Fraunhofer lines

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Wavelengths of the visual spectrum, 380 to about 740 nanometers (nm). Dips in intensity are observed as dark lines at the wavelengths of the Fraunhofer lines, (e.g., the features G, F, b, E, B). Spectrum of blue sky.svg
Wavelengths of the visual spectrum, 380 to about 740 nanometers (nm). Dips in intensity are observed as dark lines at the wavelengths of the Fraunhofer lines, (e.g., the features G, F, b, E, B).

The Fraunhofer lines are a set of spectral absorption lines. They are dark absorption lines, seen in the optical spectrum of the Sun, and are formed when atoms in the solar atmosphere absorb light being emitted by the solar photosphere. The lines are named after German physicist Joseph von Fraunhofer, who observed them in 1814.

Contents

Discovery

Solar spectrum with Fraunhofer lines as it appears visually. Fraunhofer lines.svg
Solar spectrum with Fraunhofer lines as it appears visually.

In 1802, English chemist William Hyde Wollaston [2] was the first person to note the appearance of a number of dark features in the solar spectrum. [3] In 1814, Joseph von Fraunhofer independently rediscovered the lines and began to systematically study and measure their wavelengths. He mapped over 570 lines, designating the most prominent with the letters A through K and weaker lines with other letters. [4] [5] [6] Modern observations of sunlight can detect many thousands of lines.

About 45 years later, Gustav Kirchhoff and Robert Bunsen [7] noticed that several Fraunhofer lines coincide with characteristic emission lines identified in the spectra of heated chemical elements. [8] They inferred that dark lines in the solar spectrum are caused by absorption by chemical elements in the solar atmosphere. [9] Some of the other observed features were instead identified as telluric lines originating from absorption by oxygen molecules in the Earth's atmosphere.

Sources

The Fraunhofer lines are typical spectral absorption lines. Absorption lines are narrow regions of decreased intensity in a spectrum, which are the result of photons being absorbed as light passes from the source to the detector. In the Sun, Fraunhofer lines are a result of gas in the Sun's atmosphere and outer photosphere. These regions have lower temperatures than gas in the inner photosphere, and absorbs some of the light emitted by it.

Naming

The major Fraunhofer lines, and the elements they are associated with, are shown in the following table:

Solar spectral irradiance measured with a calibrated optical spectrometer mounted with a cosine corrector. Some of the characteristic Fraunhofer lines and their corresponding elements are indicated for the extended visible spectrum (highlighted area in the graph).
For photometry and colorimetry, standard measurements are usually carried out in the range 360-830 nm. From these data and for this spectral range, the correlated color temperature (CCT) is 5470 K. Solar spectral irradiance.svg
Solar spectral irradiance measured with a calibrated optical spectrometer mounted with a cosine corrector. Some of the characteristic Fraunhofer lines and their corresponding elements are indicated for the extended visible spectrum (highlighted area in the graph).
For photometry and colorimetry, standard measurements are usually carried out in the range 360–830 nm. From these data and for this spectral range, the correlated color temperature (CCT) is 5470 K.
LineElementWavelength
(nm)
y O2 898.765
ZO2822.696
AO2759.370
BO2686.719
C Hα 656.281
aO2627.661
D1 Na 589.592
D2Na588.995
D3 (or d) He 587.5618
e Hg 546.073
E2 Fe 527.039
b1 Mg 518.362
b2Mg517.270
b3Fe516.891
b4Mg516.733
LineElementWavelength
(nm)
cFe495.761
F Hβ 486.134
dFe466.814
eFe438.355
G′ Hγ 434.047
GFe430.790
G Ca 430.774
h Hδ 410.175
HCa+396.847
KCa+393.366
LFe382.044
NFe358.121
P Ti +336.112
TFe302.108
t Ni 299.444
A demonstration of the 589 nm D2 (left) and 590 nm D1 (right) emission sodium D lines using a wick with salt water in a flame Cmglee Cambridge Science Festival 2016 sodium lines.jpg
A demonstration of the 589 nm D2 (left) and 590 nm D1 (right) emission sodium D lines using a wick with salt water in a flame

The Fraunhofer C, F, G′, and h lines correspond to the alpha, beta, gamma, and delta lines of the Balmer series of emission lines of the hydrogen atom. The Fraunhofer letters are now rarely used for those lines.

The D1 and D2 lines form a pair known as the "sodium doublet", the centre wavelength of which (589.29 nm) is given the designation letter "D". This historical designation for this line has stuck and is given to all the transitions between the ground state and the first excited state of the other alkali atoms as well. The D1 and D2 lines correspond to the fine-structure splitting of the excited states.

The Fraunhofer H and K letters are also still used for the calciumII doublet in the violet part of the spectrum, important in astronomical spectroscopy.

There is disagreement in the literature for some line designations; for example, the Fraunhofer d line may refer to the cyan iron line at 466.814 nm, or alternatively to the yellow helium line (also labeled D3) at 587.5618 nm. Similarly, there is ambiguity regarding the e line, since it can refer to the spectral lines of both iron (Fe) and mercury (Hg). In order to resolve ambiguities that arise in usage, ambiguous Fraunhofer line designations are preceded by the element with which they are associated (e.g., Mercury e line and Helium d line).

Because of their well-defined wavelengths, Fraunhofer lines are often used to specify standard wavelengths for characterising the refractive index and dispersion properties of optical materials.

See also

Related Research Articles

<span class="mw-page-title-main">Gustav Kirchhoff</span> German physicist and mathematician (1824–1887)

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<span class="mw-page-title-main">Spectroscopy</span> Study involving matter and electromagnetic radiation

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<span class="mw-page-title-main">Black body</span> Idealized physical body that absorbs all incident electromagnetic radiation

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Timeline of solar astronomy

<span class="mw-page-title-main">Joseph von Fraunhofer</span> German physicist (1787–1826)

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<span class="mw-page-title-main">Black-body radiation</span> Thermal electromagnetic radiation

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<span class="mw-page-title-main">Metallicity</span> Relative abundance of heavy elements in a star or other astronomical object

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<span class="mw-page-title-main">History of spectroscopy</span>

Modern spectroscopy in the Western world started in the 17th century. New designs in optics, specifically prisms, enabled systematic observations of the solar spectrum. Isaac Newton first applied the word spectrum to describe the rainbow of colors that combine to form white light. During the early 1800s, Joseph von Fraunhofer conducted experiments with dispersive spectrometers that enabled spectroscopy to become a more precise and quantitative scientific technique. Since then, spectroscopy has played and continues to play a significant role in chemistry, physics and astronomy. Fraunhofer observed and measured dark lines in the Sun's spectrum, which now bear his name although several of them were observed earlier by Wollaston.

<span class="mw-page-title-main">Nonmetallic material</span> How the term nonmetal is used in many disciplines

Nonmetallic material, or in nontechnical terms a nonmetal, refers to materials which are not metals. Depending upon context it is used in slightly different ways. In everyday life it would be a generic term for those materials such as plastics, wood or ceramics which are not typical metals such as the iron alloys used in bridges. In some areas of chemistry, particularly the periodic table, it is used for just those chemical elements which are not metallic at standard temperature and pressure conditions. It is also sometimes used to describe broad classes of dopant atoms in materials. In general usage in science, it refers to materials which do not have electrons that can readily move around, more technically there are no available states at the Fermi energy, the equilibrium energy of electrons. For historical reasons there is a very different definition of metals in astronomy, with just hydrogen and helium as nonmetals. The term may also be used as a negative of the materials of interest such as in metallurgy or metalworking.

References

  1. Starr, Cecie (2005). Biology: Concepts and Applications . Thomson Brooks/Cole. p.  94. ISBN   978-0-534-46226-0.
  2. Melvyn C. Usselman: William Hyde Wollaston Encyclopædia Britannica, retrieved 31 March 2013
  3. William Hyde Wollaston (1802) "A method of examining refractive and dispersive powers, by prismatic reflection," Philosophical Transactions of the Royal Society, 92: 365–380; see especially p. 378.
  4. Hearnshaw, J.B. (1986). The analysis of starlight. Cambridge: Cambridge University Press. p. 27. ISBN   978-0-521-39916-6.
  5. Joseph Fraunhofer (1814 - 1815) "Bestimmung des Brechungs- und des Farben-Zerstreuungs - Vermögens verschiedener Glasarten, in Bezug auf die Vervollkommnung achromatischer Fernröhre" (Determination of the refractive and color-dispersing power of different types of glass, in relation to the improvement of achromatic telescopes), Denkschriften der Königlichen Akademie der Wissenschaften zu München (Memoirs of the Royal Academy of Sciences in Munich), 5: 193–226; see especially pages 202–205 and the plate following page 226.
  6. Jenkins, Francis A.; White, Harvey E. (1981). Fundamentals of Optics (4th ed.). McGraw-Hill. p.  18. ISBN   978-0-07-256191-3.
  7. See:
    • Gustav Kirchhoff (1859) "Ueber die Fraunhofer'schen Linien" (On Fraunhofer's lines), Monatsbericht der Königlichen Preussische Akademie der Wissenschaften zu Berlin (Monthly report of the Royal Prussian Academy of Sciences in Berlin), 662–665.
    • Gustav Kirchhoff (1859) "Ueber das Sonnenspektrum" (On the sun's spectrum), Verhandlungen des naturhistorisch-medizinischen Vereins zu Heidelberg (Proceedings of the Natural History / Medical Association in Heidelberg), 1 (7) : 251–255.
  8. G. Kirchhoff (1860). "Ueber die Fraunhofer'schen Linien". Annalen der Physik. 185 (1): 148–150. Bibcode:1860AnP...185..148K. doi:10.1002/andp.18601850115.
  9. G. Kirchhoff (1860). "Ueber das Verhältniss zwischen dem Emissionsvermögen und dem Absorptionsvermögen der Körper für Wärme und Licht" [On the relation between the emissive power and the absorptive power of bodies towards heat and light]. Annalen der Physik. 185 (2): 275–301. Bibcode:1860AnP...185..275K. doi: 10.1002/andp.18601850205 .

Further reading