Elements of Natural Philosophy, Part 1 |
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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 the same plane about C. Deter- mine the relation between the ...
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 the same plane about C. Deter- mine the relation between the ...
Page 39
... suppose the edge , AC , to be hori- zontal . By 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 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 . Z Let OX and OZ be the directions of maximum elongation and maximum contraction respectively . Let A be ...
... suppose there to be no alteration of volume on the whole , and neither elongation nor contraction along the mean principal axis . Z Let OX and OZ be the directions of maximum elongation and maximum contraction respectively . Let A be ...
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Common terms and phrases
acceleration action amount angular velocity anticlastic applied attraction axes axis called Cambridge centre of gravity centre of inertia circle circular co-ordinates component configuration consider constant corresponding cosine couple curvature curve cylinder Demy 8vo denote density described diagram displacement distance edition elastic ellipse ellipsoid elongation equal equations equilibrium external point fixed point fluid forces acting friction geometrical given force Hence hodograph inclined infinitely small instant inversely kinetic energy length magnitude mass matter measured moment of inertia momentum moving normal P₁ P₂ parallel parallelogram particle path pendulum perpendicular portion position pressure principal axes principle produce projection proportional quantity radius radius of gyration reckoned resultant right angles rigid body rotation round shear shell simple harmonic motion solid solid angle space spherical surface spiral square straight line strain suppose tangent torsion uniform unit University of Cambridge vertical whole wire
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Page 69 - a viribus impressis cogitur statum suum mutare. Every body continues in its state of rest or of uniform motion in a straight line, except in so far as it may be compelled by impressed forces to change that state.
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