Philosophical MagazineTaylor & Francis, 1836 - Physics |
From inside the book
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Page 5
... give the name of Chimæra Townsendii ; to that in the Kimmeridge clay , Chimera Eger- tonii ; to that in the chalk marl , Chimæra Agassizii ; and to that in the chalk , Chimara Mantellii . On my submitting these fossils to Professor ...
... give the name of Chimæra Townsendii ; to that in the Kimmeridge clay , Chimera Eger- tonii ; to that in the chalk marl , Chimæra Agassizii ; and to that in the chalk , Chimara Mantellii . On my submitting these fossils to Professor ...
Page 9
... the equations ( 3. ) will give de dt = m Σ . { ¢ ( r ) + ↓ ( r ) △ x2 } △ § . Third Series . Vol . 8. No. 43. Jan. 1836 . ท ( 4. ) C Now , let be a function of ≈ and t Length of a Wave , in the Undulatory Theory of Light . 9.
... the equations ( 3. ) will give de dt = m Σ . { ¢ ( r ) + ↓ ( r ) △ x2 } △ § . Third Series . Vol . 8. No. 43. Jan. 1836 . ท ( 4. ) C Now , let be a function of ≈ and t Length of a Wave , in the Undulatory Theory of Light . 9.
Page 18
... give us the green protiodide , which on trying I found to be the case ; when equal parts of calomel and hydriodate of potassa are added to each other ( the one in solution and the other suspended in water ) an instant interchange takes ...
... give us the green protiodide , which on trying I found to be the case ; when equal parts of calomel and hydriodate of potassa are added to each other ( the one in solution and the other suspended in water ) an instant interchange takes ...
Page 22
... give out the quantity of heat necessary to produce this cubic inch of vapour . But in the experiments with dry gases ... gives the weight of the gas which would produce this effect in falling 1 ° ; from whence it is obvious that 1 ( the ...
... give out the quantity of heat necessary to produce this cubic inch of vapour . But in the experiments with dry gases ... gives the weight of the gas which would produce this effect in falling 1 ° ; from whence it is obvious that 1 ( the ...
Page 26
... give 1 1 = √ S ( H2 ) μ { - 6 S [ ( H3 ) ( ^ ? · * ) * ] ; 1 S [ ( H2 ) ( * ) * ] + 120 S ( H2 ) S ( H2 ) & c . · } supposing the series to converge rapidly enough . Now , this would manifestly be the same as the last if we were at ...
... give 1 1 = √ S ( H2 ) μ { - 6 S [ ( H3 ) ( ^ ? · * ) * ] ; 1 S [ ( H2 ) ( * ) * ] + 120 S ( H2 ) S ( H2 ) & c . · } supposing the series to converge rapidly enough . Now , this would manifestly be the same as the last if we were at ...
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