1.

A particle moving in a straight line has velocity v given by v2 = α – βy2, where α and β are constant and y is its distance from a fixed point in the line. Show that the motion of the particle is S.H.M. Find its time period and amplitude.

Answer»

Given that: v2α − βy2(i)

Differentiating it with respect to time t, we have

2v\(\frac{dv}{dt}\) = −2βy\(\frac{dy}{dt}\)

or  \(\frac{dv}{dt}\) = −βy(ii)

It means acceleration

a =\(\frac{dv}{dt}\)= −βy

As a and y have –ve sign shows that acceleration is directed towards mean position, so, if the particle is left free, it will execute S.H.M.

Here ω2 = β

ω = \(\sqrt{\beta}\) 

∴ Time period, T = \(\frac{2\pi}{\omega}\) = \(\frac{2\pi}{\sqrt \beta}\) 

We know that, v = 0, when y = r from (ii)

0 = α – βr2

or r = \(\sqrt{\frac{\alpha}{\beta}}\) 

i.e., amplitude, r = \(\sqrt{\frac{\alpha}{\beta}}\)



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