
$I=\frac{\varepsilon}{R_{3}+\frac{R_{1} R_{2}}{R_{1}+R_{2}}}=\frac{10}{1+\frac{(2)(2)}{2+2}}=\frac{10}{1+1}=5 A$
Also, $I_{R_{1}} R_{1}=I_{R_{2}} R_{2} \Rightarrow \frac{I_{R_{1}}}{I_{R_{2}}}=\frac{R_{2}}{R_{1}}$


statement$-1$ : The temperature dependence of resistance is usually given as $R=R_{0}(1+\alpha \Delta t)$. The resistance of a wire changes from $100\; \Omega$ to $150\; \Omega$ when its temperature is increased from $27^{\circ} C$ to $227^{\circ} C$. This implies that $\alpha=2.5$ $\times 10^{-3} /{ }^{\circ} C$
statement$-2\;: R=R_{0}(1+\alpha \Delta t)$ is valid only when the change in the temperature $\Delta T$ is small and $\Delta R=\left(R-R_{0}\right) < < R_{0}$



