN+1 = 0. Services: - N Coupled Oscillator Homework | N Coupled Oscillator Homework Help | N Coupled Oscillator Homework Help Services | Live N Coupled Oscillator Homework Help | N Coupled Oscillator Homework Tutors | Online N Coupled Oscillator Homework Help | N Coupled Oscillator Tutors | Online N Coupled Oscillator Tutors | N Coupled Oscillator Homework Services | N Coupled Oscillator
Let us consider a one-dimensional chain of N identical particles, each of mass m, coupled together by a flexible massless string at equal distance l. The extreme ends of the string are held fixed at position x0 = 0 and xN+1 = ( N + 1)l. The position of pth particle from left (x0 = 0) is given by xP = pl. The initial tension in the string is T. We consider the transverse oscillations of the particles about their equilibrium positions. The amplitude of oscillations is assumed to be small so that any increase in the tension of the string as the particles oscillate is neglected. Transverse oscillations of such a linear array of coupled oscillators serve as a prototype – the results obtained here are valid also for the longitudinal oscillations of an equivalent system. Suppose at any instant of time t, displacement of pth particle is yp; the displacements of adjacent particles are yp – 1 and yp + 1 as shown in fig. The pth particle is acted upon the tensions T from two segments of the string – the resultant restoring force on it along y-axis is where and are the angles as shown in fig. For small displacement, y << l, angles are so that we take the approximation.
The equation of motion of the pth particle, therefore, is where we have defined Note that there are p such equations, one for each of the N particles (p = 1 to N) with y0 = 0 and yN+1 = 0.
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