For continuous systems like fluids or solids, momentum conservation is expressed in a differential form. The rate of change of momentum density [latex]\rho \vec{v}[/latex] at a point is governed by the divergence of the موتر إجهاد كوشي [latex]\sigma[/latex] and body forces [latex]\vec{f}[/latex]. This is described by the Cauchy momentum equation: [latex]\frac{\partial (\rho \vec{v})}{\partial t} + \nabla \cdot (\rho \vec{v} \otimes \vec{v}) = \nabla \cdot \sigma + \vec{f}[/latex].

















