From $h = ut + \frac{1}{2}gt^{2}$ $h = 0 + \frac{1}{2} \times 9.8 \times (2)^{2} = 19.6\ m$ $\frac{\mathrm{\Delta}h}{h} = \pm 2\frac{\mathrm{\Delta}t}{t}\ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \lbrack\because a = g = constant\rbrack$ $= \pm 2\left( \frac{0.1}{2} \right) = \pm \frac{1}{10}$ $\therefore\ \mathrm{\Delta}h = \pm \frac{h}{10} = \pm \frac{19.6}{10} = \pm 1.96\ m$