Solutions of the problems and riders proposed in the Senate-house examination for 1854, by the moderators and examiners |
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Side 56
... equilibrium ; and shew that in every position of equilibrium the three angles at the 56 [ Jan. 18 , SENATE - HOUSE PROBLEMS AND RIDERS .
... equilibrium ; and shew that in every position of equilibrium the three angles at the 56 [ Jan. 18 , SENATE - HOUSE PROBLEMS AND RIDERS .
Side 57
... equilibrium of the ring will be satisfied , and also the relation between P and T will be such that the string may not slip round in either di- rection . To secure this latter we must have T > Pe- ( 2-0 ) , and T < P ( 2-0 ) .. ( 1 ) ...
... equilibrium of the ring will be satisfied , and also the relation between P and T will be such that the string may not slip round in either di- rection . To secure this latter we must have T > Pe- ( 2-0 ) , and T < P ( 2-0 ) .. ( 1 ) ...
Side 59
... equilibrium . The hemisphere is at rest under the action of three forces ; their directions must therefore lie in one plane , and pass through one point ; this plane must be vertical , and perpen- dicular to the two walls . In this ...
... equilibrium . The hemisphere is at rest under the action of three forces ; their directions must therefore lie in one plane , and pass through one point ; this plane must be vertical , and perpen- dicular to the two walls . In this ...
Side 65
... equilibrium , because the velocity and direction [ of motion ] of each point , [ fixed in the chain ] are the same each time it reaches the same point [ in space ; and therefore the resultant of all the effective forces on it during a ...
... equilibrium , because the velocity and direction [ of motion ] of each point , [ fixed in the chain ] are the same each time it reaches the same point [ in space ; and therefore the resultant of all the effective forces on it during a ...
Side 71
... equilibrium is at first unstable ; and find the condition which must be satisfied , in order that it may be possible to make the equilibrium stable by pouring in enough water . Let CFD ( fig . 34 ) be the base 91-121 . ] 71 PROBLEMS .
... equilibrium is at first unstable ; and find the condition which must be satisfied , in order that it may be possible to make the equilibrium stable by pouring in enough water . Let CFD ( fig . 34 ) be the base 91-121 . ] 71 PROBLEMS .
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Solutions of the Problems and Riders Proposed in the Senate-House ... Exam Papers Cambridge Univ Ingen forhåndsvisning tilgjengelig - 2016 |
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angular velocity asymptote axes Cambridge catenary centre of force centre of gravity chord circle cloth conic section constant cos² cose cosẞ cota cotß Crown 8vo curvature curve cylinder denoting described diameter direction distance dx dy dy dx ecliptic elastic ellipse equal equation equilibrium Fellow of St fixed point fluid geometrical progression given Hence horizontal hyperbola inclined plane intersection lamina latus rectum length locus longitude M.A. Fellow major axis middle point motion orbit parabola parallel particle passing perpendicular position pressure projection prove radius refraction right angles ring shew sides Similarly sine sino sinẞ straight line string Supposing surface tana tangent tanß triangle Trinity College tube V₁ vertical
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