foam-mat freeze drying of egg white and ... - McGill University
foam-mat freeze drying of egg white and ... - McGill University
foam-mat freeze drying of egg white and ... - McGill University
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N<br />
D<br />
in = − win,<br />
e<br />
∂C<br />
∂x<br />
pin<br />
N t = v p ( C pw + C pin )<br />
⎛<br />
+ ⎜<br />
⎝ C<br />
pw<br />
C<br />
pin<br />
+ C<br />
pin<br />
⎞<br />
⎟N<br />
⎟<br />
⎠<br />
t<br />
This model can be used for determining overall mass transfer by applying the<br />
boundary conditions; this model also helps to include the effect <strong>of</strong> radiation heat transfer.<br />
Some <strong>of</strong> the key assumptions made by the researchers (Liapis & Bruttini 1995;<br />
Liapis & Sadikoglu 1997; Jafar & Farid 2003; Khlloufi et al. 2005) to develop<br />
<strong>mat</strong>he<strong>mat</strong>ical model for <strong>freeze</strong> <strong>drying</strong> are,<br />
i) The maximum permissible surface temperature (Ts) is reached<br />
instantaneously<br />
ii) The surface temperature is maintained constantly by adjusting external<br />
heat output<br />
iii) Subli<strong>mat</strong>ion occurs parallel to the surface at the interface<br />
iv) At the interface the concentration water vapour <strong>and</strong> the ice are in<br />
equilibrium<br />
v) Solid layer is semi-infinite<br />
vi) Binary mixture <strong>of</strong> water vapour <strong>and</strong> inert gas pass through dried layer<br />
vii) In the dried layer, the solid <strong>and</strong> the enclosed gas are in thermal<br />
equilibrium<br />
viii) Partial pressure variation inside the <strong>drying</strong> chamber is negligible<br />
ix) There is no heat loss; all the heat input is used for subli<strong>mat</strong>ion <strong>of</strong> water<br />
33<br />
……………… (3.10)<br />
……………… (3.11)