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The impact of viscosity on the combined heat, mass and momentum transfer in laminar liquid falling films

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Abstract

In this article we present a model describing a laminar film flow over a vertical isothermal plate whilst heat and mass transfer is occurring. We focus on a formulation where most common assumptions, such as constant property data and constant film thickness, have been cancelled. The hydrodynamic model results in longitudinal and transversal velocity components and their evolution in the entrance region. Heat and mass transfer occurs simultaneously and is modelled with respect to release of differential heat of solution as well as heat flow due to interdiffusion. The numerical solution is obtained by utilising a Newton-Raphson method to solve the finite difference formulation of the governing equations. Mass transfer across the film affects the development of both longitudinal and transversal velocity components. The hydrodynamics are modelled using a boundary layer approximation of the Navier-Stokes equations. The significance of simplifications on the hydrodynamic model are illustrated and discussed using a fully developed velocity profile (Nusselt flow) and a plug flow at the inlet for comparison. Even if a Nusselt profile is assumed, it develops further since mass is absorbed or desorbed. It is found that the onset of absorption occurs at shorter flow length when applying a plug flow at the inlet. If the film is initially in equilibrium, this results in a 9.3% increase in absorbed mass over a length of 0.03 m as compared with the Nusselt flow. A fluid with a viscosity five times the one of lithium bromide solution but sharing comparable properties apart from that, leads to lower overall heat and mass transfer rates. If the respective fluids are saturated at the inlet, the accumulated mass flux absorbed by lithium bromide solution is 2.2 times higher than the one absorbed by a high viscous fluid. However, when a plug flow is applied and the fluid is sub-cooled, ab initio the absorbed mass flux is slightly higher for a high viscous fluid. Assuming a sub-cooling of 3 K at the inlet, lithium bromide solution now only performs around 11% better as compared with a high viscous fluid over the considered length of 0.03 m. The code may be downloaded from: https://github.com/mittermaier/hmt.

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Abbreviations

c p Specific heat capacity:

J/(k gK)

D Mass diffusivity:

m 2/s

g Gravitational acceleration:

m/s 2

h Enthalpy:

J/k g

\(\overline {h}\) Partial massive enthalpy:

J/k g

L e Lewis-Number = λ/(Dc p ρ):

-

\(\dot {m}\) Mass flux:

k g/(m 2s)

p Pressure:

P a

\(\dot {q}\) Heat flux:

W/m 2

T Temperature:

K

u Longitudinal velocity:

m/s

v Transversal velocity:

m/s

x Longitudinal coordinate, streamwise:

m

y Transversal coordinate:

m

\(\dot {\Gamma }\) Mass flow per unit length:

k g/(ms)

\(\overline {\Delta y}\) :

Abbreviation, please see Eq. 24

\({\Delta } \overline {h}\) :

Abbreviation, please see Eq. 27

Δh s o r Heat of sorption:

J/k g

δ Film thickness:

m

λ Thermal conductivity:

W/(mK)

μ Dynamic viscosity:

P as

ξ Mass fraction:

k g/k g

ρ Density:

k g/m 3

0 :

Inlet condition

a v g :

Average

A :

Absorbate e.g. water in liquid state

e q :

Equilibrium

if :

Interface

i :

node index in longitudinal direction (x)

j :

node index in transversal direction (y)

S :

Solution of absorbent e.g. L i B rH 2 O

V :

Vapour e.g. steam

w :

Wall

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Mittermaier, M., Ziegler, F. The impact of viscosity on the combined heat, mass and momentum transfer in laminar liquid falling films. Heat Mass Transfer 54, 1199–1215 (2018). https://doi.org/10.1007/s00231-017-2219-9

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