Rydberg constant
The Rydberg constant is a named after Johannes Rydberg constant of nature in an approximate formula for the calculation of atomic spectra, see Rydberg formula. The value is expressed as a wavenumber ionization energy of the hydrogen atom, neglecting relativistic effects and the motion of the nucleus (ie, infinite nuclear mass, hence the index).
The amounts present ( CODATA 2010) recommended value of the Rydberg constant
The relative standard uncertainty of 5.0 × 10-12. This makes it the most accurately measured fundamental constant at all.
Context of other fundamental constants
Rydberg constant α is obtained and the Compton wavelength? C, e of an electron from the fine structure constant by
With
- The mass of the electron
- The speed of light
- Planck's quantum of action
- The elementary charge
- The dielectric constant.
Rydberg frequency and Rydberg energy
The Rydberg constant is often expressed as a frequency or energy. The recommended values be
- Rydberg frequency:
- Rydberg energy:
The specific value of the Rydberg energy is called a Rydberg so is the Rydberg used as unit of measurement for energy.
Derivation
The Rydberg constant can be calculated from the following four conditions:
- The Bohr condition is
Where the radius of the electron orbit called.
- For the centripetal force
- Coulomb force between the electron and the singly charged atomic core
- The electric potential energy of the electron is:
With the relationship of de Broglie we obtained from the Bohr condition:
For a stable web is considered classic
Substituting ( 1) gives the radius
Under the assumptions made, these are therefore the only permissible path radii.
Moreover, it follows from (2) for the kinetic energy of
And for the total energy
Substituting ( 3) gives
Each orbit thus has a certain potential and kinetic energy so that when a change in the orbit from n1 to n2 takes place a change in energy. This is just
Or
Written as a change in wavelength:
The Rydberg constant is therefore just
This result was first determined by Niels Bohr as a consequence of his model of the atom.