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Resolving Power 1 1 1.

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Presentation on theme: "Resolving Power 1 1 1."— Presentation transcript:

1 Resolving Power 1 1 1

2 Not resolved Well resolved

3 Just resolved

4 Chromatic Resolving Power
The ability of the spectroscope or the interferometer to separate the components of multiplets is known as chromatic resolving power (CRP). In a two beam interferometer, like Michelson interferometer and Young’s double slit set-up, the bright fringes are as broad as the dark fringes. The fringes are not sharp. For good resolution, the bright fringes must be as sharp as possible.

5 Michelson fringes Fabry-Perot fringes 5

6 Fabry-Perot interferometer
Doublet separation in Fabry-Perot interferometer 6

7 Resolved wavelengths s: separation w: width 7

8 Unresolved wavelengths
8

9 Barely resolved 9

10 Chromatic resolving power of Fabry Perot interferometer
- Where, λ is the minimum wavelength interval of a doublet that the instrument is capable of barely resolving. - The criterion for bare resolution is called the Rayleigh criterion. - The smaller the value of λ, the higher is the resolving power of the instrument. Barely resolved Using: 2d cos θm= mλ ; ( Fabry-Perot - bright fringe in transmission ) 10

11 Telescope R.P. = 1.22 λ / D D= Diameter of the telescope objective

12 Single slit – Two point sources
R.P. = λ / b

13 Circular aperture

14 Chromatic resolving power of a grating
= m N


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