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Transport Phenomena

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to a modulus ? = stress = Fx / dux. strain A dz. Viscosity ... Summary: Q/?T ~ dT/dx heat. l ~ n number. ? ~ dux/dz velocity. Jx ~ dn/dx number ... – PowerPoint PPT presentation

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Title: Transport Phenomena


1
Transport Phenomena
  • Fourier heat conduction law.
  • Q - kt A dT
  • ?t dx

2
Transport Phenomena
  • Fourier heat conduction law.
  • Q - kt A dT
  • ?t dx
  • kt thermal conductivity.

3
Transport Phenomena
  • Fourier heat conduction law.
  • Q - kt A dT
  • ?t dx
  • kt thermal conductivity.
  • Heat Equation
  • ?T K ?2T
  • ?t ?x2

4
Transport Phenomena
  • Fourier heat conduction law.
  • Q - kt A dT
  • ?t dx
  • kt thermal conductivity.
  • Heat Equation
  • ?T K ?2T
  • ?t ?x2
  • K kt /?c

5
Transport Phenomena
  • Fourier heat conduction law.
  • Q - kt A dT
  • ?t dx
  • kt thermal conductivity.
  • Heat Equation
  • ?T K ?2T
  • ?t ?x2
  • K kt /?c ? density, c specific heat

6
Conductivity of an ideal gas
  • Mean Free Path ? l 1/4pr2 V/N

7
Conductivity of an ideal gas
  • Mean Free Path ? l 1/4pr2 V/N
  • in FGT ? ? 1/(v2 ns)

8
Conductivity of an ideal gas
  • Mean Free Path ? l 1/4pr2 V/N
  • in FGT ? ? 1/(v2 ns) where s 4pr2
  • and n
    N/V

9
Conductivity of an ideal gas
  • Mean Free Path ? l 1/4pr2 V/N
  • in FGT ? ? 1/(v2 ns) where s 4pr2
  • and n
    N/V
  • Thermal conductivity of an ideal gas is
  • kt ½ CV l vave V

10
Conductivity of an ideal gas
  • Mean Free Path ? l 1/4pr2 V/N
  • in FGT ? ? 1/(v2 ns) where s 4pr2
  • and n
    N/V
  • Thermal conductivity of an ideal gas is
  • kt ½ CV l vave vave vT
  • V

11
Conductivity of an ideal gas
  • Mean Free Path ? l 1/4pr2 V/N
  • in FGT ? ? 1/(v2 ns) where s 4pr2
  • and n
    N/V
  • Thermal conductivity of an ideal gas is
  • kt ½ CV l vave vave vT
  • V
  • where CV f Nk f P
  • V 2 V 2T

12
Viscosity
  • Viscosity transfers momentum in a fluid.

13
Viscosity
  • Viscosity transfers momentum in a fluid.
  • Motion of one layer sliding on another, if slow
    and the motion is laminar the resistance to
    shearing is viscosity

14
Viscosity
  • Viscosity transfers momentum in a fluid.
  • Motion of one layer sliding on another, if slow
    and the motion is laminar the resistance to
    shearing is viscosity
  • The equation for the coefficient is similar
  • to a modulus ? stress
  • strain

15
Viscosity
  • Viscosity transfers momentum in a fluid.
  • Motion of one layer sliding on another, if slow
    and the motion is laminar the resistance to
    shearing is viscosity
  • The equation for the coefficient is similar
  • to a modulus ? stress Fx / dux
  • strain A
    dz

16
Viscosity
  • Viscosity transfers momentum in a fluid.
  • Motion of one layer sliding on another, if slow
    and the motion is laminar the resistance to
    shearing is viscosity
  • The equation for the coefficient is similar
  • to a modulus ? stress Fx / dux
  • strain A
    dz
  • ? vT and independent of P

17
Diffusion
  • Movement of particles is diffusion

18
Diffusion
  • Movement of particles is diffusion
  • Jx - D dn/dx (Ficks Law)

19
Diffusion
  • Movement of particles is diffusion
  • Jx - D dn/dx (Ficks Law)
  • D is the diffusion coefficient n N/V

20
Diffusion
  • Movement of particles is diffusion
  • Jx - D dn/dx (Ficks Law)
  • D is the diffusion coefficient n N/V
  • D ranges from 10-5 for CO to 10-11 for
    large molecules SI unit is m2 /s.

21
Diffusion
  • Movement of particles is diffusion
  • Jx - D dn/dx (Ficks Law)
  • D is the diffusion coefficient n N/V
  • D ranges from 10-5 for CO to 10-11 for
    large molecules SI unit is m2 /s.
  • Summary Q/?T dT/dx heat
  • l n
    number
  • ? dux/dz
    velocity
  • Jx dn/dx
    number
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