A Treatise on the Mathematical Theory of the Motion of FluidsThe University Press, 1879 - 258 pagina's |
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Pagina ix
... Cyclic motion . Motion of a ring Case of two or more solids Case of two spheres CHAPTER VI . VORTEX MOTION . 126 , 127 . " Definitions . Strength ' of a vortex 128-131 . Determination of motion in terms of expansion and rotation ...
... Cyclic motion . Motion of a ring Case of two or more solids Case of two spheres CHAPTER VI . VORTEX MOTION . 126 , 127 . " Definitions . Strength ' of a vortex 128-131 . Determination of motion in terms of expansion and rotation ...
Pagina 29
... cyclic function . A function is said to be single - valued throughout any region of space when it is possible to assign to every point of that region a definite value of the function , in such a way that these values shall form a ...
... cyclic function . A function is said to be single - valued throughout any region of space when it is possible to assign to every point of that region a definite value of the function , in such a way that these values shall form a ...
Pagina 30
... cyclic . The theory of many - valued velocity - potentials will be discussed in the next chapter . 36. Example 5. A mass of liquid filling a right circular cy- linder moves from rest under the action of the forces X = Ax + By , Y = Bx + ...
... cyclic . The theory of many - valued velocity - potentials will be discussed in the next chapter . 36. Example 5. A mass of liquid filling a right circular cy- linder moves from rest under the action of the forces X = Ax + By , Y = Bx + ...
Pagina 51
... cyclic function ; i.e. it is not possible to assign to every point of the original region a de- finite value of p , such values forming a continuous system . On the contrary , whenever P describes in the region a non - evanescible ...
... cyclic function ; i.e. it is not possible to assign to every point of the original region a de- finite value of p , such values forming a continuous system . On the contrary , whenever P describes in the region a non - evanescible ...
Pagina 53
... cyclic function . In the method adopted above we have based the whole theory on the equations dw dv dy dz du = 0 , - dw = 0 , dv du = dz dx dx dy - = 0 ....... ... ( 16 ) , and have deduced the existence and properties of the velocity ...
... cyclic function . In the method adopted above we have based the whole theory on the equations dw dv dy dz du = 0 , - dw = 0 , dv du = dz dx dx dy - = 0 ....... ... ( 16 ) , and have deduced the existence and properties of the velocity ...
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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