Knowledge (XXG)

Acceptance angle (solar concentrator)

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345: 250: 139: 57: 226:, the acceptance angle is one dimensional, and the concentration has only weak dependence on off-pointing perpendicular to the focus direction. Point focus systems, on the other hand, are sensitive to off-pointing in both directions. In the general case, the acceptance angle in one direction may be different from the other. 327:
contributes to a decrease in the acceptance angle of the concentrator. The acceptance angle may then be seen as a "tolerance budget" to be spent on all these imperfections. At the end, the concentrator must still have enough acceptance to capture sunlight which also has some angular dispersion
364:, as indicated by the green rays. If the acceptance angle of the optic is wide enough, sunlight incident along the optical axis will be captured by the concentrator, as shown in the "angular aperture of sunlight" figure. However, for wider incidence angles 476:
in which the receiver is immersed. In practice, real concentrators either have a lower than ideal concentration for a given acceptance or they have a lower than ideal acceptance angle for a given concentration. This can be summarized in the expression
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Parallel rays and sunlight are therefore transmitted differently by a solar concentrator and the corresponding transmission curves are also different. Different acceptance angles may then be determined for parallel rays or for sunlight.
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to the optical axis. For an ideal concentrator, all rays are still captured. However, on the right, this figure shows yet another set of parallel rays, now incident on the concentrator at an angle
529: 246:, the more precise the tracking needs to be or the concentrator will not capture the incoming sunlight. It is, therefore, a measure of the tolerance a concentrator has to tracking errors. 91:. All rays end up on the receiver and, therefore, all light is captured. In the center, this figure shows another set of parallel rays, now incident on the concentrator at an angle 368:
some light may be lost, as shown on the right. Perfectly parallel rays (shown in blue) would be captured, but sunlight, due to its angular aperture, is partially lost.
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which defines a quantity CAP (concentration acceptance product), which must be smaller than the refractive index of the medium in which the receiver is immersed.
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now has undulations and some of the light rays that were captured before are now lost. This decreases the transmission of the concentrator for incidence angle
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in which the receiver is immersed. Maximizing the acceptance angle of a concentrator is desirable in practical systems and it may be achieved by using
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when seen from earth. It is, therefore, very important to design a concentrator with the widest possible acceptance angle. That is possible using
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to the optical axis. However, real optics are never perfect and the right part of the figure shows the effect of a badly made bottom surface
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Figure "angular aperture of sunlight" on the right shows the effect of the angular dispersion of sunlight on the acceptance angle.
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For concentrators that concentrate light in two dimensions, the acceptance angle may be different in the two directions.
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In practice, real transmission curves are not perfect and they typically have a shape similar to that of curve
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to the optical axis. All rays now miss the receiver and all light is lost. Therefore, for incidence angles
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However, other errors also affect the acceptance angle. The "optical imperfections" figure shows this.
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Sunlight is not a set of perfectly parallel rays (shown in blue), but it has a given angular aperture
56: 741: 655: 306: 147: 34: 722: 702: 673: 338: 42: 663: 219: 38: 473: 725:. Note that in this derivation theta is the full angle, not the half-angle defined here. 659: 239: 735: 296:, decreasing the acceptance angle. Actually, any imperfection in the system such as: 68: 260:
The left part of the figure shows a perfectly made lens with good optical surfaces
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all light is lost. The concentrator is then said to have a (half) acceptance angle
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Maximum angle at which incoming sunlight can be captured by a solar concentrator
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The Concentration Acceptance Product is a consequence of the conservation of
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as shown in the "transmission curves" figure. Transmission (efficiency) is
668: 643: 30: 613: 601: 384:, for a point-focus concentrator, the maximum concentration possible, 457:{\displaystyle C_{\mathrm {max} }={\frac {n^{2}}{\sin ^{2}\theta }}} 238:
of a concentrator may be seen as a measure of how precisely it must
343: 248: 137: 55: 341:, which maximize the acceptance angle for a given concentration. 538:
For a linear-focused concentrator, the equation is not squared
37:. Its value depends on the concentration of the optic and the 723:
http://www.powerfromthesun.net/Book/chapter09/chapter09.html
590:{\displaystyle C_{\mathrm {max} }={\frac {n}{\sin \theta }}} 644:"High performance Fresnel-based photovoltaic concentrator" 211:
is typically defined as the angle for which transmission
75:. The left section of the figure shows a set of parallel 204: = 0. In that case, the real acceptance angle 64:
The "acceptance angle" figure illustrates this concept.
547: 486: 400: 589: 523: 456: 694:Introduction to Nonimaging Optics, Second Edition 524:{\displaystyle CAP={\sqrt {C}}\sin \theta \leq n} 115:all light is captured while for incidence angles 274:capturing all light rays incident at an angle 642:Benitez, Pablo; et al. (26 April 2010). 8: 317:finite stiffness of the supporting structure 19:For other uses of "Acceptance angle", see 667: 569: 553: 552: 546: 499: 485: 439: 428: 422: 406: 405: 399: 131:(since it accepts light within an angle ± 79:incident on the concentrator at an angle 175: = 0 for all incidence angles 160: = 1 for all incidence angles 634: 29:is the maximum angle at which incoming 376:Concentration acceptance product (CAP) 230:Acceptance angle as a tolerance budget 7: 242:the sun in the sky. The smaller the 146:Ideally, a solar concentrator has a 314:movements of the system due to wind 560: 557: 554: 413: 410: 407: 218:For line-focus systems, such as a 14: 323:other imperfections in the system 311:imperfectly assembled components 621:, acceptance angle context for 472:is the refractive index of the 303:imperfectly manufactured optics 127:, or a total acceptance angle 2 196:, which is normalized so that 1: 380:For a given acceptance angle 215:drops to 90% of its maximum. 348:Angular aperture of sunlight 285:. Instead of being smooth, 758: 18: 320:deformation due to aging 691:Chaves, Julio (2015). 591: 525: 458: 349: 254: 143: 135:to the optical axis). 67:The concentrator is a 61: 592: 526: 459: 347: 253:Optical imperfections 252: 234:The acceptance angle 141: 59: 33:can be captured by a 669:10.1364/OE.18.000A25 545: 484: 398: 660:2010OExpr..18S..25B 307:optical aberrations 300:tracking inaccuracy 220:trough concentrator 200: = 1 for 142:Transmission curves 587: 521: 454: 350: 255: 148:transmission curve 144: 62: 35:solar concentrator 585: 504: 452: 339:nonimaging optics 43:nonimaging optics 749: 726: 719: 713: 712: 688: 682: 681: 671: 639: 596: 594: 593: 588: 586: 584: 570: 565: 564: 563: 530: 528: 527: 522: 505: 500: 463: 461: 460: 455: 453: 451: 444: 443: 433: 432: 423: 418: 417: 416: 179: >  164: <  119: >  111: <  103: >  83: <  71:with a receiver 60:Acceptance angle 39:refractive index 27:Acceptance angle 21:Acceptance angle 757: 756: 752: 751: 750: 748: 747: 746: 732: 731: 730: 729: 720: 716: 709: 690: 689: 685: 641: 640: 636: 631: 610: 574: 548: 543: 542: 482: 481: 435: 434: 424: 401: 396: 395: 390: 378: 363: 336: 291: 284: 273: 266: 232: 210: 195: 185: 170: 155: 54: 24: 17: 12: 11: 5: 755: 753: 745: 744: 734: 733: 728: 727: 714: 708:978-1482206739 707: 683: 654:(S1): A25-40. 648:Optics Express 633: 632: 630: 627: 626: 625: 616: 609: 606: 598: 597: 583: 580: 577: 573: 568: 562: 559: 556: 551: 533: 532: 520: 517: 514: 511: 508: 503: 498: 495: 492: 489: 466: 465: 450: 447: 442: 438: 431: 427: 421: 415: 412: 409: 404: 391:, is given by 388: 377: 374: 359: 332: 325: 324: 321: 318: 315: 312: 309: 304: 301: 289: 282: 271: 264: 231: 228: 208: 193: 183: 168: 153: 53: 50: 15: 13: 10: 9: 6: 4: 3: 2: 754: 743: 740: 739: 737: 724: 718: 715: 710: 704: 700: 696: 695: 687: 684: 679: 675: 670: 665: 661: 657: 653: 649: 645: 638: 635: 628: 624: 620: 617: 615: 612: 611: 607: 605: 603: 581: 578: 575: 571: 566: 549: 541: 540: 539: 536: 518: 515: 512: 509: 506: 501: 496: 493: 490: 487: 480: 479: 478: 475: 471: 448: 445: 440: 436: 429: 425: 419: 402: 394: 393: 392: 387: 383: 375: 373: 369: 367: 362: 358: 353: 346: 342: 340: 335: 331: 322: 319: 316: 313: 310: 308: 305: 302: 299: 298: 297: 295: 288: 281: 277: 270: 263: 258: 251: 247: 245: 241: 237: 229: 227: 225: 221: 216: 214: 207: 203: 199: 192: 187: 182: 178: 174: 167: 163: 159: 152: 149: 140: 136: 134: 130: 126: 122: 118: 114: 110: 106: 102: 98: 95: =  94: 90: 86: 82: 78: 74: 70: 65: 58: 51: 49: 46: 44: 40: 36: 32: 28: 22: 717: 693: 686: 651: 647: 637: 623:optic fibres 599: 537: 534: 469: 467: 385: 381: 379: 370: 365: 360: 356: 354: 351: 333: 329: 326: 293: 286: 279: 275: 268: 261: 259: 256: 243: 235: 233: 224:Fresnel lens 222:or a linear 217: 212: 205: 201: 197: 190: 188: 180: 176: 172: 165: 161: 157: 150: 145: 132: 128: 124: 120: 116: 112: 108: 104: 100: 96: 92: 89:optical axis 84: 80: 72: 66: 63: 47: 26: 25: 742:Solar power 629:References 619:Guided ray 52:Definition 699:CRC Press 582:θ 579:⁡ 516:≤ 513:θ 510:⁡ 449:θ 446:⁡ 736:Category 678:20588570 608:See also 31:sunlight 656:Bibcode 614:Etendue 602:etendue 87:to the 705:  676:  474:medium 468:where 382:θ 366:α 357:θ 330:θ 294:α 276:α 244:θ 236:θ 213:τ 206:θ 202:α 198:τ 181:θ 177:α 173:τ 166:θ 162:α 158:τ 133:θ 129:θ 125:θ 121:θ 117:α 113:θ 109:α 105:θ 101:α 97:θ 93:α 85:θ 81:α 721:See: 240:track 703:ISBN 674:PMID 267:and 171:and 77:rays 69:lens 664:doi 576:sin 507:sin 437:sin 389:max 738:: 701:. 697:. 672:. 662:. 652:18 650:. 646:. 186:. 45:. 711:. 680:. 666:: 658:: 572:n 567:= 561:x 558:a 555:m 550:C 531:, 519:n 502:C 497:= 494:P 491:A 488:C 470:n 464:, 441:2 430:2 426:n 420:= 414:x 411:a 408:m 403:C 386:C 361:S 334:S 290:2 287:s 283:2 280:s 272:2 269:s 265:1 262:s 209:R 194:R 191:c 184:I 169:I 154:I 151:c 73:R 23:.

Index

Acceptance angle
sunlight
solar concentrator
refractive index
nonimaging optics

lens
rays
optical axis

transmission curve
trough concentrator
Fresnel lens
track

optical aberrations
nonimaging optics

medium
etendue
Etendue
Guided ray
optic fibres
"High performance Fresnel-based photovoltaic concentrator"
Bibcode
2010OExpr..18S..25B
doi
10.1364/OE.18.000A25
PMID
20588570

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