Elementary Thermodynamics |
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Page 1
... quantities in terms of a very convenient set of units based on the Metric , or French , system of weights and measures , we shall give an account of the method , and also make a comparison with the less simple , but more familiar ...
... quantities in terms of a very convenient set of units based on the Metric , or French , system of weights and measures , we shall give an account of the method , and also make a comparison with the less simple , but more familiar ...
Page 12
... quantities of work which they do in any the same time are equal and opposite , or the sum of the quantities of work is zero . Hence , for the whole system , the work done by the internal contact - forces in any given time is zero , and ...
... quantities of work which they do in any the same time are equal and opposite , or the sum of the quantities of work is zero . Hence , for the whole system , the work done by the internal contact - forces in any given time is zero , and ...
Page 20
... quantity of work , W , done by contact - forces and gravitation alone , we have [ " dw = W. The simple fact we have just obtained for our ideal systems , that the energy U increases by the amount of external work done on the system , or ...
... quantity of work , W , done by contact - forces and gravitation alone , we have [ " dw = W. The simple fact we have just obtained for our ideal systems , that the energy U increases by the amount of external work done on the system , or ...
Page 27
... quantity dW of mechanical work and a quantity dQ of non - mechanical THE CONSERVATION OF ENERGY . 27.
... quantity dW of mechanical work and a quantity dQ of non - mechanical THE CONSERVATION OF ENERGY . 27.
Page 28
John Parker. mechanical work and a quantity dQ of non - mechanical work , due either to the conduction of heat or to radiation , we have dU = dw = dW + dQ ....... .. ( 8 ) , from which we draw the important conclusion that dW and dQ will ...
John Parker. mechanical work and a quantity dQ of non - mechanical work , due either to the conduction of heat or to radiation , we have dU = dw = dW + dQ ....... .. ( 8 ) , from which we draw the important conclusion that dW and dQ will ...
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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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