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Equation of Continuity II. Summary of Equations of Change.

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Presentation on theme: "Equation of Continuity II. Summary of Equations of Change."— Presentation transcript:

1 Equation of Continuity II

2 Summary of Equations of Change

3

4 molecular stresses = pressure + viscous stresses

5 Summary of Equations of Change The energy molecular flux

6 Summary of Equations of Change Recall: the combined energy flux vector e

7 Combined Energy Flux Vector Convective Energy Flux Heat Rate from Molecular Motion Work Rate from Molecular Motion Combined Energy Flux Vector: We introduce something new to replace q:

8 Combined Energy Flux Vector Combined Energy Flux Vector: We introduce something new to replace q: Recall the molecular stress tensor: When dotted with v: Substituting into e:

9 Summary of Equations of Change Recall: Substituting the equation for q into e

10 Summary of Equations of Change Recall: Substituting the equation for q into e partial molar per unit mass

11 Summary of Equations of Change Recall: Substituting the equation for q into e

12 Summary of Equations of Change

13

14 Simultaneous Heat and Mass Transfer

15 Assumptions: 1.Steady-state 2.Ideal gas behavior 3.Total c is constant 4.Uniform pressure 5.Physical properties are constant, evaluated at mean T and x. 6.Neglect radiative heat transfer

16 Simultaneous Heat and Mass Transfer Equations of Change: Continuity (A)

17 Simultaneous Heat and Mass Transfer Equations of Change: Energy * Both N Ay and e y are constant throughout the film

18 Simultaneous Heat and Mass Transfer To determine the mole fraction profile: Recall: The molar flux for diffusion of A through stagnant B

19 Concentration Profiles I. Diffusion Through a Stagnant Gas Film Since B is stagnant,

20 Simultaneous Heat and Mass Transfer To determine the mole fraction profile: Recall: The molar flux for diffusion of A through stagnant B Recall: Integration of the above equation

21 Concentration Profiles I. Diffusion Through a Stagnant Gas Film Let C 1 = -ln K 1 and C 2 = -ln K 2, B.C. at z = z 1, x A = x A1 at z = z 2,x A = x A2

22 Simultaneous Heat and Mass Transfer To determine the mole fraction profile: Recall: The molar flux for diffusion of A through stagnant B Using the appropriate B.C.s at y = 0, x A = x A0 at y = δ,x A = x Aδ

23 Simultaneous Heat and Mass Transfer To determine the mole fraction profile: Evaluating N Ay from the equations above Note that:

24 Simultaneous Heat and Mass Transfer BUT…

25 Simultaneous Heat and Mass Transfer

26 Rearranging and combining

27 Simultaneous Heat and Mass Transfer @ y = y, x A = x A

28 Simultaneous Heat and Mass Transfer @ y = y, x A = x A @ y = δ, x A = x Aδ Taking the ratios of the two equations

29 Simultaneous Heat and Mass Transfer To determine the temperature profile: Note: where the enthalpy of mixing is often neglected for gases at low to moderate pressures

30 Simultaneous Heat and Mass Transfer To determine the temperature profile: The general solution is

31 Simultaneous Heat and Mass Transfer At y = 0, T = T 0 At y = δ, T = T δ Subtracting the two equations

32 Simultaneous Heat and Mass Transfer Since

33 Simultaneous Heat and Mass Transfer

34 If we did not consider mass transfer

35 Simultaneous Heat and Mass Transfer With mass transfer

36 Simultaneous Heat and Mass Transfer Comparison of the energy flux with & without the presence of mass transfer: Rate of heat transfer is directly affected by simultaneous mass transfer BUT mass flux is not directly affected by simultaneous heat transfer


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