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Equation of Continuity II
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Summary of Equations of Change
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molecular stresses = pressure + viscous stresses
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Summary of Equations of Change The energy molecular flux
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Summary of Equations of Change Recall: the combined energy flux vector e
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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:
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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:
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Summary of Equations of Change Recall: Substituting the equation for q into e
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Summary of Equations of Change Recall: Substituting the equation for q into e partial molar per unit mass
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Summary of Equations of Change Recall: Substituting the equation for q into e
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Summary of Equations of Change
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Simultaneous Heat and Mass Transfer
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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
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Simultaneous Heat and Mass Transfer Equations of Change: Continuity (A)
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Simultaneous Heat and Mass Transfer Equations of Change: Energy * Both N Ay and e y are constant throughout the film
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Simultaneous Heat and Mass Transfer To determine the mole fraction profile: Recall: The molar flux for diffusion of A through stagnant B
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Concentration Profiles I. Diffusion Through a Stagnant Gas Film Since B is stagnant,
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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
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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
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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
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Simultaneous Heat and Mass Transfer To determine the mole fraction profile: Evaluating N Ay from the equations above Note that:
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Simultaneous Heat and Mass Transfer BUT…
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Simultaneous Heat and Mass Transfer
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Rearranging and combining
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Simultaneous Heat and Mass Transfer @ y = y, x A = x A
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Simultaneous Heat and Mass Transfer @ y = y, x A = x A @ y = δ, x A = x Aδ Taking the ratios of the two equations
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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
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Simultaneous Heat and Mass Transfer To determine the temperature profile: The general solution is
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Simultaneous Heat and Mass Transfer At y = 0, T = T 0 At y = δ, T = T δ Subtracting the two equations
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Simultaneous Heat and Mass Transfer Since
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Simultaneous Heat and Mass Transfer
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If we did not consider mass transfer
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Simultaneous Heat and Mass Transfer With mass transfer
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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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