共查询到20条相似文献,搜索用时 78 毫秒
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采用数值模拟方法研究了不同模型的相变蓄热单元蓄/放热过程以及入口流体温度对蓄热过程的影响。结果表明:沿轴向方向,不同截面的蓄/放热时间相差很大,轴向方向的自然对流对蓄/放热的影响较小;添加分形肋片提高蓄/放热速率的效果最好;在蓄热过程中,模型4和模型5的蓄热时间相比于模型1均缩短了45.4%;在放热过程中,模型2~模型5相比于模型1的放热时间分别缩短了12.3%、13.7%、27.4%和34.2%;提高入口流体温度可以显著缩短蓄热时间,但蓄热速率的增幅逐渐减小,当入口流体温度高于358.15 K时,入口流体温度对融化时间的影响明显减小。 相似文献
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蓄热可应对太阳能光热利用中的间歇性问题,可提供平稳的热能输出,提高能源品质。固液相变蓄热因其蓄热密度大、蓄/放热过程温度恒定等优点备受关注。固液相变蓄热过程中存在相变材料熔化与温度不均匀的现象,难熔区域极大地延长了整体相变蓄热时间。本工作提出了一种通过改变蓄热罐形状来改善熔化不均匀现象的设计方法,设计了5种具有不同梯度比的梯形相变蓄热罐;通过数值模拟方法研究了5种梯形蓄热罐的蓄热性能,得出以下结论:增加上部区域相变材料的比例有利于将热量及时传递到固态区域,减小了热量传递的阻力,加快了整体传热速率。增加上部区域相变材料比例(即模型1和模型2)的完全熔化时间较基准模型3的完全熔化时间都有缩短,分别减少了39.06%和29.37%。研究结果为相变蓄热罐结构设计和工程应用提供一定参考。 相似文献
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以赤藻糖醇为相变材料,采用Fluent软件对同心套管式相变蓄热单元的熔化和凝固过程进行了三维非稳态数值研究。在考虑自然对流的前提下,对比了水平入射式、顶部入射式及底部入射式相变蓄热单元的传热特性,得到了固液界面分布图和温度云图随时间的变化特性,对比了各自的蓄放热速率。研究表明:自然对流在熔化过程中起主要作用,而在凝固过程中起的作用很小;蓄热速率从大到小排列,依次是水平入射式、顶部入射式和底部入射式,相比于底部入射式,水平入射式的总熔化时间可减少27.2%,而顶部入射式的总熔化时间仅减少3.7%;放热速率从大到小排列,依次是顶部入射式、水平入射式和底部入射式,相比于底部入射式,顶部入射式的总凝固时间可减少9.2%,而水平入射式的总凝固时间仅减少0.6%;水平入射式蓄热单元是满足蓄放热速率快这一要求的首选型式。 相似文献
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高温肋板式蓄热器蓄/放热特性的数值模拟 总被引:1,自引:0,他引:1
采用计算流体动力学方法对高温不锈钢肋板式相变蓄热器的蓄/放热特性进行了数值模拟。分析了多孔肋片和锯齿肋片对蓄热器蓄/放热特性的影响以及载热体入口温度和流量对相变材料熔化和凝固速度的影响,计算结果表明:在该新型肋板式相变蓄热器中,多孔翅片的性能优于锯齿肋片;随着蓄热器传热温差的增大和载热体流量的增加,蓄热器的蓄/放热性能越好;肋片作为换热元件可以很好的提高蓄热器的蓄/放热性能。所得结论可为高温肋板式蓄热器的优化设计提供有益的参考。 相似文献
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针对解决太阳能热利用过程中所面临的辐射强度不稳定、不连续和不均匀等关键问题,相变蓄热技术常与太阳能热利用系统耦合协同匹配,以实现稳定连续的热量输出。为了强化固液相变蓄热/放热过程、提高系统热储能效率,对金属泡沫内石蜡类相变材料(PCMs)在不同蓄热流体温度下的固液相变蓄热/放热特性开展了实验研究。设计并搭建了相界面可视化的蓄热/放热实验系统,实验过程中使用高清相机对相变过程中的相界面变化进行了记录。同时,通过在蓄热单元内部布置多个热电偶测点,对蓄热/放热过程中的温度变化规律进行了探究。实验结果表明,受自然对流影响,熔化过程中相界面由上至下变化;而凝固过程中由于初始时蓄热单元下部温度较低且存在自然对流,此时相界面自下而上变化。蓄热流体温度越高,熔化所需时间越短,与蓄热流体温度为65℃的工况相比,蓄热流体温度为85℃、80℃、75℃、70℃工况的完全熔化时间分别减少了56.0%、46.7%、15.4%和26.7%。当采用不同温度的流体进行蓄热工况时,相变材料内部温度呈现出具有明显差别的温升规律。尽管如此,当采用相同温度的换热流体进行放热工况时,相变材料的放热温度仍趋于一致。 相似文献
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Beatriz López-Walle Michaël Gauthier Nicolas Chaillet 《International Journal of Thermal Sciences》2010,49(11):2108-2116
Thermal actuators are extensively used in microelectromechanical systems (MEMS). Heat transfer through and around these microstructures are very complex. Knowing and controlling them in order to improve the performance of the micro-actuator, is currently a great challenge. This paper deals with this topic and proposes a dynamic thermal modelling of thermal micro-actuators. Thermal problems may be modelled using electrical analogy. However, current equivalent electrical models (thermal networks) are generally obtained considering only heat transfers through the thickness of structures having considerable height and length in relation to width (walls). These models cannot be directly applied to micro-actuators. In fact, micro-actuator configurations are based on 3D beam structures, and heat transfers occur through and around length. New dynamic and static thermal networks are then proposed in this paper. The validities of both types of thermal networks have been studied. They are successfully validated by comparison with finite elements simulation and analytical calculations. 相似文献
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Thermal diffusion of hydrogen atoms in zirconium taking into account thermal stresses is investigated. As mathematical model the steady-state temperature in the hollow cylinder is considered. The first invariant of the tensor of thermal stresses in the hollow cylinder has a logarithmic dependence on the radial coordinate. Such dependence permits an exact analytical solution of diffusion kinetics problem in view of thermal stresses. 相似文献
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Simple thermal decomposition reactions have been investigated for the purpose of solar thermal energy storage. Ten criteria regarding the thermodynamics and kinetics of the reaction and the physical properties of the components of the reaction have been established. One particular reaction, the decomposition of ammonium hydrogen sulfate, has been evaluated in a preliminary manner and appears to satisfy all of the established criteria. The efficiency of storage is high and the decomposition occurs in the vicinity of 500°C. Other compounds such as ammonium halides, alkali and alkaline earth metal hydroxides, carbonates, sulfates and oxides have also been examined. 相似文献
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In a photovoltaic/thermal combi-panel solar cells generate electricity while residual heat is extracted to be used for tap water heating or room heating. In such a panel the entire solar spectrum can be used in principle. Unfortunately long wavelength solar irradiance is poorly absorbed by the semiconductor material in standard solar cells. A computer model was developed to determine the thermal absorption factor of crystalline silicon solar cells. It was found that for a standard untextured solar cell with a silver back contact a relatively large amount of long wavelength irradiance is lost by reflection resulting in an absorption factor of only 74%. The model was then used to investigate ways to increase this absorption factor. One way is absorbing long wavelength irradiance in a second absorber behind a semi-transparent solar cell. According to the model this will increase the total absorption factor to 87%. The second way is to absorb irradiance in the back contact of the solar cell by using rough interfaces in combination with a non-standard metal as back contact. Theoretically the absorption factor can then be increased to 85%. 相似文献
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Andreas E. Moschatos 《Solar Energy》1993,51(5)
In this study a combination of the two basic storages, the water storage and the bed storage, is examined. Formulas and limitations of the combined storage process, for a specific geometrical shape, are presented and the exploitation of the thermal losses of the water storage is attempted. 相似文献
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Standard methods of charging solar thermal energy into rock bed storage for space heating tend to reduce stratification because of decreasing collector temperatures in the afternoon. This creates inaccessible regions of higher temperature rocks and may reduce the amount of energy within the bed. Stratification of the segmented bed has the advantages of supplying the highest temperature air to the dwelling and the lowest temperature air to the collector. A method of preserving the stratification by segmenting the storage bed was numerically studied. Discharging was not studied.Segmenting a standard rock bed and routing the flow to segments cooler than the inlet air during charging was shown to preserve stratification throughout the bed. The simulated segmented bed contained 1% less maximum energy than an otherwise identical standard bed for an approximated solar day. This was a consequence of the segment control temperature locations. 相似文献
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Solar energy is an attractive renewable energy source because the sun's energy is plentiful and carbon-free. However, solar energy is intermittent and not suitable for base load electricity generation without an energy backup system. Concentrated solar power (CSP) is unique among other renewable energy options because it can approach base load generation with molten salt thermal energy storage (TES). This paper describes the development of an engineering economic model that directly compares the performance, cost, and profit of a 110-MW parabolic trough CSP plant operating with a TES system, natural gas-fired backup system, and no backup system. Model results are presented for 0–12 h backup capacities with and without current U.S. subsidies. TES increased the annual capacity factor from around 30% with no backup to up to 55% with 12 h of storage when the solar field area was selected to provide the lowest levelized cost of energy (LCOE). Using TES instead of a natural gas-fired heat transfer fluid heater (NG) increased total plant capital costs but decreased annual operation and maintenance costs. These three effects led to an increase in the LCOE for PT plants with TES and NG backup compared with no backup. LCOE increased with increasing backup capacity for plants with TES and NG backup. For small backup capacities (1–4 h), plants with TES had slightly lower LCOE values than plants with NG backup. For larger backup capacities (5–12 h), plants with TES had slightly higher LCOE values than plants with NG backup. At these costs, current U.S. federal tax incentives were not sufficient to make PT profitable in a market with variable electricity pricing. Current U.S. incentives combined with a fixed electricity price of $200/MWh made PT plants with larger backup capacities more profitable than PT plants with no backup or with smaller backup capacities. In the absence of incentives, a carbon price of $100–$160/tonne CO2eq would be required for these PT plants to compete with new coal-fired power plants in the U.S. If the long-term goal is to increase renewable base load electricity generation, additional incentives are needed to encourage new CSP plants to use thermal energy storage in the U.S. 相似文献