Elementary Thermodynamics |
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Page 5
... angles to the force , the force is said to do Work on the particle , or the particle is said to do work against the ... angle between the positive directions of p and ds , the work done by the force will therefore be p cos e . ds , and ...
... angles to the force , the force is said to do Work on the particle , or the particle is said to do work against the ... angle between the positive directions of p and ds , the work done by the force will therefore be p cos e . ds , and ...
Page 6
... angle ( a , B , y ) , respectively . Then , by the principles of statics , R = X cos a + Y cos B + Z cos y . But if ( dx , dy , dz ) be the projections of the displace ment ds on the axes , we have , since the axes are rect angular ...
... angle ( a , B , y ) , respectively . Then , by the principles of statics , R = X cos a + Y cos B + Z cos y . But if ( dx , dy , dz ) be the projections of the displace ment ds on the axes , we have , since the axes are rect angular ...
Page 15
... angle between the directions of PQ and P'Q ' , MNr cos e = r , small quantities of the second order being rejected . Thus dw1 + dw2 = -λ mm ' p2 dr , and the work done on the system by all the internal gravitational forces may be ...
... angle between the directions of PQ and P'Q ' , MNr cos e = r , small quantities of the second order being rejected . Thus dw1 + dw2 = -λ mm ' p2 dr , and the work done on the system by all the internal gravitational forces may be ...
Page 38
... angle in the same direction as before , and then give to every part of the body a displacement equal and parallel to that of O. In order to find the relation between the rotations corresponding to any two different base points 0 , 0 ...
... angle in the same direction as before , and then give to every part of the body a displacement equal and parallel to that of O. In order to find the relation between the rotations corresponding to any two different base points 0 , 0 ...
Page 39
... angle as before about an axis parallel to Oz , passing through Q , the final position of O ' . Thus the axes of rotation corresponding to all base points are parallel and the angles of rotation equal and in the same direction . Hence ...
... angle as before about an axis parallel to Oz , passing through Q , the final position of O ' . Thus the axes of rotation corresponding to all base points are parallel and the angles of rotation equal and in the same direction . Hence ...
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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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