Elements of Dynamic: An Introduction to the Study of Motion and Rest in Solid and Fluid Bodies. Kinematic, Parte1,Libro 1Macmillan and Company, 1878 |
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Página 11
... centre , of the points a ,, a ......... ɑ „ : Similarly , it may be shewn that there is a point g such that , if , ... are any numbers , n ( 112 + 1 + ... + 1 ) og = 11 . oa1 + 1. oa2 + whatever point o is . 2 ... + In.oan ' n nn And ...
... centre , of the points a ,, a ......... ɑ „ : Similarly , it may be shewn that there is a point g such that , if , ... are any numbers , n ( 112 + 1 + ... + 1 ) og = 11 . oa1 + 1. oa2 + whatever point o is . 2 ... + In.oan ' n nn And ...
Página 19
... centre . The motions of p and q relative to o may be combined by completing the parallelogram oprq ; then the motion of r is the resultant . We may consider the paral- lelogram oprq to be made of four jointed rods , of which op and oq ...
... centre . The motions of p and q relative to o may be combined by completing the parallelogram oprq ; then the motion of r is the resultant . We may consider the paral- lelogram oprq to be made of four jointed rods , of which op and oq ...
Página 22
... centre of cc ' draw a plane perpen- dicular to the axis of the cylinder , which will cut the cylinder in a circle aba'b ' . Let bb ' be the in- tersection of the two planes . A plane through o perpendicular to bb ' will contain cc ' and ...
... centre of cc ' draw a plane perpen- dicular to the axis of the cylinder , which will cut the cylinder in a circle aba'b ' . Let bb ' be the in- tersection of the two planes . A plane through o perpendicular to bb ' will contain cc ' and ...
Página 24
... centre will be continually proportional to the height of the compound tide . For this purpose a series of horizontal lines at equal distances is drawn across the face of the clock , and the height is read off by running the eye along ...
... centre will be continually proportional to the height of the compound tide . For this purpose a series of horizontal lines at equal distances is drawn across the face of the clock , and the height is read off by running the eye along ...
Página 25
... centre of projection a to move away to an infinite distance , the lines converging to it will all become parallel . Thus we see that parallel projection is only a particular case of central projection in which the centre of projection ...
... centre of projection a to move away to an infinite distance , the lines converging to it will all become parallel . Thus we see that parallel projection is only a particular case of central projection in which the centre of projection ...
Otras ediciones - Ver todas
Elements of Dynamic; An Introduction to the Study of Motion and Rest in ... William Kingdon Clifford,Robert Tucker Sin vista previa disponible - 2016 |
Elements of Dynamic; An Introduction to the Study of Motion and Rest in ... William Kingdon Clifford,Robert Tucker Sin vista previa disponible - 2016 |
Elements of Dynamic; An Introduction to the Study of Motion and Rest in ... William Kingdon Clifford,Robert Tucker Sin vista previa disponible - 2016 |
Términos y frases comunes
abcd acceleration angular velocity approximately axes axis ca² called centimeter centrode circle circulation round College component conic section conjugate diameters constant cross-ratio Crown 8vo curvature curve of positions cycloidal cylinder cylindroid described direction displacement draw eccentric anomalies Edition ellipse equal equation equipotential surface Fcap fixed point flux function Hence hodograph homogeneous strain hyperbola hyperboloid infinite instant interval inverse length lines of flow magnitude mean velocity moving plane moving point multiplied numerous Illustrations orbit Owens College parabola parallelogram path perpendicular Professor projection quantity radius rate of change ratio represented resultant right angles rigid body rotation SCIENCE SCIENTIFIC CATALOGUE screw shew simple harmonic motion sphere spin step straight line strain-flux suppose surfaces of revolution theorem tion translation triangles twist uniform circular motion vector velocity-potential velocity-system zero
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