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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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Presentation on theme: "Measures of Source Intensity 1. Radiant Flux, Φ Rate of transfer of energy Φ = δQ/δt (W)"— Presentation transcript:

1 Measures of Source Intensity 1. Radiant Flux, Φ Rate of transfer of energy Φ = δQ/δt (W)

2 Measures of Source Intensity 2. Radiant Intensity, I Radiant flux per unit solid angle from a point source I = δΦ/δΩ (W/sr)

3 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 )

4 Measures of Source Intensity 4. Irradiance, E Radiant flux per unit projected area E = δΦ/δA (W cm -1 )

5 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 )

6 Optical Components of Imaging Systems 1. Windows 2. Lenses 3. Mirrors 4. Turning Prisms 5. Beam Splitters 6. Fiber Optics

7 Transmittance of Window Materials

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9 Reflectance of Mirror Materials

10 Interaction of Light with an Interface

11 Law of Specular Reflection Θ 1 = Θ 3 Snell’s Law of Refraction n 1 sin Θ 1 = n 2 sin Θ 2

12 Reflection Losses at an Interface (unpolarized light)

13 Reflection Losses at an Interface a = unpolarized b = perpendicularly polarized c = parallel polarized (Note Brewster’s Angle)

14 Reflection at an Interface (Total Internal Reflection) Propagating from high to low n

15 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

16 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

17 Lens Formula 1/S1 + 1/S2 = 1/f S1 = object distance S2 = image distance f = focal length

18 1/S1 + 1/S2 = 1/f

19 Relative Aperture of an Optical Component D/S 1 where: D = limiting diameter S 1 = distance from source

20 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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22 Beam Splitters

23 Optical Fibers

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25 Turning Prisms

26 Sample Cells


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