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From the above analysis, the pressure drop along the HADT, which is also the pressure<br />

difference between the chamber and the mask, can be expressed as:<br />

du<br />

P P P f u L<br />

(2.22)<br />

Ta 2<br />

T<br />

C M (2 T T Ta<br />

) T<br />

DTi dt<br />

The HADT inner wall is corrugated. However, since the relative roughness is small, the<br />

pitch is long and the Reynolds number is no more than 10 5 . This inner surface friction<br />

may not be too much different from a smooth tube. Darcy-Weisbach friction factor may<br />

be applicable [42]:<br />

0.3164<br />

fT (2.23)<br />

Re<br />

After substituting Eq. (2.23) in, Eq. (2.22) can be rearranged as follow to calculate<br />

pressure in the mask:<br />

25<br />

0.25<br />

Ti<br />

P 0.6328<br />

du<br />

P L [ u u ]<br />

2.3.6 Mask air mass balance<br />

0.75<br />

C T<br />

M Ta<br />

T T T <br />

Ta<br />

L D<br />

T<br />

TiTa 0.25<br />

DTi<br />

( )<br />

dt<br />

Ta<br />

(2.24)<br />

The mask is the interface for patient to use the CPAP machine. The mask is strapped<br />

tightly onto patient’s face to prevent leakage. When a patient inhales, air flows into the<br />

mask through an elbow with bias vent holes and gets mixed with air already in the mask<br />

before being inspired into the patient’s upper airway. When the patient exhales, exhaled<br />

air from patient gets mixed before leaving the mask. One of the objectives for this<br />

project is to investigate the influence of mask capacity on the CPAP machine’s<br />

performance.

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