A Treatise on Hydromechanics, Part 1 |
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Page 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 ...
Page 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 .
Page 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 ...
Page 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 ...
Page 5
... fluid at a dis- tance x from Q. Hence PQ p ' = p + [ " poƒ da , pf 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 ...
... fluid at a dis- tance x from Q. Hence PQ p ' = p + [ " poƒ da , pf 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 ...
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Common terms and phrases
2nd edition 3rd edition 4th edition Aeneid angular velocity axis vertical body Books Camb Cambridge catenary catenoid centre of gravity centre of pressure cone constant cosē Crown 8vo curvature cylinder Demy 8vo density depth distance dx dy dy dx elastic English equal pressure equation equilibrium equilibrium is stable F. A. PALEY Fcap floats fluid pressure force free surface given horizontal immersed J. H. FREESE John's College lamina latus rectum LL.D mass mercury metacentre obtain paraboloid particle perpendicular plane of floatation position of equilibrium prove quantity radius resultant pressure revised revolution rotation sewed shew Small post 8vo solid solid of revolution spherical spheroid surface of revolution surfaces of equal tangent temperature Texts Translated Trinity College vertex vessel vols volume weight whole pressure
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