We now consider a wall separating two environments whose temperatures T1 and T2 are equal (T1 ≥ T2), but whose relative humidities HR1 and HR 2 are different, with HR1 > HR 2 .
To each relative humidity of the air, HR1 and HR 2 , corresponds a partial pressure Pp1 and Pp2 of water vapour, with of course: Pp1 > Pp2 .
A diffusion flow, g, of water vapour is established through the wall according to Fick's law (figure 3):
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