Augustus Edward Hough Love,
1911 Encyclopædia Britannica
(1911)
“ There will be compression, the same at all points, and proportional to the pressure; and the amount of the compression can be expressed as The quantity is the modulus of compression. In this case the linear contraction in any direction is ; but in general the linear extension (or contraction) is not one-third of the cubical dilatation (or compression) . 24. To define the rigidity, we suppose that a solid body is subjected to forces in such a way that there is shearing stress within it. ”
