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0.875 0.5<br />

0.02925ReTi Sca<br />

ev wa<br />

k D<br />

(3.84)<br />

<br />

Based on the conditions here, an average value of 2.67×10 -5 m 2 /s for D wa is used for<br />

simplifying the computation.<br />

Based on the analysis above, condensation rate at the same place can be expressed as:<br />

m 1.2 k A ( C C )<br />

(3.85)<br />

cndns ev Tli Tsv Tav<br />

m cndns is condensation rate and quantitatively equals to 120% of evaporation rate but<br />

with opposite sign because CTsv CTav<br />

when condensation is occurring.<br />

Eq. (3.83) and Eq. (3.85) can be combined as:<br />

m k k A ( C C )<br />

(3.86)<br />

Tlec ec ev Tli Tsv Tav<br />

Where m Tlec is HADT lump inner surface condensation or evaporation rate, kec may be<br />

named as condensation-to-evaporation coefficient. When CTsv CTav<br />

, evaporation may<br />

occur and kec 1.<br />

When CTsv CTav<br />

, condensation occurs and kec 1.2 .<br />

Integration of positive part of m Tlec within a breath cycle gives the cycle-wise total<br />

amount of potential evaporation and integration of negative part of m Tlec within a breath<br />

cycle gives that of condensation.<br />

And:<br />

mTlecP kev ATli ( CTsv CTav ) dt<br />

when CTsv CTav<br />

0 (3.87)<br />

mTlecN 1.2 kev ATli ( CTsv CTav ) dt when CTsv CTav<br />

0 (3.88)<br />

mTlec mTlecP mTlecN<br />

(3.89)<br />

The sum of the two integrals gives the net condensation or evaporation within a breath<br />

cycle on inner surface of this lump. If the sum is positive, it means there is no<br />

condensation remaining within a whole breath cycle. It may mean that there is no<br />

68

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