We report the discovery of nonlinear Weyl normal modes in two-dimensional (2D) mechanical lattices. These modes form a degenerate loop in the Brillouin zone, which is topologically protected by the Chern number of the nonlinear band structure. The projection of the Weyl loop onto the surface Brillouin zone exhibits anomalous behavior, leading to an edge-mode response on one boundary and bulk-mode behavior on the other, due to the presence of Fermi arcs on only one of the surface Brillouin zones. Our findings introduce the new concepts of nonlinear Weyl normal modes and nonlinear Weyl loop, and provide a pathway towards amplitude-controlled flexible metamaterials with topologically polarized, Weyl, and unpolarized rich phases.