The Lorentz gauge condition in classical electrodynamics simplifies the wave equations for scalar and vector potentials, facilitating easier solutions for charge and current distributions. This constraint, expressed as the divergence of the four-potential being zero, is crucial for maintaining Poincaré invariance in the equations of motion. While the potentials themselves lack direct physical meaning, the gauge condition aids in solving relativistic equations more efficiently. Different gauges, such as the Coulomb gauge, may be more suitable for specific problems, highlighting the importance of gauge choice in electrodynamics. Ultimately, the physical meaning of the Lorentz gauge lies in its role in simplifying complex equations while ensuring consistency with relativistic principles.