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Published byBarry Booth Modified over 9 years ago
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Measures of Source Intensity 1. Radiant Flux, Φ Rate of transfer of energy Φ = δQ/δt (W)
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Measures of Source Intensity 2. Radiant Intensity, I Radiant flux per unit solid angle from a point source I = δΦ/δΩ (W/sr)
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Measures of Source Intensity 3. Radiance, B Radiant flux per unit solid angle per unit projected area B = δ 2 Φ/(δΩ δA) (W sr -1 cm -1 )
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Measures of Source Intensity 4. Irradiance, E Radiant flux per unit projected area E = δΦ/δA (W cm -1 )
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Measures of Source Intensity 5. Spectral Radiance, B λ Radiance per unit wavelength interval B λ = B/δλ (W sr -1 cm -1 nm -1 )
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Optical Components of Imaging Systems 1. Windows 2. Lenses 3. Mirrors 4. Turning Prisms 5. Beam Splitters 6. Fiber Optics
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Transmittance of Window Materials
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Reflectance of Mirror Materials
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Interaction of Light with an Interface
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Law of Specular Reflection Θ 1 = Θ 3 Snell’s Law of Refraction n 1 sin Θ 1 = n 2 sin Θ 2
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Reflection Losses at an Interface (unpolarized light)
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Reflection Losses at an Interface a = unpolarized b = perpendicularly polarized c = parallel polarized (Note Brewster’s Angle)
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Reflection at an Interface (Total Internal Reflection) Propagating from high to low n
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Total Internal Reflection n 1 sin Θ 1 = n 2 sin Θ 2 n 1 > n 2 Θ 2 = 90 sin Θ 1 = n 2 / n 1
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Lens Maker’s Formula R 2 < 0 1/f = (n-1) (1/R 1 – 1/R 2 ) For a Biconvex Lens, R 1 = -R 2
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Lens Formula 1/S1 + 1/S2 = 1/f S1 = object distance S2 = image distance f = focal length
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1/S1 + 1/S2 = 1/f
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Relative Aperture of an Optical Component D/S 1 where: D = limiting diameter S 1 = distance from source
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F-number (F/n) F/n = S 1 /D The solid angle of light collected by an optical component is given by: Ω = (π/4) (F/n) -2
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Beam Splitters
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Optical Fibers
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Turning Prisms
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Sample Cells
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