Let us write equations of motion of the car, assuming it moves with constant retardation (and hence constant braking force):
"S(t) = v_0 t - \\frac{a t^2}{2}", "v(t) = v_0 - a t".
At the moment of time, when the car stops completely "v(t') = v_0 - a t' = 0", from where the time it takes to completely stop is "t' = \\frac{v_0}{a}".
The horizontal distance covered in time "t'" is given ("L = 800m)", therefore: "L = S(t') = \\frac{v_0^2}{a} - \\frac{v_0^2}{2 a} = \\frac{v_0^2}{2 a}", from where the acceleration is "a = \\frac{v_0^2}{2 L}", and from second Newton's law "a = \\frac{F}{m}", so "\\frac{v_0^2}{2 L} = \\frac{F}{m}", from where the force is "F = \\frac{m v_0^2}{2 L} = 1600 N".
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