New Theories of Matter And of Force
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In our eReader you can find the full English version of the book. Read New Theories of Matter And of Force Online - link to read the book on full screen. Our eReader also allows you to upload and read Pdf, Txt, ePub and fb2 books. In the Mini eReder on the page below you can quickly view all pages of the book - Read Book New Theories of Matter And of Force
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To quickly assess the difficulty of the text, read a short excerpt:
27, p. 273), represent the inter- sections of some of the prism-axes of the group with the surface of the crystal laid with its axis horizontal.
Project these intersections in the way above described, the plane of projection cutting the original plane in y y' (this is a simple proceeding, as every vertical length in the original is represented by an equal length in the projec- tion, and every horizontal length by a length which bears to it the given ratio of the two velocities). Let A' A' A', e...tc. (fig. 30), represent the resulting projections. Then, since the projections of all ellipses drawn as pre- scribed will be circles, the projections of the loci of the intersections of pairs of these ellipses (which loci we have seen are those traced by the surfaces of maximum condensation in a plane just within the crystal parallel to its surface) will be straight lines drawn to bisect at right angles lines joining the projections (A') of the wave centres. When these bisectors have been drawn to meet one another (see fig.
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You can find similar books in the "Read Also" column, or choose other free books by William Barlow to read onlineMoreLess
To quickly assess the difficulty of the text, read a short excerpt:
27, p. 273), represent the inter- sections of some of the prism-axes of the group with the surface of the crystal laid with its axis horizontal.
Project these intersections in the way above described, the plane of projection cutting the original plane in y y' (this is a simple proceeding, as every vertical length in the original is represented by an equal length in the projec- tion, and every horizontal length by a length which bears to it the given ratio of the two velocities). Let A' A' A', e...tc. (fig. 30), represent the resulting projections. Then, since the projections of all ellipses drawn as pre- scribed will be circles, the projections of the loci of the intersections of pairs of these ellipses (which loci we have seen are those traced by the surfaces of maximum condensation in a plane just within the crystal parallel to its surface) will be straight lines drawn to bisect at right angles lines joining the projections (A') of the wave centres. When these bisectors have been drawn to meet one another (see fig.
What to read after New Theories of Matter And of Force?
You can find similar books in the "Read Also" column, or choose other free books by William Barlow to read onlineMoreLess
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