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Solve the previous problem if the pulley has a moment of inertia I about its axis and the string does not slip over it. |
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Answer» During oscilating at ny positin x below the equlibrium positon let tehh velocilty of m be v and angular velocity of the puley be OMEGA. If r is the radius of the pulley, then `v=romega` At any instant total energy =constant (For SHM) `:. 1/2 mv^2+1/2Iomega^2+1/2k[(x+delta)^2-delta^2]-mgx` =constant `rarr(1/2mv^2+(1/2)Iomega^2+(1/2)kx^2+kxd-mgx` ltbrgeconstant `rarr (1/2)mv^2+(1/2)1(v^2+r^2)+(1/2)kx^2` =constant `(delta=mg/k)` Taking derivative ofboth sides with respect of t `mv.(dv)/(dt)1/r^2v.(dv)/(dt)+kx(dx)/(dt)=0` `rarr a((m+1)/r^2)=-kx` `(:.=(dx)/(dt)and a =(dv)/(dt))` `rarr a/r=k/((m+1)/r^2)=omega^2` `rarr T=2pisqrt((m+1/r^2)/k)` |
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