The Elementary Theory of the Symmetrical Optical Instrument

Cover The Elementary Theory of the Symmetrical Optical Instrument
The Elementary Theory of the Symmetrical Optical Instrument
J G John Gaston Leathem
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It is therefore a suitable quantity to take as a measure of the extent to which the material behaves differently to the two standard colours, and is called the " dispersive power " of the sub- stance. It is usually written (A/O/fc-l) (93), the operator symbol A being used to denote the increment of the function of /x on which it operates when /* is changed from /^ to /* 2, and the suffix being dropped in the case of colour No. 3. For brevity the dispersive power is denoted by the symbol w. It m...ust be noted that a numerical value of TO for any particular substance is meaningless unless it is accompanied by a precise definition of the standard colours to which it refers.
The dispersive power w is usually a very small quantity. When colour No. 1 corresponds to the C line (in the red), colour No. 2 to the F line (in the blue), and colour No. 3 to the D line (in the yellow), the values of w for some different kinds of Jena glass are roughly 1/67, 1/55, 1/65, 1/51, 1/44.
48. Powers of a thin lens for different colours.


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