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References

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  1. H. Kayser, Handbuch der Spectroscopie (Leipzig, 1900), Vol. I, p. 258.
  2. A. C. Hardy and F. H. Perrin, The Principles of Optics (McGraw-Hill, Book Company, Inc., New York, 1923), pp. 86–87.
  3. See reference 2, p. 95.
  4. See reference 2, p. 103.

Hardy, A. C.

A. C. Hardy and F. H. Perrin, The Principles of Optics (McGraw-Hill, Book Company, Inc., New York, 1923), pp. 86–87.

Kayser, H.

H. Kayser, Handbuch der Spectroscopie (Leipzig, 1900), Vol. I, p. 258.

Perrin, F. H.

A. C. Hardy and F. H. Perrin, The Principles of Optics (McGraw-Hill, Book Company, Inc., New York, 1923), pp. 86–87.

Other (4)

H. Kayser, Handbuch der Spectroscopie (Leipzig, 1900), Vol. I, p. 258.

A. C. Hardy and F. H. Perrin, The Principles of Optics (McGraw-Hill, Book Company, Inc., New York, 1923), pp. 86–87.

See reference 2, p. 95.

See reference 2, p. 103.

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Figures (1)

Fig. 1
Fig. 1

Refraction of light ray in cross-sectional plane of prism.

Tables (1)

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Table I i1/i2 necessary to minimize spherical aberration and coma for a positive spherical lens.

Equations (9)

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n sin 1 2 A sin 1 2 ( A + D ) .
Prism apex angle = A = r 1 + r 2 .
Deviation of light ray = D = i 1 + i 2 - A ,
n sin r 1 = sin i 1 ,
n sin r 2 = sin i 2 .
n sin 1 2 A cos 1 2 ( r 1 - r 2 ) = sin 1 2 ( A + D ) cos 1 2 ( i 1 - i 2 ) .
n cos 1 2 A sin 1 2 ( r 1 - r 2 ) = cos 1 2 ( A + D ) sin 1 2 ( i 1 - i 2 ) .
n [ ( A / 2 ) - A 3 / 48 ] [ 1 - ( i 1 - i 2 ) 2 / 8 n 2 ] [ 1 2 ( A + D ) - ( A + D ) 3 / 48 ] [ 1 - ( i 1 - i 2 ) 2 / 8 ] .
D ( n - 1 ) A + [ n A 3 ( n 2 - 1 ) / 24 ] + ( i 1 - i 2 ) 2 A ( n 2 - 1 ) / 8 n .