Variables are x (position), Ka (attraction constant), Kr (repulsion constant), m (mass of particle), v (velocity), a (acceleration), t (time) and initial conditions of x = xo and v = vo at t=0. From the description Fa = -Ka/(x+1) and Fr=Kr/(X-1). Note that the sum of the two forces can result in motion where a = ((Ka+Kr)x+Ka-Kr)/(x2-1)/m. Note that if Ka=Kr, a=(Ka+Kr)x/(x2-1)/m. Note further that if at t=0, x=0, a=0, vo=0 then no motion occurs. Note that in the case where vo=0 and xo=(Kr-Ka)/(Ka+Kr) at t=0, no motion occurs as the sum of the forces =0. Note that in the case where vo<>0 and/or xo<>(Kr-Ka)/(Kr+Ka), oscillary motion continues forever as this system has no losses (friction) oscillating about (Kr-Ka)/(Kr+Ka) according to the equation below:
x3/6-xlnx+x=(Ka+Kr)t2/2m+Ct+C1 C and C1 are determined by xo, vo which is found by setting a=d2x/dt2 and solving the resulting separable differential equation.