A Treatise on Hydromechanics, Parte1Deighton, Bell, 1891 - 268 páginas |
Dentro del libro
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Página 4
... homogeneous , and therefore supposing the solid indefinitely diminished , while it retains always a similar form , the latter force vanishes in comparison with the pressures on the faces ; and these pressures con- sequently form of ...
... homogeneous , and therefore supposing the solid indefinitely diminished , while it retains always a similar form , the latter force vanishes in comparison with the pressures on the faces ; and these pressures con- sequently form of ...
Página 9
... homogeneous fluid such that the mass of a volume v is equal to m , or such that m = pv ; then p may be defined as the mean density of the portion v of the heterogeneous fluid , and the ultimate value of p when v is indefinitely ...
... homogeneous fluid such that the mass of a volume v is equal to m , or such that m = pv ; then p may be defined as the mean density of the portion v of the heterogeneous fluid , and the ultimate value of p when v is indefinitely ...
Página 12
... homogeneous or heterogeneous , to be at rest under the action of given forces , and let it be required to determine the conditions of equilibrium , and the pressure at any point . Let x , y , z be the co - ordinates referred to ...
... homogeneous or heterogeneous , to be at rest under the action of given forces , and let it be required to determine the conditions of equilibrium , and the pressure at any point . Let x , y , z be the co - ordinates referred to ...
Página 14
... Homogeneous Liquids . If the fluid be homogeneous and incompressible , Xdx + Ydy + Zdz must be a perfect differential in order that equilibrium may be possible . In other words , the system of forces must be a conser- vative system ...
... Homogeneous Liquids . If the fluid be homogeneous and incompressible , Xdx + Ydy + Zdz must be a perfect differential in order that equilibrium may be possible . In other words , the system of forces must be a conser- vative system ...
Página 15
... homogeneous fluid under the action of such forces is always possible . Elastic Fluids . When the fluid is elastic , an ad- ditional condition is introduced , for , if the temperature be constant , dp p = p = kp ; 1 kc ( Xdæ + Ydy + Zdz ) ...
... homogeneous fluid under the action of such forces is always possible . Elastic Fluids . When the fluid is elastic , an ad- ditional condition is introduced , for , if the temperature be constant , dp p = p = kp ; 1 kc ( Xdæ + Ydy + Zdz ) ...
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Términos y frases comunes
action angular velocity attraction axes axis vertical catenary catenoid centre of gravity centre of pressure co-ordinates conditions of equilibrium cone constant cos² cylinder density depth determine displaced fluid distance dx dy Edition elastic Elastica equal pressure equation equilibrium equilibrium is stable F. A. Paley Fcap film fluid displaced fluid pressure force free surface given Hence homogeneous liquid horizontal immersed lamina latus rectum Lintearia mercury metacentre obtain oscillation parabola paraboloid parallel particle perpendicular plane of floatation portion position of equilibrium principal tensions prove quantity radius of curvature ratio resultant pressure rotation shew sin² solid solid of revolution sphere spherical spheroid supposed surface of revolution surfaces of equal tangent temperature tube vapour varies vertical angle vertical plane vessel volume weight whole pressure
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