A Treatise on Hydromechanics, Part 1 |
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... temperature . 101-110 Mixture of gases . Dew . Specific heat 111-118 The atmosphere . Determination of heights CHAPTER VIII . 119-121 Tension of flexible surfaces 122-126 Lintearia and Elastica 127-142 Tension and Pressure PAGE 130 1 ...
... temperature . 101-110 Mixture of gases . Dew . Specific heat 111-118 The atmosphere . Determination of heights CHAPTER VIII . 119-121 Tension of flexible surfaces 122-126 Lintearia and Elastica 127-142 Tension and Pressure PAGE 130 1 ...
Page 7
... temperature , as well as upon the nature of the fluid itself . When the temperature is constant , experiment shews that the pressure varies inversely as the space occupied by the fluid , that is , directly as its density . This law was ...
... temperature , as well as upon the nature of the fluid itself . When the temperature is constant , experiment shews that the pressure varies inversely as the space occupied by the fluid , that is , directly as its density . This law was ...
Page 8
... temperature throughout , is necessarily heterogeneous : the density at a point of a fluid must there- fore be measured in the same way as the pressure at a point , or any other continuously varying quantity . Measure of the density at ...
... temperature throughout , is necessarily heterogeneous : the density at a point of a fluid must there- fore be measured in the same way as the pressure at a point , or any other continuously varying quantity . Measure of the density at ...
Page 15
... temperature be constant , p = kp ; dp_1 p = k ( Xd + Ydy + Zdz ) ......... ( 8 ) . If the forces are derivable from a potential V , i.e. if Xdx + Ydy + Zdz be a perfect differential - dV , k dp — — dV , p = V , .log - V V k C 1 p = Oe ...
... temperature be constant , p = kp ; dp_1 p = k ( Xd + Ydy + Zdz ) ......... ( 8 ) . If the forces are derivable from a potential V , i.e. if Xdx + Ydy + Zdz be a perfect differential - dV , k dp — — dV , p = V , .log - V V k C 1 p = Oe ...
Page 16
... temperature be variable , the relation between the pressure , density , and temperature is found to be p = kp ( 1+ at ) , where t is the temperature , measured by a Centigrade Thermometer , and a = 003665 . From this we obtain p = kpaa ...
... temperature be variable , the relation between the pressure , density , and temperature is found to be p = kp ( 1+ at ) , where t is the temperature , measured by a Centigrade Thermometer , and a = 003665 . From this we obtain p = kpaa ...
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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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