We know that in an inertial reference frame the motion follows an equation
"ma = m\\cdot \\dfrac{d^2r}{dt^2} = F."
The constant acceleration means "\\dfrac{d^2r}{dt^2} =a" , so
"v(t) = \\dfrac{dr}{dt} = at+v_0"
and "r(t) = a\\dfrac{t^2}{2} + v_0t + r_0."
Here "v_0" is the initial velocity and "r_0" is the initial position.
The last equation can be rewritten in terms of the distance: "s(t) = a\\dfrac{t^2}{2} + v_0t" .
Here (https://thecuriousastronomer.wordpress.com/2014/11/11/newtons-equations-of-motion-revisited/) the author presents three additional equations ([3], [4], [5]), that can be obtained by rewriting the equation above in terms of the velocity after time t (v(t)). The most important of the three is [4], because it helps us to link the velocity and the distance without the time.
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