Nonimaging Optics Winston Episode 2 pot

Markov Processes, Gaussian Processes, and Local Times-CUP Episode 2 pot

Markov Processes, Gaussian Processes, and Local Times-CUP Episode 2 pot

... processes 523 11.7 Notes and references 526 12 Local times of diffusions 530 12. 1 Ray’s Theorem for diffusions 530 12. 2 Eisenbaum’s version of Ray’s Theorem 534 12. 3 Ray’s original theorem 537 12. 4 Markov ... of local times of diffusions 543 12. 5 Local limit laws for h-transforms of diffusions 549 12. 6 Notes and references 550 13 Associated Gaussian processes 551 13....

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Smog - A REPORT TO THE PEOPLE Episode 2 pot

Smog - A REPORT TO THE PEOPLE Episode 2 pot

... However, propane supply is increasing rapidly in the 1970's, Canadian propane supplies are available, and the figure of 8% is regarded by the Pace Company as a reasonable initial target that would not place too great a ... against the economic and social costs of these measures. The Clean Air Act of 1970 (as amended) appears to give the Administrator of the EPA discre...

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Nonimaging Optics Winston Episode 1 doc

Nonimaging Optics Winston Episode 1 doc

... n 2 a 2 q 2 . 11 . Global Optimization of High-Performance Concentrators (by Narkis Shatz and John C. Bortz) 265 11 .1 Introduction 265 11 .2 Mathematical Properties of Mappings in Nonimaging Optics 266 11 .3 ... Optics 17 2 7.7 Freeform Optical Designs for Point Sources in 3D 17 3 References 17 8 8. Simultaneous Multiple Surface Design Method 18 1 8 .1 Introduction 18 1 8...

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Nonimaging Optics Winston Episode 2 pot

Nonimaging Optics Winston Episode 2 pot

... falls off (r/R) 2 = (1/sinq) 2 . Concave Focusing Mirror q s q s q s rq s F r D /2 D = 2 r sin f C = (D/d) 2 = (1/4) sin 2 2f / sin 2 q s £ (1/4)1/ sin 2 q s £ (1/4) C max d = 2 r sin q / cos ... sing C a a n n max sin =  ấ ậ =  ấ ậ 22 q C n n max sin =  q 22 Chapter 2 Some Basic Ideas in Geometrical Optics from obvious geometrical considerations q cannot exc...

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Nonimaging Optics Winston Episode 3 doc

Nonimaging Optics Winston Episode 3 doc

... angles. Appl. Opt. 15, 2880–28 83. Ries, H., and Rabl, A. (1994). Edge-ray principle of nonimaging optics, J. Opt. Soc. Am. A 11, 2627–2 632 . Weatherburn, C. E. (1 931 ). “Differential Geometry of ... design. Sol. Energy 16, 89–95. Winston, R. (1976a). Dielectric compound parabolic concentrators. Appl. Opt. 15, 291–292. Winston, R. (1976b). U.S. letters patent 39 23 381, “Radiant Ene...

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Nonimaging Optics Winston Episode 4 docx

Nonimaging Optics Winston Episode 4 docx

... Konzentra- tionswirkung. Optik 25, 31 43 . Ries, H. R., and Wintson, R. (19 94) . Tailored edge-ray reflectors for illumination. JOSA, A, 11, 1259–12 64. Winston, R. (19 74) . Principles of solar concentrators ... ++ ( ) - [] + ẽ è ễ ể ễ á ễ ễ p p 2 4 1 2 4 1 222 222 2 22 12 222 222 2 22 12 102 Chapter 6 The Flow-line Method for Designing Nonimaging Optical Systems A B P J C D E C Â...

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Nonimaging Optics Winston Episode 5 pot

Nonimaging Optics Winston Episode 5 pot

... Designing Nonimaging Optical Systems Symmetry axis i 3 line ray cos -1 (u 1 /a 1 ) i 2 line i 1 line cos -1 (u 2 /a 2 ) 0,0 0 ,5 1,0 1 ,5 2,0 2 ,5 3,0 -1 ,5 -1,0 -0 ,5 0,0 0 ,5 1,0 1 ,5 x 3 i 3 ... =a ii j j j j j j 22 0123 a a ,, 124 Chapter 6 The Flow-line Method for Designing Nonimaging Optical Systems (6.64) Derivation of Eqs. (6 .54 ) and (6 .55 ) gives (6....

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Nonimaging Optics Winston Episode 6 ppt

Nonimaging Optics Winston Episode 6 ppt

... 4, 66 68 . Winston, R., and Welford, W. T. (1979). Geometrical Vector Flux and some new imaging concentrators. J. Opt. Soc. Am. A. 69 , 532–5 36. 158 Chapter 6 The Flow-line Method for Designing Nonimaging ... is obtained: (6. 1 36) It is straightforward to see that the 15 equations Eq. (6. 1 36) and the 18 equations Eq. (6. 129) are equivalent: Eq. (6. 1 36) can be obtained from Eq...

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Nonimaging Optics Winston Episode 7 docx

Nonimaging Optics Winston Episode 7 docx

... a prescribed 7. 7 Freeform Optical Designs for Point Sources in 3D 173 which can also be written as (7. 34) 7. 7.3 Mathematical Statement of the Problem Eqs. (7. 29), (7. 32), and (7. 34) form a system ... means of (7. 37) Assume that we have two functions sˆ(u, v) yrˆ(u, v) satisfying the system of Eq. (7. 36), then we have two functions r(u, v) ys(u, v) fulfilling Eq. (7. 28) y Eq. (...

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Nonimaging Optics Winston Episode 8 doc

Nonimaging Optics Winston Episode 8 doc

... 98. 2 98. 3 95.7 T t considering shadow losses (%) 99.4 98. 2 97 .8 94.3 T t considering shadow reflection and 84 .9 84 .5 85 .2 82 .6 Fresnel losses (%) Concentrator aperture diameter 91.9 77.5 51 .8 ... Transfer III (Winston, R., ed.). Proceedings of SPIE, Vol. 25 38, 30–41. Gleckman, P., O’Gallagher, J., and Winston, R. (1 989 ). Approaching the irradiance of the sun through nonimag...

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Nonimaging Optics Winston Episode 9 pptx

Nonimaging Optics Winston Episode 9 pptx

... Luneburg, R. K. ( 196 4). Mathematical Theory of Optics. University of California, Berkeley. Schulz, G. ( 198 2). Higher order aplanatism. Optics Communications 41, 315–3 19. Schulz, G. ( 198 5). Aberration-free ... LXII, 2–8. Welford, W. T., and Winston, R. ( 197 8). On the problem of ideal flux concentrators. J. Opt. Soc. Am. 68, 531–534. Welford, W. T., and Winston, R. ( 197 9). On th...

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Nonimaging Optics Winston Episode 10 potx

Nonimaging Optics Winston Episode 10 potx

... are given in Eqs. (10. 71) and (10. 81), respectively. We assume the total surface area of the target is (10. 86) Eq. (10. 71) then allows us to calculate the target étendue: (10. 87) When the source ... Eqs. (10. 81) and (10. 87) give the following value for the total surface area of the source: (10. 88) For this equal-étendue case, Figure 10. 11 depicts the skewness distributions of Eqs...

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Nonimaging Optics Winston Episode 11 pps

Nonimaging Optics Winston Episode 11 pps

... f: (11. 64) Substitution of Eq. (11. 63) into Eq. (11. 61) gives the x-coordinate as a function of f: (11. 65) For the special case of b = 0°, Eqs. (11. 64) and (11. 65) become (11. 66) and (11. 67) For the special ... . rrf () = 0 290 Chapter 11 Global Optimization of High-Performance Concentrators (11. 80) and (11. 81) For b = 90°, we find that (11. 82) and (11. 83) For b = 180°, w...

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Nonimaging Optics Winston Episode 12 pptx

Nonimaging Optics Winston Episode 12 pptx

... efficiency drops only 3% over a span of 13.3 Nonimaging Concentrators for Solar Thermal Applications 341 Figure 13.23 Stationary primary with tracking nonimaging secondary solar concentrator for ... a necessary space or gap between absorber and reflector, Cg falls short of 1. With the advent of nonimaging optics and the recognition of the sine law of concentra- tion the situation change...

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