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 2
... divided into two parts : Static , ( δυναμις , which treats of those circumstances under which rest or null motion is possible , and Kinetic , which treats of cir- ON STEPS . cumstances under which actual motion always takes 2 DYNAMIC .
... divided into two parts : Static , ( δυναμις , which treats of those circumstances under which rest or null motion is possible , and Kinetic , which treats of cir- ON STEPS . cumstances under which actual motion always takes 2 DYNAMIC .
Página 8
... divided in c so that ac is to cb as m to l , where 7 and m are any two numbers . Then 1. ac m.cb and ( l + m ) . ac = m . ab . = a Now oc = oa + ac ; that is to say , the step oc is the resultant of oa and ac . Therefore ( l + m ) oc ...
... divided in c so that ac is to cb as m to l , where 7 and m are any two numbers . Then 1. ac m.cb and ( l + m ) . ac = m . ab . = a Now oc = oa + ac ; that is to say , the step oc is the resultant of oa and ac . Therefore ( l + m ) oc ...
Página 10
... divided . Multiplying these equations together , we find that the product Imn divides out , and that fa.ec. db = bf . ae . cd . Hence if ad , be , cf meet in a point , then af.ce.bd ea . dc.fb. This theorem is a = useful criterion for ...
... divided . Multiplying these equations together , we find that the product Imn divides out , and that fa.ec. db = bf . ae . cd . Hence if ad , be , cf meet in a point , then af.ce.bd ea . dc.fb. This theorem is a = useful criterion for ...
Página 27
... divided into such rectangles together with pieces over , by drawing lines across it at equal distances per- pendicular to the intersection of the two planes , and then lines parallel to the intersection through the points when they meet ...
... divided into such rectangles together with pieces over , by drawing lines across it at equal distances per- pendicular to the intersection of the two planes , and then lines parallel to the intersection through the points when they meet ...
Página 42
... divided by b and c ) . And sin avb . sin cvd : sin avc . sin bvd is called a cross - ratio of the four lines va , vb , vc , vd . Hence as the cross - ratio of the points abcd is equal to the corresponding cross - ratio of the lines va ...
... divided by b and c ) . And sin avb . sin cvd : sin avc . sin bvd is called a cross - ratio of the four lines va , vb , vc , vd . Hence as the cross - ratio of the points abcd is equal to the corresponding cross - ratio of the lines va ...
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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