Elementary Thermodynamics |
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Page 8
... complete differential of some function of ( x , y , z ) , that we may write W = F ( x , y , z ) + C , where C is an arbitrary constant . Hence if the particle move from the position A to th position B , the work done by the forces takes ...
... complete differential of some function of ( x , y , z ) , that we may write W = F ( x , y , z ) + C , where C is an arbitrary constant . Hence if the particle move from the position A to th position B , the work done by the forces takes ...
Page 9
... complete differential and the integration will be impossible until something further is specified about the path . This will be made clear by an example . y P M N x Let us suppose that X Then we = му , THE CONSERVATION OF ENERGY . 9.
... complete differential and the integration will be impossible until something further is specified about the path . This will be made clear by an example . y P M N x Let us suppose that X Then we = му , THE CONSERVATION OF ENERGY . 9.
Page 23
... complete differential . It is obvious that the only effect of the internal ether- forces is a transformation of kinetic into an equal amount of potential , energy , and vice versa . Since the principle of energy does not require us to ...
... complete differential . It is obvious that the only effect of the internal ether- forces is a transformation of kinetic into an equal amount of potential , energy , and vice versa . Since the principle of energy does not require us to ...
Page 28
... complete differentials of functions of the independent variables . 14. If the surface of the smoothest body be examined by a powerful microscope , it is found to be so irregular that it may be said to be covered with a great number of ...
... complete differentials of functions of the independent variables . 14. If the surface of the smoothest body be examined by a powerful microscope , it is found to be so irregular that it may be said to be covered with a great number of ...
Page 32
... complete differential if p be a function of v only , or a constant , or if v be constant . When p is constant , and dW = -d ( pv ) , dQ = d ( U + pv ) . The mechanical work done by the body during a change of volume may be represented ...
... complete differential if p be a function of v only , or a constant , or if v be constant . When p is constant , and dW = -d ( pv ) , dQ = d ( U + pv ) . The mechanical work done by the body during a change of volume may be represented ...
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Common terms and phrases
angle angular momentum angular velocity atmo axis of figure axis of rotation body C₂ calories Cambridge Warehouse carbonic acid Carnot's principle centre of mass constant pressure contact-forces Crown 8vo cryohydrate cubic centimetres curve cycle cylinder denote distance earth Edition electric entropy equal equation ergs external forces freezing given gramme gravitation heat absorbed Hence independent variables indicator diagram liquid M.A. Demy 8vo mechanical kinetic energy mechanical motions mercury momenta non-frictional non-mechanical kinetic energy obtained orbit parallel particle piston plane positive potential at constant potential energy quantity of heat radiation rectangular axes result reversible salt solution specific heat square centimetre stable equilibrium steam substance suppose surface temperature and pressure thermodynamic potential thermometer tidal friction tube vessel volume zero
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