Knowledge (XXG)

Thermodynamic efficiency limit

Source πŸ“

122: 1486: 177: 191: 1498: 72:, and so their energy is not converted to useful output and only generates heat if absorbed. For photons with an energy above the band gap energy, only a fraction of the energy above the band gap can be converted to useful output. When a photon of greater energy is absorbed, the excess energy above the band gap is converted to 83:
Solar cells with multiple band gap absorber materials improve efficiency by dividing the solar spectrum into smaller bins where the thermodynamic efficiency limit is higher for each bin. The thermodynamic limits of such cells (also called multi-junction cells, or tandem cells) can be analyzed using
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for the efficiency of a single-junction solar cell under unconcentrated sunlight. This calculated curve uses actual solar spectrum data, and therefore the curve is wiggly from IR absorption bands in the atmosphere. This efficiency limit of about 34% can be exceeded by
161:, the theoretical maximum efficiency is 43% whereas for a solar cell powered by the Sun's full concentrated radiation, the efficiency limit is up to 85%. These high values of efficiencies are possible only when the solar cells use 80:. The excess kinetic energy is converted to heat through phonon interactions as the kinetic energy of the carriers slows to equilibrium velocity. Hence, the solar energy cannot be converted to electricity beyond a certain limit. 157:
generation for each photon absorbed. Efficiency limits for photovoltaic cells can be theoretically higher considering thermodynamic effects. For a solar cell powered by the Sun's unconcentrated
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solar cells. The efficiency of the excitonic solar cells and inorganic solar cells (with less exciton-binding energy) cannot go beyond 31% as explained by Shockley and Queisser.
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Cheng-Hsiao Wu and Richard Williams (1983). "Limiting efficiencies for multiple energy-gap quantum devices".
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Excitonic solar cells generates free charge by bound and intermediate exciton states unlike inorganic and
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Giebink, Noel C.; Wiederrecht, Gary P.; Wasielewski, Michael R.; Forrest, Stephen R. (May 2011).
337: 154: 69: 1037: 1058: 1053: 986: 782: 721: 652: 642: 462: 1115: 1083: 1073: 544: 454: 421: 382: 280: 447:"Thermodynamic efficiency limits for semiconductor solar cells with carrier multiplication" 121: 1027: 958: 417: 378: 276: 1437: 1412: 1078: 930: 832: 822: 792: 549: 92:
Thermodynamic efficiency limits for different solar cell technologies are as follows:
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Khan, Mohammad Ryyan; Jin, Xin; Alam, Muhammad A. (20 March 2016).
60:, and are therefore subject to the thermodynamic efficiency limit. 402:"Detailed Balance Limit of Efficiency of p-n Junction Solar Cells" 120: 482: 486: 16:
Maximum possible efficiency of electrical power from sunlight
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Brendel, Rolf; Werner, JΓΌrgen H.; Queisser, Hans J. (1996).
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Thermodynamic efficiency limits with carrier multiplication
363:"Thermodynamic efficiency limit of excitonic solar cells" 117:
Thermodynamic efficiency limit for excitonic solar cells
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Hot carrier- or impact ionization-based devices β‰ˆ 54-68%
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Efficiency limits for different solar cell technologies
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Solar cell with an upconverter for operation in the
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Its value is about 86%, which is the 451:Solar Energy Materials and Solar Cells 7: 1497: 1214:List of photovoltaic power stations 240:"Nanostructured Organic Solar Cell" 1230:Rooftop photovoltaic power station 633:Polycrystalline silicon (multi-Si) 582:Third-generation photovoltaic cell 205:Quantum efficiency of a solar cell 99:3-cell stacks and impure PVs β‰ˆ 50% 38:, based on the temperature of the 34:, an approximation related to the 14: 1235:Building-integrated photovoltaics 732:Carbon nanotubes in photovoltaics 638:Monocrystalline silicon (mono-Si) 84:and online simulator in nanoHUB. 1496: 1485: 1484: 607:Polarizing organic photovoltaics 189: 175: 742:Cadmium telluride photovoltaics 623:List of semiconductor materials 105:Commercial modules are β‰ˆ 12-21% 854:Incremental conductance method 648:Copper indium gallium selenide 597:Thermodynamic efficiency limit 42:emitted by the Sun's surface. 20:Thermodynamic efficiency limit 1: 1161:South African Solar Challenge 326:(in German). 14 October 2022. 808:Photovoltaic mounting system 459:10.1016/0927-0248(95)00125-5 453:. 41–42. Elsevier: 419–425. 210:Energy conversion efficiency 165:and carrier multiplication. 32:Chambadal-Novikov efficiency 813:Maximum power point tracker 1551: 1064:Solar panels on spacecraft 911:Solar-powered refrigerator 869:Concentrated photovoltaics 849:Perturb and observe method 628:Crystalline silicon (c-Si) 406:Journal of Applied Physics 387:10.1103/PhysRevB.83.195326 1480: 762:Heterojunction solar cell 737:Dye-sensitized solar cell 577:Multi-junction solar cell 567:Nominal power (Watt-peak) 132:multijunction solar cells 64:with an energy below the 58:energy conversion devices 46:Effect of band gap energy 1245:Strasskirchen Solar Park 1136:American Solar Challenge 982:Solar-powered flashlight 969:Solar-powered calculator 964:Solar cell phone charger 653:Amorphous silicon (a-Si) 324:"Solar Yield calculator" 1535:Thermodynamic processes 1151:Frisian Solar Challenge 1121:List of solar car teams 879:Space-based solar power 859:Constant voltage method 788:Solar charge controller 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Index

conversion efficiency
electricity
Chambadal-Novikov efficiency
Carnot limit
photons
Solar cells
quantum
energy conversion devices
Photons
band gap
electron-hole pair
kinetic energy
carrier recombination
AM1.5

Shockley-Queisser limit
multijunction solar cells
crystalline
Carrier multiplication
electron-hole pair
black-body radiation
radiative recombination
icon
Renewable energy portal
icon
Energy portal
Quantum efficiency of a solar cell
Energy conversion efficiency
Photoelectric effect
Solar cell efficiency

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