1.

Derive expresion for capacitance of a parallel plate capacitor and explain the combination of capacitors in series. Or. Write expression for three capacitors in series and parallel combinations.

Answer»

Solution :Capacitors in Series. Capacitors are said to be connected in series when charge proceeds from one point to the other through a single path.
If figure `C_(1),C_(2), . . ,C_(n)` etc, are connected in series. Let CAHRGE +q be given to the left plate of `C_(1)`, a charge-q is induced on inner side of right plate of `C_(1) and +q` on the outer side of this plate. charge thus flows from left to rightl. let `V_(1),V_(2),. . .V_(n)` be the potential differences between two sides of `C_(1),C_(2), . . ,C_(n)` respectively V be the total P.D. across all the plates.

`therefore V_(1)=(q)/(C_(1)),V_(2)=(q)/(C_(2)), . . .,V_(n)=(q)/(C_(n)) and V=(q)/(C_(s))`
where `C_(s)` is the resultant CAPACITANCE of the arrangement in series.
Now `V=V_(1)+V_(2)+ . .+V_(n)`
or `(q)/(C_(s))=(q)/(C_(1))+(q)/(C_(2))+ . .+(q)/(C_(n))`
or `(1)/(C_(s))=(1)/(C_(1))+(1)/(C_(2))+ . .. +(1)/(C_(n))`
NOTE: if we have two capacitors of capacitance `C_(1) and C_(2)`, then `(1)/(C_(s))=(1)/(C_(1))+(1)/(C_(2))`
Capacitors in parallel. capacitors are said to be connected in parallel if the .positively charged. plates of all the capacitors are connected together at a point A while the .earthed. plates are connected together at another point B. the point B is also connected to earth while the source of charge is connected between the points A and B (fig).

Capacitors having capacities `C_(1),C_(2), ... ,C_(n)`, draw charges `q_(1),q_(2), . . . ,q_(n)` in ACCORDANCE with their capacities. if q is the total charge drawn from the source, then
`q=q_(1)+q_(2)+ . . .+q_(n)`. . (1)
Since all the capacitors are connected between two COMMON points A and B therefore, the potential difference across each of them is the same i.e. V. this is also the potential difference across the two terminals of the source of charge.
When `q_(1)=C_(1)V`,
`q_(2)=C_(2)V`,
. . . .
. . . ..
. . . . . . .
`q_(n)=C_(n)V`.
If `.C_(p).` is the capacity of the combination, then
`V=(q)/(C)`
or `q=CV`
Putting the values of `q,q_(1),q_(2), . ..,q_(n)` in Eq. (i),
we get
`CV=C_(1)V+C_(2)V+ . . .+C_(n)V`
or `C_(p)=C_(1)+C_(2)+ ... . +C_(n)`
Note. For three capacitors, we shall use only three capacitors `C_(1),C_(2) and C_(3)`, then
`(1)/(C_(s))=(1)/(C_(1))+(1)/(C_(2))+(1)/(C_(3))`
and `C_(p)=C_(1)+C_(2)+C_(3)`.


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