Elementary Thermodynamics |
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Page 4
... experiment and experience , from a more obvious result known as the principle of Work , which will now be obtained as a direct theoretical consequence of Newton's three Laws of Motion . In order to apply these laws correctly , it is ...
... experiment and experience , from a more obvious result known as the principle of Work , which will now be obtained as a direct theoretical consequence of Newton's three Laws of Motion . In order to apply these laws correctly , it is ...
Page 21
... experiment and experience , that the system satisfies a relation of the form or U2- U1 = [ " dw , P 0 dU = dw , where U is a single - valued function of the independent variables which define the state of the system together with an ...
... experiment and experience , that the system satisfies a relation of the form or U2- U1 = [ " dw , P 0 dU = dw , where U is a single - valued function of the independent variables which define the state of the system together with an ...
Page 24
... experiments which raise this suspicion to a certainty . We therefore define the Mechanical Kinetic Energy of a system of bodies to be the kinetic energy that the system would have if its motions were the same as they appear to be , or ...
... experiments which raise this suspicion to a certainty . We therefore define the Mechanical Kinetic Energy of a system of bodies to be the kinetic energy that the system would have if its motions were the same as they appear to be , or ...
Page 27
... experiment that the non - mechanical work done by contact - forces is what we understand when we speak of the conduction of heat . In the case of gravitation , the force between any two particles depends only on their distance and ...
... experiment that the non - mechanical work done by contact - forces is what we understand when we speak of the conduction of heat . In the case of gravitation , the force between any two particles depends only on their distance and ...
Page 29
... experiment it further appears , at least very approxi- mately , that when the total normal pressures are as n to 1 , the limiting amounts of friction will be in this ratio whatever be the proportion of the common areas . Hence , if R be ...
... experiment it further appears , at least very approxi- mately , that when the total normal pressures are as n to 1 , the limiting amounts of friction will be in this ratio whatever be the proportion of the common areas . Hence , if R be ...
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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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