Treatise on Natural Philosophy, Volume 1, Part 1At the University Press, 1879 - Mechanics, Analytic |
From inside the book
Results 1-5 of 65
Page xii
... Particle and Point - Inertia . SECTIONS 205-216 Force - Specification of a Force - Place of Application - Direc- tion - Magnitude - Accelerative Effect - Measure of Force 217-220 Standards of Weight are Masses , and not primarily ...
... Particle and Point - Inertia . SECTIONS 205-216 Force - Specification of a Force - Place of Application - Direc- tion - Magnitude - Accelerative Effect - Measure of Force 217-220 Standards of Weight are Masses , and not primarily ...
Page xiv
... Particle - Application to System of free mutually influencing Particles -- and to Generalized System Slightly disturbed Equilibrium - Simultaneous Transformation of two Quadratic Functions to Sums of Squares - Gene- ralized Orthogonal ...
... Particle - Application to System of free mutually influencing Particles -- and to Generalized System Slightly disturbed Equilibrium - Simultaneous Transformation of two Quadratic Functions to Sums of Squares - Gene- ralized Orthogonal ...
Page xvi
... Particle moving on a Smooth Surface Incommensurable Oscillations - Oscil- latory Kinetic Stability - Limited Kinetic Stability- Kinetic Stability of a Projectile - General criterion - Ex- amples - Motion of a Particle on an anticlastic ...
... Particle moving on a Smooth Surface Incommensurable Oscillations - Oscil- latory Kinetic Stability - Limited Kinetic Stability- Kinetic Stability of a Projectile - General criterion - Ex- amples - Motion of a Particle on an anticlastic ...
Page 1
... particle , however , there cannot generally be any such abrupt changes of direction , since ( as we shall afterwards see ) this would imply the action of an infinite force , except in the case in which the velocity becomes zero at the ...
... particle , however , there cannot generally be any such abrupt changes of direction , since ( as we shall afterwards see ) this would imply the action of an infinite force , except in the case in which the velocity becomes zero at the ...
Page 6
... particle , and the statics of a flexible cord . dφ To find the tortuosity , o , we have only to apply the general equation above , with λ , μ , v substituted for l , m , n , and 1 dμ 1 dv αλ 2 Tds ' T ds for a , β , γ . Thus we have r ...
... particle , and the statics of a flexible cord . dφ To find the tortuosity , o , we have only to apply the general equation above , with λ , μ , v substituted for l , m , n , and 1 dμ 1 dv αλ 2 Tds ' T ds for a , β , γ . Thus we have r ...
Contents
227 | |
233 | |
242 | |
251 | |
264 | |
271 | |
282 | |
294 | |
102 | |
108 | |
114 | |
119 | |
125 | |
127 | |
136 | |
148 | |
154 | |
160 | |
167 | |
307 | |
338 | |
340 | |
358 | |
384 | |
428 | |
440 | |
457 | |
479 | |
493 | |
500 | |
Other editions - View all
Common terms and phrases
acceleration action altered angular velocity anticlastic application Cambridge centre of inertia change of direction circle co-ordinates coefficients component condition configuration constant corresponding course curvature curve cycloidal cylinder degrees of freedom denote determined diagram differential equation direction cosines distance dt dt dx dy dy dz ellipse ellipsoid elongation equal equations of motion equilibrium expression finite fixed fluid force function geometrical given gyrostatic Hence infinitely small initial instant integral kinetic energy length linear ment momentum moving parallel parallelepiped particle perpendicular polygon position principal axes quantity radius ratio rectangular resultant right angles rigid body rolling roots rotation round shear simple harmonic simple harmonic motions simple shear solution spherical harmonic spherical surface strain suppose synclastic tangent plane tangential displacement theorem tion twist values whole αξ λ²
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.