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 xiii
... ............. 547 6. Kinetic Energy Budget of Mean Flow .............................. 554 7. Kinetic Energy Budget of Turbulent Flow .......................... 556 8. Turbulence Production and Cascade..........................
... ............. 547 6. Kinetic Energy Budget of Mean Flow .............................. 554 7. Kinetic Energy Budget of Turbulent Flow .......................... 556 8. Turbulence Production and Cascade..........................
Página 5
... mean free path of the molecules. For ordinary cases, however, this is not a great restriction, since the mean free path is usually very small. For example, the mean free path for standard atmospheric air is ≈5 × 10−8 m. In special ...
... mean free path of the molecules. For ordinary cases, however, this is not a great restriction, since the mean free path is usually very small. For example, the mean free path for standard atmospheric air is ≈5 × 10−8 m. In special ...
Página 7
... mean free path) are too small to feel the curvature of theC-profile. Second, the nonlinear terms involving higher powers of∇C do not appear. Although this is only expected for small magnitudes of ∇C, experiments show that such linear ...
... mean free path) are too small to feel the curvature of theC-profile. Second, the nonlinear terms involving higher powers of∇C do not appear. Although this is only expected for small magnitudes of ∇C, experiments show that such linear ...
Página 28
... mean xj = C1jx1 + C2j x2 + C3j x3. Likewise, any letter can also be used for the free index, as long as the same free index is used on both sides of the equation. For example, denoting the free index by i and the summed index by k ...
... mean xj = C1jx1 + C2j x2 + C3j x3. Likewise, any letter can also be used for the free index, as long as the same free index is used on both sides of the equation. For example, denoting the free index by i and the summed index by k ...
Página 44
... mean the same thing. Let Q(x) be a scalar, vector, or tensor field of any order. Gauss' theorem states that ∫ V∂Q∂xidV= ∫ AdAi Q. (2.30) The most common form of Gauss' theorem is when Q. Figure 2.10 Illustration of Gauss' theorem ...
... mean the same thing. Let Q(x) be a scalar, vector, or tensor field of any order. Gauss' theorem states that ∫ V∂Q∂xidV= ∫ AdAi Q. (2.30) The most common form of Gauss' theorem is when Q. Figure 2.10 Illustration of Gauss' theorem ...
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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Términos y frases comunes
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