A solvable n-body problem is exhibited, which features equations of mo
tion of Newtonian type, m(j)xdouble over dot(j)=F-j, j=1,...,n, with '
'forces'' F-j that are linear and quadratic in the particle velocities
, F-j=xover dot(j){Sigma(k=1)(n)[f(jk)((1))(x)+xover dot(k)f(jk)((2))(
x)]}, and depend highly nonlinearly on the positions x(k)=x(k)(t), k=1
,...,n, of the n ''particles'' on the line. Explicit expressions of th
e functions f(jk)((i))(x), in terms of elliptic functions, are given;
they contain n+4 arbitrary constants, in addition to the n ''masses''
m(k) and to n arbitrary functions g(k)(x(k)). Special cases in which t
he elliptic functions reduce to trigonometric or rational functions ar
e of course included. The technique whereby this model has been arrive
d at entails that its initial-value problem is solvable by quadratures
[for any n and arbitrary initial data x(0) and xover dot(0)]. A discu
ssion of the actual behavior of the solution, and of special cases, is
postponed to future papers. (C) 1996 American Institute of Physics.