Let the mass of the bead be m and it is rotating with angular velocity ω .
Applying the conservation of energy,
⇒L=2mv2+2mrω2−mgrsinθ
Now, applying Lagrangian equation,
δtδ(δvδL)−δrδL=0
⇒δrδL=mr(δtδω)2−mgsinθ
⇒δvδL=mdtdr
⇒δtδ(δvδL)=mdt2d2r
mr˙˙=mrω2−mgsinωt
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