A Treatise on Hydromechanics, Parte1Deighton, Bell, 1891 - 268 páginas |
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Página 1
... an indefinitely thin plane be made to divide such a fluid in any direction , no resistance will be offered to the division , and the pressure exerted by the fluid on the plane B. H. 1 will be entirely normal to it ; that is ,
... an indefinitely thin plane be made to divide such a fluid in any direction , no resistance will be offered to the division , and the pressure exerted by the fluid on the plane B. H. 1 will be entirely normal to it ; that is ,
Página 2
... normal to any surface with which it is in contact . As a matter of fact , all fluids do more or less offer a resistance to separation or division , but , just as the idea of a rigid body is obtained from the observation of bodies in ...
... normal to any surface with which it is in contact . As a matter of fact , all fluids do more or less offer a resistance to separation or division , but , just as the idea of a rigid body is obtained from the observation of bodies in ...
Página 9
... normal to ds drawn inwards . Then the work done in a small compression = pΣdsdn = — pdv , and the work done in compressing from V to V = - Jpdv = - [ Odv , if f pv = C , V V V = C log V ' = pulog . V ' EXAMPLES . ( In these Examples g ...
... normal to ds drawn inwards . Then the work done in a small compression = pΣdsdn = — pdv , and the work done in compressing from V to V = - Jpdv = - [ Odv , if f pv = C , V V V = C log V ' = pulog . V ' EXAMPLES . ( In these Examples g ...
Página 11
... normal to the surface of equal density containing the point ; and of direc- tions in the tangent plane to this surface , the tangents to its principal sections are those in which the rate of variation of density is greatest and least ...
... normal to the surface of equal density containing the point ; and of direc- tions in the tangent plane to this surface , the tangents to its principal sections are those in which the rate of variation of density is greatest and least ...
Página 18
... normal at the point ( x , y , z ) of the surface A , are equal to dp dp dp dx ' dy ' dz ' respectively , i.e. to pX , pY , pZ , and are therefore proportional to X , Y , Z. Hence the resultant force at any point is in direction of the ...
... normal at the point ( x , y , z ) of the surface A , are equal to dp dp dp dx ' dy ' dz ' respectively , i.e. to pX , pY , pZ , and are therefore proportional to X , Y , Z. Hence the resultant force at any point is in direction of the ...
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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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