Elements of Dynamic: An Introduction to the Study of Motion and Rest in Solid and Fluid Bodies. Kinematic, Del 1,Bok 1Macmillan and Company, 1878 |
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Resultat 1-5 av 48
Side 3
... 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 a ' , a " must come ...
... 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 a ' , a " must come ...
Side 6
... consequently the resul- tant ae will be the same as before . Next , any change whatever in the order can be pro- duced by a sufficient number of interchanges of successive steps . This statement clearly does not apply to steps only ...
... consequently the resul- tant ae will be the same as before . Next , any change whatever in the order can be pro- duced by a sufficient number of interchanges of successive steps . This statement clearly does not apply to steps only ...
Side 20
... Consequently or is of constant length , and makes always the same angle with op or 09. Hence r goes round uniformly in a circle of radius or . Let op = p1 , oq = P2 , orp . Then , if a , b are the amplitudes , i , j unit steps at right ...
... Consequently or is of constant length , and makes always the same angle with op or 09. Hence r goes round uniformly in a circle of radius or . Let op = p1 , oq = P2 , orp . Then , if a , b are the amplitudes , i , j unit steps at right ...
Side 24
... consequently on = ol + om . Therefore the motion of n is compounded of the motions of 7 and m . But sincer moves uniformly in a circle , the motion of n is a simple harmonic motion . And we have seen that , when then Pi = a cos ( nt + ...
... consequently on = ol + om . Therefore the motion of n is compounded of the motions of 7 and m . But sincer moves uniformly in a circle , the motion of n is a simple harmonic motion . And we have seen that , when then Pi = a cos ( nt + ...
Side 26
... consequently be cut by the plane of projection in the parallel lines ab ' , c'd ' . Moreover the triangles pbb ' , qdd , having their respective Ст a sides parallel , are similar ; therefore pb : qd = pb ' : qd ' , and so also ab : cd ...
... consequently be cut by the plane of projection in the parallel lines ab ' , c'd ' . Moreover the triangles pbb ' , qdd , having their respective Ст a sides parallel , are similar ; therefore pb : qd = pb ' : qd ' , and so also ab : cd ...
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Elements of Dynamic; An Introduction to the Study of Motion and Rest in ... William Kingdon Clifford,Robert Tucker Ingen forhåndsvisning tilgjengelig - 2016 |
Elements of Dynamic; An Introduction to the Study of Motion and Rest in ... William Kingdon Clifford,Robert Tucker Ingen forhåndsvisning tilgjengelig - 2016 |
Elements of Dynamic; An Introduction to the Study of Motion and Rest in ... William Kingdon Clifford,Robert Tucker Ingen forhåndsvisning tilgjengelig - 2016 |
Vanlige uttrykk og setninger
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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