Elements of Natural Philosophy |
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Page 31
... suppose the figure to be a mere flat disc or plane - for the preceding statements apply to any one of a set of parallel planes in a rigid body , moving in any way subject to the condition that the points of any one plane in it remain ...
... suppose the figure to be a mere flat disc or plane - for the preceding statements apply to any one of a set of parallel planes in a rigid body , moving in any way subject to the condition that the points of any one plane in it remain ...
Page 32
William Thomson Baron Kelvin, Peter Guthrie Tait. 97. Again , suppose ABDC to be a jointed frame , AB having a reciprocating motion about A , and by a link BD turning CD in A B the same plane about C. Deter . mine the relation between ...
William Thomson Baron Kelvin, Peter Guthrie Tait. 97. Again , suppose ABDC to be a jointed frame , AB having a reciprocating motion about A , and by a link BD turning CD in A B the same plane about C. Deter . mine the relation between ...
Page 39
... suppose the edge , AC , to be hori- zontal . By S 30 , if the upper board move horizontally to the right , the constraint will give it , in addition , a vertically upward motion , and the rates of these motions are in the constant ratio ...
... suppose the edge , AC , to be hori- zontal . By S 30 , if the upper board move horizontally to the right , the constraint will give it , in addition , a vertically upward motion , and the rates of these motions are in the constant ratio ...
Page 40
... Suppose a rigid body bounded by any curved surface to be touched at any point by another such body . Any motion of one on the other must be of one or more of the forms sliding , rolling , or spinning . The consideration of the first is ...
... Suppose a rigid body bounded by any curved surface to be touched at any point by another such body . Any motion of one on the other must be of one or more of the forms sliding , rolling , or spinning . The consideration of the first is ...
Page 47
... suppose there to be no alteration of volume on the whole , and neither elongation nor contraction along the mean principal axis . Let OX and OZ be the directions of maximum elongation and maximum contraction respectively . Let A be any ...
... suppose there to be no alteration of volume on the whole , and neither elongation nor contraction along the mean principal axis . Let OX and OZ be the directions of maximum elongation and maximum contraction respectively . Let A be any ...
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Common terms and phrases
acceleration action amount angular velocity anticlastic attraction axis called centimetre centre of gravity centre of inertia circle circular co-ordinates component configuration consider constant cord corresponding cosine couple curvature curve cylinder denote density described diagram displacement distance ellipse ellipsoid elongation equal equations equilibrium external point finite fixed point flexure fluid forces acting formulae friction geometrical given force Hence hodograph horizontal inclined infinitely small instant inversely kinetic energy length magnitude mass matter measured moment of inertia momentum moving normal section P₁ parallel parallelogram particle path pendulum perpendicular plane perpendicular portion position pressure principal axes principle produce projection proportional quantity radius radius of gyration reckoned rectangular relative right angles rigid body rotation round shear shell sides simple harmonic motion solid angle space spherical surface spiral square straight line strain stress suppose tangent theorem tion torsion uniform unit vertical weight whole wire