n the physical literature about the n-body n >= 3 sometimes the statement can be found about the impossibility of solving the n-body problem. (This seems to be similar to theorems by Abel and Galois about the impossibility of solving algebraic equations of degree higher than five by means of formulas only involving roots). However one has to be careful here. This statement is based on the method of first integrals.
The n-body problem contains 6n variables, since each point particle is represented by 3 space and 3 velocity components. First integrals (for ordinary differential equations) are functions that remain constant along any given solution of the system, the constant depending on the solution. In other words, integrals provide relations between the variables of the system, so each scalar integral would normally allow the reduction of the system's dimension by one unit. Of course, this reduction can take place only if the integral is an algebraic function not very complicated with respect to its variables. If the integral is transcendent the reduction can not be performed.
The n-body problem has 10 independent algebraic integrals
1. 3 for the centre of mass
2. 3 for the linear momentum
3. 3 for the angular momentum
4. 1 for the energy.
This allows the reduction of variables to 6n-10 . The question at that time was whether there exists other integrals besides these 10. The answer was given in 1887 by H. Bruns.
Theorem (First integrals of the n-body problem) The only linearly independent integrals of the n-body problem, which are algebraic with respect to q,p and t are the 10 described above.
(This theorem was later generalised by Poincaré). These results however do not imply that there does not exist a general solution of the n-body problem or that the perturbation series (Linstedt series) diverges. Indeed Sundman provided such a solution by means of convergent series. (See #Sundman's theorem for the 3-body problem).