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Balmer series - перевод на русский
![Rutherford Bohr model]] of the [[hydrogen atom]], the Balmer lines result from an electron jump between the second energy level closest to the nucleus, and those levels more distant. Shown here is a photon emission. The 3→2 transition depicted here produces [[H-alpha]], the first line of the Balmer series. For hydrogen (''Z'' = 1) this transition results in a photon of [[wavelength]] 656 nm (red).](https://commons.wikimedia.org/wiki/Special:FilePath/Bohr atom model.svg?width=200 "Rutherford Bohr model]] of the [[hydrogen atom]], the Balmer lines result from an electron jump between the second energy level closest to the nucleus, and those levels more distant. Shown here is a photon emission. The 3→2 transition depicted here produces [[H-alpha]], the first line of the Balmer series. For hydrogen (''Z'' = 1) this transition results in a photon of [[wavelength]] 656 nm (red).")
![Two of the Balmer lines (α and β) are clearly visible in this emission spectrum of a [[deuterium lamp]]](https://commons.wikimedia.org/wiki/Special:FilePath/Deuterium lamp 1.png?width=200 "Two of the Balmer lines (α and β) are clearly visible in this emission spectrum of a [[deuterium lamp]]")
![visible range]]. Lines five and six can be seen with the [[naked eye]], but are considered to be [[ultraviolet]] as they have wavelengths less than 400 nm.](https://commons.wikimedia.org/wiki/Special:FilePath/Visible spectrum of hydrogen.jpg?width=200 "visible range]]. Lines five and six can be seen with the [[naked eye]], but are considered to be [[ultraviolet]] as they have wavelengths less than 400 nm.")
астрономия
бальмерова серия
![isbn=978-0-521-82073-8}} Goes to partial nine, unnumbered.</ref> partials 1–5 numbered
----<br />[[File:Harmonic series klang.mid]]Otonality[[File:Utonality 5-limit.mid]]Utonality[[File:Just major triad on C.mid]]Major chord on C[[File:Just minor triad on F.mid]]Minor chord on F](https://commons.wikimedia.org/wiki/Special:FilePath/Otonality and utonality 5-limit.png?width=200 "isbn=978-0-521-82073-8}} Goes to partial nine, unnumbered.</ref> partials 1–5 numbered
----<br />[[File:Harmonic series klang.mid]]Otonality[[File:Utonality 5-limit.mid]]Utonality[[File:Just major triad on C.mid]]Major chord on C[[File:Just minor triad on F.mid]]Minor chord on F")
![Undertone series on C.<ref name="Nattiez" />[[File:Undertone series on C.mid]]](https://commons.wikimedia.org/wiki/Special:FilePath/Undertone series on C.png?width=200 "Undertone series on C.<ref name=\"Nattiez\" />[[File:Undertone series on C.mid]]")
общая лексика
субгармоника
субгармонический
Определение
Википедия
The Balmer series, or Balmer lines in atomic physics, is one of a set of six named series describing the spectral line emissions of the hydrogen atom. The Balmer series is calculated using the Balmer formula, an empirical equation discovered by Johann Balmer in 1885.
The visible spectrum of light from hydrogen displays four wavelengths, 410 nm, 434 nm, 486 nm, and 656 nm, that correspond to emissions of photons by electrons in excited states transitioning to the quantum level described by the principal quantum number n equals 2. There are several prominent ultraviolet Balmer lines with wavelengths shorter than 400 nm. The number of these lines is an infinite continuum as it approaches a limit of 364.5 nm in the ultraviolet.
After Balmer's discovery, five other hydrogen spectral series were discovered, corresponding to electrons transitioning to values of n other than two .
