Along with more than new figures, the text has been reorganized and consolidated to provide a better flow and more cohesion of topics. Changes made to the book's pedagogy in the first several chapters accommodate the needs of students who have completed minimal prior study of fluid mechanics.
More than new or revised end-of-chapter problems illustrate fluid mechanical principles and draw on phenomena that can be observed in everyday life. Introduction Chapter Objectives 1.
Cartesian Tensors Chapter Objectives 2. Kinematics Chapter Objectives 3. Conservation Laws Chapter Objectives 4. Vorticity Dynamics Chapter Objectives 5. Ideal Flow Chapter Objectives 6. Gravity Waves Chapter Objectives 7. Laminar Flow Chapter Objectives 8. Computational Fluid Dynamics Chapter Objectives Instability Chapter Objectives Turbulence Chapter Objectives Geophysical Fluid Dynamics Chapter Objectives Aerodynamics Chapter Objectives Compressible Flow Chapter Objectives Introduction to Biofluid Mechanics Chapter Objectives Mathematical Tools and Resources B.
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Reviews 0. Consider the viscous flow in a channel of width 2b. Start from 1. Start from the result of Example 1. Manometers are used as pressure measuring devices. Hint: Equate the pressures at X and Y. Start by equating the pressures at X and Y. Start with the first member of 1. Starting from the property relationships 1. Equations 1. The air is compressed until its pressure rises to 8 bars. What is the initial volume? Find the final volume for both isothermal compression and isentropic compression.
Derive 1. Starting with the hydrostatic pressure law 1. Is this atmosphere stable? Consider a heat-insulated enclosure that is separated into two compartments of volumes V1 and V2, containing perfect gases with pressures and temperatures of p1, p2, and T1, T2, respectively. The compartments are separated by an impermeable membrane that conducts heat but not mass. Calculate the final steady-state temperature assuming each gas has constant specific heats.
Since no work is done and no heat is transferred out of the enclosure, the final energy Ef is the sum of the energies, E1 and E2, in the two compartments. Read Now. Go explore.
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