We're going to use the fact that "s_1 = s_2 = 0.5~\\text{km} = s" to simplify some calculations.
Given times: "t_1 = 16~\\text{s}, t_2 = 20~\\text{s}."
Let's assume the initial position of the train as "s_0 = 0." Then, the kinematic equations for the given reference positions:
"s = v_0t_1 + \\frac{a}{2}t_1^2; \\\\\n2s = v_0(t_1+t_2) + \\frac{a}{2}(t_1+t_2)^2; \\\\\ns_{stop} = v_0t_{stop} + \\frac{a}{2}t_{stop}^2; \\\\\nv_{stop} = 0 = v_0t_{stop} + at_{stop}."
Please pay attention that here the auxiliary values "s_{stop}, t_{stop}" are counted from the initial position and time.
By excluding the values from the above system of equations,
"v_0 = s\\frac{t_2^2+2t_1t_2-t_1^2}{t_1t_2(t_1+t_2)}; \\\\\na = -2s\\frac{t_2-t_1}{t_2(t_2^2+3t_1t_2+2t_1^2)}; \\\\\nt_{stop} = -\\frac{v_0}{a}; \\\\\ns_{stop} = -\\frac{v_0^2}{2a} = \\frac{1}{4}s\\frac{(t_2^2+3t_1t_2+2t_1^2)(t_2^2+2t_1t_2-t_1^2)^2}{t_1^2t_2(t_2-t_1)(t_1+t_2)^2}."
One can see that a is negative, which indicates retardation.
The further distance (after the first two portions) the train passed will be given by
"{\\Delta}s = s_{stop} - 2s. \\\\"
By entering the numerical values into the formula, and canceling all the seconds units,
"{\\Delta}s = 0.5~\\text{km}~*~(\\frac{1}{4}\\frac{(20^2+3*16*20+2*16^2)(20^2+2*16*20-16^2)^2}{16^220(20-16)(16+20)^2} - 2) \\approx 4.42~\\text{km}."
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