Treatise on Natural Philosophy, Volume 1, Issue 1University Press, 1879 - Calculators |
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Page xii
... Particle and Point - Inertia . Force - Specification of a Force - Place of Application - Direc- tion - Magnitude - Accelerative Effect - Measure of Force Standards of Weight are Masses , and not primarily intended for Measurement of ...
... Particle and Point - Inertia . Force - Specification of a Force - Place of Application - Direc- tion - Magnitude - Accelerative Effect - Measure of Force Standards of Weight are Masses , and not primarily intended for Measurement of ...
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 ...
... 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 ...
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 . To find the tortuosity , do we have only to apply the general " equation above , with λ , μ , v substituted for l , m , n , and 1 du 1 dv - 7 ds ' 7 ds T for a , B , y . Thus we have r2 ...
... particle , and the statics of a flexible cord . To find the tortuosity , do we have only to apply the general " equation above , with λ , μ , v substituted for l , m , n , and 1 du 1 dv - 7 ds ' 7 ds T for a , B , y . Thus we have r2 ...
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Common terms and phrases
acceleration action algebraic angular velocity anticlastic application arbitrary axis Cambridge centre of inertia circle co-ordinates coefficients component configuration constant corresponding course curvature curve cycloidal cylinder denote determined differential equation direction cosines displacement distance dt dt dt dy dx dy dy dy dy dz ellipsoid equal equations of motion equilibrium expression finite fixed force formula function give given gyrostatic harmonic motions Hence impulse infinitely small instant integral kinetic energy Lagrange's linear mass measured momentum moving negative 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 simple harmonic motions solution spherical harmonic spherical surface St John's College strain suppose tangent plane theorem tion values variable whole Y₁ αξ λ² аф
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