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A particle of mass m is moving in a horizontal circle of radius r under a centripetal force given by `( -k/r^2)`, where k is a constant, them


Options:
A .  the total energy of the particle is `-((k)/(2r))`
B .  the kinetic energy of the particle is `(k/r)`
C .  the potential energy of the particle is `((k)/(2r))`
D .  the kinetic energy of the particle is `( - k/r)`
Answer: Option A

Centripetal force = `(mv^2)/(r) =  k/r^2`

`:.`           `mv^2 = k/r`

`:.`   Kinetic energy is `1/2 mv^2 = (k)/(2r)`

`:.`               `F = - (k)/(2r),                      F = (du)/(dr)`

At infinity , potential energy is zero

`:.`           `int_u^0    du = - int _r^oo   Fdr`

`:.`           `u = - k [ - 1/r]_r^oo = - k/r`

`:.`       Total energy = `K.E. + u`

                                 = `(k)/(2r) - k/r = - (k)/(2r)`       



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