Treatise on Natural Philosophy, Volume 1, Part 1At the University Press, 1879 - Mechanics, Analytic |
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Page v
... complete account of what is now known of Natural Philosophy , in language adapted to the non - mathematical reader ; and to furnish , to those who have the privilege which high mathematical acquire- ments confer , a connected outline of ...
... complete account of what is now known of Natural Philosophy , in language adapted to the non - mathematical reader ; and to furnish , to those who have the privilege which high mathematical acquire- ments confer , a connected outline of ...
Page vii
... complete the chapter . The third chapter , " Experience , " treats briefly of Observa- tion and Experiment as the basis of Natural Philosophy . The fourth chapter deals with the fundamental Units , and the chief Instruments used for the ...
... complete the chapter . The third chapter , " Experience , " treats briefly of Observa- tion and Experiment as the basis of Natural Philosophy . The fourth chapter deals with the fundamental Units , and the chief Instruments used for the ...
Page xiv
... complete Integral - Practical In- terpretation of the complete Solution of the Characteristic Equation - Properties of Surfaces of Equal Action- Examples of Varying Action - Application to common Optics or Kinetics of a Single Particle ...
... complete Integral - Practical In- terpretation of the complete Solution of the Characteristic Equation - Properties of Surfaces of Equal Action- Examples of Varying Action - Application to common Optics or Kinetics of a Single Particle ...
Page 3
... complete , notation , 1 Ρ = 2 + ' d'a 2 ds curve . 7. If all points of the curve lie in one plane , it is called a Tortuous plane curve , and in the same way we speak of a plane polygon or broken line . If various points of the line do ...
... complete , notation , 1 Ρ = 2 + ' d'a 2 ds curve . 7. If all points of the curve lie in one plane , it is called a Tortuous plane curve , and in the same way we speak of a plane polygon or broken line . If various points of the line do ...
Page 8
... complete the explanation , as it depends on the theory of rolling , which will be treated afterwards ( §§ 110-137 ) . But it is enough at present to remark , that if a plane roll on the sphere , along the spherical curve , turning ...
... complete the explanation , as it depends on the theory of rolling , which will be treated afterwards ( §§ 110-137 ) . But it is enough at present to remark , that if a plane roll on the sphere , along the spherical curve , turning ...
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Common terms and phrases
acceleration action algebraic angular velocity anticlastic application Cambridge centre of inertia circle co-ordinates coefficients component configuration constant corresponding course curvature curve cycloidal cylinder degrees of freedom denote determined differential equation direction cosines displacement distance dt dt dt dy dx dy dy dy dy dz dynamical ellipsoid equal equations of motion equilibrium expression finite fluid force formula function give given gyrostatic Hence impulse infinitely small instant integral kinetic energy length linear mass measured momentum moving negative notation osculating plane P₁ parallel particle path perpendicular polygon position principal axes principle quadratic quadratic function quantity radius rectangular resultant rigid body rolling roots rotation round simple harmonic motions solution space spherical harmonic spherical surface St John's College strain suppose tangent plane theorem tion values whole zero αξ
Popular passages
Page 241 - Every body continues in its state of rest or of uniform motion in a straight line, except in so far as it may be compelled by impressed forces to change that state.