Treatise on Natural Philosophy, Volume 1, Issue 1University Press, 1879 - Calculators |
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Page x
... Body due to given Rotations Most general Motion of a Rigid Body Precessional Rotation - Model illustrating Precession of Equi- noxes . • SECTIONS 78-94 95-101 102 , 103 • 104-107 · Free rotation of a Body kinetically symmetrical about ...
... Body due to given Rotations Most general Motion of a Rigid Body Precessional Rotation - Model illustrating Precession of Equi- noxes . • SECTIONS 78-94 95-101 102 , 103 • 104-107 · Free rotation of a Body kinetically symmetrical about ...
Page xi
... Body - Change of Plane in the Body- Conical Surface of equal elongation - Two Planes of no distortion , being the Circular Sections of the Strain Ellip- soid - Distortion in Parallel Planes without Change of Volume - Initial and altered ...
... Body - Change of Plane in the Body- Conical Surface of equal elongation - Two Planes of no distortion , being the Circular Sections of the Strain Ellip- soid - Distortion in Parallel Planes without Change of Volume - Initial and altered ...
Page xii
... Body - Moment of Momentum of a Rigid Body - Conservation of Momentum , and of Moment of Momentum - The " Invariable Plane " is a Plane through the Centre of Inertia , perpendicular to the Resultant Axis -Terrestrial Application - Rate ...
... Body - Moment of Momentum of a Rigid Body - Conservation of Momentum , and of Moment of Momentum - The " Invariable Plane " is a Plane through the Centre of Inertia , perpendicular to the Resultant Axis -Terrestrial Application - Rate ...
Page 60
... body . of a rigid body or group of points whose relative positions are unalterable . The simplest case we can consider is that of the motion of a plane figure in its own plane , and this , as far as kinematics is concerned , is entirely ...
... body . of a rigid body or group of points whose relative positions are unalterable . The simplest case we can consider is that of the motion of a plane figure in its own plane , and this , as far as kinematics is concerned , is entirely ...
Page 63
... body revolve in succession through equal angles , but in opposite di- rections , about two parallel axes , it finally takes a position to which it could have been brought by a simple translation per- pendicular to the lines of the body ...
... body revolve in succession through equal angles , but in opposite di- rections , about two parallel axes , it finally takes a position to which it could have been brought by a simple translation per- pendicular to the lines of the body ...
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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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