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A thin metallic ring of radius R and area of cross section A carries an electric charge q that is uniformly distributed. A point charge Q is placed at the centre. The signs of charges on the ring and that of Q are same. Young's modulus for the material of the ring is Y. What is the tension developed in the ring? |
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Answer» `(qQ)/(4piepsilon_0R^2)` Charge on the segment : `q/(2pi)Deltatheta` Force between point charge Q at the centre and this segment can be written as follows :`F=1/(4piepsilon_0)((Q/(2pi)Deltatheta)Q)/R^2 =(qQ)/(8pi^2epsilon_0 R^2) Deltatheta` …(i) The components of tension T cos `(Deltatheta)/2` are cancelled from each other and T sin `(Deltatheta)/2` are added to act against electric force F. For EQUILIBRIUM : 2 T sin `(Deltatheta)/2=F` 2T sin `(Deltatheta)/2 = (qQ)/(8pi^2 epsilon_0 R^2)Deltatheta` For small values of `Deltatheta` we can approximate sin `(Deltatheta//2)` as `Deltatheta//2` , hence we GET the following :`2T (Deltatheta)/2 = (qQ)/(8pi^2 epsilon_0 R^2) Deltatheta rArr T= (qQ)/(8pi^2 epsilon_0 R^2)`
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