A Treatise on Hydromechanics, Parte1Deighton, Bell, 1891 - 268 páginas |
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Página 1
... fluid can be reduced by mixture with a large portion of another fluid , the rarefaction of air which can be effected by means of an air - pump , and other facts of a similar kind , it is clear that , practically , the divisibility of ...
... fluid can be reduced by mixture with a large portion of another fluid , the rarefaction of air which can be effected by means of an air - pump , and other facts of a similar kind , it is clear that , practically , the divisibility of ...
Página 2
... fluid is assumed to have no " viscosity , " no property of the nature of friction . The following fundamental property of a fluid is there- fore obtained from the ... Fluids are acted upon by the force of gravity 2 DEFINITION OF A FLUID .
... fluid is assumed to have no " viscosity , " no property of the nature of friction . The following fundamental property of a fluid is there- fore obtained from the ... Fluids are acted upon by the force of gravity 2 DEFINITION OF A FLUID .
Página 3
... fluid at rest under the action of any forces , and let A be the area of a plane surface exposed to the action of the fluid , that is , in contact with it , and P the force which is required to counterbalance the action of the fluid upon ...
... fluid at rest under the action of any forces , and let A be the area of a plane surface exposed to the action of the fluid , that is , in contact with it , and P the force which is required to counterbalance the action of the fluid upon ...
Página 4
William Henry Besant. of a fluid ; it can be deduced from the fundamental property of a fluid in the following manner : If we consider the equilibrium of a small tetrahedron of fluid , we observe that the pressures on its faces , and the ...
William Henry Besant. of a fluid ; it can be deduced from the fundamental property of a fluid in the following manner : If we consider the equilibrium of a small tetrahedron of fluid , we observe that the pressures on its faces , and the ...
Página 5
... fluid at a dis- tance x from Q. Hence [ PQ p ' = p + pƒ da , 0 or p ' is constant for all positions of the plane through P. * The following considerations may complete this part of the proof : Let AB , A'B ' be the two planes through P ...
... fluid at a dis- tance x from Q. Hence [ PQ p ' = p + pƒ da , 0 or p ' is constant for all positions of the plane through P. * The following considerations may complete this part of the proof : Let AB , A'B ' be the two planes through P ...
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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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