A Collection of Problems in Illustration of the Principles of Theoretical MechanicsDeighton, Bell, 1876 - 667 páginas |
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Página vi
... Impact and Collision . Smooth Spherical Bodies CHAPTER II . Rectilinear Motion of a Particle I. Motion in Vacuum II . Motion in Resisting Media CHAPTER III . 206 219 220 234 Free Curvilinear Motion of a Particle . 248 I. Forces Acting ...
... Impact and Collision . Smooth Spherical Bodies CHAPTER II . Rectilinear Motion of a Particle I. Motion in Vacuum II . Motion in Resisting Media CHAPTER III . 206 219 220 234 Free Curvilinear Motion of a Particle . 248 I. Forces Acting ...
Página 205
... the point and the parallel tangent plane of the other face of the lens . Cayley ; Messenger of Mathematics , Vol . v . p . 194 . DYNAMICS . CHAPTER I. IMPACT AND COLLISION . SMOOTH SPHERICAL MISCELLANEOUS PROBLEMS . 205.
... the point and the parallel tangent plane of the other face of the lens . Cayley ; Messenger of Mathematics , Vol . v . p . 194 . DYNAMICS . CHAPTER I. IMPACT AND COLLISION . SMOOTH SPHERICAL MISCELLANEOUS PROBLEMS . 205.
Página 206
William Walton. DYNAMICS . CHAPTER I. IMPACT AND COLLISION . SMOOTH SPHERICAL BODIES . CONCEIVE two spherical bodies , which are composed of the same material , to be moving in the same ... Impact and Collision Smooth Spherical Bodies.
William Walton. DYNAMICS . CHAPTER I. IMPACT AND COLLISION . SMOOTH SPHERICAL BODIES . CONCEIVE two spherical bodies , which are composed of the same material , to be moving in the same ... Impact and Collision Smooth Spherical Bodies.
Página 207
... impact as e to 1 ; while the large body experiences no appreciable motion from the collision . This is evidently the case of bodies impinging and rebounding upon the surface of the earth , or upon other bodies firmly attached to it ...
... impact as e to 1 ; while the large body experiences no appreciable motion from the collision . This is evidently the case of bodies impinging and rebounding upon the surface of the earth , or upon other bodies firmly attached to it ...
Página 208
... , a ' , their velo- cities before collision . Then , putting in the formulæ ( A ) and ( B ) , u = a , u ' - a ' , e = 0 , we have v ′ – v = 0 , m ( a — v ) = m ' ( v ' + a ' ) , - and therefore - m ( a — v ) = 208 IMPACT AND COLLISION .
... , a ' , their velo- cities before collision . Then , putting in the formulæ ( A ) and ( B ) , u = a , u ' - a ' , e = 0 , we have v ′ – v = 0 , m ( a — v ) = m ' ( v ' + a ' ) , - and therefore - m ( a — v ) = 208 IMPACT AND COLLISION .
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Términos y frases comunes
absolute force acted angular velocity attraction axes axis beam body catenary centre of force centre of gravity circle co-ordinates coefficient of friction cos² curve cycloid cylinder denote density descends determine distance dt dt dt² dx dy dx² elastic ellipse equal equation Euler find the centre fixed point hence horizontal plane inclined plane inertia integrating James Bernoulli John Bernoulli lamina mass middle point moment of inertia motion natural length oscillation parabola perpendicular position of equilibrium pressure radius of gyration radius vector resolving forces rest right angles SECT sin² smooth sphere square straight line string supposing surface taking moments tangent tension triangle tube uniform rod varying inversely vertex vertical plane Vis Viva weight
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Página 203 - A centre of force attracting inversely as the square of the distance is at the centre of a spherical cavity within an infinite mass of liquid, the pressure on which at an infinite distance is...