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 3
... equal and parallel . Consequently aa ' is equal and parallel to bb ' , and aa " to bb " . If therefore the path aa'a " be moved so that a comes to b , and the lines ad , aa " , are kept parallel to their original positions , the points ...
... equal and parallel . Consequently aa ' is equal and parallel to bb ' , and aa " to bb " . If therefore the path aa'a " be moved so that a comes to b , and the lines ad , aa " , are kept parallel to their original positions , the points ...
Página 4
... equal in length and in the same direction ; that is , not merely parallel , but drawn in the same sense on two ... equal , is used in the sense of equivalent . It means more than that the length aa ' is equal to the length bb ' , namely ...
... equal in length and in the same direction ; that is , not merely parallel , but drawn in the same sense on two ... equal , is used in the sense of equivalent . It means more than that the length aa ' is equal to the length bb ' , namely ...
Página 6
... equal and parallel to cd , and then from c ' a line equal and parallel to bc . But this line will end precisely at d , because bcdc ' is a parallelogram . Nothing after the point d will be altered , and consequently the resul- tant ae ...
... equal and parallel to cd , and then from c ' a line equal and parallel to bc . But this line will end precisely at d , because bcdc ' is a parallelogram . Nothing after the point d will be altered , and consequently the resul- tant ae ...
Página 15
... equal distances are gone over in equal times , the motion is said to be uniform . In uniform motion , the distances gone over in unequal times are proportional to the times ( Archimedes ) . For let t and Tbe unequal times in which the ...
... equal distances are gone over in equal times , the motion is said to be uniform . In uniform motion , the distances gone over in unequal times are proportional to the times ( Archimedes ) . For let t and Tbe unequal times in which the ...
Página 16
... equal to mT , ns is equal to mS ; and if nt is less than mT , ns is less than mS . Hence by Euclid's definition of proportion , SsT : t . Letv be the number of centimeters gone over ( or described ) in one second ; then s : v = t : 1 ...
... equal to mT , ns is equal to mS ; and if nt is less than mT , ns is less than mS . Hence by Euclid's definition of proportion , SsT : t . Letv be the number of centimeters gone over ( or described ) in one second ; then s : v = t : 1 ...
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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