In the given figure the capacitors $C_1, C_3, C_4, C_5$ have a capacitance 4 μ μ F each if the capacitor C 2 has a capacitance 10 μ μ F, then effective capacitance between A and B will be

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Capacitance of capacitors $C_1, C_3, C_4, C_5 = 4 \mu \mathrm{F}$ each and capacitance of capacitor $c_2 = 10 \mu \mathrm{F}$ . If a battery is applied across A and B , the points b and c will be at the same potential (since $C_1 = C_4 = C_3 = C_5 = 4 \mu \mathrm{F}$ ).
Therefore no charge flows through $C_{2}$ .
We have the capacitors $c_1$ and $\mathrm{C}_5$ in series. Therefore their equivalent capacitance,
$c' = \frac{C_1 \times C_5}{C_1 + C_5} = \frac{4 \times 4}{4 + 4} = 2 \mu F$
Similarly, $C_4$ and $C_{3}$ are in series. Therefore their equivalent capacitance,
$C'' = \frac{C_3 \times C_4}{C_3 + C_4} = \frac{4 \times 4}{4 + 4} = 2 \mu \mathrm{F}$
Now $C'$ and $C''$ are in parallel. Therefore effective capacitance between A and $\mathbf{B} = C' + C'' = 2 + 2 = 4 \mu \mathrm{F}$
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