Philosophical Transactions of the Royal Society of London, Volume 175,Deel 1W. Bowyer and J. Nichols for Lockyer Davis, printer to the Royal Society, 1884 |
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Resultaten 1-5 van 47
Pagina 7
... gives A = -18 . For the velocity parallel to x we have 2 W == u2 sin 2kx , V [ e - By { — sin ẞy - 1 cos By + 1ẞy cos By - 1ẞy sin ẞy - e - By } + ߬1e¬2ky { B − 2k ( A + By ) } ] . In order that u should vanish when y = 0 , we must ...
... gives A = -18 . For the velocity parallel to x we have 2 W == u2 sin 2kx , V [ e - By { — sin ẞy - 1 cos By + 1ẞy cos By - 1ẞy sin ẞy - e - By } + ߬1e¬2ky { B − 2k ( A + By ) } ] . In order that u should vanish when y = 0 , we must ...
Pagina 9
... gives rise in this case to no difficulty . But it is possible that the behaviour of the sand is materially influenced by the vertical motion of the vessel by which in these experiments the liquid vibra- tions are maintained . * § 2. In ...
... gives rise in this case to no difficulty . But it is possible that the behaviour of the sand is materially influenced by the vertical motion of the vessel by which in these experiments the liquid vibra- tions are maintained . * § 2. In ...
Pagina 10
... give u = 0 , v = v , sin kx cos nt , when y = 0 . This is sufficient for a first approximation , but in proceeding further we must remember п that these prescribed velocities apply in strictness not to 10 LORD RAYLEIGH ON THE CIRCULATION.
... give u = 0 , v = v , sin kx cos nt , when y = 0 . This is sufficient for a first approximation , but in proceeding further we must remember п that these prescribed velocities apply in strictness not to 10 LORD RAYLEIGH ON THE CIRCULATION.
Pagina 14
... gives 3 4 v2 sin 2kx 2V ( ( —1 By + ... ) . ( 53 ) , ( 54 ) , ( 55 ) . from which it appears that quite close to the plate the mean velocity is in the opposite direction to that which is found outside the frictional layer . * § 3. In ...
... gives 3 4 v2 sin 2kx 2V ( ( —1 By + ... ) . ( 53 ) , ( 54 ) , ( 55 ) . from which it appears that quite close to the plate the mean velocity is in the opposite direction to that which is found outside the frictional layer . * § 3. In ...
Pagina 31
... give a curve which is nearly a straight line . Our figures are uniformly somewhat lower than those of GAY LUSSAC . Curves constructed with the two sets of figures are nearly parallel . Hence we SOLUBILITY OF SALTS IN WATER AT HIGH ...
... give a curve which is nearly a straight line . Our figures are uniformly somewhat lower than those of GAY LUSSAC . Curves constructed with the two sets of figures are nearly parallel . Hence we SOLUBILITY OF SALTS IN WATER AT HIGH ...
Overige edities - Alles bekijken
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action Adopted numbers alkali aluminium ammonia ammonium amyl-ammonium appears approximation arterial pressure auricle barium broad cadmium cadmium lines calcium camera centims chloride circulation compound ammonias continuous contraction corona curve Description of lines determined diastole diethyl-ammonium Direct stimulation discontinuous Ditto dx dy electrodes erbium ethyl experiments extended faint and short Fairly strong fiducial lines fluid Frog gastrocnemius given Heart beating humerus inch increased indium iodide irritability lactic acid lanthanum left ventricle lengthened lengths limb MDCCCLXXXIV measurements metal methyl millims motion motor nerves muscle nebulous nimbus numbers observed obtained outflow paralyzed photographs portion potash potassium prominences pulse-rate reflex refrangible rubidium salt Scale sharp short lines shortening side slightly slit Society sodium solar solubility solution spark spasm spectra spectrum stream function sulphate surface systole tellurium temperature tetanus Thallium triethylamine tube velocity venous pressure Wave wave-lengths weak in centre yttrium