Fluid MechanicsAcademic Press, 2010 M01 20 - 904 páginas Fluid mechanics, the study of how fluids behave and interact under various forces and in various applied situations—whether in the liquid or gaseous state or both—is introduced and comprehensively covered in this widely adopted text. Fluid Mechanics, Fourth Edition is the leading advanced general text on fluid mechanics.
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Página ii
... given in Appendix C.) Photograph of Ludwig Prandtl is reprinted with permission from the Annual Review of Fluid Mechanics, Vol. 19, Copyright 1987 by Annual Reviews www.AnnualReviews.org. Photograph of Geoffrey Ingram Taylor at age 69 ...
... given in Appendix C.) Photograph of Ludwig Prandtl is reprinted with permission from the Annual Review of Fluid Mechanics, Vol. 19, Copyright 1987 by Annual Reviews www.AnnualReviews.org. Photograph of Geoffrey Ingram Taylor at age 69 ...
Página xxiv
... given. After a discussion of Dynamic Similarity in Chapter 8, the study of viscous flow starts with Chapter 9, which discusses Laminar Flow. The material is standard, but the concept and analysis of similarity solutions are explained in ...
... given. After a discussion of Dynamic Similarity in Chapter 8, the study of viscous flow starts with Chapter 9, which discusses Laminar Flow. The material is standard, but the concept and analysis of similarity solutions are explained in ...
Página 6
... given by q = −k∇T, (1.2) where q is the heat flux (Jm−2 s−1), ∇T is the temperature gradient, and k is the thermal conductivity of the material. Next, consider the effect of velocity gradient du/dy (Figure 1.3). It is clear that ...
... given by q = −k∇T, (1.2) where q is the heat flux (Jm−2 s−1), ∇T is the temperature gradient, and k is the thermal conductivity of the material. Next, consider the effect of velocity gradient du/dy (Figure 1.3). It is clear that ...
Página 14
... given. For certain processes common in fluid flows, the heat exchange can be related to the specific heats. Consider a reversible process in which the work done is given by pdv, so that the first law of thermodynamics has the form of ...
... given. For certain processes common in fluid flows, the heat exchange can be related to the specific heats. Consider a reversible process in which the work done is given by pdv, so that the first law of thermodynamics has the form of ...
Página 15
... given by 2 S2−S1 = 1 dQrevT, (1.16) ∫ where the integral is taken along any reversible process between the two states. (ii) For an arbitrary process between 1 and 2, the entropy change is S2 − S1 ⩾ ∫ 2 1 dQ T (Clausius-Duhem) ...
... given by 2 S2−S1 = 1 dQrevT, (1.16) ∫ where the integral is taken along any reversible process between the two states. (ii) For an arbitrary process between 1 and 2, the entropy change is S2 − S1 ⩾ ∫ 2 1 dQ T (Clausius-Duhem) ...
Contenido
1 | |
25 | |
53 | |
81 | |
139 | |
Irrotational Flow | 165 |
Gravity Waves | 213 |
Dynamic Similarity | 279 |
Turbulence | 537 |
Geophysical Fluid Dynamics | 603 |
Aerodynamics | 679 |
Compressible Flow | 713 |
Introduction to Biofluid
Mechanics | 765 |
Some Properties of
Common Fluids | 841 |
Curvilinear Coordinates | 845 |
Founders of
Modern Fluid Dynamics | 851 |
Laminar Flow | 295 |
Boundary Layers and Related
Topics | 339 |
Computational Fluid
Dynamics | 411 |
Instability | 467 |
Visual Resources | 855 |
Index | 857 |
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approximation assumed atmosphere average becomes blood body boundary conditions boundary layer called Chapter circulation components Consider constant continuity coordinates cylinder decreases defined density depends derivative determined developed direction discussed distribution drag dynamics effects element energy equal equation example expressed field Figure finite flow fluid follows force function given gives gravity heat horizontal important increases initial instability integral irrotational length limit linear mass mean Mechanics method momentum motion moving normal Note obtain particle plane plate positive potential pressure problem propagation region relation represents requires result Reynolds number rotation scale shear shock shown shows side similarity solution speed steady streamlines stress surface surface tension temperature tensor theory tube turbulent unit variables vector velocity viscous volume vortex vorticity wall wave written zero