Elementary Thermodynamics |
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Page 2
... equal to the weight of a gramme at Paris . The acceleration of any body falling freely at Paris under its own weight being 980-868 centimetres per second , we see that the weight of a gramme at Paris is 980-868 dynes . To determine the ...
... equal to the weight of a gramme at Paris . The acceleration of any body falling freely at Paris under its own weight being 980-868 centimetres per second , we see that the weight of a gramme at Paris is 980-868 dynes . To determine the ...
Page 3
... equal to the weight ( at Paris ) of 1033-279 grammes per square centimetre , or to a pressure of 1013510 dynes per square centimetre . The Atmo , the name of which is due to Prof. J. Thomson , is about equal to the average pressure of ...
... equal to the weight ( at Paris ) of 1033-279 grammes per square centimetre , or to a pressure of 1013510 dynes per square centimetre . The Atmo , the name of which is due to Prof. J. Thomson , is about equal to the average pressure of ...
Page 5
... equal to the product of the force and the projection of the displacement along the force . The absolute unit of work ... equal to the sum of the resolved parts of the component forces in the same direction , it is evident the work done ...
... equal to the product of the force and the projection of the displacement along the force . The absolute unit of work ... equal to the sum of the resolved parts of the component forces in the same direction , it is evident the work done ...
Page 6
John Parker. equal to the sum of the quantities of work done by the forces separately . Thus if R be the sum of the resolved parts of the forces along the displacement ds , and dW the work done on the particle , we have dW = Rds . To put ...
John Parker. equal to the sum of the quantities of work done by the forces separately . Thus if R be the sum of the resolved parts of the forces along the displacement ds , and dW the work done on the particle , we have dW = Rds . To put ...
Page 7
... equal to the work done upon it . It is clear that kinetic energy is measured in the same way as work , that is , in ergs ( or foot - poundals ) . 5. The forces which act on the particle are due THE CONSERVATION OF ENERGY . 7.
... equal to the work done upon it . It is clear that kinetic energy is measured in the same way as work , that is , in ergs ( or foot - poundals ) . 5. The forces which act on the particle are due THE CONSERVATION OF ENERGY . 7.
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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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