History of mass spectrometry

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The history of mass spectrometry has its roots in physical and chemical studies regarding the nature of matter. The study of gas discharges in the mid 19th century led to the discovery of anode and cathode rays, which turned out to be positive ions and electrons. Improved capabilities in the separation of these positive ions enabled the discovery of stable isotopes of the elements. The first such discovery was with the element neon, which was shown by mass spectrometry to have at least two stable isotopes: 20Ne (neon with 10 protons and 10 neutrons) and 22Ne (neon with 10 protons and 12 neutrons). Mass spectrometers were used in the Manhattan Project for the separation of isotopes of uranium necessary to create the atomic bomb.

Prout's Hypothesis[edit]

Prout's hypothesis was an early 19th-century attempt to explain the properties of the chemical elements using the internal structure of the atom. In 1815, the English chemist William Prout observed that the atomic weights that had been measured were integer multiples of the atomic weight of hydrogen.[1][2] Prout's hypothesis remained influential in chemistry throughout the 1820s. However, more careful measurements of the atomic weights, such as those compiled by Jöns Jakob Berzelius in 1828 or Edward Turner in 1832, appeared to disprove it. In particular the atomic weight of chlorine, which is 35.45 times that of hydrogen, could not at the time be explained in terms of Prout's hypothesis. It would take the better part of a century for this problem to be resolved.

Canal rays[edit]

In the mid-nineteenth century, Julius Plücker investigated the light emitted in discharge tubes and the influence of magnetic fields on the glow.[3] Later, in 1869, Johann Wilhelm Hittorf studied discharge tubes with energy rays extending from a negative electrode, the cathode. These rays produced a fluorescence when they hit a tube's glass walls, and when interrupted by a solid object they cast a shadow.

Canal rays, also called anode rays, were observed by Eugen Goldstein, in 1886. Goldstein used a gas discharge tube which had a perforated cathode. The rays are produced in the holes (canals) in the cathode and travels in a direction opposite to the "cathode rays," which are streams of electrons. Goldstein called these positive rays "Kanalstrahlen" - canal rays. In 1907 a study of how this "ray" was deflected in a magnetic field, revealed that the particles making up the ray were not all the same mass.

Discovery of isotopes[edit]

In the bottom right corner of this photographic plate are markings for the two isotopes of neon: neon-20 and neon-22.

In 1913, as part of his exploration into the composition of canal rays, J. J. Thomson channeled a stream of ionized neon through a magnetic and an electric field and measured its deflection by placing a photographic plate in its path. Thomson observed two patches of light on the photographic plate (see image on right), which suggested two different parabolas of deflection. Thomson concluded that the neon gas was composed of atoms of two different atomic masses (neon-20 and neon-22).[4]

Thomson's student Francis William Aston[5] continued the research at the Cavendish Laboratory in Cambridge, building the first full functional mass spectrometer that was reported in 1919.[6] He was able to identify isotopes of chlorine (35 and 37), bromine (79 and 81), and krypton (78, 80, 82, 83, 84 and 86), proving that these natural occurring elements are composed of a combination of isotopes. The use of electromagnetic focusing in mass spectrograph which rapidly allowed him to identify no fewer than 212 of the 287 naturally occurring isotopes. In 1921, F. W. Aston became a fellow of the Royal Society and received a Nobel Prize in Chemistry in the same year.

His work on isotopes also led to his formulation of the Whole Number Rule which states that "the mass of the oxygen isotope being defined [as 16], all the other isotopes have masses that are very nearly whole numbers," a rule that was used extensively in the development of nuclear energy. The exact mass of many isotopes was measured leading to the result that hydrogen has a 1% higher mass than expected by the average mass of the other elements. Aston speculated about the subatomic energy and the use of it in 1936.

In 1918, Arthur Jeffrey Dempster[7] reported on his mass spectrometer and established the basic theory and design of mass spectrometers that is still used to this day. Dempster's research over his career centered around the mass spectrometer and its applications, leading in 1935 to his discovery of the uranium isotope 235U. This isotope's ability to cause a rapidly expanding fission nuclear chain reaction allowed the development of the atom bomb and nuclear power.

In 1932, Kenneth Bainbridge developed a mass spectrometer with a resolving power of 600 and a relative precision of one part in 10,000.[8] He used this instrument to verify the equivalence of mass and energy, E = mc2.[9]

Manhattan Project[edit]

A Calutron is a sector mass spectrometer that was used for separating the isotopes of uranium developed by Ernest O. Lawrence[10] during the Manhattan Project and was similar to the Cyclotron invented by Lawrence. Its name is a concatenation of Cal. U.-tron, in tribute to the University of California, Lawrence's institution and the contractor of the Los Alamos laboratory.[11] They were implemented for industrial scale uranium enrichment at the Oak Ridge, Tennessee Y-12 plant established during the war and provided much of the uranium used for the "Little Boy" nuclear weapon, which was dropped onto Hiroshima in 1945.

Development of gas chromatography-mass spectrometry[edit]

The use of a mass spectrometer as the detector in gas chromatography was developed during the 1950s by Roland Gohlke and Fred McLafferty.[12][13] The development of affordable and miniaturized computers has helped in the simplification of the use of this instrument, as well as allowed great improvements in the amount of time it takes to analyze a sample.

Fourier transform mass spectrometry[edit]

Fourier transform ion cyclotron resonance mass spectrometry was developed by Alan G. Marshall and Melvin B. Comisarow at the University of British Columbia in 1974.[14] The inspiration was earlier developments in conventional ICR and Fourier Transform Nuclear Magnetic Resonance (FT-NMR) spectroscopy.

Soft ionization methods[edit]

Field desorption ionization was first reported by Beckey in 1969.[15] In field ionization, a high-potential electric field is applied to an emitter with a sharp surface, such as a razor blade, or more commonly, a filament from which tiny "whiskers" have been grown. This produces a very high electric field in which electron tunneling can result in ionization of gaseous analyte molecules. FI produces mass spectra with little or no fragmentation, dominated by molecular radical cations M+. and occasionally protonated molecules [M+H]^+.

Chemical ionization was developed in the 1960s.[16][17][18] Ionization of sample (analyte) is achieved by interaction of its molecules with reagent ions. The analyte is ionized by ion-molecule reactions during collisions in the source. The process may involve transfer of an electron, a proton or other charged species between the reactants. This is a less energetic procedure than electron ionization and the ions produced are, for example, protonated molecules: [M + H]+. These ions are often relatively stable, tending not to fragment as readily as ions produced by electron ionization.

Matrix-assisted laser desorption/ionization (MALDI) is a soft ionization technique used in mass spectrometry, allowing the analysis of biomolecules (biopolymers such as proteins, peptides and sugars) and large organic molecules (such as polymers, dendrimers and other macromolecules), which tend to be fragile and fragment when ionized by more conventional ionization methods. It is most similar in character to electrospray ionization both in relative softness and the ions produced (although it causes much fewer multiply charged ions). The term was first used in 1985 by Franz Hillenkamp, Michael Karas and their colleagues.[19] These researchers found that the amino acid alanine could be ionized more easily if it was mixed with the amino acid tryptophan and irradiated with a pulsed 266 nm laser. The tryptophan was absorbing the laser energy and helping to ionize the non-absorbing alanine. Peptides up to the 2843 Da peptide melittin could be ionized when mixed with this kind of “matrix”.[20] The breakthrough for large molecule laser desorption ionization came in 1987 when Koichi Tanaka of Shimadzu Corp. and his co-workers used what they called the “ultra fine metal plus liquid matrix method” that combined 30 nm cobalt particles in glycerol with a 337 nm nitrogen laser for ionization.[21] Using this laser and matrix combination, Tanaka was able to ionize biomolecules as large as the 34,472 Da protein carboxypeptidase-A. Tanaka received one-quarter of the 2002 Nobel Prize in Chemistry for demonstrating that, with the proper combination of laser wavelength and matrix, a protein can be ionized.[22] Karas and Hillenkamp were subsequently able to ionize the 67 kDa protein albumin using a nicotinic acid matrix and a 266 nm laser.[23] Further improvements were realized through the use of a 355 nm laser and the cinnamic acid derivatives ferulic acid, caffeic acid and sinapinic acid as the matrix.[24] The availability of small and relatively inexpensive nitrogen lasers operating at 337 nm wavelength and the first commercial instruments introduced in the early 1990s brought MALDI to an increasing number of researchers.[25] Today, mostly organic matrices are used for MALDI mass spectrometry.

Timeline[edit]

19th century[edit]

1886
Eugen Goldstein observes canal rays.
1898
Wilhelm Wien demonstrates that canal rays can be deflected using strong electric and magnetic fields. He shows that the mass-to-charge ratio of the particles have opposite polarity and is much larger compared to the electron. He also realizes that the particle mass is similar to the one of hydrogen particle.
1898
J. J. Thomson measures the mass-to-charge ratio of electrons.

20th century[edit]

1901
Walter Kaufmann uses a mass spectrometer to measure the relativistic mass increase of electrons.
1905
J. J. Thomson begins his study of positive rays.
1906
Thomson is awarded the Nobel Prize in Physics "in recognition of the great merits of his theoretical and experimental investigations on the conduction of electricity by gases"
1913
Thomson is able to separate particles of different mass-to-charge ratios. He separates the 20Ne and the 22Ne isotopes, and he correctly identifies the m/z = 11 signal as a doubly charged 22Ne particle.[26]
1919
Francis Aston constructs the first velocity focusing mass spectrograph with mass resolving power of 130.
1922
Aston is awarded the Nobel Prize in chemistry "for his discovery, by means of his mass spectrograph, of isotopes, in a large number of non-radioactive elements, and for his enunciation of the whole-number rule."
1931
Ernest O. Lawrence invents the cyclotron.
1934
Josef Mattauch and Richard Herzog develop the double-focusing mass spectrograph.
1936
Arthur J. Dempster develops the spark ionization source.
1937
Aston constructs a mass spectrograph with resolving power of 2000.
1939
Lawrence receives the Nobel Prize in Physics for the cyclotron.
1942
Lawrence develops the Calutron for uranium isotope separation.
1943
Westinghouse markets its mass spectrometer and proclaims it to be "A New Electronic Method for fast, accurate gas analysis".
1946
William Stephens presents the concept of a time-of-flight mass spectrometer.
1954
A. J. C. Nicholson (Australia) proposes a hydrogen transfer reaction that will come to be known as the McLafferty rearrangement.[27]
1959
Researchers at Dow Chemical interface a gas chromatograph to a mass spectrometer.
1964
British Mass Spectrometry Society established as first dedicated mass spectrometry society. It holds its first meeting in 1965 in London.
1966
F. H. Field and M. S. B. Munson develop chemical ionization.
1968
Malcolm Dole develops electrospray ionization.
1969
H. D. Beckey develops field desorption.
1974
Comisarow and Marshall develop Fourier Transform Ion Cyclotron Resonance mass spectrometry.
1976
Ronald MacFarlane and co-workers develop plasma desorption mass spectrometry.
1984
John Bennett Fenn and co-workers use electrospray to ionize biomolecules.
1985
Franz Hillenkamp, Michael Karas and co-workers describe and coin the term matrix-assisted laser desorption ionization (MALDI).
1987
Koichi Tanaka uses the “ultra fine metal plus liquid matrix method” to ionize intact proteins.
1989
Wolfgang Paul receives the Nobel Prize in Physics "for the development of the ion trap technique".
1999
Alexander Makarov presents the Orbitrap mass spectrometer.[28]

21st century[edit]

2002
John Bennett Fenn and Koichi Tanaka are awarded one-quarter of the Nobel Prize in chemistry each "for the development of soft desorption ionisation methods ... for mass spectrometric analyses of biological macromolecules."

See also[edit]

References[edit]

  1. ^ William Prout (1815). On the relation between the specific gravities of bodies in their gaseous state and the weights of their atoms. Annals of Philosophy, 6: 321–330. Online reprint
  2. ^ William Prout (1816). Correction of a mistake in the essay on the relation between the specific gravities of bodies in their gaseous state and the weights of their atoms. Annals of Philosophy, 7: 111–13. Online reprint
  3. ^ "Julius Plücker". Encyclopædia Britannica Online Academic Edition. Encyclopædia Britannica Inc. 
  4. ^ JJ Thomson (1913), Rays of positive electricity, Proceedings of the Royal Society, A 89, 1-20 — Discovery of neon isotopes
  5. ^ Downard KM (2009) Francis William Aston - The Man Behind the Mass Spectrograph, Eur. Mass Spectrom., 13, 177-190
  6. ^ Aston FW (1919) A positive ray spectrograph. Philosophical Magazine, 38, 707–714
  7. ^ Dempster AJ (1918) A New Method of Positive Ray Analysis, Phys. Rev. 11 (4): 316–325
  8. ^ Audi, Georges (2006-04-01). "The history of nuclidic masses and of their evaluation". International Journal of Mass Spectrometry 251 (2–3): 85–94. arXiv:physics/0602050. Bibcode:2006IJMSp.251...85A. doi:10.1016/j.ijms.2006.01.048. |url=http://www.sciencedirect.com/science/article/B6VND-4JKRWJX-2/2/628018a7bf50a32b4cdba32b77f181c8%7Cformat=%7Caccessdate=2008-04-11
  9. ^ Bainbridge, Kenneth T. (July 1933). "The Equivalence of Mass and Energy". Phys. Rev. 44 (2): 123. Bibcode:1933PhRv...44..123B. doi:10.1103/PhysRev.44.123.2. |url=|format=|accessdate=2008-04-11
  10. ^ "Lawrence and His Laborator". LBL Newsmagazine. Lawrence Berkeley Lab. 1981. Retrieved 2007-09-03. [dead link]
  11. ^ Parkins, William E. (2005-05-01). "The Uranium Bomb, the Calutron, and the Space-Charge Problem". Physics Today 58 (5): 45–51. Bibcode:2005PhT....58e..45P. doi:10.1063/1.1995747. |url=http://masspec.scripps.edu/MSHistory/timelines/time_pdf/1947_ParkinsWE.pdf%7Cformat=PDF%7Caccessdate=2007-09-01
  12. ^ Gohlke, R. S., Time-of-flight mass spectrometry and gas-liquid partition chromatography. Anal. Chem. 1959, 31, 535-41
  13. ^ Gohlke, R. S.; McLafferty, F. W., Early gas chromatography/mass spectrometry. J. Am. Soc. Mass Spectrom. 1993, 4, (5), 367-371.
  14. ^ Comisarow, M (1974). "Fourier transform ion cyclotron resonance spectroscopy". Chemical Physics Letters 25 (2): 282–283. Bibcode:1974CPL....25..282C. doi:10.1016/0009-2614(74)89137-2. 
  15. ^ Beckey H.D. (1969). "Field ionization mass spectrometry". Research/Development 20 (11): 26. 
  16. ^ Munson M.S.B., Field F.H. (1966). "Chemical Ionization Mass Spectrometry. I. General Introduction". J. Am. Chem. Soc. 88 (12): 2621–2630. doi:10.1021/ja00964a001. 
  17. ^ Fales HM, Milne GW, Pisano JJ, Brewer HB, Blum MS, MacConnell JG, Brand J, Law N (1972). "Biological applications of electron ionization and chemical ionization mass spectrometry". Recent Prog. Horm. Res. 28: 591–626. PMID 4569234. 
  18. ^ Dougherty RC (1981). "Negative chemical ionization mass spectrometry: applications in environmental analytical chemistry". Biomed. Mass Spectrom. 8 (7): 283–92. doi:10.1002/bms.1200080702. PMID 7025931. 
  19. ^ Karas, M.; Bachmann, D.; Hillenkamp, F. (1985). "Influence of the Wavelength in High-Irradiance Ultraviolet Laser Desorption Mass Spectrometry of Organic Molecules". Anal. Chem. 57 (14): 2935–9. doi:10.1021/ac00291a042. 
  20. ^ Karas, M.; Bachman, D.; Bahr, U.; Hillenkamp, F. (1987). "Matrix-Assisted Ultraviolet Laser Desorption of Non-Volatile Compounds". Int J Mass Spectrom Ion Proc 78: 53–68. doi:10.1016/0168-1176(87)87041-6. 
  21. ^ Tanaka, K.; Waki, H.; Ido, Y.; Akita, S.; Yoshida, Y.; Yoshida, T. (1988). "Protein and Polymer Analyses up to m/z 100 000 by Laser Ionization Time-of flight Mass Spectrometry". Rapid Commun Mass Spectrom 2 (20): 151–3. doi:10.1002/rcm.1290020802. 
  22. ^ Markides, K; Gräslund, A. "Advanced information on the Nobel Prize in Chemistry 2002" (PDF). 
  23. ^ Karas M, Hillenkamp F (1988). "Laser desorption ionization of proteins with molecular masses exceeding 10,000 daltons". Anal. Chem. 60 (20): 2299–301. doi:10.1021/ac00171a028. PMID 3239801. 
  24. ^ Beavis RC, Chait BT (1989). "Matrix-assisted laser-desorption mass spectrometry using 355 nm radiation". Rapid Commun. Mass Spectrom. 3 (12): 436–9. doi:10.1002/rcm.1290031208. PMID 2520224. 
  25. ^ Karas, M.; Bahr, U. (1990). "Laser Desorption Ionization Mass Spectrometry of Large Biomolecules". Trends Anal. Chem. 9 (10): 321–5. doi:10.1016/0165-9936(90)85065-F. 
  26. ^ "Joseph John Thomson (1856-1940) Rays of positive electricity". Classic Chemistry. Retrieved 2009-12-01. 
  27. ^ Nicholson AJC (1954). "Photochemical Decomposition of Aliphatic Methyl Ketones". Trans Faraday Soc. 50: 1067–1063. doi:10.1039/tf9545001067. 
  28. ^ http://www.asms.org/asms99pdf/095.pdf

Bibliography[edit]

  • Measuring Mass: From Positive Rays to Proteins by Michael A. Grayson (Editor) (ISBN 0-941901-31-9)

External links[edit]