Fluid Mechanics -  Ira M. Cohen,  David R Dowling,  Pijush K. Kundu

Fluid Mechanics (eBook)

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2015 | 6. Auflage
928 Seiten
Elsevier Science (Verlag)
978-0-12-407151-3 (ISBN)
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The classic textbook on fluid mechanics is revised and updated by Dr. David Dowling to better illustrate this important subject for modern students. With topics and concepts presented in a clear and accessible way, Fluid Mechanics guides students from the fundamentals to the analysis and application of fluid mechanics, including compressible flow and such diverse applications as aerodynamics and geophysical fluid mechanics. Its broad and deep coverage is ideal for both a first or second course in fluid dynamics at the graduate or advanced undergraduate level, and is well-suited to the needs of modern scientists, engineers, mathematicians, and others seeking fluid mechanics knowledge.

NEW TO THE SIXTH EDITION

  • Over 100 new examples designed to illustrate the application of the various concepts and equations featured in the text.
  • A completely new chapter on computational fluid dynamics (CFD) authored by Prof. Gretar Tryggvason of the University of Notre Dame. This new CFD chapter includes sample MatlabTM codes and 20 exercises.
  • New material on elementary kinetic theory, non-Newtonian constitutive relationships, internal and external rough-wall turbulent flows, Reynolds-stress closure models, acoustic source terms, and unsteady one-dimensional gas dynamics.
  • Plus 110 new exercises and nearly 100 new figures.


While in college, David R. Dowling held summer positions at Hughes Aircraft Co. and the Los Angeles Air Force Station. He completed his doctorate in 1988 at Graduate Aeronautical Laboratories of the California Institute of Technology and moved north to Seattle to accomodate his wife's career in medicine. While there, he worked for a year in the laser technology group at Boeing Aerospace, and then for almost three years as a post-doc at the Applied Physics Laboratory of the University of Washington. In 1992, he accepted a faculty position at the University of Michigan. Prof. Dowling is currently conducting research in acoustics and fluid mechanics. He is a fellow of the Acoustical Society of America, a member of the American Society of Mechanical Engineers, and a member of the American Physical Society. He is a US citizen.
Positions at the University of Michigan :
Professor, Sept 2005 to Present
Associate Professor, Sept 1999 thru August 2005
Assistant Professor, Sept 1992 thru August 1999
Visiting Assistant Professor, July 1992 thru August 1992
The classic textbook on fluid mechanics is revised and updated by Dr. David Dowling to better illustrate this important subject for modern students. With topics and concepts presented in a clear and accessible way, Fluid Mechanics guides students from the fundamentals to the analysis and application of fluid mechanics, including compressible flow and such diverse applications as aerodynamics and geophysical fluid mechanics. Its broad and deep coverage is ideal for both a first or second course in fluid dynamics at the graduate or advanced undergraduate level, and is well-suited to the needs of modern scientists, engineers, mathematicians, and others seeking fluid mechanics knowledge. Over 100 new examples designed to illustrate the application of the various concepts and equations featured in the text A completely new chapter on computational fluid dynamics (CFD) authored by Prof. Gretar Tryggvason of the University of Notre Dame. This new CFD chapter includes sample MatlabTM codes and 20 exercises New material on elementary kinetic theory, non-Newtonian constitutive relationships, internal and external rough-wall turbulent flows, Reynolds-stress closure models, acoustic source terms, and unsteady one-dimensional gas dynamics Plus 110 new exercises and nearly 100 new figures

Nomenclature


Notation (Relevant Equation Numbers Appear in Parentheses)


¯= principle-axis version of f, background or quiescent-fluid value of f, or average or ensemble average of f , Darcy friction factor (12.101, 12.102)
ˆ = complex amplitude of f
˜ = full field value of f
= derivative of f with respect to its argument, or perturbation of f from its reference state
= complex conjugate of f, or the value of f at the sonic condition
f+ = the dimensionless, law-of-the-wall value of f
= ∂f/∂ξ (6.105)
fcr = critical value of f
fav = average value of f
fCL = centerline value of f
fj = the jth component of the vector f, f at location j (6.14)
)in, in = f at time n at horizontal x-location j (6.13)
fij = the i-j component of the second order tensor f
i,jn, )i,jn = f at time n at horizontal x-location i and vertical y-location j (6.52, Fig. 6.10)
fR = rough-wall value of f
fS = smooth-wall value of f
f0 = reference, surface, or stagnation value of f
f∞ = reference value of f or value of f far away from the point of interest
Δf = change in f

Symbols (Relevant Equation Numbers Appear in Parentheses)


α = contact angle (Fig. 1.8), thermal expansion coefficient (1.26), angle of rotation, iteration number (6.57), angle of attack (Fig. 14.6)
a = triangular area, cylinder radius, sphere radius, amplitude
a = generic vector, Lagrangian acceleration (3.1)
A = generic second-order (or higher) tensor
A, A = a constant, an amplitude, area, surface, surface of a material volume, planform area of a wing
A∗ = control surface, sonic throat area
Ao = Avogadro’s number
A0 = reference area
Aij = representative second-order tensor
β = angle of rotation, coefficient of density change due to salinity or other constituent, convergence acceleration parameter (6.57), variation of the Coriolis frequency with latitude (13.10), camber parameter (Fig. 14.13)
b = generic vector, control surface velocity (Fig. 3.20)
B, B = a constant, Bernoulli function (4.70), log-law intercept parameter (12.88)
B, Bij = generic second-order (or higher) tensor
Bo = Bond number (4.118)
c = speed of sound (1.25, 15.1h), phase speed (8.4), chord length (14.2Figs. 14.2, 14.6)
c = phase velocity vector (8.8)
cg, cg = group velocity magnitude (8.67) and vector (8.141)
χ = scalar stream function (Fig. 4.1)
°C = degrees centigrade
C = a generic constant, hypotenuse length, closed contour
Ca = Capillary number (4.119)
Cf = skin friction coefficient (10.15, 10.32)
Cp = pressure (coefficient) (4.106, 7.32)
cp = specific heat capacity at constant pressure (1.20)
CD = coefficient of drag (4.107, 10.33)
CL = coefficient of lift (4.108)
cv = specific heat capacity at constant volume (1.21)
Cij = matrix of direction cosines between original and rotated coordinate system axes (2.5)
C± = Characteristic curves along which the I± invariants are constant (15.57)
d = diameter, distance, fluid layer depth
d = dipole strength vector (7.28), displacement vector
δ = Dirac delta function (B.4.1), similarity-variable length scale (9.32), boundary-layer thickness, generic length scale, small increment, flow deflection angle (15.64)
¯ = average boundary-layer thickness
δ∗ = boundary-layer displacement thickness (10.16)
δij = Kronecker delta function (2.16)
δ99 = 99% layer thickness
D = distance, drag force, diffusion coefficient (6.10)
D = drag force vector (Example 14.1)
Di = lift-induced drag (14.15)
D/Dt = material derivative (3.4), (3.5), or (B.1.4)
DT = turbulent diffusivity of particles (12.156)
= generalized field derivative (2.31)
ε = roughness height, kinetic energy dissipation rate (4.58), a small distance, fineness ratio h/L (9.14), downwash angle (14.14)
¯ = average dissipation rate of the turbulent kinetic energy (12.47)
¯T = average dissipation rate of the variance of temperature fluctuations (12.141)
εijk = alternating tensor (2.18)
e = internal energy per unit mass (1.16)
ei = unit vector in the i-direction (2.1)
¯ = average kinetic energy of turbulent fluctuations (12.47)
Ec = Eckert number (4.115)
Ek = kinetic energy per unit horizontal area (8.39)
Ep = potential energy per unit horizontal area (8.41)
E = numerical error (6.21), average energy per unit horizontal area (13.18)
¯ = kinetic energy of the average flow (12.46)
EF = time average energy flux per unit length of wave crest (8.43)
f = generic function, Maxwell distribution function (1.1) and (1.4), Helmholtz free energy per unit mass, longitudinal correlation coefficient (12.38), Coriolis frequency (13.6), dimensionless friction parameter (15.45)
¯ = Darcy friction factor (12.101, 12.102)
fi = unsteady body force distribution (15.5)
ϕ = velocity potential (7.10), an angle
f = surface force vector per unit area (2.154.13)
F = force magnitude, generic flow field property, generic flux, generic or profile function
Ff = perimeter friction force (15.25)
F = force vector, average wave energy flux vector (8.157)
Φ = body force potential (4.18), undetermined spectrum function (12.53)
FD, ¯D = drag force (4.107), average drag force
FL = lift force (4.108)
Fr = Froude number (4.104)
γ = ratio of specific heats (1.30), velocity gradient, vortex sheet strength,...

Erscheint lt. Verlag 8.6.2015
Sprache englisch
Themenwelt Naturwissenschaften Physik / Astronomie Strömungsmechanik
Technik Maschinenbau
ISBN-10 0-12-407151-1 / 0124071511
ISBN-13 978-0-12-407151-3 / 9780124071513
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