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To further model the liquid hydrogen cryogenic pump, the pbCFD default grid size (21x71x21) and stretch factor (12) was used to continue this study The inlet conditions were created in CCAD 4, with the total pressure and temperature set to the standard reference conditions The solution took about 20 CPU minutes on a Pentium 400 MHz platform to converge to within 1 per cent of the air-equivalent compressor flow rate The predicted rotor efficiency was 09655, within half a point of the measured data The rotor head rise coefficient was measured at 07; the pbCFD value was \f = 079 In the computed pbCFD solution, there existed recirculation regions near the splitter blade suction surface and in front of the LE, which were observed from previous pbCFD computations Figures 518 to 522 show the computed streamlines.

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Computed streamlines are shown on a number of key surfaces in this pump Figure 518 is located close to the main blade pressure surface and nearly collateral flow is observed, although a small bubble appears to exist just before the leading edge of the main blade The leading edge is not shown distinctly in this figure, but it is perpendicular to the axis of the plot and is located just aft of the little bubbles shown along the shroud streamline Similar results are shown near the suction side of the splitter blade, and again, some evidence of a small recirculation zone in front of the leading edge may be observed with larger recirculation downstream of this point, but upstream of the splitter blade (location not shown, but approximately after the separation vortex) Streamline results adjacent to the pressure side are as displayed in Fig 520.

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The separation zone is small and the distortion in the streamlines is only moderate Near the mid-channel region, between the splitter and the blade, the flow field is more complex as shown in Fig 521 On the suction side of the main blade, the flow becomes very complex with considerable secondary flow in some regions with local recirculation displayed as revealed in Fig 522 Within the parameters available to influence this design, the condition could not be improved further..

Medicine: a Journal of the British Diabetic, Association 11, 701 4. Williamson, D.F., Pamuk, E., Thun, M. et al. (1995) Prospective study of intentional weight loss and mortality in never-smoking overweight US white women aged 40 64 years. American Journal of Epidemiology, 141, 1128 41. Williamson, D.F., Thompson, T.J., Thun, M. et al. (2000) Intentional weight loss and mortality among overweight individuals with diabetes. Diabetes Care, 23 (10), 1499 504.

Therefore, we set the defocusing coef cient B 5:0 10 3 and the spherical aberration coef cient G 5:0 10 3 . These interferograms without B C 0 and with B 5:0 10 3 tilt are shown in Figures 2.43(c,f). The fringe patterns at the medium focus with B 10:0 10 3 are in Figures 2.43(b,e). 3. Coma. All the patterns for coma were obtained using F 5:0 10 3 . Figure 2.44 shows them for the paraxial focus D 0 and Figure 2.45 with a small defocusing D 5:0 10 3 . In both gures the central pattern has no tilt E F 0 and the surrounding pictures are for different tilt combinations B 5:0 10 3 ; C 5:0 10 3 . 4. Astigmatism. All the patterns for astigmatism were computed for C 3:0 10 3 . If 0, we obtain the Petzval focus. The OPD for astigmatism can be written from Eq. (2.36) as OPD D E x2 D 3E y2 : 2:58

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