The global rotational degrees of freedom in the Schrodinger equation for an
N-body system are completely separated from the internal ones. After remov
ing the motion of the center of mass, we find a complete set of (2l + 1) in
dependent base functions with angular momentum l. These are homogeneous pol
ynomials in the components of the coordinate vectors and the solutions of t
he Laplace equation, where the Euler angles do not appear explicitly. Any f
unction with given angular momentum and given parity in the system can be e
xpanded with respect to the base functions, where the coefficients are the
functions of the internal variables. With the right choice of the base func
tions and the internal variables, we explicitly establish the equations for
those functions. Only (3N-6) internal variables are involved both in the f
unctions and in the equations. The permutation symmetry of the wave functio
ns for identical particles is discussed.