A Treatise on the Mathematical Theory of the Motion of FluidsThe University Press, 1879 - 258 pagina's |
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Pagina 1
... surface . This property is the basis of Hydrostatics , and is veri- fied by the complete agreement of the deductions of that science with experiment . Very slight observation is enough , however , to convince us that oblique stresses ...
... surface . This property is the basis of Hydrostatics , and is veri- fied by the complete agreement of the deductions of that science with experiment . Very slight observation is enough , however , to convince us that oblique stresses ...
Pagina 2
... surface . For if the mutual action were everywhere wholly normal , it is obvious that the moment of momentum , about the axis of the vessel , of any portion of fluid bounded by a surface of revolution about this axis , would be constant ...
... surface . For if the mutual action were everywhere wholly normal , it is obvious that the moment of momentum , about the axis of the vessel , of any portion of fluid bounded by a surface of revolution about this axis , would be constant ...
Pagina 5
... surface - integral of the normal velocity outwards , taken all over the boundary . If the region in question be that occupied by the matter which at time t fills the rectangular element of Art . 6 , the parts of this 5-8 . ] པ་ EULERIAN ...
... surface - integral of the normal velocity outwards , taken all over the boundary . If the region in question be that occupied by the matter which at time t fills the rectangular element of Art . 6 , the parts of this 5-8 . ] པ་ EULERIAN ...
Pagina 6
Sir Horace Lamb. element of Art . 6 , the parts of this surface - integral due to the two yz - faces are u du d.x du ... surfaces at which the latter restriction does not hold . If the fluid move so as always to form a continuous ...
Sir Horace Lamb. element of Art . 6 , the parts of this surface - integral due to the two yz - faces are u du d.x du ... surfaces at which the latter restriction does not hold . If the fluid move so as always to form a continuous ...
Pagina 7
... surface bounding the fluid . The velocity relative to this surface of a particle lying in it must be wholly tangential ( or else zero ) , for otherwise we should have a finite flow of liquid across the surface , which contradicts the ...
... surface bounding the fluid . The velocity relative to this surface of a particle lying in it must be wholly tangential ( or else zero ) , for otherwise we should have a finite flow of liquid across the surface , which contradicts the ...
Overige edities - Alles bekijken
A Treatise on the Mathematical Theory of the Motion of Fluids Sir Horace Lamb Volledige weergave - 1879 |
A Treatise on the Mathematical Theory of the Motion of Fluids Sir Horace Lamb Volledige weergave - 1879 |
A Treatise on the Mathematical Theory of the Motion of Fluids Sir Horace Lamb Volledige weergave - 1879 |
Veelvoorkomende woorden en zinsdelen
angle angular velocity Ave Maria Lane axes axis C. J. CLAY Cambridge University Press centre Christ's College circle circuit CLAY & SONS co-ordinates constant corresponding Crown 8vo curves const cyclic Demy 8vo denote direction dt dt dx dx dx dy dz dy dy Edited element equation of continuity Fellow finite fluid forces formulę given Green's Theorem Hence impulse infinitely small infinity integral internal boundary irrotational irrotational motion J. E. SANDYS liquid LL.D mass moving Notes obtain origin P. G. TAIT P₁ parallel particle plane xy portion pressure Professor quantities radius RENDEL HARRIS satisfied shews simply-connected solid sphere St John's College stream-lines surface theorem Thomson Trinity College University of Cambridge University Press Warehouse velocity-potential vertical vortex waves zero аф
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