Rydberg constant: Difference between revisions
Jump to navigation
Jump to search
imported>John R. Brews (Rydberg constant stub) |
imported>John R. Brews No edit summary |
||
Line 7: | Line 7: | ||
</ref> | </ref> | ||
:<math>R_{\infty} = \frac{m_ee^4}{4\pi \hbar^3 c}\ \left( {\mu_0 c^2}{4 \pi}\right)^2 \ . </math> | :<math>R_{\infty} = \frac{m_ee^4}{4\pi \hbar^3 c}\ \left( \frac{\mu_0 c^2}{4 \pi}\right)^2 \ . </math> | ||
==Notes== | ==Notes== | ||
<references/> | <references/> |
Revision as of 10:11, 13 March 2011
The Rydberg constant, often denoted as R∞, originally defined empirically in terms of the spectrum of hydrogen, is given a theoretical value by the Bohr theory of the atom as:[1]
Notes
- ↑ GW Series (1988). “Chapter 10: Hydrogen and the fundamental atomic constants”, The Spectrum of atomic hydrogen--advances: a collection of progress reports by experts. World Scientific, p. 485. ISBN 9971502615.