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 26
Side 9
... zero , we find that ga + gb + gc = 0. This is independently clear , be- cause ga + gb = 2gf , and 2gf + ge = 0 by construction . Hence also we see that g is of the way from a to d , and from b to e , if d , e are the middle points of bc ...
... zero , we find that ga + gb + gc = 0. This is independently clear , be- cause ga + gb = 2gf , and 2gf + ge = 0 by construction . Hence also we see that g is of the way from a to d , and from b to e , if d , e are the middle points of bc ...
Side 52
... zero velocity , which can be readily observed and conceived . - · 1 = - In the motion of a falling body , for example , we have sta , where a is the distance fallen in the first second , and s the distance fallen in the first t seconds ...
... zero velocity , which can be readily observed and conceived . - · 1 = - In the motion of a falling body , for example , we have sta , where a is the distance fallen in the first second , and s the distance fallen in the first t seconds ...
Side 75
... 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 a curve and having the same curva- ture on the same side at the ...
... 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 a curve and having the same curva- ture on the same side at the ...
Side 79
... zero does not alter , but remains constant . There- fore sks , where k is constant ; so that in any interval equal ... zero or always zero . For let such a quantity be zero at a and have a finite value bq at b . At the middle point c of ...
... zero does not alter , but remains constant . There- fore sks , where k is constant ; so that in any interval equal ... zero or always zero . For let such a quantity be zero at a and have a finite value bq at b . At the middle point c of ...
Side 87
... ( mod . qt ) ; because the modulus of q " is the nth power of the modulus of q . We have before noticed that when the step p grows at the complex log . rate x + yi , its length or modulus r grows at the log . rate x . zero . Hence.
... ( mod . qt ) ; because the modulus of q " is the nth power of the modulus of q . We have before noticed that when the step p grows at the complex log . rate x + yi , its length or modulus r grows at the log . rate x . zero . Hence.
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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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