$\frac{\Delta \mathrm{R}}{\mathrm{R}_0}=\alpha \Delta \mathrm{T}$
Case-I
$0{ }^{\circ} \mathrm{C} \rightarrow 100^{\circ} \mathrm{C}$
$\frac{10.2-10}{10}=\alpha(100-0)$
Case-II
$0^{\circ} \mathrm{C} \rightarrow t^{\circ} \mathrm{C}$
$\frac{10.95-10}{10}=\alpha(t-0)$
$\Rightarrow \frac{t}{100}=\frac{0.95}{0.2}=475^{\circ} \mathrm{C}$
$t=475+273=748 \mathrm{~K}$


The current in resistance $R _2$ would be zero if
$(A)$ $V_1=V_2$ and $R_1=R_2=R_3$
$(B)$ $V_1=V_2$ and $R_1=2 R_2=R_3$
$(C)$ $V_1=2 V_2$ and $2 R_1=2 R_2=R_3$
$(D)$ $2 V _1= V _2$ and $2 R _1= R _2= R _3$

