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 v
... Velocities Fluxions Derived Functions Hodograph . Acceleration The Inverse Method 3 4 7 11 14 15 16 18 20 24 27 31 33 38 41 44 47 51 56 59 62 64 67 68 Curvature Tangential and Normal Acceleration Logarithmic Motion On Series Exponential.
... Velocities Fluxions Derived Functions Hodograph . Acceleration The Inverse Method 3 4 7 11 14 15 16 18 20 24 27 31 33 38 41 44 47 51 56 59 62 64 67 68 Curvature Tangential and Normal Acceleration Logarithmic Motion On Series Exponential.
Página vi
... Curvature Tangential and Normal Acceleration Logarithmic Motion On Series Exponential Series The Logarithmic Spiral . Quasi - Harmonic Motion in a Hyperbola CHAPTER III . CENTRAL ORBITS . The Theorem of Moments Product of two Vectors ...
... Curvature Tangential and Normal Acceleration Logarithmic Motion On Series Exponential Series The Logarithmic Spiral . Quasi - Harmonic Motion in a Hyperbola CHAPTER III . CENTRAL ORBITS . The Theorem of Moments Product of two Vectors ...
Página 73
... CURVATURE . A plane curve may be described by a point and a straight line which move together so that the point al- ways moves along the line and the line always turns round the point . ( Plücker . ) Let s be the arc of the curve ...
... CURVATURE . A plane curve may be described by a point and a straight line which move together so that the point al- ways moves along the line and the line always turns round the point . ( Plücker . ) Let s be the arc of the curve ...
Página 74
... curvature divided by the length of the arc is called the mean curvature of the arc ; and the cur- vature at any point is the value to which the mean cur- vature approaches as nearly as we like when the two ends of the arc are made to ...
... curvature divided by the length of the arc is called the mean curvature of the arc ; and the cur- vature at any point is the value to which the mean cur- vature approaches as nearly as we like when the two ends of the arc are made to ...
Página 75
... CURVATURE . 75 point 0 while s is finite , and the curvature is zero . When both motions are reversed , we have a rhamphoid 기 1 cusp or node - cusp ; the curvature is in general finite and the same on both branches . A circle touching ...
... CURVATURE . 75 point 0 while s is finite , and the curvature is zero . When both motions are reversed , we have a rhamphoid 기 1 cusp or node - cusp ; the curvature is in general finite and the same on both branches . A circle touching ...
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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