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Fysische transportverschijnselen I125practicum

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In a porous solid - due to. Velocity distribution inside a pore; ... C voor formule. 12/6/09. Guido Wyseure. 11. Class A pan. 12/6/09. Guido Wyseure. 12 ... – PowerPoint PPT presentation

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Title: Fysische transportverschijnselen I125practicum


1
Fysische transport-verschijnselenI125-practicum
  • Massatransport
  • stationair

Acad. Jaar 2003-2004 Eerste ingenieursjaar
Bio-ingenieur
2
Dispersion (in feite verzamel-term)
  • Spreading from higher to lower concentration
  • In a fluid - due to turbulence
  • In a porous solid - due to
  • Velocity distribution inside a pore variation in
    pore sizes and Tortuosity and branching
  • Similar to diffusion treated with analogous to
    formulas
  • Dispersion much faster than molecular diffusion

m2 s
3
Mechanische dispersie
Microscopische snelheid
Zeer traag
grootte
richting
4
Dispersie/diffusie in poreuze materialen
10000
100
gelijk
5
Estimation of E-coeff. in porous media.
  • Molecular diffusion ( no flow)
  • with ? volumetric water content and
  • with ? tortuosity (gt1 def.effective length over
    length of medium )
  • E-coefficient with flow (small scale Datta,
    2002, Appendix D6 page351)
  • with ?Ld a coefficient (gt lt ? pag 351) and
  • d the average pore diameter

6
Problem 10.dispersioncoeff.
7
Turbulentie in Fluidum
8
Convective mass transfer coefficient
  • cA1 is the concentration of A in the fluid (not
    solid ) but on the surface in equilibrium with A
    in the solid.
  • cA2 is the concentration of A in the bulk fluid

9
Units of equation 10.33 (pag 215)
  • Eenvoudigste oplossing (bemerk de zin in Datta,
    2002, eq 10.33 is not a law but a defining
    equation) er zijn alternatieven mogelijk.
  • hm in m/s ( volgens Table 14.2 pag 302)
  • A in m2
  • NA1-2 in kg/s
  • CA1 en CA2 dan kg/m³

10
CA1 en CA2 in kg/m³
  • CA1 en CA2 dan kg/m³ dikwijls via het
    Mollierdiagramma (Datta, 2002, C9 pag 341) en
    Appendix C8 (pag 340-
  • Mollier diagramma geeft MCmollier (in g water/kg
    droge lucht)
  • C8 geeft de densiteit ?da (kg/m³) voor droge
    lucht
  • C voor formule

11
Class A pan
12
Problem Evaporation
13
Dispersion, Convection, Diffusion
  • Bulk flow effect can be separated the process as
    convectiondispersion
  • Bulk flow effect cannot be separated as
    dispersion only
  • Diffusion is always present but slow

14
Convective Mass Transfer
  • Movement of mass due to bulk flow of the system.
    This is in addition to diffusive mass transfer
  • Forced convection is due to an external force
    such as a fan
  • Free convection is due to density differences
  • Formula
  • complete analogy to heat transfer
  • hm includes effect of diffusion
  • hm depends on flow geometry, fluid prop., etc.

15
Bepaling van h-convectie coefficiënt
  • Eerst hm bepalen zoals met h voor warmte
  • Volgende week stationair en niet-stationair

Convectie coefficiënt
16
Governing Equation for mass transfer(Chapter 11)
Ez
  • Same equation gt Same solutions!
  • B.C. more complex simultaneous equations

17
(No Transcript)
18
Steady-state diffusion in a slab (Chapter 12)
Integrating
Boundary Conditions
19
Steady-state diffusion in a composite media
x
Same fluid
Same K
Mass Transfer
Heat Transfer
20
Steady-state diffusion in composite media
Complication of equilibrium ? (solved by K)
21
ProblemDatta 12.6.3
22
Steady-state diffusion in a slab with reaction
23
Steady-state diffusion in a slab with reaction
24
Steady-state diffusion in a slab with reaction
For Finite Size
This is lower than Flux with reaction
25
Problem Oxygen diffusion in soil
0.03
26
Comparison soil air-water saturated
27
ProblemDatta 12.6.7
Oxygen in top is of shoot is 0.199 g/m3
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