Philosophical MagazineTaylor & Francis, 1836 - Physics |
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Page vii
CONTENTS . Page Sir D. Brewster's Observations on the Lines of the Solar Spec- trum , and on those produced by the Earth's Atmosphere , and by the Action of Nitrous Acid Gas Mr. W. S. B. Woolhouse on the Theory of Vanishing Fractions ...
CONTENTS . Page Sir D. Brewster's Observations on the Lines of the Solar Spec- trum , and on those produced by the Earth's Atmosphere , and by the Action of Nitrous Acid Gas Mr. W. S. B. Woolhouse on the Theory of Vanishing Fractions ...
Page 9
... lines , all in one direction . This is a case of polarized light . Let x be taken in the direction of the vibrations ; then and will be zero , and the first of the equations ( 3. ) will give de dt = m Σ . { ¢ ( r ) + ↓ ( r ) △ x2 } ...
... lines , all in one direction . This is a case of polarized light . Let x be taken in the direction of the vibrations ; then and will be zero , and the first of the equations ( 3. ) will give de dt = m Σ . { ¢ ( r ) + ↓ ( r ) △ x2 } ...
Page 66
... lines from parabolic arcs , so as to have a point of inflection at about one sixth part from the bow of the vessel , before which the bow is concave externally , giving the finest possible entrance at the stern , at an angle of contact ...
... lines from parabolic arcs , so as to have a point of inflection at about one sixth part from the bow of the vessel , before which the bow is concave externally , giving the finest possible entrance at the stern , at an angle of contact ...
Page 97
... lines ; but where the formula gives more than 40 miles an hour the results of the computa- tion are not stated . Thus , for example , assuming , as you do , 25 miles to be the velocity on a horizontal plane , and t = 1 250 ' the formula ...
... lines ; but where the formula gives more than 40 miles an hour the results of the computa- tion are not stated . Thus , for example , assuming , as you do , 25 miles to be the velocity on a horizontal plane , and t = 1 250 ' the formula ...
Page 111
... lines drawn from any point of the radiating surface to a given point of the cry- stal are of equal length , and form the same angle with the cry- stal and canister in each case ; while the other sides of the ca- nister cannot interfere ...
... lines drawn from any point of the radiating surface to a given point of the cry- stal are of equal length , and form the same angle with the cry- stal and canister in each case ; while the other sides of the ca- nister cannot interfere ...
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