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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)

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