Introduction to CFD on the Basis of FEM

2 控制方程 2.1 流体与固体 日常生活中我们会遇到四种物质状态——固体、液体、气体与等离子体——它们乍看之下由对约束的响应来区分:固体既保持形状又保持体积,液体保持体积但会顺应容器的形状,气体则会膨胀充满一切可用的空间。然而对于连续介质力学而言,真正具有决定性意义的区别并非几何的,而是动力学的,它关乎物质对剪切应力的响应。 流体是一种在静止时无法承受剪切应力的物质:只要施加一个剪切力,无...

applied maths

Rev Eng

But not reversed engineering

computer science

Lie Algebra

In this article, I will introduce Lie algebra, which essentially is related to the Poisson brackets we studied before. Definition Lie AlgebraFor a vector space #mjx-37e73578{ ...

maths

From the θ-Scheme to the Stokes Saddle-Point System

Why a matrix formulation in the first place We want to solve the instationary Stokes equations, but a PDE that carries a time derivative cannot be handed to a stationary linear solver directly. The...

Computational Fluid Dynamics

Poisson Brackets

The whole of mechanics can be summarized in a single bracket. — paraphrasing the spirit of Hamilton and Jacobi. In classical mechanics every observable lives on the phase space, the space of state...

classical mechanics

Intuitions and Speculations on Variational Formulation

Solving a Linear System We begin with a deceptively simple question that every undergraduate student encounters in their first linear algebra course: solving the linear system #m...

maths

Tao's Real Analysis - Peano Axiom

Kindergarten-level Maths.

maths

Quantum Dissipative System

About the Modelling of Open Systems

quantum mechanics

Properties of Arnoldi process for skew symmetric matrices

Lagerhaus

maths

NODE Übungsmenü

Lagerhaus

maths
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