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The ratio of the time periods of small oscillation of the insulated spring and mass system before and after charging the masses is A. `ge 1`B. ` gt 1`C. `le 1`D. `=1` |
Answer» In equilibrium of the charged small bodies `(1)/(4piepsilon_(0))(q^(2))/((l_(0)+x_(0))^(2))=kx_(0)` where `x_(0)` is the elongation in the spring in equilibrium. Let a further small elongation of `x` is given to the spring. Then net restoring force on any of the charged particle is given by, `F=-[k(x_(0)+x)-(1)/(4piepsilon_(0))(q^(2))/((l_(0)+x_(0)+x)^(2))]=-kx`. Since `x lt lt x_(0)` `rArr a=-(2k)/(m)x` As `F=mua`, where reduced mass `mu=(mxxm)/(m+m)=(m)/(2)` `rArr a=-omega^(2)x`, Hence `omega=sqrt((2k)/(m))rArrT=2pisqrt((m)/(2k))` In absence of charge, `T_(0)=2pisqrt((m)/(2k))` Therefore `(T)/(T_(0))=1` `:. (D)` |
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