Fluid Mechanics (Book): Difference between revisions

m
no edit summary
No edit summary
mNo edit summary
Line 16: Line 16:
Because of the prevalence of computational methods, fluid mechanics is also a great entry point to the general study of numerical computing. We take this opportunity to introduce fluid mechanics and numerical ideas simultaneously while still provoking the geometric themes from earlier in our resources. Pope's text on turbulent flows indicates the three basic methods of simulation in fluid mechanics: DNS (Direct Numerical Simulation), LES (Large Eddy Simulation), and RANS (Reynolds-Averaged-Navier-Stokes) and equally importantly the statistical interpretation of turbulence. While we expect turbulence to be technically deterministic, due to the very fine detail we may treat it like noise and calculate the frequencies involved (power spectrum) which as it sounds is the Fourier decomposition used in electromagnetism and quantum mechanics. For LES, it makes simulation easier than DNS by being able to ignore the high frequency/small spatial detail part of the spectrum and still captures the coarser features of the flow. Aside from mathematics or numerical methods, some important applications of fluid mechanics are also provided - cloud physics, plasma. Our guide to numerical thinking should also be sufficient to implement these applications. Maybe you will help predict the weather or even control it, not to mention applications to nuclear fusion! Plasma applications are largely fluid-mechanical, but will be contained under Landau 10 as that is where Landau's work on plasmas is discussed.
Because of the prevalence of computational methods, fluid mechanics is also a great entry point to the general study of numerical computing. We take this opportunity to introduce fluid mechanics and numerical ideas simultaneously while still provoking the geometric themes from earlier in our resources. Pope's text on turbulent flows indicates the three basic methods of simulation in fluid mechanics: DNS (Direct Numerical Simulation), LES (Large Eddy Simulation), and RANS (Reynolds-Averaged-Navier-Stokes) and equally importantly the statistical interpretation of turbulence. While we expect turbulence to be technically deterministic, due to the very fine detail we may treat it like noise and calculate the frequencies involved (power spectrum) which as it sounds is the Fourier decomposition used in electromagnetism and quantum mechanics. For LES, it makes simulation easier than DNS by being able to ignore the high frequency/small spatial detail part of the spectrum and still captures the coarser features of the flow. Aside from mathematics or numerical methods, some important applications of fluid mechanics are also provided - cloud physics, plasma. Our guide to numerical thinking should also be sufficient to implement these applications. Maybe you will help predict the weather or even control it, not to mention applications to nuclear fusion! Plasma applications are largely fluid-mechanical, but will be contained under Landau 10 as that is where Landau's work on plasmas is discussed.


While more complex methods like mesh or multi/adaptive-grid can be used to approximately solve these PDEs, it is instructive to learn about DNS on a lattice - the step size needed to capture the features of the flow accurately can be determined algebraically from the Reynolds number. Inspecting the process of numerically solving PDEs on a lattice, one finds that the problem resolves (in the implicit step case) to solving linear systems - this is typically why linear algebra is introduced in an engineering context. This gets to the essential mathematical features of numerical methods. Some introductory course notes on numerical analysis by Olver are [https://www-users.cse.umn.edu/~olver/num.html here], and a related book of his [https://www.google.com/books/edition/Applied_Linear_Algebra/LfJdDwAAQBAJ?hl=en&gbpv=1 here]. Solving linear systems efficiently means, for instance, looking for efficient ways to multiply matrices (e.g. Strassen's algorithm) and to interpolate data. Hoping to capture the basics needed and some of the cutting edge here, Landsberg's book explain how one can think of the matrix multiplication function as a tensor itself, and do algebraic geometry in the space of tensors to better understand the complexity of the algorithms involved and to find efficient solutions. A later related book of his on tensor geometry that mentions Hackbusch's motivation is grouped with condensed matter physics. Hackbusch's books work from a similar ground of tensor geometry but focuses on the numerical PDE application. His later books develop the cutting edge of the aforementioned multigrid methods. And since interpolation/galerkin/finite element methods involve inherently functional-analytical ideas, quantum mechanics background helps in thinking about the function spaces involved but is not strictly necessary.
While more complex methods like mesh or multi/adaptive-grid can be used to approximately solve these PDEs, it is instructive to learn about DNS on a lattice - the step size needed to capture the features of the flow accurately can be determined algebraically from the Reynolds number. Inspecting the process of numerically solving PDEs on a lattice, one finds that the problem resolves (in the implicit step case) to solving linear systems - this is typically why linear algebra is introduced in an engineering context. This gets to the essential mathematical features of numerical methods. Some introductory course notes on numerical analysis by Olver are [https://www-users.cse.umn.edu/~olver/num.html here], and a related book of his [https://www.google.com/books/edition/Applied_Linear_Algebra/LfJdDwAAQBAJ?hl=en&gbpv=1 here]. Solving linear systems efficiently means, for instance, looking for efficient ways to multiply matrices (e.g. Strassen's algorithm) and to interpolate data. Hoping to capture the basics needed and some of the cutting edge here, Landsberg's book explains how one can think of the matrix multiplication function as a tensor itself, and do algebraic geometry in the space of tensors to better understand the complexity of the algorithms involved and to find efficient solutions. A later related book of his on tensor geometry that mentions Hackbusch's motivation is grouped with condensed matter physics. Hackbusch's books work from a similar ground of tensor geometry but focuses on the numerical PDE application. His later books develop the cutting edge of the aforementioned multigrid methods. And since interpolation/galerkin/finite element methods involve inherently functional-analytical ideas, quantum mechanics background helps in thinking about the function spaces involved but is not strictly necessary.


Numerical methods are still young, Monte Carlo was developed during the Manhattan Project, and software tools stick to rudimentary approaches to rely on high performance computing. As with our previous philosophy, the future is in geometric physics - numerical methods which preserve differential-geometric structures. Starting from the previous numerical and specifically finite-element-mesh ideas, we present some resources for the very active area of differential-form-based interpolation and symplectic integration methods. Their importance cannot be understated, the implementation of conservation laws at the numerical level makes numerical methods not only produce apparently more physically accurate results, but also be more useful theoretically in the description of physics.
Numerical methods are still young, Monte Carlo was developed during the Manhattan Project, and software tools stick to rudimentary approaches to rely on high performance computing. As with our previous philosophy, the future is in geometric physics - numerical methods which preserve differential-geometric structures. Starting from the previous numerical and specifically finite-element-mesh ideas, we present some resources for the very active area of differential-form-based interpolation and symplectic integration methods. Their importance cannot be understated, the implementation of conservation laws at the numerical level makes numerical methods not only produce apparently more physically accurate results, but also be more useful theoretically in the description of physics.