The work performed by the retarding force on the block within the rough area is calculated as:\[W = \int_{x_i}^{x_f} F_r dx = \int_{0.1}^{1.9} (-kx) dx\]With \( k = 10 \) N/m, the equation becomes:\[W = \int_{0.1}^{1.9} (-10x) dx = -10 \left[ \frac{x^2}{2} \right]_{0.1}^{1.9}\]Evaluating the integral yields:\[W = -5 \left[ (1.9)^2 - (0.1)^2 \right] = -5 [3.61 - 0.01] = -5 [3.60] = -18 \, \text{J}\]The work-energy theorem states that the net work done on an object equals its change in kinetic energy:\[W_{net} = \Delta KE = KE_f - KE_i = \frac{1}{2} m v_f^2 - \frac{1}{2} m v_i^2\]Given a mass \( m = 1 \) kg and an initial speed \( v_i = 10 \) m/s, and considering the work done by the retarding force as the net work:\[-18 = \frac{1}{2} (1) v_f^2 - \frac{1}{2} (1) (10)^2\]Simplifying the equation:\[-18 = \frac{1}{2} v_f^2 - \frac{1}{2} (100)\]\[-18 = \frac{1}{2} v_f^2 - 50\]Rearranging to solve for \( v_f^2 \):\[\frac{1}{2} v_f^2 = 50 - 18 = 32\]\[v_f^2 = 64\]Therefore, the final speed is:\[v_f = \sqrt{64} = 8 \, \text{m/s}\]The block's final speed upon exiting the rough region is 8 m/s.