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Warm pressurant gas model

Ln addition, examination of Equation (3.16) shows that the current bubble point model does not account for variations in pressurant gas temperature, so warm gas data will be valuable for improving the prediction for cryogenic systems. Previous attempts were made to quantify the effect of warm gas on LAD degradation in the literature, but there were numerous reported inconsistencies in results as well as issues reported with the test apparatus. Historical attempts to quantify this effect are reserved for Appendix E. Clearly, carefully designed and controlled tests are required to accurately quantify the effect of warm pressurant gas on LAD performance. [Pg.205]

Another factor which may cause disparity between model and data is that the simplified model does not take into account possible gains in performance due to forced convection of the liquid on the screen. As warm pressurant gas impinges on the LAD screen, cold liquid is brought into the bottom of the channel and routed up to the top of the... [Pg.258]

In ocean drilling, hydrated sediment cores are often obtained. Because the cores frequently traverse warm waters for periods of about 1 h, hydrated cores dissociate and release gas, to yield higher pressures. When core liners are retrieved on the deck of a drilling vessel, frequently the warm weather can cause additional hydrate dissolution, resulting in further pressure increases. The modeling of this dissociation has been done by Wright et al. (2005) and by Davies et al. (2006). [Pg.677]

Figure 5.4. Left. The overall SZ effect in Coma produced by the combination of various electron populations thermal hot gas with ksT = 8.2 keV and r = 4.9 10-3 (solid blue curve) which best fits the available SZ data relativistic electrons which best fit the radio-halo spectrum (yellow curve) provide a small additional SZ effect (Colafrancesco 2004a) warm gas with ksT v 0.1 keV and n 10-3 cm-3 (cyan curve) provides a small SZ effect due to its low pressure (Colafrancesco 2004c) DM produced secondary electrons with Mx = 10 (black dotted curve), 20 GeV (black solid curve) and 30 GeV (dashed solid curve). A pure-gaugino x reference model is assumed in the computations. The relative overall SZ effect is shown as the dotted, solid and dashed red curves, respectively. A zero peculiar velocity of Coma is assumed consistently with the available limits. SZ data are from OVRO (magenta), WMAP (cyan) and MITO (blue). Right. The constraints on the Figure 5.4. Left. The overall SZ effect in Coma produced by the combination of various electron populations thermal hot gas with ksT = 8.2 keV and r = 4.9 10-3 (solid blue curve) which best fits the available SZ data relativistic electrons which best fit the radio-halo spectrum (yellow curve) provide a small additional SZ effect (Colafrancesco 2004a) warm gas with ksT v 0.1 keV and n 10-3 cm-3 (cyan curve) provides a small SZ effect due to its low pressure (Colafrancesco 2004c) DM produced secondary electrons with Mx = 10 (black dotted curve), 20 GeV (black solid curve) and 30 GeV (dashed solid curve). A pure-gaugino x reference model is assumed in the computations. The relative overall SZ effect is shown as the dotted, solid and dashed red curves, respectively. A zero peculiar velocity of Coma is assumed consistently with the available limits. SZ data are from OVRO (magenta), WMAP (cyan) and MITO (blue). Right. The constraints on the <tV)a - Mx plane set by the SZ effect from Coma. The heavily dashed area is excluded by the analysis of the SZ dm- The SZ constraints are combined with the WMAP constraint 0.085 <, Qm/i2 iS 0.152 which are translated on the quantity (<jV)a (from Colafrancesco 2004b).

See other pages where Warm pressurant gas model is mentioned: [Pg.261]    [Pg.279]    [Pg.289]    [Pg.298]    [Pg.261]    [Pg.279]    [Pg.289]    [Pg.298]    [Pg.112]    [Pg.259]    [Pg.299]    [Pg.322]    [Pg.411]    [Pg.117]    [Pg.262]    [Pg.141]    [Pg.1637]    [Pg.250]    [Pg.5028]    [Pg.414]    [Pg.233]    [Pg.670]    [Pg.392]    [Pg.2221]    [Pg.490]    [Pg.46]    [Pg.153]   


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