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Titlebook: Computational Techniques for Fluid Dynamics 1; Fundamental and Gene Clive A. J. Fletcher Textbook 19881st edition Springer-Verlag Berlin He

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書目名稱Computational Techniques for Fluid Dynamics 1
副標(biāo)題Fundamental and Gene
編輯Clive A. J. Fletcher
視頻videohttp://file.papertrans.cn/234/233176/233176.mp4
叢書名稱Springer Series in Computational Physics
圖書封面Titlebook: Computational Techniques for Fluid Dynamics 1; Fundamental and Gene Clive A. J. Fletcher Textbook 19881st edition Springer-Verlag Berlin He
描述The purpose of this two-volume textbook is to provide students of engineer- ing, science and applied mathematics with the specific techniques, and the framework to develop skill in using them, that have proven effective in the various branches of computational fluid dynamics (CFD). Volume 1 de- scribes both fundamental and general techniques that are relevant to all branches of fluid flow. Volume 2 provides specific techniques, applicable to the different categories of engineering flow behaviour, many of which are also appropriate to convective heat transfer. An underlying theme of the text ist that the competing formulations which are suitable for computational fluid dynamics, e.g. the finite differ- ence, finite element, finite volume and spectral methods, are closely related and can be interpreted as part of a unified structure. Classroom experience indicates that this approach assists, considerably, the student in acquiring a deeper understanding of the strengths and weaknesses of the alternative computational methods. Through the provision of 24 computer programs and associated exam- ples and problems, the present text is also suitable for established research workers and prac
出版日期Textbook 19881st edition
關(guān)鍵詞Dissipation; Navier-Stokes equation; computational fluid dynamics; convection; fluid dynamics; fluid- and
版次1
doihttps://doi.org/10.1007/978-3-642-97035-1
isbn_ebook978-3-642-97035-1
copyrightSpringer-Verlag Berlin Heidelberg 1988
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Theoretical Background,the truncation errors given in Sects. 3.2 and 3.3, that more accurate solutions could be obtained on a refined grid. These aspects are considered further in Sect. 4.4. However for a given required solution accuracy it may be more economical to solve a higher-order finite difference scheme on a coars
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Weighted Residual Methods,ed analytically. For example, to obtain the solution of the diffusion equation (3.1) the following approximate solution would be assumed: .,where ..(.) are unknown coefficients and ..(.) are known analytic functions. The terms ..(.) are often referred to as trial functions and (5.1) as the trial sol
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Linear Convection-Dominated Problems,mics (Chap. 11) the fluid motion is characterised by the velocity components . in the . (Cartesian coordinates) directions. In the one-dimensional .-momentum equation. the velocity component . appears in the inertia term (.)and the viscous diffusion term .(....). The other terms are density (.),pres
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