5,723 research outputs found

    Rayleigh number dependence of the Archimedes number dependent large-scale flow structure formation in mixed convection

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    We report on experimental investigations of large-scale flow structure formation in mixed convection. We characterize the flow field by measuring the velocity fields within a rectangular model room using 2D2C PIV. The control parameters are the Reynolds number Re, the Rayleigh number Ra and the Prandtl number Pr. All parameters are linked through the Archimedes number Ar. In 6.4x10-2 ≤ Ar ≤ 1.39x101, 4.2x103 ≤ Re ≤ 6.35x104 and Ra = 3.1x107, Ra = 1.8x108 and Pr = 0.713 we found flow 3 different flow structures. While keeping Ra and Pr constant and varying Ar through Re variations, we found an Ar dependence of the largescale flow structure formation within 6.4x10-2 ≤ Ar ≤ 1.39x101. Furthermore, we found a Ra dependence of the structure formation, which shifts the transition points between the structures to higher Archimedes numbers and reduces the mean velocities within the investigated domain

    Reynolds numbers near the ultimate state of turbulent Rayleigh-Bénard convection

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    We report on measurements of the mean-flow Reynolds number ReU and the rms fluctuation Reynolds number ReV in turbulent Rayleigh-Bénard convection as a function of the Rayleigh number Ra for 4 x 1011 < Ra < 2 1014 and Pr ' 0:8. Both can be described by the same power law with an effective exponent = 0:44, in agreement with predictions for ReU but in disagreement with predictions for ReV

    Logarithmic variance profiles and the corresponding f-1 spectra of temperature fluctuations in turbulent Rayleigh-Bénard convection

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    We report experimental results for the temperature variance 2(z) and the corresponding frequency spectra P(f) in turbulent Rayleigh-Bénard convection (RBC) in a cylindrical sample of aspect ratioT= D/L = 1:00 (D = 1:12 m is the diameter and L = 1:12 m the height). The measurements were conducted in the Rayleigh-number range 1011 < Ra < 1:35 1014 and Pr ' 0:8. For Ra = 1:35x1014, 2(z) could be described well by a logarithmic dependence on the vertical position z in a range of z 1 < z < z 2 with z 1 ' 70 and z 2 = 0:1L. Here L=(2Nu) is the thickness of a thin thermal sublayer adjacent to the horizontal plate where the heat flux (denoted by the Nusselt number Nu) is carried mostly by thermal diffusion. In the log layer, we found that the temperature spectra had a significant frequency range over which P(f) f with close to 1. As Ra decreased, increased so that the log layer became thinner. At Ra = 2:05 1011, z 2 < z 1 and therefore there was no range for a log layer. Correspondingly, the temperature spectrum near the horizontal plate did not have the f1 scaling form either

    Impact of a theoretically based sex education programme (SHARE) delivered by teachers on NHS registered conceptions and terminations: final results of cluster randomised trial

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    &lt;b&gt;Objective&lt;/b&gt;: To assess the impact of a theoretically based sex education programme (SHARE) delivered by teachers compared with conventional education in terms of conceptions and terminations registered by the NHS. Design Follow-up of cluster randomised trial 4.5 years after intervention. &lt;b&gt;Setting&lt;/b&gt;: NHS records of women who had attended 25 secondary schools in east Scotland. &lt;b&gt;Participants&lt;/b&gt;: 4196 women (99.5% of those eligible). &lt;b&gt;Intervention&lt;/b&gt;: SHARE programme (intervention group) v existing sex education (control group). &lt;b&gt;Main outcome measure&lt;/b&gt;: NHS recorded conceptions and terminations for the achieved sample linked at age 20. &lt;b&gt;Results&lt;/b&gt;: In an "intention to treat" analysis there were no significant differences between the groups in registered conceptions per 1000 pupils (300 SHARE v 274 control; difference 26, 95% confidence interval –33 to 86) and terminations per 1000 pupils (127 v 112; difference 15, –13 to 42) between ages 16 and 20. &lt;b&gt;Conclusions&lt;/b&gt;: This specially designed sex education programme did not reduce conceptions or terminations by age 20 compared with conventional provision. The lack of effect was not due to quality of delivery. Enhancing teacher led school sex education beyond conventional provision in eastern Scotland is unlikely to reduce terminations in teenagers

    Accuracy and interobserver reliability of three-dimensional rotational angiography versus mathematical models for volumetric measurement of intracranial aneurysms

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    We aimed to compare the inter-rater reliability relating to the volumetric measurement of intracranial aneurysms obtained with three-dimensional rotational angiography (3D-RA) compared with two commonly used mathematical models. Ten randomly selected aneurysms were measured by 3 independent assessors using 3D-RA and 2 mathematical models for the calculation of an ellipsoid: Equation (1), Vab = 4/3π × (a/2) × (b/2) × (a + b/4); and Equation (2), Vabc = (4/3)π × (a/2) × (b/2) × (c/2). The inter-rater reliability for each method was: 3D-RA, 0.99; Vabc, 0.90; and Vab, 0.89. The 95% confidence interval for the mean difference between 3D-RA and Vabc was not significantly different, whereas there was a significant difference between 3D-RA and Vab. Vab gave consistently higher estimates than 3D-RA. This was especially true for aneurysms with larger volumes. The use of 3D-RA to undertake volumetric measurements of intra-cranial aneurysms is both valid and reproducible for different assessors

    Lagrangian Raylaigh-Bénard convection

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    Using passive tracers as sensors, we obtain Lagrangian measurements of tracers position, velocity and temperature in Rayleigh-Bénard convection at Ra=10^7-10^9. We report on statistics of temperature, velocity, and heat transport (Nusselt number). We observe that the Nusselt number is characterized by a largely intermittent behavior, likely due to the interaction of temperature with turbulent velocity fluctuations

    Photochemical behavior of some p-styryistilbenes and related compounds: Spectral properties and photoisomerization in solution and in solid state

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    Author Posting. © The Authors (2006) This is the author's version of the work. It is posted here for personal use, not for redistribution. The definitive version was published in PHOTOCHEMISTRY AND PHOTOBIOLOGY, 82(6): 1645-1650. https://doi.org/10.1562/2006-01-17-RA-780ArticlePhotochemistry and Photobiology. 82(6): 1645-1650 (2006)journal articl

    Aspect-ratio dependence of the transition to the ultimate state of turbulent Rayleigh-Bénard convection

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    We report on measurements of the ultimate-state transition in turbulent Rayleigh-B\'enard convection obtained in a large facility known as the ``Uboot of G\"ottingen" and using pressurized sulfur hexafluoride as the convecting fluid. We found that the transition occurs over a range of RaRa which becomes more narrow as Γ\Gamma increases, ranging from Ra1Ra_1^* which is at most weakly dependent on Γ\Gamma and close to 101310^{13} to Ra2Ra_2^* which varies from about 2×10152\times 10^{15} for Γ=0.33\Gamma = 0.33 to about 7×10137\times 10^{13} for Γ=1.00\Gamma = 1.00
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