Cambridge Senate-house Problems and Riders for the Year 1860: With SolutionsMacmillan, 1860 - 198 sider |
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Side 17
... ( 1-7 ) - 108 5 .log " Ρ log ут k x , that where is the thickness of the very small layers into which the atmosphere was supposed divided . C = = If W weight of the piston , A 11-4 . ] 17 SENATE - HOUSE PROBLEMS AND RIDERS .
... ( 1-7 ) - 108 5 .log " Ρ log ут k x , that where is the thickness of the very small layers into which the atmosphere was supposed divided . C = = If W weight of the piston , A 11-4 . ] 17 SENATE - HOUSE PROBLEMS AND RIDERS .
Side 46
... supposed , let f be the focal length for the direct ray and x the refractive index for rays which are in- cident at the angle ; therefore to satisfy the required con- dition we must have the following relation between 4 and x , - ƒ { 1 ...
... supposed , let f be the focal length for the direct ray and x the refractive index for rays which are in- cident at the angle ; therefore to satisfy the required con- dition we must have the following relation between 4 and x , - ƒ { 1 ...
Side 70
... supposed to be the positions of m'm at the moment under consideration . Thus the whole attraction of m ' on a unit of mass of m when resolved along BC is m ' ( CD − x ) + m ' ( EC — y ) cos C. By treating m " in the same way we get the ...
... supposed to be the positions of m'm at the moment under consideration . Thus the whole attraction of m ' on a unit of mass of m when resolved along BC is m ' ( CD − x ) + m ' ( EC — y ) cos C. By treating m " in the same way we get the ...
Side 71
... supposed is √ ( l2 + 4π3n2 k2 ) ' the number of revolutions of the ellipse corresponding to the whole length of the barrel being n , and k being the radius of gyration of the ball about the axis coinciding with the axis of the barrel ...
... supposed is √ ( l2 + 4π3n2 k2 ) ' the number of revolutions of the ellipse corresponding to the whole length of the barrel being n , and k being the radius of gyration of the ball about the axis coinciding with the axis of the barrel ...
Side 117
... supposed bounded by similar ellip- soids , hence μ is really variable and proportional to the thick- ness h of the shell . Let uμh . Also by similar figures this thickness is proportional to p ; let n be the infinitely small ratio of ...
... supposed bounded by similar ellip- soids , hence μ is really variable and proportional to the thick- ness h of the shell . Let uμh . Also by similar figures this thickness is proportional to p ; let n be the infinitely small ratio of ...
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Cambridge Senate-house Problems and Riders for the Year 1860: With Solutions Henry William Watson,Edward John Routh Uten tilgangsbegrensning - 1860 |
Cambridge Senate-house Problems and Riders for the Year 1860: With Solutions Henry William Watson,Edward John Routh Uten tilgangsbegrensning - 1860 |
Cambridge Senate-house Problems and Riders for the Year 1860: With Solutions Henry William Watson,Edward John Routh Uten tilgangsbegrensning - 1860 |
Vanlige uttrykk og setninger
acceleration angular velocity Arabic numbers asymptotes attraction axes axis bisects Cambridge centre of force centre of gravity chord circle circular cloth co-ordinates cone conic conic section constant cos² Crown 8vo curvature cylinder described diameter differential equation direction directrix distance drawn dt dt ellipse ellipsoid equal angles equiangular spiral equilibrium extremity Fcap fixed point fluid foci focus given point Hence horizontal hyperbola inclined intersection latus rectum length locus MACMILLAN & CO.'S meridian motion normal parabola parallel particle perpendicular point of contact position pressure prove ratio respectively right angles Roman numbers SENIOR MODERATOR shew sides sin² singular solution smooth sphere spherical straight line string subtend surface tangent tension triangle Trinity College uniform vertex vertical Vis Viva weight аф
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