在连续体中 力学质量守恒原理指出,封闭系统的质量必须随时间保持不变。对于流体,这可以用连续性方程来表示。其欧拉微分形式可以写成 [latex]frac{partial rho}{partial t} + nabla cdot (rho mathbf{u}) = 0[/latex],其中 [latex]rho[/latex] 是密度,[latex]mathbf{u}[/latex] 是速度场。

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在连续体中 力学质量守恒原理指出,封闭系统的质量必须随时间保持不变。对于流体,这可以用连续性方程来表示。其欧拉微分形式可以写成 [latex]frac{partial rho}{partial t} + nabla cdot (rho mathbf{u}) = 0[/latex],其中 [latex]rho[/latex] 是密度,[latex]mathbf{u}[/latex] 是速度场。
质量守恒是物理学中的一个基本原理,它在连续介质力学中的数学表述被称为连续性方程。该方程精确地描述了物质密度如何随空间和时间变化。方程 [latex]frac{partial rho}{partial t} + nabla cdot (rho mathbf{u}) = 0[/latex] 适用于连续介质中的每一点。项 [latex]frac{partial rho}{partial t}[/latex] 表示固定点处密度的变化率(局部项或非定常项),而项 [latex]nabla cdot (rho mathbf{u})[/latex] 是质量通量 ([latex]rho mathbf{u}[/latex]) 的散度,表示从该点周围无穷小体积流出的净质量流率。
The equation essentially states that if the density at a point is increasing, it must be because more mass is flowing into the infinitesimal volume than is flowing out, and vice versa. For a special case known as an incompressible flow, the density [latex]\rho[/latex] of a fluid parcel is assumed to be constant as it moves. In this case, the continuity equation simplifies significantly to [latex]\nabla \cdot \mathbf{u} = 0[/latex]. This simplified form is widely used in modeling liquids like water and in low-speed aerodynamics. The continuity equation is one of the core governing equations, alongside the conservation of momentum and energy, used in virtually all analyses in fluid dynamics and solid mechanics.
质量守恒
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