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IEA Solar Heating and Cooling Programm - NachhaltigWirtschaften.at

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<strong>IEA</strong> SHC Task 38 <strong>Solar</strong> Air Conditioning <strong>and</strong> Refriger<strong>at</strong>ion Subtask C2-A, November 9, 2009<br />

Equ<strong>at</strong>ions (7), (8), (9) <strong>and</strong> (10) are coupled, hyperbolic <strong>and</strong> non-linear. With the assumption<br />

of the Lewis number (Le), equal unity <strong>and</strong> the desiccant m<strong>at</strong>rix in equilibrium with air means<br />

th<strong>at</strong> (T d = T eq <strong>and</strong> w eq = w a ). Banks [8] used m<strong>at</strong>rix algebra <strong>and</strong> demonstr<strong>at</strong>ed th<strong>at</strong> these<br />

equ<strong>at</strong>ions (7 to 10) can be reduced by applying the potential function Fi(T,w) to the following<br />

system:<br />

∂Fi<br />

, eq ∂F<br />

, a<br />

∂F<br />

, a<br />

γ iµ + u<br />

+<br />

= 0 i=1;2<br />

∂t<br />

∂t<br />

∂z<br />

(11)<br />

∂Fi<br />

, d<br />

γ<br />

iµ<br />

+ J<br />

m<br />

( Fi<br />

, eq<br />

− Fi<br />

, a<br />

) = 0 i=1;2<br />

∂t<br />

(12)<br />

These equ<strong>at</strong>ions are similar to those for the sensible regener<strong>at</strong>or (Equ<strong>at</strong>ions 1 <strong>and</strong> 2), with<br />

the potential function F i replacing the temper<strong>at</strong>ure <strong>and</strong> the parameters γ i replacing the<br />

specific he<strong>at</strong> r<strong>at</strong>io, <strong>and</strong> they can be solved using analogy with he<strong>at</strong> transfer alone as<br />

suggested by Maclaine-cross <strong>and</strong> Banks [7] <strong>and</strong> Close <strong>and</strong> Banks [9]. There are many<br />

expressions for the potential functions of moist air-silica gel; we chose those proposed by<br />

Jurinak [10] <strong>and</strong> Stab<strong>at</strong> [11].<br />

F = h<br />

1<br />

(13)<br />

1.5<br />

( 273.15 + T ) 0. 8<br />

2<br />

1. 1<br />

F = + w<br />

(14)<br />

6360<br />

The solution sequence for the desiccant wheel is then:<br />

. j<br />

i<br />

C j<br />

= m a<br />

C<br />

C<br />

M<br />

=<br />

* d i(<br />

moy)<br />

ri<br />

. min j<br />

*<br />

i<br />

=<br />

m<br />

C<br />

C<br />

a<br />

i<br />

min<br />

i<br />

max<br />

N<br />

γ<br />

NUT<br />

0<br />

1<br />

=<br />

C<br />

min<br />

⎛<br />

⎜<br />

⎝<br />

1<br />

+<br />

1<br />

( h A) ( h A)<br />

m<br />

s<br />

m<br />

r<br />

⎞<br />

⎟<br />

⎠<br />

−1<br />

⎡<br />

( )<br />

( ) ⎥ ⎥ ⎤<br />

=<br />

m 1<br />

⎢ −<br />

*<br />

ε<br />

i<br />

ε<br />

cc<br />

NUT0<br />

, Ci<br />

1<br />

or ε<br />

* 1. 93 i<br />

= C ri<br />

( C<br />

* ri<br />

≤ 0. 4 ) for very low rot<strong>at</strong>ion speed<br />

⎢⎣<br />

9 Cri<br />

⎦<br />

page 29

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