共查询到19条相似文献,搜索用时 156 毫秒
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《内燃机与动力装置》2016,(1):51-54
斯特林发动机作为一种外部燃烧的发动机,具有燃料来源广、污染小、噪声低和维修方便等优点,对节能与环保具有积极的意义,而其中的β型斯特林发动机更是具有体积小、传动平稳、易于密封等优点,具有广泛的应用前景。本文针对一款β型三曲拐闭式循环斯特林发动机,进行了工作过程数学建模、运用simulink软件进行仿真,根据仿真与分析结果,得到了不同气体工质功率输出与热效率随转速变化的规律。结果表明,在斯特林发动机不同转速运行范围内,应采用不同的气体作为工质,才能获得较高的功率输出与热效率。 相似文献
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正据《Энергетцка》2013年5-6月刊报道,亚美尼亚国立工程大学的学者研究了斯特林发动机近实际条件下的效率,并尝试考虑与热交换有限值有关的热量回收损失。在工质为范德华尔斯气体的条件下,得到在无回热器和有回热器情况下斯特林发动机的绝对内效率。结果表明,在考虑分子体积情况下,斯特林发动机的热效率取决于工质的克分子数并且比理想气体稍有增加。同时,考虑了斯特林发动机在热量与回收情况下的运行热损失,得到了回热度与热交换时间的相互关系。 相似文献
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钱达仁 《能源技术(上海)》2000,21(1):61-61
1979年Ceperley首先提出热声斯特林发动机的设想,但是他做的模型未能运转。其后的热声发动机(又称热声热机)采用不可逆驻波热声循环,热效率较低。1999年5月,“NATURE”刊载美国能源部LosAlamos国家试验室科学家S.Backhaus和G.Swift的文章:“热声斯特林热发动机(AthermoacousticStirlingHeatEngine)”,采用可逆斯特林循环热声热机,使热效率大大提高。热声斯特林发动机被认为是21世纪的发动机,将有可能替代传统的发动机——内燃机。国外许多刊物的“未来的发动机”、“没有运动件的发动机”、“无活塞热气机——热声发展的方向”等为题… 相似文献
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考虑热阻时发动机理论循环分析 总被引:3,自引:0,他引:3
根据发动机仅考虑热阻时,其混合加热循环的有限时间热力学模型,建立了发动机输出功率,热效率与循环参数εc,λp,ρo之间的函数关系,并依此对某实际柴油机进行了计算。计算结果表明,有限时间热力学较之传统热力学更深刻地反映发动机的实际循环。 相似文献
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Optimization of Output Power and Thermal Efficiency of Solar‐Dish Stirling Engine Using Finite Time Thermodynamic Analysis
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This paper presents an investigation on finite time thermodynamic (FTT) evaluation of a solar‐dish Stirling heat engine. FTTs has been applied to determine the output power and the corresponding thermal efficiency, exergetic efficiency, and the rate of entropy generation of a solar Stirling system with a finite rate of heat transfer, regenerative heat loss, conductive thermal bridging loss, and finite regeneration process time. Further imperfect performance of the dish collector and convective/radiative heat transfer mechanisms in the hot end as well as the convective heat transfer in the heat sink of the engine are considered in the developed model. The output power of the engine is maximized while the highest temperature of the engine is considered as a design parameter. In addition, thermal efficiency, exergetic efficiency, and the rate of entropy generation corresponding to the optimum value of the output power is evaluated. Results imply that the optimized absorber temperature is some where between 850 K and 1000 K. Sensitivity of results against variations of the system parameters are studied in detail. The present analysis provides a good theoretical guidance for the designing of dish collectors and operating the Stirling heat engine system. 相似文献
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Iskander Tlili 《Renewable & Sustainable Energy Reviews》2012,16(4):2234-2241
Maximum power and efficiency at the maximum power point of an endoreversible Stirling heat engine with finite heat capacitance rate of external fluids in the heat source/sink reservoirs with regenerative losses are treated. It was found that the thermal efficiency depends on the regenerator effectiveness and the internal irreversibility resulting from the working fluid for a given value of reservoir temperature. It was also concluded that it is desirable to have larger heat capacity of the heat sink in comparison to the heat source reservoir for higher maximum power output and lower heat input. 相似文献
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P. C. T. de Boer 《国际能源研究杂志》2009,33(9):813-832
The key component of a Stirling engine is its regenerative heat exchanger. This device is subject to losses due to dissipation arising from the flow through the regenerator as well as due to imperfect heat transfer between the regenerator material and the gas. The magnitudes of these losses are characterized by the Stanton number St and the Fanning friction factor f, respectively. Using available data for the ratio St/f, results are found for the Carnot efficiency and the power output of the regenerator. They depend on the conductance and on the ratio of pressures at the two sides of the regenerator. Optimum results for efficiency and power output of the regenerator are derived in the limit of zero Mach number. The results are applied to the Stirling engine. The efficiency and the power output of the engine are found for given amplitude of the compression piston. Optimization with respect to regenerator conductance and piston phase angle leads to a maximum possible value of the power output. Under optimal conditions, the Carnot efficiency just below this maximum is close to 100%. Copyright © 2009 John Wiley & Sons, Ltd. 相似文献
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In the recent years, numerous studies have been done on Stirling cycle and Stirling engine which have been resulted in different output power and engine thermal efficiency analyses. Finite speed thermodynamic analysis is one of the most prominent ways which considers external irreversibilities. In the present study, output power and engine thermal efficiency are optimized and total pressure losses are minimized using NSGA algorithm and finite speed thermodynamic analysis. The results are successfully verified against experimental data. 相似文献
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James D. Van de Ven 《Renewable Energy》2009,34(11):2317-2322
Conventional mobile hydraulic power supplies involve numerous kinematic connections and are limited by the efficiency, noise, and emissions of internal combustion engines. The Stirling cycle possesses numerous benefits such as the ability to operate from any heat source, quiet operation, and high theoretical efficiency. The Stirling engine has seen limited success due to poor heat transfer in the working chambers, difficulty sealing low-molecular weight gases at high pressure, and non-ideal piston displacement profiles. As a solution to these limitations, a liquid piston Stirling engine pump is proposed. The liquid pistons conform to irregular volumes, allowing increased heat transfer through geometry features on the interior of the working chambers. Creating near-isothermal operation eliminates the costly external heat exchangers and increases the engine efficiency through decreasing the engine dead space. The liquid pistons provide a positive gas seal and thermal transport to the working chambers. Controlling the flow of the liquid pistons with valves enables matching the ideal Stirling cycle and creates a direct hydraulic power supply. Using liquid hydrogen as a fuel source allows cooling the compression side of the engine before expanded the fuel into a gas and combusting it to heat the expansion side of the engine. Cooling the compression side not only increases the engine power, but also significantly increases the potential thermal efficiency of the engine. A high efficiency Stirling engine makes energy regeneration through reversing the Stirling cycle practical. When used for regeneration, the captured energy can be stored in thermal batteries, such as a molten salt. The liquid piston Stirling engine pump requires further research in numerous areas such as understanding the behavior of the liquid pistons, modeling and optimization of a full engine pump, and careful selection of materials for the extreme operating temperatures. Addressing these obtainable research quandaries will enable a transformative Stirling engine pump with the potential to excel in numerous applications. 相似文献
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Kiran Mansuriya Bansi D. Raja Ali R. Yıldız Anurag Mudgal Vivek K. Patel 《亚洲传热研究》2021,50(8):8155-8172
With the daily rise in environmental issues due to the use of conventional fuels, researchers are motivated to use renewable energy sources. One of such waste heat and low-temperature differential driven energy sources is the Stirling engine. The performance of the Stirling engine can be improved by finding out the optimum operating and geometrical parameters with suitable working gas and thermal model. Based on this motivation, the current work focuses on the multiobjective optimization of the Stirling engine using the finite speed thermodynamic model and methane gas as the working fluid. Considering output power and pressure drop as two objective functions, the system is optimized using 11 geometrical and thermal design parameters. The optimization results are obtained in the form of the Pareto frontier. A sensitivity assessment is carried out to observe the decision variables, which are having a more sensitive effect on the optimization objectives. Optimization results reveal that 99.83% change in power output and 78% change in total pressure drop can take place in the two-dimensional optimization space. The optimal solution closest to the ideal solution has output power and pressure drop values as 12.31 kW and 22.76 kPa, respectively. 相似文献
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This paper provides a theoretical investigation on the optimum absorber temperature of a once-reflecting full conical concentrator for maximizing overall efficiency of a solar-powered low temperature differential Stirling engine. A mathematical model for the overall efficiency of the solar-powered Stirling engine is developed. The optimum absorber temperature for maximum overall efficiency for both limiting conditions of maximum possible engine efficiency and maximum possible engine power output is determined. The results indicated that the optimum absorber temperatures calculated from these two limiting cases are not significantly different. For a given concentrated solar intensity, the maximum overall efficiency characterized by the condition of maximum possible engine power output is very close to that of the real engine of 55% Carnot efficiency, approximately. 相似文献
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Performance of a twin power piston low temperature differential Stirling engine powered by a solar simulator 总被引:1,自引:1,他引:0
This paper provides an experimental investigation on the performance of a low-temperature differential Stirling engine. In this study, a twin power piston, gamma-configuration, low-temperature differential Stirling engine is tested with non-pressurized air by using a solar simulator as a heat source. The engine testing is performed with four different simulated solar intensities. Variations of engine torque, shaft power and brake thermal efficiency with engine speed and engine performance at various heat inputs are presented. The Beale number, obtained from the testing of the engine, is also investigated. The results indicate that at the maximum simulated solar intensity of 7145 W/m2, or heat input of 261.9 J/s, with a heater temperature of 436 K, the engine produces a maximum torque of 0.352 N m at 23.8 rpm, a maximum shaft power of 1.69 W at 52.1 rpm, and a maximum brake thermal efficiency of 0.645% at 52.1 rpm, approximately. 相似文献