The definition is considered by some experimenters as somewhat better if the analyser be used above the eye-piece, and is certainly more easily rotated.

[Illustration: Fig. 180.--Prism mounted as an Eye-piece.]

The Microscope. Its History, Construction, and Application 15th ed. — Part 158

_Method of employing the Polarising Prism_ (Fig. 179).--After having adapted it to slide into a groove on the under-surface of the stage, where it is secured and kept in place by the small milled-head screw, the other prism (Fig. 179_a_) is screwed on above the object-glass, and thus passes directly into the body of the microscope. The light from the mirror having been reflected through them the axes of the two prisms must be made to coincide; this is done by regulating the milled-head screw until, by revolving the _polarising_ prism, the field of view is entirely darkened twice during its revolution. If very minute salts or crystals are submitted for examination then it will be found preferable to place the analyser above the eye-piece, as in Fig. 180. Thus the _polariscope_ is seen to consist of two parts; one for _polarising_, the other for _analysing_ or testing the light. There is no essential difference between the two parts, except what convenience or economy may lead us to adopt; and either part, therefore, may be used as polariser or analyser; but whichever is used as the polariser, the other becomes the analyser.

The Microscope. Its History, Construction, and Application 15th ed. — Part 158

[Illustration: Fig. 181.--More Modern Polariser and Analyser.]

The Microscope. Its History, Construction, and Application 15th ed. — Part 158

Opticians have their own methods of adapting the polariser and analyser to their several microscopes. Watson’s special form of apparatus is represented in Fig. 181, the polariser being adapted to the sub-stage, and the analyser to screw into the objective.

_Tourmaline._--A semi-transparent mineral, of a neutral or bluish tint, called tourmaline, when cut into thin slices (about 1/20-inch thick) with their faces parallel to their axes exhibit the same phenomena as the Nicol prism. The only objection to which is that the transmitted polarised beam is more or less coloured. The tourmaline to be preferred stops the most light when its axis is at right-angles to that of the polariser, and yet admits the most when in the same plane. Make choice of a tourmaline as perfect as possible; size is of less importance when intended for use with the microscope.