2.23 Summary of equations

  • Force eqn at a surface:
    df = dS p pressure, Sec. 2.1 df = tdS traction, Sec. 2.6 df = dS ☐☐☐ stress, Sec. 2.6 \relax \special {t4ht=
  • Rate of deformation
    D = sym(ru) Sec. 2.10 \relax \special {t4ht=

Conservation laws

Constitutive models

  • Newtonian fluid, Sec. 2.12
    ☐☐☐ = 2 devD and ☐☐☐ = ☐☐☐ pI \relax \special {t4ht=
  • Fourier’s law, Sec. 2.16
    q = rT \relax \special {t4ht=
  • Ideal gas, Sec. 2.16
    p = RT \relax \special {t4ht=
  • Specific heat capacity, Sec. 2.18
     @e- cV = @T V \relax \special {t4ht=
  • Energy-temperature relation, Sec. 2.19
     Z T e = cVdT + eref: Tref \relax \special {t4ht=

Derivatives

  • Material time derivative, Sec. 2.5
    D---- @---- Dt = @t + u r \relax \special {t4ht=
  • Divergence, Sec. 2.4 , eqn is vector, tensor
     Z -1-- r = lVim!0 V S(dS ) \relax \special {t4ht=
  • Gradient, Sec. 2.12
     Z -1-- r = liVm!0 V S(dS ) \relax \special {t4ht=
  • Laplacian, Sec. 2.14 , eqn
     1 Z r ( r ) = liVm!0 --V- (dS rn ) S \relax \special {t4ht=
Notes on CFD: General Principles - 2.23 Summary of equations