A particle of mass m moves in a screened coulomb potential given as (r)=-k where k and a are positive constants. The condition for the existence of circular orbits for this motion %3D r would be given by (a) = k (1+ar,)r²e -1/2-ar/2 for cisecular oY (b) ở =(1+ar, )r," e -3'2 k (c) : -(1-ar,)r,² -3/2-a/2 %3D (d) =, (1-ar,)e
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