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chapter 2, Propagation of Optical Radiation

Author(s): James M. Palmer, Barbara G. Grant
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Chapter Contents

  • 2.1 Basic Definitions
  • 2.1.1 Rays and angles
  • 2.1.2 System parameters
  • 2.1.3 Optical definitions
  • 2.2 Fundamental Radiometric Quantities
  • 2.2.1 Radiance
  • 2.2.2 Radiant exitance
  • 2.2.3 Irradiance
  • 2.2.4 Radiant intensity
  • 2.3 Radiometric Approximations
  • 2.3.1 Inverse square law
  • 2.3.2 Cosine3 law
  • 2.3.3 Lambertian approximation
  • 2.3.4 Cosine4 law
  • 2.4 Equation of Radiative Transfer
  • 2.5 Configuration Factors
  • 2.6 Effect of Lenses on Power Transfer
  • 2.7 Common Radiative Transfer Configurations
  • 2.7.1 On-axis radiation from a circular Lambertian disc
  • 2.7.2 On-axis radiation from a non-Lambertian disc
  • 2.7.3 On-axis radiation from a spherical Lambertian source
  • 2.8 Integrating Sphere
  • 2.9 Radiometric Calculation Examples
  • 2.9.1 Intensities of a distant star and the sun
  • 2.9.2 Lunar constant
  • 2.9.2.1 Calculation
  • 2.9.2.2 Moon-sun comparisons
  • 2.9.3 “Solar furnace”
  • 2.9.4 Image irradiance for finite conjugates
  • 2.9.5 Irradiance of the overcast sky
  • 2.9.6 Near extended source
  • 2.9.7 Projection system
  • 2.10 Generalized Expressions for Image-Plane Irradiance
  • 2.10.1 Extended source
  • 2.10.2 Point source
  • 2.11 Summary of Some Key Concepts
  • For Further Reading
  • References

Excerpt

2.1 Basic Definitions

2.1.1 Rays and angles

A ray is represented by a vector: a straight line indicating the magnitude and direction of propagation. A wavefront is a notional surface locally normal to a ray. Thus, a wavefront could be a plane (all rays parallel, as if from infinity) or a curved surface (indicating diverging rays, as if emanating from a point). Figure 2.1 illustrates rays and wavefronts for both cases.

A beam can be defined by two separated elements of area as shown in Fig. 2.2. It is thus the locus of possible rays that pass through the two areas separated by distance d. As dA1 and dA2 approach zero, the beam approaches a single ray. Since there is a small, but nevertheless finite, cross-sectional area associated with a beam, it is capable of carrying power without the flux density (power per unit area) approaching infinity.



©2010 Society of Photo-Optical Instrumentation Engineers
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BOOK DATA

Print ISBN:

9780819472458

eISBN:

9780819479167

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