To determine the condition under which the power consumed by a resistor \(R\) connected to a battery of EMF \(E\) and internal resistance \(r\) is maximized, we use the Maximum Power Transfer Theorem.
The current in the circuit is:
\[ I = \frac{E}{R + r} \]
The power consumed by the resistor \(R\) is:
\[ P = I^2 R = \frac{E^2 R}{(R + r)^2} \]
To find the maximum power, differentiate \(P\) with respect to \(R\) and equate to zero:
\[ \frac{d}{dR}\left(\frac{E^2 R}{(R + r)^2}\right) = 0 \]
Solving this condition gives:
\[ R = r \]
Hence, the power delivered to the resistor is maximum when the external resistance equals the internal resistance of the battery.
\(\boxed{R = r}\)
A point charge \(q = 1\,\mu\text{C}\) is located at a distance \(2\,\text{cm}\) from one end of a thin insulating wire of length \(10\,\text{cm}\) having a charge \(Q = 24\,\mu\text{C}\), distributed uniformly along its length, as shown in the figure. Force between \(q\) and wire is ________ N. 