A Treatise on Hydromechanics, Part 1 |
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Page 3
... vessel , exhausted as far as possible : moreover , the phe- nomena of the tides shew that fluids are subject to the attractive forces of the sun and moon as well as of the earth , and it is assumed , from these and other similar facts ...
... vessel , exhausted as far as possible : moreover , the phe- nomena of the tides shew that fluids are subject to the attractive forces of the sun and moon as well as of the earth , and it is assumed , from these and other similar facts ...
Page 6
... vessel full of water two apertures be made and pistons A , A ' fitted in them , any force P applied to one piston must be counteracted by a force P ' on the other piston , such that P ' : P in the ratio of the area A ' : A , for the ...
... vessel full of water two apertures be made and pistons A , A ' fitted in them , any force P applied to one piston must be counteracted by a force P ' on the other piston , such that P ' : P in the ratio of the area A ' : A , for the ...
Page 7
... vessel separately . For doubling the quantity of gas in the vessel would double the pressure , and a similar propor- tionate change of pressure would take place for any other change of quantity . Hence if p be the density of a certain ...
... vessel separately . For doubling the quantity of gas in the vessel would double the pressure , and a similar propor- tionate change of pressure would take place for any other change of quantity . Hence if p be the density of a certain ...
Page 9
... vessel containing it , and dn an element of the 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 - [ pdv = - [ Cdv , if pv = C , = - V V = = C log V ...
... vessel containing it , and dn an element of the 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 - [ pdv = - [ Cdv , if pv = C , = - V V = = C log V ...
Page 10
... that the density of the liquid when mixed up so as to be uniform will be that of the liquid originally at the depth of one - fourth of the axis of the cone . 11. From a vessel full of liquid of density p 10 EXAMPLES .
... that the density of the liquid when mixed up so as to be uniform will be that of the liquid originally at the depth of one - fourth of the axis of the cone . 11. From a vessel full of liquid of density p 10 EXAMPLES .
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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 cos² 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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