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A capacitor is charged to potential V(1)...

A capacitor is charged to potential `V_(1)`. The power supply id disconnected and capacitor is connected in parallel to another uncharged capacitor. Calculate common potential of the combination of capacitors. Show that total energy of the combination is less than sum of energies stored in them before they are connected.

Text Solution

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Let `C_(1) and C_(2)` be the capacitances of the two capacitors and V be their common potential .
As `V = ("total Charge")/("total C apacity") = (q_(1) + q_(2))/(C_(1) + C_(2))`
`V = (C_(1) V_(1) + C_(2) V_(2))/(C_(1) + C_(2)) = (C_(1) V_(1))/(C_(1) + C_(2)) ( :' V_(2) = 0)`
Initial energy stored stored, `U_(1) = (1)/(2) C_(1) V_(1)^(2)`
Final energy after connection, `U_(2) = (1)/(2) (C_(1) + C_(2)) V^(2)`
`U_(2) = (1)/(2) (C_(1) + C_(2)) ((C_(1) V_(1))^(2))/((C_(1) + C_(2))^(2))`
`= (1)/(2) (C_(1)^(2) V_(1)^(2))/(C_(1) + C_(2)) = (U_(1) C_(1))/(C_(1) + C_(2))`
Clearly, `U_(2) lt U_(1)`.
which was to be proved.
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Knowledge Check

  • A capacitor of capacitance of 2muF is charged to a potential difference of 200V , after disconnecting from the battery, it is connected in parallel with another uncharged capacitor. The final common potential is 20V then the capacitance of second capacitor is :

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  • A 10 muF capacitor is charged to a potential difference of 50 V and is connected to another uncharged capacitor in parallel. Now the common potential difference becomes 20 volt. The capacitance of second capacitor is

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  • A capacitor of capacitance C_(1) is kept charged to a potential V. If this capacitor is then connected in parallel to an uncharged capacitor of capacitance C_(2) then fin the final potential difference across the combination.

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