From the real beam
$\Sigma M_D = 0$
$4R_1 = 3(500) + 200$
$R_1 = 425 \, \text{ N}$
$\Sigma M_A = 0$
$4R_2 + 200 = 1(500)$
$R_2 = 75 \, \text{ N}$
From the conjugate beam
$\Sigma M_A = 0$
$4F_2 + \frac{1}{2}(2)(1000)[1 + \frac{2}{3}(2)] = \frac{1}{2}(3)(1275)[\frac{2}{3}(3)] + \frac{1}{2}(1)(75)[3 + \frac{1}{3}(1)]$
$F_2 = 404.17 \, \text{ N}\cdot\text{m}^3$
$M_C = \frac{1}{2}(1)(75)[\frac{1}{3}(1)] - 1(F_2)$
$M_C = 12.5 - 1(404.17)$
$M_C = -391.67 \, \text{ N}\cdot\text{m}^3$
Therefore, the deflection at C is
$EI \, \delta_C = M_C$
$EI \, \delta_C = -391.67 \, \text{ N}\cdot\text{m}^3$
$EI \, \delta_C = 391.67 \, \text{ N}\cdot\text{m}^3$ downward answer