Summary

Portrait of Jagadish Chandra Bose Jagadish Chandra Bose Proceedings of the Royal Society of London Vol 60 (1897)

The electric ray at first falls on the grating at a large angle of incidence. A series of flashes of electric radiation are now produced by manipulating the key, and the angle of incidence gradually decreased till the receiver suddenly responds. The angle of incidence corresponding to the zero angle of diffraction is thus determined. The receiver is then placed at a new position on the focal curve, and the corresponding angle of incidence determined as before. In this way a series of angles of incidence, with their corresponding angles of diffraction, are found for each grating.
Source: Wikisource

Portrait of Jagadish Chandra Bose Jagadish Chandra Bose Proceedings of the Royal Society of London Vol 60 (1897)

The vibrations transmitted through the gratings are thus perpendicular to the direction of maximum conductivity—or parallel to the direction of greatest resistance. The vibration absorbed is parallel to the direction of maximum conductivity.
As the nemalite and chrysotile polarised the electric ray by unequal absorption in the two directions, I was led to investigate whether they, too, exhibited unequal conductivities in the two directions of absorption and transmission.
Source: Wikisource

Portrait of Jagadish Chandra Bose Jagadish Chandra Bose Proceedings of the Royal Society of London Vol 60 (1897)

I found the positions of the radiator on the focal curve producing action on the receiver, to be well defined, and I experienced no further disturbance due to stray radiations.
The grating is fixed vertically on the table, so that its centre is at the same height as that of the middle of the receiving and radiating tubes. A small mirror is fixed at the middle of the central strip. The observer, placing his eye at the same height as that of the radiator, levels the grating till the image of the eye is seen reflected by the mirror.
Source: Wikisource

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