Fluid Dynamics

Download Advanced Transport Phenomena: Fluid Mechanics and Convective by L. Gary Leal PDF

By L. Gary Leal

Complex delivery Phenomena is perfect as a graduate textbook. It encompasses a exact dialogue of contemporary analytic equipment for the answer of fluid mechanics and warmth and mass move difficulties, concentrating on approximations in response to scaling and asymptotic equipment, starting with the derivation of uncomplicated equations and boundary stipulations and concluding with linear balance idea. additionally coated are unidirectional flows, lubrication and thin-film idea, creeping flows, boundary layer conception, and convective warmth and mass delivery at low and high Reynolds numbers. The emphasis is on uncomplicated physics, scaling and nondimensionalization, and approximations that may be used to acquire ideas which are due both to geometric simplifications, or huge or small values of dimensionless parameters. the writer emphasizes developing difficulties and extracting as a lot details as attainable wanting acquiring exact strategies of differential equations. The booklet additionally specializes in the strategies of consultant difficulties. This displays the book's aim of educating readers to consider the answer of shipping difficulties.

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Additional resources for Advanced Transport Phenomena: Fluid Mechanics and Convective Transport Processes (Cambridge Series in Chemical Engineering)

Sample text

7 We first note that every point x(t) within a material control volume is a material point whose position is prescribed by (2–9). Hence, once the (arbitrary) initial shape of the material control volume is chosen (so that all initial values of x0 are specified), a scalar quantity B associated with any point within the material control volume can be completely specified as a function of time only, that is, B[x(t), t]. Thus the usual definition of an ordinary time derivative can be applied to the left-hand side of (2–10), and we write D Dt B[x(t), t]d V ≡ lim δt→0 Vm (t) 1 δt B(t + δt) d V − B(t)d V Vm (t+δt) .

Brenner, Low Reynolds Number Hydrodynamics (Noordhoff International, Leyden, The Netherlands, 1973). 4. This is not to say that there are no unresolved issues in formulating the basic principals for a continuum description of fluid motions. Effective descriptions of the constitutive behavior of almost all complex, viscoelastic fluids are still an important fundamental research problem. The same is true of the boundary conditions at a fluid interface in the presence of surfactants, and effective methods to make the transition from a pure continuum description to one which takes account of the molecular character of the fluid in regions of very small scale is still largely an open problem.

Specifically, B changes for a moving material point both because B may vary with respect to time at each fixed point at a rate ∂ B/∂t and because the material point moves through space and B may be a function of spatial position in the direction of motion. The rate of change of B with respect to spatial position is just ∇ B. The rate at which B changes with time for a material point with velocity u is then just the projection of ∇ B onto the direction of motion multiplied by the speed, which is u · ∇ B.

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