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 14
... instant of time . The path may be assigned by drawing it , or by stating its geometrical properties . The position of the point in the path may be assigned by giving the length ap measured along the path at every instant ; and this may ...
... instant of time . The path may be assigned by drawing it , or by stating its geometrical properties . The position of the point in the path may be assigned by giving the length ap measured along the path at every instant ; and this may ...
Página 15
... instant . Thus , at the instant t , about 3 seconds from the beginning of the motion , the distance traversed was tq , on the scale of centimeters marked on oY . Drawing qp horizontal to meet o Y , we find the distance about 7 ...
... instant . Thus , at the instant t , about 3 seconds from the beginning of the motion , the distance traversed was tq , on the scale of centimeters marked on oY . Drawing qp horizontal to meet o Y , we find the distance about 7 ...
Página 16
... instant , if we specify the step which must be taken to go to p from o at that instant . Now op = oa + ap . Let ab be the distance traversed in one second , then ap , being the distance traversed in t seconds , is tab . Hence we have op ...
... instant , if we specify the step which must be taken to go to p from o at that instant . Now op = oa + ap . Let ab be the distance traversed in one second , then ap , being the distance traversed in t seconds , is tab . Hence we have op ...
Página 18
... instant equal to the dis- tance ap measured along the path . P While this motion takes place , let the straight line oY have a uniform hori- zontal translation of one centimeter in every second ; then by this com- bination of motions ...
... instant equal to the dis- tance ap measured along the path . P While this motion takes place , let the straight line oY have a uniform hori- zontal translation of one centimeter in every second ; then by this com- bination of motions ...
Página 19
... instant . Draw pm , ob , perpendicular to oa . Then ор = om + mp . от Now as far as lengths are concerned , = cos aop , and mp = sin aop . Or , since op oa = ob ор ор and mp ob sin aop . In the in length , om- oa cos aop equation om ...
... instant . Draw pm , ob , perpendicular to oa . Then ор = om + mp . от Now as far as lengths are concerned , = cos aop , and mp = sin aop . Or , since op oa = ob ор ор and mp ob sin aop . In the in length , om- oa cos aop equation om ...
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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