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air flowing through the elbow, a centrifugal force is created and increases the pressure<br />

at the outside radius of the elbow thus increases the bias flow and makes the discharge<br />

coefficient greater [45, 63]. On the other hand, when pressure setting becomes greater,<br />

the discharge coefficient decreases to 0.97. This is because when the pressure increases,<br />

the flow rate and flow velocity through the holes also increases. When the velocity is<br />

low, the Vena Contracta [45] may be close to the narrowest point of the holes near the<br />

shrinkage at the edge of the inner surface. However, when velocity increases, the higher<br />

velocity may make the Vena Contracta phenomenon gradually more significant (Figure<br />

5.8). Overall the constant discharge coefficient 0.985 matches well with the<br />

experimental result over the CPAP working range.<br />

Figure 5.8 High velocity vena contracta phenomena at bias vent holes<br />

5.2.2 Fluid dynamic model under breathing added fluctuating flow<br />

The fluid dynamic outputs should include pressure fluctuation in the mask and the<br />

dynamic fluctuating airflow velocity in HADT. All these outputs should be tested over<br />

the CPAP pressure setting range. However, due to instruments availability, the<br />

validations have not been fully conducted. The setups for future validation are shown in<br />

Appendix XXI. The already conducted experiments are described and compared with<br />

the model outputs below.<br />

117

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