Balmer series of hydrogen
E408510
The Balmer series of hydrogen is the set of spectral emission lines in the visible region produced when electrons in a hydrogen atom transition from higher energy levels down to the second principal energy level.
All labels observed (2)
| Label | Occurrences |
|---|---|
| Balmer series | 2 |
| Balmer series of hydrogen canonical | 1 |
How this entity was disambiguated
This entity first appeared as the object of triple T4046082 — resolving that mention is where its identity was fixed. The disambiguator weighed these candidate entities and picked the highlighted one (or “None”, minting a new entity). This is how homonymy is resolved: the same surface form can point to different entities.
Target entity: Balmer series of hydrogen Context triple: [Bohr model of the atom, explains, Balmer series of hydrogen]
-
A.
Lyman series in hydrogen spectrum
The Lyman series in the hydrogen spectrum is a set of ultraviolet emission or absorption lines produced when electrons in hydrogen atoms transition from higher energy levels down to the ground state (n=1).
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B.
Rydberg constant
The Rydberg constant is a fundamental physical constant that characterizes the limiting value of the highest wavenumber (or lowest wavelength) of any photon that can be emitted from the hydrogen atom, playing a key role in atomic spectroscopy and quantum theory.
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C.
Atombau und Spektrallinien
*Atombau und Spektrallinien* is Arnold Sommerfeld’s influential textbook on atomic structure and spectral lines that helped shape the development of early quantum theory.
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D.
Stark effect
The Stark effect is the splitting and shifting of atomic or molecular spectral lines caused by an external electric field.
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E.
Sommerfeld fine-structure formula
The Sommerfeld fine-structure formula is a relativistic extension of the Bohr model that accurately predicts the fine-structure energy levels of the hydrogen atom.
- F. None of above. chosen
- G. Unsure - the case is ambiguous/there is not enough information to decide.
Target entity: Balmer series of hydrogen Target entity description: The Balmer series of hydrogen is the set of spectral emission lines in the visible region produced when electrons in a hydrogen atom transition from higher energy levels down to the second principal energy level.
-
A.
Lyman series in hydrogen spectrum
The Lyman series in the hydrogen spectrum is a set of ultraviolet emission or absorption lines produced when electrons in hydrogen atoms transition from higher energy levels down to the ground state (n=1).
-
B.
Rydberg constant
The Rydberg constant is a fundamental physical constant that characterizes the limiting value of the highest wavenumber (or lowest wavelength) of any photon that can be emitted from the hydrogen atom, playing a key role in atomic spectroscopy and quantum theory.
-
C.
Atombau und Spektrallinien
*Atombau und Spektrallinien* is Arnold Sommerfeld’s influential textbook on atomic structure and spectral lines that helped shape the development of early quantum theory.
-
D.
Stark effect
The Stark effect is the splitting and shifting of atomic or molecular spectral lines caused by an external electric field.
-
E.
Sommerfeld fine-structure formula
The Sommerfeld fine-structure formula is a relativistic extension of the Bohr model that accurately predicts the fine-structure energy levels of the hydrogen atom.
- F. None of above. chosen
Statements (50)
| Predicate | Object |
|---|---|
| instanceOf |
atomic emission spectrum feature
ⓘ
spectral line series ⓘ |
| appliesTo | hydrogen atom ⓘ |
| approximateWavelengthRange | 400 nm to 700 nm ⓘ |
| canAlsoAppearAs | absorption line in stellar spectra ⓘ |
| correspondsTo | electron transitions from higher levels to n = 2 ⓘ |
| describedByFormula | 1/λ = R (1/2² − 1/n²) ⓘ |
| describes | visible spectral lines of hydrogen ⓘ |
| discoveredBy | Johann Balmer ⓘ |
| discoveryYear | 1885 ⓘ |
| energyChange | photon emission ⓘ |
| explainedBy |
Bohr model of the atom
ⓘ
surface form:
Bohr model of hydrogen atom
quantum mechanics ⓘ |
| H-alphaTransition | n = 3 to n = 2 ⓘ |
| H-alphaWavelength | 656.3 nm ⓘ |
| H-betaTransition | n = 4 to n = 2 ⓘ |
| H-betaWavelength | 486.1 nm ⓘ |
| H-deltaTransition | n = 6 to n = 2 ⓘ |
| H-deltaWavelength | 410.2 nm ⓘ |
| H-gammaTransition | n = 5 to n = 2 ⓘ |
| H-gammaWavelength | 434.0 nm ⓘ |
| hasFirstLineUpperLevel | principal quantum number n = 3 ⓘ |
| hasFourthLineUpperLevel | principal quantum number n = 6 ⓘ |
| hasLine |
H-alpha
ⓘ
H-beta ⓘ H-delta ⓘ H-gamma ⓘ |
| hasSecondLineUpperLevel | principal quantum number n = 4 ⓘ |
| hasSeriesLimit | n → ∞ to n = 2 ⓘ |
| hasThirdLineUpperLevel | principal quantum number n = 5 ⓘ |
| hasTransitionLowerLevel | principal quantum number n = 2 ⓘ |
| hasTransitionUpperLevel | principal quantum number n ≥ 3 ⓘ |
| isSubsetOf | hydrogen spectral series ⓘ |
| lineType | emission line ⓘ |
| namedAfter | Johann Balmer ⓘ |
| partOf | hydrogen emission spectrum ⓘ |
| photonEnergyRelation | E = hν = hc/λ ⓘ |
| relatedSeries |
Brackett series of hydrogen
ⓘ
Humphreys series of hydrogen ⓘ Lyman series in hydrogen spectrum ⓘ
surface form:
Lyman series of hydrogen
Paschen series ⓘ
surface form:
Paschen series of hydrogen
Pfund series ⓘ
surface form:
Pfund series of hydrogen
|
| RydbergConstantApproxValue | 1.097 × 10^7 m⁻¹ ⓘ |
| selectionRule | Δl = ±1 ⓘ |
| seriesLimitWavelengthApprox | 364.6 nm ⓘ |
| spectralRegion | visible ⓘ |
| usedIn |
determination of Rydberg constant
ⓘ
spectroscopic identification of hydrogen in stars ⓘ tests of Bohr model of the atom ⓘ |
| usesConstant | Rydberg constant ⓘ |
How these facts were elicited
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Subject: Balmer series of hydrogen Description of subject: The Balmer series of hydrogen is the set of spectral emission lines in the visible region produced when electrons in a hydrogen atom transition from higher energy levels down to the second principal energy level.
Referenced by (3)
Full triples — surface form annotated when it differs from this entity's canonical label.