Fraunhoffer's lines Assignment Help

Assignment Help: >> Dispersion of light >> Fraunhoffer's lines

Fraunhoffer's lines: The central part (photosphere) of the sun is very hot and emits all possible wavelengths of the visible light. However, the outer part (chromospheres) consists of vapors of different components. When the light emitted from the photosphere passes through the chromospheres, certain wavelengths are real, Hence, in the spectrum of wave a large number of dark lines are seen called Fraunhoffer lines.

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(i) The prominent waves in the yellow section of the visible spectrum were labeled as D-lines, those in blue part as F-lines and in red part as C-line.

(ii) From the study of Fraunhoffer's lines the presence of various elements in the sun's atmosphere can be verified.

(iii) In the event of a solar eclipse, black lines convert into bright. This is because of the reason that the presence of an opaque obstacle in between sun and earth cuts the light off from the central region (photo-sphere), while light from corner portion (chromospheres) is still being achieved. The bright lines seem exactly at the places where dark lines were present.

Spectrometer: A spectrometer is needed for creating pure spectrum of a source in laboratory and calculation of μ of material of prism and μ of a transparent liquid.

It has of three parts: Collimator which provides a parallel beam of light; Prism Table for holding the prism and Telescope for observing the spectrum and making measurements on it.

The telescope is first set for parallel rays and then collimator is set for parallel waves. When prism is fixed in minimum deviation position, the spectrum seen is real spectrum. Angle of prism (A) and angle of minimum deviation (δm) are measured and m of material of prism is calculated using prism formula. For μ of a transparent liquid, we consider a hollow prism with thin mirror sides. Fill it with the liquid and measure (δm) and A of liquid prism. μ Of liquid is calculated using prism formula.

Direct vision spectroscope: It is an instrument used to observe pure spectrum. It produces dispersion without deviation with the help of n crown prisms and (n - 1½ flint prisms alternately arranged in a tabular structure.

For no deviation n(μ-1)A = (n-1)(μ′ - 1)A′.

 

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