We consider nonlinear Klein-Gordon wave equations and illustrate that standard discretizations thereof (involving nearest neighbors) may preserve either standardly defined linear momentum or total energy but not both. This has a variety of intriguing implications for the "non-potential" discretizations that preserve only the linear momentum, such as the self-accelerating or self-decelerating motion of coherent structures such as discrete kinks in these nonlinear lattices. On the other hand, spatially discrete systems (of coupled nonlinear ordinary differential equations) are also relevant as discretizations and computational implementations of the corresponding continuum field theories that are applicable to a variety of contexts such as statistical mechanics [10], solid state physics [11], fluid mechanics [12] and particle physics [13] (see also references therein). Nonlinear Klein-Gordon type equations are a prototypical example among such wave models and their variants span a variety of applications including Josephson junctions in superconductivity, cosmic domain walls in cosmology, elementary particles in particle physics and denaturation bubbles in the DNA, among others.In this communication, we examine some of the key properties that ensue when discretizing nonlinear KleinGordon (KG) equations, using nearest neighbor approximations (which are the most standard ones implemented in the literature; see e.g., [1]). In particular, we focus on the physically relevant invariances of the continuum equation (more specifically, the conservation of the linear momentum and of the total energy of the system) and illustrate the surprising result that if we demand that the energy be conserved, then the momentum cannot be conserved, while if we demand that the momentum be conserved then the energy cannot be conserved (resulting in a so-called non-potential model [14]). Our presentation will be structured as follows. First, we will provide the general mathematical setting of KG equations and study their discretizations that conserve linear momentum and energy, comparing and constructing the properties of the two. Then, we are going to give an application of our