Elements of Natural Philosophy, Volume 1 |
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... II . ABSTRACT DYNAMICS . PAGE I 56 III 122 V. 19 INTRODUCTORY · 136 VI . " 9 STATICS OF A PARTICLE . ATTRACTION . • 140 VII . STATICS OF SOLIDS AND FLUIDS 9 : APPENDIX 199 · 282 DIVISION I. PRELIMINARY . CHAPTER I. - KINEMATICS . 1.
... II . ABSTRACT DYNAMICS . PAGE I 56 III 122 V. 19 INTRODUCTORY · 136 VI . " 9 STATICS OF A PARTICLE . ATTRACTION . • 140 VII . STATICS OF SOLIDS AND FLUIDS 9 : APPENDIX 199 · 282 DIVISION I. PRELIMINARY . CHAPTER I. - KINEMATICS . 1.
Page 60
... attracted by the earth with a given force . A merchant , with a balance and a set of standard weights , would give his customers the same quantity of the same kind of matter however the earth's attraction might vary , depending as he ...
... attracted by the earth with a given force . A merchant , with a balance and a set of standard weights , would give his customers the same quantity of the same kind of matter however the earth's attraction might vary , depending as he ...
Page 68
... attraction of the sun on a planet if the planet describe a circle with the sun in the centre , are all instances in which no work is done by the force . 206. The work done by a force , or by a couple , upon a body turning about an axis ...
... attraction of the sun on a planet if the planet describe a circle with the sun in the centre , are all instances in which no work is done by the force . 206. The work done by a force , or by a couple , upon a body turning about an axis ...
Page 70
... attraction of other bodies in the universe , alter his speed and that of the earth's rotation . 215. If two material points be projected from one position , 4 , at the same instant with any velocities in any directions , and each left ...
... attraction of other bodies in the universe , alter his speed and that of the earth's rotation . 215. If two material points be projected from one position , 4 , at the same instant with any velocities in any directions , and each left ...
Page 72
... attraction at these places . Again , if equal forces be exerted on different bodies , the changes of velocity produced in equal times must be inversely as the masses of the various bodies . This is approximately the case , for instance ...
... attraction at these places . Again , if equal forces be exerted on different bodies , the changes of velocity produced in equal times must be inversely as the masses of the various bodies . This is approximately the case , for instance ...
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Common terms and phrases
acceleration action amount angular velocity anticlastic attraction axis called centre of gravity centre of inertia circle circular co-ordinates component configuration consider constant cord corresponding cosine couple curvature curve cylinder denote density described diagram displacement distance ellipse ellipsoid elongation equal equations equilibrium external point finite fixed point flexure fluid forces acting formulae friction geometrical given force Hence hodograph horizontal inclined infinitely small instant inversely kinetic energy length magnitude mass matter measured moment of inertia momentum moving normal section P₁ parallel particle path pendulum perpendicular plane perpendicular portion position pressure principal axes principle produce projection proportional quantity radius radius of gyration reckoned rectangular right angles rigid body rotation round shear shell sides simple harmonic motion solid angle space spherical surface spiral square straight line strain stress suppose tangent theorem tion torsion uniform unit vertical weight whole wire