|(b) The grating has 2,500 blazes/mm. The relationship between the reciprocal linear dispersion ( D-1), the focal length f, the order of the diffraction n and the distance between blazes (d) is given by the following equation. D-I = d Substitute the value of the focal length f(0.78 m), the order of the diffraction n (1) and the 1 mm distance between rulings (d) ( =) in the above equation 2,500 lines ( 1 mm D-1 - (2,500 lines 1x(0.78 m) nm - (2,500 lines ) (100 mm) 2,500 lines mm 1x(0.78 m )x(108 prend = 0.51 nm mm nm Therefore, the reciprocal linear dispersion ( D-1) for the first order diffraction is 0.51 mm
|(c)2.0 с of grating is illuminated The number N of grating lines illuminated is as calculated below N 2,500 lines x 20 cm = 1 mm = 50,000 lines 1 * 10 mm x 10 - em
The resolving power of a grating (R) is given by the following equation R = nN Where n is the diffraction order and N is the number of grating lines illuminated.
Substitute the value of the diffraction order n (1) and the number Nof grating lines illuminated in the above equation R = nN = 1 x 50,000 lines = 50,000 Therefore, the first order resolving power is 50,000
lid) The wavelength (a) is 410 nm. The resolving power of the grating is as given below R =- M = 50,000 Substitute the value of the wavelength (a) in the above equation 410 nm 50,000 M2 Rearrange the above equation 410 nm M = 50,000 = 8.2 x 10 nm Therefore, the minimum wavelength difference that can be theoretically completely resolved by the instrument is 8.2x10-3 nm ·