Philosophical MagazineTaylor & Francis., 1875 - Matter |
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Page 33
... supposed not to be so hot as the white stars , perhaps the vapour of carbon may exist glowing and incandescent in Sirius , which is so noted a member of the latter class of stars . We may , too , perhaps be privileged to see the actual ...
... supposed not to be so hot as the white stars , perhaps the vapour of carbon may exist glowing and incandescent in Sirius , which is so noted a member of the latter class of stars . We may , too , perhaps be privileged to see the actual ...
Page 41
ing to their magnitudes . In the one case the magnitudes are supposed to be wholly due to the various combinations of 17 alternatives , and the elements of the drawing are obtained from the several terms of the expansion of ( 1 + 1 ) 17 ...
ing to their magnitudes . In the one case the magnitudes are supposed to be wholly due to the various combinations of 17 alternatives , and the elements of the drawing are obtained from the several terms of the expansion of ( 1 + 1 ) 17 ...
Page 74
... supposed that the dip of any bed is due to gre movements of the earth's crust ; from the facts mentioned the auth argued that our inferences as to such movements will vary accordin to the beds which happen to be exposed at the surface ...
... supposed that the dip of any bed is due to gre movements of the earth's crust ; from the facts mentioned the auth argued that our inferences as to such movements will vary accordin to the beds which happen to be exposed at the surface ...
Page 84
... supposed to be in the plane of the magnetic meridian . Apparatus . The support of the needles is merely a small stick , thin and light , of sealing - wax , hard and not readily fusible . The directing needle A B ( fig . 2 ) is attached ...
... supposed to be in the plane of the magnetic meridian . Apparatus . The support of the needles is merely a small stick , thin and light , of sealing - wax , hard and not readily fusible . The directing needle A B ( fig . 2 ) is attached ...
Page 86
... supposed . Corrections and Mode of Observation . The axis of the tube T is never quite horizontal ; but when we confine ourselves to rela- tive measurements ( we shall see how absolute measures are reduced to relative ones ) , it is ...
... supposed . Corrections and Mode of Observation . The axis of the tube T is never quite horizontal ; but when we confine ourselves to rela- tive measurements ( we shall see how absolute measures are reduced to relative ones ) , it is ...
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acid alcohol angle aurora axis band-spectrum bands boron bright calorimeter carbon carbonic acid cast iron cent centims chloride circuit colour compound constant continuous corresponding crater cryohydrate crystals curve determined diameter diamond discharge distance duplex effect electromotive force elements equal equation equipotential erbia eruption experiments flame flow-lines freezing-mixture galvanometer gaseous gases give given glass graphite grms hydrogen integral lava Leyden jar light line-spectrum lines of flow liquid magnetic magnetic moment means method metres millim molecules needle observed obtained paper phenomena Phil Piazzi Smyth placed Plate platinum polarization poles position pressure produced protocatechuic acid quantity ratio represent resistance salt saturated silicon solid solidify solution spark specific gravity specific heat spectra spectroscope spectrum substance supersaturated supposed surface telegraphy temperature thickness tion tube vanilline vapour vibrations vis viva weight دو دو
Popular passages
Page 29 - “I have uttered that I understood not; things too wonderful for me, which I knew not.” “Wherefore I abhor myself, and repent in
Page 321 - respectively. Then, at the points where 1 and 1', 2 and 2', 3 and 3', 4 and 4' respectively intersect each other, the potentials will be the sums of the potentials of the intersecting lines; and therefore the potential at all these points is the same, namely
Page 203 - in the same direction; and here, again, the spectrum we obtain from elements in a state of vapour (a spectrum characterized by spaces and bands) is similar to that we obtain from vapours of which the compound nature is unquestioned. (/3) At high temperatures, produced by combustion, the vapours of
Page 121 - 0 will be B, A, B', A; but since B and B' are complementary, their suppression will not affect the resulting tint except as to intensity, and the overlap will be effectively deprived of A alone; in other words, it will be of the same tint as the image 0 would be if the combination Q,
Page 155 - In his ‘Essay on the Application of Mathematical Analysis to the Theories of Electricity and Magnetism' (Nottingham, 1828),
Page 243 - that, from the point (about 600°) at which the specific heat of carbon ceases to vary with increase of temperature and becomes comparable with that of other elements, any real difference in the specific heats of the two modifications disappears, and carbon obeys the law of Dulong and Petit.
Page 201 - and Energy,” printed in Phil. Trans. 1873), as conclusively proving that such slags are not denser in the molten than in the solid state, and that the floating referred to is due to other causes. The author returns thanks to several persons for facilities liberally afforded him in making these experiments.
Page 121 - having lost the same tints as B 0, will have lost also the tint A, and will have received besides the addition of two measures of the tint A'. Effect of Combinations of two Colours.—A similar train of reasoning might be applied to the triple overlaps. But the main interest of these parts of the' figure consists in
Page 289 - openings. Thus the resonator's mouth was exposed to the vibrations during an interval which equalled that during which it was screened from them. A rubber tube led from the nipple of the resonator to one ear, while the other ear was tightly closed with a lump of beeswax.
Page 204 - end. (This absorption may ¿ break up into channelled spaces.) Fifth stage ... Unique continuous absorption. 9. I shall content myself in the present note by giving one or two instances of the passage of spectra from one stage to another, beginning at the fifth stage. From 5 to 4.