Is it S.H.M?

A weightless rigid rod with a load at the end is hinged at point A A to the walls so that it can rotate in all directions. The rod is kept in the horizontal position by a vertical in-extensible thread of length l l , fixed at its midpoint. The load receives a momentum in the direction perpendicular to the plane of the figure (which is shown below). If the period T T of small oscillations of the system can be described as
2 π 2\pi k l g \dfrac{\sqrt{kl}}{\sqrt{g}} Find the value of k k


The answer is 2.

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3 solutions

Let L L be the length of the rod and \ell the length of the thread.

Let x x the the horizontal distance over which the load m m swings outward, and v v its horizontal speed. Let y y be the vertical distance over which it is displaced. Geometric constraint of the string requires ( 1 2 x ) 2 + ( 1 2 y ) 2 = 2 ; (\tfrac12x)^2 + (\ell - \tfrac12y)^2 = \ell^2; In small angle approximation we ignore the term of order y 2 y^2 and obtain. y x 2 4 . y \approx \frac{x^2}{4\ell}. For the energy of the system we may therefore write E = K + U = 1 2 m v 2 + m g y = 1 2 m ( v 2 + g x 2 / 2 ) = const. . E = K + U = \tfrac12mv^2 + mgy = \tfrac12m\left(v^2 + gx^2/2\ell\right) = \text{const.}. This describes harmonic motion with angular period ω = g / 2 , \omega = \sqrt{g/2\ell}, and period T = 2 π / ω = 2 π 2 g . T = 2\pi/\omega = 2\pi\frac{\sqrt{2\ell}}{\sqrt g}. Thus, k = 2 k = \boxed{2} .

why level 5 ? still by the constraints of the force by string( i don't think i need to tell even that !) , the time period exactly comes which is given in the ques , with k as 2 !:)

Rakshith Lokesh
Mar 31, 2018

consider the above system as a simple pendulum with l= root of l^2+(l/2)^2 and g effective as gcos(theta) and cos(theta) =l/ root of l^2+(l/2)^2

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