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Bernhard Riemann (1826 Bernhard Riemann (1826-1866) Bernhard ...

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► <strong>Riemann</strong> considered an appropriate new basis and<br />

compared the two forms associated to the “particle of<br />

substance” b ” at times t and d t’. ’ The h difference dff between b the h<br />

two forms is given by<br />

2 2 2 2 2 2 2<br />

δ ( ds) = ds'<br />

−ds<br />

= ( G −1)<br />

ds + ( G −1)<br />

ds + ( G −1)<br />

ds<br />

where<br />

ds<br />

1<br />

, ds<br />

2<br />

, ds<br />

3<br />

is<br />

1<br />

the<br />

new<br />

1<br />

basis.<br />

His result can be interpreted in terms of the classical<br />

theory y of elasticity. y Since ether is an elastic, , homogeneous g<br />

and isotropic substance, then one can consider an<br />

infinitesimal displacement u and deduce that the difference<br />

δ(ds) depends on the strain tensor due to the<br />

displacement. <strong>Riemann</strong> supposed that this variation δ(ds)<br />

produced a force able to modify the particle in such a way<br />

that the same particle, by opposing this deformation, would<br />

propagate p p g the pphysical y forces through g space. p<br />

2<br />

2<br />

3<br />

2<br />

3

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