Cambridge Senate-house Problems and Riders for the Year 1860: With SolutionsMacmillan, 1860 - 198 Seiten |
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Seite 17
... cylinder by a piston of given weight ; shew how to find the volume of the fluid . It is proved in Goodwin's Course , if pp ' be the pressures of the atmosphere at two points whose vertical distance is T x = 108 ( 1-7 ) - 108 5 .log " Ρ ...
... cylinder by a piston of given weight ; shew how to find the volume of the fluid . It is proved in Goodwin's Course , if pp ' be the pressures of the atmosphere at two points whose vertical distance is T x = 108 ( 1-7 ) - 108 5 .log " Ρ ...
Seite 18
... cylinder , then pA and Ax becomes the volume of the fluid . - W , p'A = W + W ' , Hence we have x = T ут log ( 1-7 ) k W · log W + W ' ' In this equation 7 is any very small quantity . If τ = 0 it is proved in the Course cited above ...
... cylinder , then pA and Ax becomes the volume of the fluid . - W , p'A = W + W ' , Hence we have x = T ут log ( 1-7 ) k W · log W + W ' ' In this equation 7 is any very small quantity . If τ = 0 it is proved in the Course cited above ...
Seite 30
... cylinder that the position of the cone in space may be unaltered . Let AB , CD be the old and new planes of floatation , cutting the cone in EF , HC . The condition that the posi- tion of the cone may be unaltered is the volume HF = vol ...
... cylinder that the position of the cone in space may be unaltered . Let AB , CD be the old and new planes of floatation , cutting the cone in EF , HC . The condition that the posi- tion of the cone may be unaltered is the volume HF = vol ...
Seite 47
... cylinder touching the plane of the meridian of the place along the axis of the heavens . The parallax in R. A. for bodies satisfying the condition mentioned in the question is α cos / sin h cos & 9 a being the Earth's radius , r the ...
... cylinder touching the plane of the meridian of the place along the axis of the heavens . The parallax in R. A. for bodies satisfying the condition mentioned in the question is α cos / sin h cos & 9 a being the Earth's radius , r the ...
Seite 67
... cylinder being parallel to the intersection of the plane with the horizon . Prove that the time in which the whole will be π unrolled is very approximately 4 the diameter of the original coil . ✓ sina ) , where d is gh We shall ...
... cylinder being parallel to the intersection of the plane with the horizon . Prove that the time in which the whole will be π unrolled is very approximately 4 the diameter of the original coil . ✓ sina ) , where d is gh We shall ...
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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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