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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 />

A basic element in the angular <strong>and</strong> width direction of the desiccant wheel is considered <strong>and</strong><br />

can be presented as follows:<br />

dθ<br />

R<br />

dz<br />

Air<br />

Figure 19: Basic element of the desiccant wheel<br />

Fundamental equ<strong>at</strong>ions of he<strong>at</strong> <strong>and</strong> mass transfer for the basic element<br />

Mass conserv<strong>at</strong>ion equ<strong>at</strong>ion<br />

∂W<br />

⎛ ∂wa<br />

∂wa<br />

⎞<br />

M<br />

d<br />

+ ma<br />

⎜ + u ⎟ = 0<br />

(27)<br />

∂t<br />

⎝ ∂t<br />

∂z<br />

⎠<br />

Mass transfer equ<strong>at</strong>ion<br />

M<br />

d<br />

∂W<br />

∂t<br />

= h<br />

m<br />

S<br />

( w − w )<br />

a<br />

eq<br />

He<strong>at</strong> conserv<strong>at</strong>ion equ<strong>at</strong>ion<br />

∂H<br />

⎛ ∂ha<br />

∂ha<br />

⎞<br />

M<br />

d<br />

+ ma<br />

⎜ + u ⎟ = 0<br />

(29)<br />

∂t<br />

⎝ ∂t<br />

∂z<br />

⎠<br />

He<strong>at</strong> transfer equ<strong>at</strong>ion<br />

M<br />

d<br />

∂H<br />

∂t<br />

= h<br />

m<br />

S<br />

( w − w )( h + c T ) + h S( T − T )<br />

a<br />

eq<br />

fg<br />

pv<br />

a<br />

t<br />

a<br />

d<br />

(28)<br />

(30)<br />

Variable change<br />

The time t is rel<strong>at</strong>ed to the angular position θ with the following equ<strong>at</strong>ion<br />

t<br />

τ<br />

ro<br />

=<br />

θ<br />

π<br />

so<br />

τ ro<br />

t = θ ,<br />

π<br />

Where τ ro is the rot<strong>at</strong>ion period of the process or regener<strong>at</strong>ion <strong>and</strong> N is the angular speed of<br />

the wheel.<br />

page 47

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