thermal saturation
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Processes ◽  
2020 ◽  
Vol 8 (5) ◽  
pp. 621 ◽  
Author(s):  
Miroslav Rimar ◽  
Marcel Fedak ◽  
Jakub Vahovsky ◽  
Andrii Kulikov ◽  
Peter Oravec ◽  
...  

The study deals with the possibility of elimination of stagnation of thermal systems. The state of stagnation of thermal systems leads to overheating and evaporation of the heat transfer medium, which increases pressure and can lead to damage to the solar thermal system. Stagnation can occur due to a fault and stopping of the circulation pump, which causes the circulation of the heat transfer medium to stop. Another possibility is to achieve thermal saturation in the system, which can be affected by low heat consumption from the system. Elimination of stagnation is possible by various construction designs of collectors or by using other technical means. This study describes an experiment verifying the usability of a thermal collector’s tilting system to eliminate thermal stagnation of the system. The system is fully automatic, and when recording the limit values, ensures that the panel is rotated out of the ideal position, thus reducing the amount of received energy. In this way, the temperature of the medium in the system can be reduced by up to 10% in one hour. In the case of thermal saturation of the system, the solution is the automatic circulation of heat-transfer fluid through the system during the night and the release of thermal energy to the outside. These results suggest that the methods used actively eliminate stagnation of thermal systems.


2020 ◽  
Vol 494 (4) ◽  
pp. 5542-5567 ◽  
Author(s):  
Matus Rybak ◽  
J A Hodge ◽  
S Vegetti ◽  
P van der Werf ◽  
P Andreani ◽  
...  

ABSTRACT We present a sub-kpc resolved study of the interstellar medium properties in SDP.81, a $z$ = 3.042 strongly gravitationally lensed, dusty star-forming galaxy, based on high-resolution, multiband ALMA observations of the far-infrared (FIR) continuum, CO ladder, and the [C ii] line. Using a visibility-plane lens modelling code, we achieve a median source-plane resolution of ∼200 pc. We use photon-dominated region (PDR) models to infer the physical conditions – far-ultraviolet (FUV) field strength, density, and PDR surface temperature – of the star-forming gas on 200-pc scales, finding a FUV field strength of ∼103−104G0, gas density of ∼105 cm−3, and cloud surface temperatures up to 1500 K, similar to those in the Orion Trapezium region. The [C ii] emission is significantly more extended than that FIR continuum: ∼50 per cent of [C ii] emission arises outside the FIR-bright region. The resolved [C ii]/FIR ratio varies by almost 2 dex across the source, down to ∼2 × 10−4 in the star-forming clumps. The observed [C ii]/FIR deficit trend is consistent with thermal saturation of the C+ fine-structure-level occupancy at high gas temperatures. We make the source-plane reconstructions of all emission lines and continuum data publicly available.


2019 ◽  
Vol 631 ◽  
pp. A122 ◽  
Author(s):  
P. J. Käpylä

Context. Convective motions that overshoot into regions that are formally convectively stable cause extended mixing. Aims. We aim to determine the scaling of the overshooting depth (dos) at the base of the convection zone as a function of imposed energy flux (ℱn) and to estimate the extent of overshooting at the base of the solar convection zone. Methods. Three-dimensional Cartesian simulations of hydrodynamic compressible non-rotating convection with unstable and stable layers were used. The simulations used either a fixed heat conduction profile or a temperature- and density-dependent formulation based on Kramers opacity law. The simulations covered a range of almost four orders of magnitude in the imposed flux, and the sub-grid scale diffusivities were varied so as to maintain approximately constant supercriticality at each flux. Results. A smooth heat conduction profile (either fixed or through Kramers opacity law) leads to a relatively shallow power law with dos ∝ ℱn0.08 for low ℱn. A fixed step-profile of the heat conductivity at the bottom of the convection zone leads to a somewhat steeper dependency on dos ∝ ℱn0.12 in the same regime. Experiments with and without subgrid-scale entropy diffusion revealed a strong dependence on the effective Prandtl number, which is likely to explain the steep power laws as a function of ℱn reported in the literature. Furthermore, changing the heat conductivity artificially in the radiative and overshoot layers to speed up thermal saturation is shown to lead to a substantial underestimation of the overshooting depth. Conclusions. Extrapolating from the results obtained with smooth heat conductivity profiles, which are the most realistic set-up we considered, suggest that the overshooting depth for the solar energy flux is about 20% of the pressure scale height at the base of the convection zone. This is two to four times higher than the estimates from helioseismology. However, the current simulations do not include rotation or magnetic fields, which are known to reduce convective overshooting.


2019 ◽  
Vol 15 (S352) ◽  
pp. 293-294
Author(s):  
Matus Rybak ◽  
J. A. Hodge ◽  
G. Calistro Rivera ◽  

AbstractSubmillimeter galaxies at redshift z⩾1 show a pronounced [CII]/FIR deficit down to sub-kpc scales; however, the physical origin of this deficit remains poorly understood. We use resolved ALMA observations of the [CII], FIR and CO(3–2) emission in two z = 3 SMGs to distinguish between the different proposed scenarios; the thermal saturation of the [CII] emission is the most likely explanation.


2019 ◽  
Vol 7 (37) ◽  
pp. 11449-11456 ◽  
Author(s):  
Yirong Xu ◽  
Shuxing Li ◽  
Peng Zheng ◽  
Le Wang ◽  
Shihai You ◽  
...  

Clarification of thermal saturation helps to guide the design of high-brightness yellow and green components for laser lighting and displays.


2016 ◽  
Vol 140 (4) ◽  
pp. 3034-3034 ◽  
Author(s):  
Timothy A. Brungart ◽  
James J. Chatterley ◽  
Benjamin S. Beck ◽  
Brian L. Kline ◽  
Zachary W. Yoas

2016 ◽  
Author(s):  
Timothy A. Brungart ◽  
James J. Chatterley ◽  
Benjamin S. Beck ◽  
Brian L. Kline ◽  
Zachary W. Yoas

2015 ◽  
Vol 109 ◽  
pp. 291-303 ◽  
Author(s):  
Anuj Mathur ◽  
Ankit Kumar Surana ◽  
Poonam Verma ◽  
Sanjay Mathur ◽  
G.D. Agrawal ◽  
...  

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