Optical projection: a treatise on the use of the lantern in exhibition and scientific demonstration (1906)

Record Details:

Something wrong or inaccurate about this page? Let us Know!

Thanks for helping us continually improve the quality of the Lantern search engine for all of our users! We have millions of scanned pages, so user reports are incredibly helpful for us to identify places where we can improve and update the metadata.

Please describe the issue below, and click "Submit" to send your comments to our team! If you'd prefer, you can also send us an email to mhdl@commarts.wisc.edu with your comments.




We use Optical Character Recognition (OCR) during our scanning and processing workflow to make the content of each page searchable. You can view the automatically generated text below as well as copy and paste individual pieces of text to quote in your own work.

Text recognition is never 100% accurate. Many parts of the scanned page may not be reflected in the OCR text output, including: images, page layout, certain fonts or handwriting.

H2$ OPTICAL PROJECTION Sometimes the heat of the lantern will destroy the film too rapidly. In that case an alum cell in the slide-stage will remove the difficulty. Horizontal bands being caused by the action of gravitation on the film, if we can make the gradual thinning take a circular form, the bands will become annular. This is effected by a beautiful modification of the experiment often employed by Lord Eayleigh, and which is very easy if any sort of bellows, or weighted bag filled with air, be at hand, to furnish a slight blast. Even the breath will answer, but needs some practice and a thin rubber balloon to steady the pressure. Connected with the air-blast (a gentle one) by rubber tubing is a piece of glass tube drawn into a small but A B FIG. 180.—Rotating Films not capillary orifice: one of the ' fillers' sold for use with fountain pens answers excellently. This is fixed in another small Bunsen holder, and adjusted so as to direct a blast at a small angle with the surface of the film. Adjusted near the edge as at A (fig. 180) the above is converted into a single whirling vortex, which shows rapid and magnificent gradation of colour: adjusted as at B, a little to one side of the centre, the stream divides into two vortices, in which the play of colour is still more rapid. This experiment never fails to 'bring down the house.' 187. Films of air—Newton's Rings.—Two squares of plate glass, with rounded edges, cleaned and polished, are readily