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The study of HNC is a relatively simple pursuit, and this is one of the greatest motivations for its study. Aside from having its ''J''&nbsp;=&nbsp;1→0 transition in a clear portion of the atmospheric window, as well as having numerous isotopomers also available for easy study, and in addition to having a large dipole moment that makes observations particularly simple, HNC is, in its molecular nature, a quite simple molecule. This makes the study of the reaction pathways that lead to its formation and destruction a good means of obtaining insight to the workings of these reactions in space. Furthermore, the study of the tautomerization of HNC to HCN (and vice versa), which has been studied extensively, has been suggested as a model by which more complicated isomerization reactions can be studied.<ref name="Bentley1993" /><ref>{{cite journal|author=Skurski, P.|display-authors=etal|year=2001|title=''Ab initio'' electronic structure of HCN<sup>−</sup> and HNC<sup>−</sup> dipole-bound anions and a description of electron loss upon tautomerization|journal=J. Chem. Phys.|volume=114|issue=17|page=7446|bibcode=2001JChPh.114.7443S|doi=10.1063/1.1358863}}</ref><ref>{{cite journal|author1=Jakubetz, W.|author2=Lan, B. L.|year=1997|title=A simulation of ultrafast state-selective IR-laser-controlled isomerization of hydrogen cyanide based on global 3D ab initio potential and dipole surfaces|journal=Chem. Phys.|volume=217|issue=2–3|pages=375–388|bibcode=1997CP....217..375J|doi=10.1016/S0301-0104(97)00056-6}}</ref>
The study of HNC is a relatively simple pursuit, and this is one of the greatest motivations for its study. Aside from having its ''J''&nbsp;=&nbsp;1→0 transition in a clear portion of the atmospheric window, as well as having numerous isotopomers also available for easy study, and in addition to having a large dipole moment that makes observations particularly simple, HNC is, in its molecular nature, a quite simple molecule. This makes the study of the reaction pathways that lead to its formation and destruction a good means of obtaining insight to the workings of these reactions in space. Furthermore, the study of the tautomerization of HNC to HCN (and vice versa), which has been studied extensively, has been suggested as a model by which more complicated isomerization reactions can be studied.<ref name="Bentley1993" /><ref>{{cite journal|author=Skurski, P.|display-authors=etal|year=2001|title=''Ab initio'' electronic structure of HCN<sup>−</sup> and HNC<sup>−</sup> dipole-bound anions and a description of electron loss upon tautomerization|journal=J. Chem. Phys.|volume=114|issue=17|page=7446|bibcode=2001JChPh.114.7443S|doi=10.1063/1.1358863}}</ref><ref>{{cite journal|author1=Jakubetz, W.|author2=Lan, B. L.|year=1997|title=A simulation of ultrafast state-selective IR-laser-controlled isomerization of hydrogen cyanide based on global 3D ab initio potential and dipole surfaces|journal=Chem. Phys.|volume=217|issue=2–3|pages=375–388|bibcode=1997CP....217..375J|doi=10.1016/S0301-0104(97)00056-6}}</ref>


Hajj
==Chemistry in the interstellar medium==

HNC is found primarily in dense molecular clouds, though it is ubiquitous in the interstellar medium. Its abundance is closely linked to the abundances of other nitrogen-containing compounds.<ref name="Turner1997">{{cite journal|author=Turner, B. E.|display-authors=etal|year=1997|title=The Physics and Chemistry of Small Translucent Molecular Clouds. VIII. HCN and HNC|journal=Astrophysical Journal|volume=483|issue=1|pages=235–261|bibcode=1997ApJ...483..235T|doi=10.1086/304228}}</ref> HNC is formed primarily through the [[dissociative recombination]] of [[HCNH+|HNCH<sup>+</sup>]] and H<sub>2</sub>NC<sup>+</sup>, and it is destroyed primarily through ion-neutral reactions with {{chem|H|3|+}} and C<sup>+</sup>.<ref name="Hiraoka2006">{{cite journal|author=Hiraoka, K.|display-authors=etal|year=2006|title=How are CH<sub>3</sub>OH, HNC/HCN, and NH<sub>3</sub> Formed in the Interstellar Medium?|url=|journal=AIP Conf. Proc.|volume=855|issue=|pages=86–99|doi=10.1063/1.2359543}}</ref><ref>{{cite journal|author=Doty, S. D.|display-authors=etal|year=2004|title=Physical-chemical modeling of the low-mass protostar IRAS 16293-2422|journal=Astronomy and Astrophysics|volume=418|issue=3|pages=1021–1034|arxiv=astro-ph/0402610|bibcode=2004A&A...418.1021D|doi=10.1051/0004-6361:20034476}}</ref> Rate calculations were done at 3.16&nbsp;×&nbsp;10<sup>5</sup> years, which is considered early time, and at 20&nbsp;K, which is a typical temperature for dense molecular clouds.<ref>{{Cite web|url=http://udfa.net/|title=The UMIST Database for Astrochemistry|last=|first=|date=|website=|archive-url=|archive-date=|dead-url=|access-date=}}</ref><ref>{{cite journal|author=Millar, T. J.|display-authors=etal|year=1997|title=The UMIST database for astrochemistry 1995|journal=Astronomy and Astrophysics Supplement Series|volume=121|issue=|pages=139–185|doi=10.1051/aas:1997118|arxiv=1212.6362|bibcode=1997A&AS..121..139M}}</ref>

{| border="1" cellpadding="5" cellspacing="0"
|-
! colspan="7" style="text-align:center;"| '''Formation Reactions'''
|-
| style="text-align:center;"| '''Reactant 1''' || '''Reactant 2''' || '''Product 1''' || '''Product 2''' || '''Rate constant''' || '''Rate/[H<sub>2</sub>]<sup>2</sup>''' || '''Relative Rate'''
|-
| HCNH<sup>+</sup> || e<sup>−</sup> || HNC || H || {{val|9.50e-8}} || {{val|4.76e-25}} || 3.4
|-
| H<sub>2</sub>NC<sup>+</sup> || e<sup>−</sup> || HNC || H || {{val|1.80e-7}} || {{val|1.39e-25}} || 1.0
|-
! colspan="7" style="text-align:center;"| '''Destruction Reactions'''
|-
| style="text-align:center;"| '''Reactant 1''' || '''Reactant 2''' || '''Product 1''' || '''Product 2''' || '''Rate constant''' || '''Rate/[H<sub>2</sub>]<sup>2</sup>''' || '''Relative Rate'''
|-
| {{chem|H|3|+}} || HNC || HCNH<sup>+</sup> || H<sub>2</sub> || {{val|8.10e-9}} || {{val|1.26e-24}} || 1.7
|-
| C<sup>+</sup> || HNC || C<sub>2</sub>N<sup>+</sup> || H || {{val|3.10e-9}} || {{val|7.48e-25}} || 1.0
|}

These four reactions are merely the four most dominant, and thus the most significant in the formation of the HNC abundances in dense molecular clouds; there are dozens more reactions for the formation and destruction of HNC. Though these reactions primarily lead to various protonated species, HNC is linked closely to the abundances of many other nitrogen containing molecules, for example, NH<sub>3</sub> and CN.<ref name="Turner1997" /> The abundance HNC is also inexorably linked to the abundance of HCN, and the two tend to exist in a specific ratio based on the environment.<ref name="Hiraoka2006" /> This is because the reactions that form HNC can often also form HCN, and vice versa, depending on the conditions in which the reaction occurs, and also that there exist isomerization reactions for the two species.


==Astronomical detections==
==Astronomical detections==

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'{{chembox | Watchedfields = changed | verifiedrevid = 443863009 | ImageFileL1 = Hydrogen-isocyanide-2D.png | ImageNameL1 = Hydrogen cyanide bonding | ImageFileR1 = Hydrogen-isocyanide-3D-vdW.png | ImageNameR1 = Hydrogen cyanide space filling | IUPACName = hydrogen isocyanide<br>azanylidyniummethanide | OtherNames = isohydrocyanic acid<br>hydroisocyanic acid<br>isoprussic acid |Section1={{Chembox Identifiers | StdInChI_Ref = {{stdinchicite|correct|chemspider}} | StdInChI = 1S/CHN/c1-2/h2H | StdInChIKey_Ref = {{stdinchicite|correct|chemspider}} | StdInChIKey = QIUBLANJVAOHHY-UHFFFAOYSA-N | CASNo_Ref = {{cascite|correct|??}} | CASNo = | EINECS = | PubChem = 6432654 | ChemSpiderID_Ref = {{chemspidercite|correct|chemspider}} | ChemSpiderID = 4937885 | ChEBI_Ref = {{ebicite|correct|EBI}} | ChEBI = 36856 | SMILES = [C-]#[NH+] | InChI = 1/CHN/c1-2/h2H | RTECS = }} |Section2={{Chembox Properties | Formula = HNC | MolarMass = 27.03 g/mol | Appearance = | Density = | MeltingPt = | BoilingPt = | Solubility = | VaporPressure = | ConjugateAcid = [[Hydrocyanonium]] | ConjugateBase = [[Cyanide]] }} |Section3={{Chembox Hazards | MainHazards = | FlashPt = | AutoignitionPt = }} }} '''Hydrogen isocyanide''' is a chemical with the molecular formula HNC. It is a minor [[tautomer]] of [[hydrogen cyanide]] (HCN). Its importance in the field of [[astrochemistry]] is linked to its ubiquity in the [[interstellar medium]]. == Nomenclature == Both ''hydrogen isocyanide'' and ''azanylidyniummethanide'' are correct [[IUPAC name]]s for HNC. There is no [[preferred IUPAC name]]. The second one is according to the ''[[substitutive nomenclature]] rules'', derived from the ''[[parent hydride]]'' [[azane]] (NH<sub>3</sub>) and the anion [[methanide]] (C<sup>−</sup>).<ref>The suffix ''ylidyne'' refers to the loss of three hydrogen atoms from the nitrogen atom in [[azanium]] ({{chem|NH|4|+}}) See the [http://www.iupac.org/publications/books/rbook/Red_Book_2005.pdf ''IUPAC Red Book'' 2005] Table III, "Suffixes and endings", p. 257.</ref> ==Molecular properties== Hydrogen isocyanide (HNC) is a linear triatomic molecule with C<sub>∞v</sub> [[Molecular symmetry|point group symmetry]]. It is a [[zwitterion]] and an [[isomer]] of [[hydrogen cyanide]] (HCN).<ref>{{Cite journal|last=Pau|first=Chin Fong|last2=Hehre|first2=Warren J.|date=1982-02-01|title=Heat of formation of hydrogen isocyanide by ion cyclotron double resonance spectroscopy|journal=The Journal of Physical Chemistry|volume=86|issue=3|pages=321–322|doi=10.1021/j100392a006|issn=0022-3654}}</ref> Both HNC and HCN have large, similar [[Molecular dipole moment|dipole moment]]s, with ''μ''<sub>HNC</sub>&nbsp;=&nbsp;3.05 [[Debye]] and ''μ''<sub>HCN</sub>&nbsp;=&nbsp;2.98 Debye respectively.<ref name="Tennekes2006">{{cite journal|author=Tennekes, P. P.|display-authors=etal|year=2006|title=HCN and HNC mapping of the protostellar core Chamaeleon-MMS1|journal=Astronomy and Astrophysics|volume=456|issue=3|pages=1037–1043|arxiv=astro-ph/0606547|bibcode=2006A&A...456.1037T|doi=10.1051/0004-6361:20040294}}</ref> These large dipole moments facilitate the easy observation of these species in the [[interstellar medium]]. === HNC−HCN tautomerism === As HNC is higher in energy than HCN by 3920&nbsp;cm<sup>−1</sup> (46.9&nbsp; kJ/mol), one might assume that the two would have an equilibrium ratio<math display="inline">\left ( \frac{[HNC]}{[HCN]} \right )_{eq}</math> at temperatures below 100 Kelvin of 10<sup>−25</sup>.<ref>{{cite journal|author=Hirota, T.|display-authors=etal|year=1998|title=Abundances of HCN and HNC in Dark Cloud Cores|journal=Astrophysical Journal|volume=503|issue=2|pages=717–728|bibcode=1998ApJ...503..717H|doi=10.1086/306032}}</ref> However, observations show a very different conclusion; <math display="inline">\left ( \frac{[HNC]}{[HCN]} \right )_{observed}</math> is much higher than 10<sup>−25</sup>, and is in fact on the order of unity in cold environments. This is because of the potential energy path of the tautomerization reaction; there is an activation barrier on the order of roughly 12,000&nbsp;cm<sup>−1</sup> for the tautomerization to occur, which corresponds to a temperature at which HNC would already have been destroyed by neutral-neutral reactions.<ref name="Bentley1993">{{cite journal|author=Bentley, J. A.|display-authors=etal|year=1993|title=Highly virationally excited HCN/HNC: Eigenvalues, wave functions, and stimulated emission pumping spectra|journal=J. Chem. Phys.|volume=98|issue=7|page=5209|bibcode=1993JChPh..98.5207B|doi=10.1063/1.464921}}</ref> ==Spectral properties== In practice, HNC is almost exclusively observed astronomically using the ''J''&nbsp;=&nbsp;1→0 transition. This transition occurs at ~90.66&nbsp;GHz, which is a point of good visibility in the [[Radio window|atmospheric window]], thus making astronomical observations of HNC particularly simple. Many other related species (including HCN) are observed in roughly the same window.<ref name=Schilke1992>{{cite journal|author=Schilke, P.|display-authors=etal|year=1992|title=A study of HCN, HNC and their isotopomers in OMC-1. I. Abundances and chemistry|journal=Astronomy and Astrophysics|volume=256|issue=|pages=595–612|bibcode=1992A&A...256..595S}}</ref><ref name="Pratap1997">{{cite journal|author=Pratap, P.|display-authors=etal|year=1997|title=A Study of the Physics and Chemistry of TMC-1|journal=Astrophysical Journal|volume=486|issue=2|pages=862–885|bibcode=1997ApJ...486..862P|doi=10.1086/304553}}</ref> ==Significance in the interstellar medium== HNC is intricately linked to the formation and destruction of numerous other molecules of importance in the interstellar medium—aside from the obvious partners HCN, [[HCNH+|protonated hydrogen cyanide (HCNH<sup>+</sup>)]], and [[Cyanide|cyanide (CN)]], HNC is linked to the abundances of many other compounds, either directly or through a few degrees of separation. As such, an understanding of the chemistry of HNC leads to an understanding of countless other species—HNC is an integral piece in the complex puzzle representing interstellar chemistry. Furthermore, HNC (alongside HCN) is a commonly used tracer of dense gas in molecular clouds. Aside from the potential to use HNC to investigate [[gravitational collapse]] as the means of star formation, HNC abundance (relative to the abundance of other nitrogenous molecules) can be used to determine the evolutionary stage of protostellar cores.<ref name="Tennekes2006" /> The HCO<sup>+</sup>/HNC line ratio is used to good effect as a measure of density of gas.<ref>{{cite journal|author=Loenen, A. F.|display-authors=etal|year=2007|title=Molecular properties of (U)LIRGs: CO, HCN, HNC and HCO<sup>+</sup>|journal=Proceedings IAU Symposium|volume=242|issue=|pages=1–5}}</ref> This information provides great insight into the mechanisms of the formation of (Ultra-)Luminous Infrared Galaxies ((U)LIRGs), as it provides data on the nuclear environment, [[star formation]], and even [[black hole]] fueling. Furthermore, the HNC/HCN line ratio is used to distinguish between [[Photodissociation region|photodissociation regions]] and X-ray-dissociation regions on the basis that [HNC]/[HCN] is roughly unity in the former, but greater than unity in the latter. The study of HNC is a relatively simple pursuit, and this is one of the greatest motivations for its study. Aside from having its ''J''&nbsp;=&nbsp;1→0 transition in a clear portion of the atmospheric window, as well as having numerous isotopomers also available for easy study, and in addition to having a large dipole moment that makes observations particularly simple, HNC is, in its molecular nature, a quite simple molecule. This makes the study of the reaction pathways that lead to its formation and destruction a good means of obtaining insight to the workings of these reactions in space. Furthermore, the study of the tautomerization of HNC to HCN (and vice versa), which has been studied extensively, has been suggested as a model by which more complicated isomerization reactions can be studied.<ref name="Bentley1993" /><ref>{{cite journal|author=Skurski, P.|display-authors=etal|year=2001|title=''Ab initio'' electronic structure of HCN<sup>−</sup> and HNC<sup>−</sup> dipole-bound anions and a description of electron loss upon tautomerization|journal=J. Chem. Phys.|volume=114|issue=17|page=7446|bibcode=2001JChPh.114.7443S|doi=10.1063/1.1358863}}</ref><ref>{{cite journal|author1=Jakubetz, W.|author2=Lan, B. L.|year=1997|title=A simulation of ultrafast state-selective IR-laser-controlled isomerization of hydrogen cyanide based on global 3D ab initio potential and dipole surfaces|journal=Chem. Phys.|volume=217|issue=2–3|pages=375–388|bibcode=1997CP....217..375J|doi=10.1016/S0301-0104(97)00056-6}}</ref> ==Chemistry in the interstellar medium== HNC is found primarily in dense molecular clouds, though it is ubiquitous in the interstellar medium. Its abundance is closely linked to the abundances of other nitrogen-containing compounds.<ref name="Turner1997">{{cite journal|author=Turner, B. E.|display-authors=etal|year=1997|title=The Physics and Chemistry of Small Translucent Molecular Clouds. VIII. HCN and HNC|journal=Astrophysical Journal|volume=483|issue=1|pages=235–261|bibcode=1997ApJ...483..235T|doi=10.1086/304228}}</ref> HNC is formed primarily through the [[dissociative recombination]] of [[HCNH+|HNCH<sup>+</sup>]] and H<sub>2</sub>NC<sup>+</sup>, and it is destroyed primarily through ion-neutral reactions with {{chem|H|3|+}} and C<sup>+</sup>.<ref name="Hiraoka2006">{{cite journal|author=Hiraoka, K.|display-authors=etal|year=2006|title=How are CH<sub>3</sub>OH, HNC/HCN, and NH<sub>3</sub> Formed in the Interstellar Medium?|url=|journal=AIP Conf. Proc.|volume=855|issue=|pages=86–99|doi=10.1063/1.2359543}}</ref><ref>{{cite journal|author=Doty, S. D.|display-authors=etal|year=2004|title=Physical-chemical modeling of the low-mass protostar IRAS 16293-2422|journal=Astronomy and Astrophysics|volume=418|issue=3|pages=1021–1034|arxiv=astro-ph/0402610|bibcode=2004A&A...418.1021D|doi=10.1051/0004-6361:20034476}}</ref> Rate calculations were done at 3.16&nbsp;×&nbsp;10<sup>5</sup> years, which is considered early time, and at 20&nbsp;K, which is a typical temperature for dense molecular clouds.<ref>{{Cite web|url=http://udfa.net/|title=The UMIST Database for Astrochemistry|last=|first=|date=|website=|archive-url=|archive-date=|dead-url=|access-date=}}</ref><ref>{{cite journal|author=Millar, T. J.|display-authors=etal|year=1997|title=The UMIST database for astrochemistry 1995|journal=Astronomy and Astrophysics Supplement Series|volume=121|issue=|pages=139–185|doi=10.1051/aas:1997118|arxiv=1212.6362|bibcode=1997A&AS..121..139M}}</ref> {| border="1" cellpadding="5" cellspacing="0" |- ! colspan="7" style="text-align:center;"| '''Formation Reactions''' |- | style="text-align:center;"| '''Reactant 1''' || '''Reactant 2''' || '''Product 1''' || '''Product 2''' || '''Rate constant''' || '''Rate/[H<sub>2</sub>]<sup>2</sup>''' || '''Relative Rate''' |- | HCNH<sup>+</sup> || e<sup>−</sup> || HNC || H || {{val|9.50e-8}} || {{val|4.76e-25}} || 3.4 |- | H<sub>2</sub>NC<sup>+</sup> || e<sup>−</sup> || HNC || H || {{val|1.80e-7}} || {{val|1.39e-25}} || 1.0 |- ! colspan="7" style="text-align:center;"| '''Destruction Reactions''' |- | style="text-align:center;"| '''Reactant 1''' || '''Reactant 2''' || '''Product 1''' || '''Product 2''' || '''Rate constant''' || '''Rate/[H<sub>2</sub>]<sup>2</sup>''' || '''Relative Rate''' |- | {{chem|H|3|+}} || HNC || HCNH<sup>+</sup> || H<sub>2</sub> || {{val|8.10e-9}} || {{val|1.26e-24}} || 1.7 |- | C<sup>+</sup> || HNC || C<sub>2</sub>N<sup>+</sup> || H || {{val|3.10e-9}} || {{val|7.48e-25}} || 1.0 |} These four reactions are merely the four most dominant, and thus the most significant in the formation of the HNC abundances in dense molecular clouds; there are dozens more reactions for the formation and destruction of HNC. Though these reactions primarily lead to various protonated species, HNC is linked closely to the abundances of many other nitrogen containing molecules, for example, NH<sub>3</sub> and CN.<ref name="Turner1997" /> The abundance HNC is also inexorably linked to the abundance of HCN, and the two tend to exist in a specific ratio based on the environment.<ref name="Hiraoka2006" /> This is because the reactions that form HNC can often also form HCN, and vice versa, depending on the conditions in which the reaction occurs, and also that there exist isomerization reactions for the two species. ==Astronomical detections== HCN (not HNC) was first detected in June 1970 by L. E. Snyder and D. Buhl using the 36-foot radio telescope of the National Radio Astronomy Observatory.<ref>{{cite journal|author1=Snyder, L. E.|author2=Buhl, D.|year=1971|title=Observations of Radio Emission from Interstellar Hydrogen Cyanide|journal=Astrophysical Journal|volume=163|issue=|pages=L47–L52|bibcode=1971ApJ...163L..47S|doi=10.1086/180664}}</ref> The main molecular isotope, H<sup>12</sup>C<sup>14</sup>N, was observed via its ''J''&nbsp;=&nbsp;1→0 transition at 88.6&nbsp;GHz in six different sources: W3 (OH), Orion&nbsp;A, Sgr&nbsp;A(NH3A), W49, W51, DR&nbsp;21(OH). A secondary molecular isotope, H<sup>13</sup>C<sup>14</sup>N, was observed via its ''J''&nbsp;=&nbsp;1→0 transition at 86.3&nbsp;GHz in only two of these sources: Orion A and Sgr A(NH3A). HCN was then later detected extragalactically in 1988 using the [[IRAM 30-m]] telescope at the [[Veleta (Sierra Nevada)|Pico de Veleta]] in Spain.<ref>{{cite journal|author=Henkel, C.|display-authors=etal|year=1988|title=Molecules in external galaxies: the detection of CN, C<sub>2</sub>H, and HNC, and the tentative detection of HC<sub>3</sub>N|journal=Astronomy and Astrophysics|volume=201|issue=|pages=L23–L26|bibcode=1988A&A...201L..23H}}</ref> It was observed via its ''J''&nbsp;=&nbsp;1→0 transition at 90.7&nbsp;GHz toward IC&nbsp;342. A number of detections have been made towards the end of confirming the temperature dependence of the abundance ratio of [HNC]/[HCN]. A strong fit between temperature and the abundance ratio would allow observers to [[Spectroscopy|spectroscopically]] detect the ratio and then extrapolate the temperature of the environment, thus gaining great insight into the environment of the species. The abundance ratio of rare isotopes of HNC and HCN along the OMC-1 varies by more than an order of magnitude in warm regions versus cold regions.<ref>{{cite journal|author=Goldsmith, P. F.|display-authors=etal|year=1986|title=Variations in the HCN/HNC Abundance Ratio in the Orion Molecular Cloud|journal=Astrophysical Journal|volume=310|issue=|pages=383–391|bibcode=1986ApJ...310..383G|doi=10.1086/164692}}</ref> In 1992, the abundances of HNC, HCN, and deuterated analogs along the OMC-1 ridge and core were measured and the temperature dependence of the abundance ratio was confirmed.<ref name=Schilke1992 /> A survey of the W&nbsp;3 Giant Molecular Cloud in 1997 showed over 24 different molecular isotopes, comprising over 14 distinct chemical species, including HNC, HN<sup>13</sup>C, and H<sup>15</sup>NC. This survey further confirmed the temperature dependence of the abundance ratio, [HNC]/[HCN], this time ever confirming the dependence of the isotopomers.<ref>{{cite journal|author1=Helmich, F. P.|author2=van Dishoeck, E. F.|year=1997|title=Physical and chemical variations within the W3 star-forming region|journal=Astronomy and Astrophysics|volume=124|issue=2|pages=205–253|bibcode=1997A&AS..124..205H|doi=10.1051/aas:1997357}}</ref> These are not the only detections of importance of HNC in the interstellar medium. In 1997, HNC was observed along the TMC-1 ridge and its abundance relative to HCO<sup>+</sup> was found to be constant along the ridge—this led credence to the reaction pathway that posits that HNC is derived initially from HCO<sup>+</sup>.<ref name="Pratap1997" /> One significant astronomical detection that demonstrated the practical use of observing HNC occurred in 2006, when abundances of various nitrogenous compounds (including HN<sup>13</sup>C and H<sup>15</sup>NC) were used to determine the stage of evolution of the protostellar core Cha-MMS1 based on the relative magnitudes of the abundances.<ref name="Tennekes2006" /> On 11 August 2014, astronomers released studies, using the [[Atacama Large Millimeter Array|Atacama Large Millimeter/Submillimeter Array (ALMA)]] for the first time, that detailed the distribution of [[Hydrogen cyanide|HCN]], HNC, [[Formaldehyde|H<sub>2</sub>CO]], and [[dust]] inside the [[Coma (cometary)|comae]] of [[comet]]s [[C/2012 F6 (Lemmon)]] and [[Comet ISON|C/2012 S1 (ISON)]].<ref name="NASA-20140811">{{cite web |last=Zubritsky |first=Elizabeth |last2=Neal-Jones |first2=Nancy |title=RELEASE 14-038 - NASA's 3-D Study of Comets Reveals Chemical Factory at Work |url=http://www.nasa.gov/press/2014/august/goddard/nasa-s-3-d-study-of-comets-reveals-chemical-factory-at-work |date=11 August 2014 |work=[[NASA]] |accessdate=12 August 2014 }}</ref><ref name="AJL-20140811">{{cite journal |author=Cordiner, M.A.|title=Mapping the Release of Volatiles in the Inner Comae of Comets C/2012 F6 (Lemmon) and C/2012 S1 (ISON) Using the Atacama Large Millimeter/Submillimeter Array |url=http://iopscience.iop.org/2041-8205/792/1/L2/article |date=11 August 2014 |journal=[[The Astrophysical Journal]] |volume=792 |pages=L2 |number=1 |doi=10.1088/2041-8205/792/1/L2 |accessdate=12 August 2014 |display-authors=etal|arxiv=1408.2458|bibcode=2014ApJ...792L...2C}}</ref> == See also == * [[Isocyanide]] == External links == * [http://webbook.nist.gov/cgi/cbook.cgi?ID=6914-07-4 Hydrogen isocyanide on NIST Chemistry WebBook] ==References== {{reflist}} {{Hydrogen compounds}} {{Molecules detected in outer space}} {{DEFAULTSORT:Hydrogen Isocyanide}} [[Category:Hydrogen compounds]] [[Category:Isocyanides]] [[Category:Zwitterions]]'
New page wikitext, after the edit (new_wikitext)
'{{chembox | Watchedfields = changed | verifiedrevid = 443863009 | ImageFileL1 = Hydrogen-isocyanide-2D.png | ImageNameL1 = Hydrogen cyanide bonding | ImageFileR1 = Hydrogen-isocyanide-3D-vdW.png | ImageNameR1 = Hydrogen cyanide space filling | IUPACName = hydrogen isocyanide<br>azanylidyniummethanide | OtherNames = isohydrocyanic acid<br>hydroisocyanic acid<br>isoprussic acid |Section1={{Chembox Identifiers | StdInChI_Ref = {{stdinchicite|correct|chemspider}} | StdInChI = 1S/CHN/c1-2/h2H | StdInChIKey_Ref = {{stdinchicite|correct|chemspider}} | StdInChIKey = QIUBLANJVAOHHY-UHFFFAOYSA-N | CASNo_Ref = {{cascite|correct|??}} | CASNo = | EINECS = | PubChem = 6432654 | ChemSpiderID_Ref = {{chemspidercite|correct|chemspider}} | ChemSpiderID = 4937885 | ChEBI_Ref = {{ebicite|correct|EBI}} | ChEBI = 36856 | SMILES = [C-]#[NH+] | InChI = 1/CHN/c1-2/h2H | RTECS = }} |Section2={{Chembox Properties | Formula = HNC | MolarMass = 27.03 g/mol | Appearance = | Density = | MeltingPt = | BoilingPt = | Solubility = | VaporPressure = | ConjugateAcid = [[Hydrocyanonium]] | ConjugateBase = [[Cyanide]] }} |Section3={{Chembox Hazards | MainHazards = | FlashPt = | AutoignitionPt = }} }} '''Hydrogen isocyanide''' is a chemical with the molecular formula HNC. It is a minor [[tautomer]] of [[hydrogen cyanide]] (HCN). Its importance in the field of [[astrochemistry]] is linked to its ubiquity in the [[interstellar medium]]. == Nomenclature == Both ''hydrogen isocyanide'' and ''azanylidyniummethanide'' are correct [[IUPAC name]]s for HNC. There is no [[preferred IUPAC name]]. The second one is according to the ''[[substitutive nomenclature]] rules'', derived from the ''[[parent hydride]]'' [[azane]] (NH<sub>3</sub>) and the anion [[methanide]] (C<sup>−</sup>).<ref>The suffix ''ylidyne'' refers to the loss of three hydrogen atoms from the nitrogen atom in [[azanium]] ({{chem|NH|4|+}}) See the [http://www.iupac.org/publications/books/rbook/Red_Book_2005.pdf ''IUPAC Red Book'' 2005] Table III, "Suffixes and endings", p. 257.</ref> ==Molecular properties== Hydrogen isocyanide (HNC) is a linear triatomic molecule with C<sub>∞v</sub> [[Molecular symmetry|point group symmetry]]. It is a [[zwitterion]] and an [[isomer]] of [[hydrogen cyanide]] (HCN).<ref>{{Cite journal|last=Pau|first=Chin Fong|last2=Hehre|first2=Warren J.|date=1982-02-01|title=Heat of formation of hydrogen isocyanide by ion cyclotron double resonance spectroscopy|journal=The Journal of Physical Chemistry|volume=86|issue=3|pages=321–322|doi=10.1021/j100392a006|issn=0022-3654}}</ref> Both HNC and HCN have large, similar [[Molecular dipole moment|dipole moment]]s, with ''μ''<sub>HNC</sub>&nbsp;=&nbsp;3.05 [[Debye]] and ''μ''<sub>HCN</sub>&nbsp;=&nbsp;2.98 Debye respectively.<ref name="Tennekes2006">{{cite journal|author=Tennekes, P. P.|display-authors=etal|year=2006|title=HCN and HNC mapping of the protostellar core Chamaeleon-MMS1|journal=Astronomy and Astrophysics|volume=456|issue=3|pages=1037–1043|arxiv=astro-ph/0606547|bibcode=2006A&A...456.1037T|doi=10.1051/0004-6361:20040294}}</ref> These large dipole moments facilitate the easy observation of these species in the [[interstellar medium]]. === HNC−HCN tautomerism === As HNC is higher in energy than HCN by 3920&nbsp;cm<sup>−1</sup> (46.9&nbsp; kJ/mol), one might assume that the two would have an equilibrium ratio<math display="inline">\left ( \frac{[HNC]}{[HCN]} \right )_{eq}</math> at temperatures below 100 Kelvin of 10<sup>−25</sup>.<ref>{{cite journal|author=Hirota, T.|display-authors=etal|year=1998|title=Abundances of HCN and HNC in Dark Cloud Cores|journal=Astrophysical Journal|volume=503|issue=2|pages=717–728|bibcode=1998ApJ...503..717H|doi=10.1086/306032}}</ref> However, observations show a very different conclusion; <math display="inline">\left ( \frac{[HNC]}{[HCN]} \right )_{observed}</math> is much higher than 10<sup>−25</sup>, and is in fact on the order of unity in cold environments. This is because of the potential energy path of the tautomerization reaction; there is an activation barrier on the order of roughly 12,000&nbsp;cm<sup>−1</sup> for the tautomerization to occur, which corresponds to a temperature at which HNC would already have been destroyed by neutral-neutral reactions.<ref name="Bentley1993">{{cite journal|author=Bentley, J. A.|display-authors=etal|year=1993|title=Highly virationally excited HCN/HNC: Eigenvalues, wave functions, and stimulated emission pumping spectra|journal=J. Chem. Phys.|volume=98|issue=7|page=5209|bibcode=1993JChPh..98.5207B|doi=10.1063/1.464921}}</ref> ==Spectral properties== In practice, HNC is almost exclusively observed astronomically using the ''J''&nbsp;=&nbsp;1→0 transition. This transition occurs at ~90.66&nbsp;GHz, which is a point of good visibility in the [[Radio window|atmospheric window]], thus making astronomical observations of HNC particularly simple. Many other related species (including HCN) are observed in roughly the same window.<ref name=Schilke1992>{{cite journal|author=Schilke, P.|display-authors=etal|year=1992|title=A study of HCN, HNC and their isotopomers in OMC-1. I. Abundances and chemistry|journal=Astronomy and Astrophysics|volume=256|issue=|pages=595–612|bibcode=1992A&A...256..595S}}</ref><ref name="Pratap1997">{{cite journal|author=Pratap, P.|display-authors=etal|year=1997|title=A Study of the Physics and Chemistry of TMC-1|journal=Astrophysical Journal|volume=486|issue=2|pages=862–885|bibcode=1997ApJ...486..862P|doi=10.1086/304553}}</ref> ==Significance in the interstellar medium== HNC is intricately linked to the formation and destruction of numerous other molecules of importance in the interstellar medium—aside from the obvious partners HCN, [[HCNH+|protonated hydrogen cyanide (HCNH<sup>+</sup>)]], and [[Cyanide|cyanide (CN)]], HNC is linked to the abundances of many other compounds, either directly or through a few degrees of separation. As such, an understanding of the chemistry of HNC leads to an understanding of countless other species—HNC is an integral piece in the complex puzzle representing interstellar chemistry. Furthermore, HNC (alongside HCN) is a commonly used tracer of dense gas in molecular clouds. Aside from the potential to use HNC to investigate [[gravitational collapse]] as the means of star formation, HNC abundance (relative to the abundance of other nitrogenous molecules) can be used to determine the evolutionary stage of protostellar cores.<ref name="Tennekes2006" /> The HCO<sup>+</sup>/HNC line ratio is used to good effect as a measure of density of gas.<ref>{{cite journal|author=Loenen, A. F.|display-authors=etal|year=2007|title=Molecular properties of (U)LIRGs: CO, HCN, HNC and HCO<sup>+</sup>|journal=Proceedings IAU Symposium|volume=242|issue=|pages=1–5}}</ref> This information provides great insight into the mechanisms of the formation of (Ultra-)Luminous Infrared Galaxies ((U)LIRGs), as it provides data on the nuclear environment, [[star formation]], and even [[black hole]] fueling. Furthermore, the HNC/HCN line ratio is used to distinguish between [[Photodissociation region|photodissociation regions]] and X-ray-dissociation regions on the basis that [HNC]/[HCN] is roughly unity in the former, but greater than unity in the latter. The study of HNC is a relatively simple pursuit, and this is one of the greatest motivations for its study. Aside from having its ''J''&nbsp;=&nbsp;1→0 transition in a clear portion of the atmospheric window, as well as having numerous isotopomers also available for easy study, and in addition to having a large dipole moment that makes observations particularly simple, HNC is, in its molecular nature, a quite simple molecule. This makes the study of the reaction pathways that lead to its formation and destruction a good means of obtaining insight to the workings of these reactions in space. Furthermore, the study of the tautomerization of HNC to HCN (and vice versa), which has been studied extensively, has been suggested as a model by which more complicated isomerization reactions can be studied.<ref name="Bentley1993" /><ref>{{cite journal|author=Skurski, P.|display-authors=etal|year=2001|title=''Ab initio'' electronic structure of HCN<sup>−</sup> and HNC<sup>−</sup> dipole-bound anions and a description of electron loss upon tautomerization|journal=J. Chem. Phys.|volume=114|issue=17|page=7446|bibcode=2001JChPh.114.7443S|doi=10.1063/1.1358863}}</ref><ref>{{cite journal|author1=Jakubetz, W.|author2=Lan, B. L.|year=1997|title=A simulation of ultrafast state-selective IR-laser-controlled isomerization of hydrogen cyanide based on global 3D ab initio potential and dipole surfaces|journal=Chem. Phys.|volume=217|issue=2–3|pages=375–388|bibcode=1997CP....217..375J|doi=10.1016/S0301-0104(97)00056-6}}</ref> Hajj ==Astronomical detections== HCN (not HNC) was first detected in June 1970 by L. E. Snyder and D. Buhl using the 36-foot radio telescope of the National Radio Astronomy Observatory.<ref>{{cite journal|author1=Snyder, L. E.|author2=Buhl, D.|year=1971|title=Observations of Radio Emission from Interstellar Hydrogen Cyanide|journal=Astrophysical Journal|volume=163|issue=|pages=L47–L52|bibcode=1971ApJ...163L..47S|doi=10.1086/180664}}</ref> The main molecular isotope, H<sup>12</sup>C<sup>14</sup>N, was observed via its ''J''&nbsp;=&nbsp;1→0 transition at 88.6&nbsp;GHz in six different sources: W3 (OH), Orion&nbsp;A, Sgr&nbsp;A(NH3A), W49, W51, DR&nbsp;21(OH). A secondary molecular isotope, H<sup>13</sup>C<sup>14</sup>N, was observed via its ''J''&nbsp;=&nbsp;1→0 transition at 86.3&nbsp;GHz in only two of these sources: Orion A and Sgr A(NH3A). HCN was then later detected extragalactically in 1988 using the [[IRAM 30-m]] telescope at the [[Veleta (Sierra Nevada)|Pico de Veleta]] in Spain.<ref>{{cite journal|author=Henkel, C.|display-authors=etal|year=1988|title=Molecules in external galaxies: the detection of CN, C<sub>2</sub>H, and HNC, and the tentative detection of HC<sub>3</sub>N|journal=Astronomy and Astrophysics|volume=201|issue=|pages=L23–L26|bibcode=1988A&A...201L..23H}}</ref> It was observed via its ''J''&nbsp;=&nbsp;1→0 transition at 90.7&nbsp;GHz toward IC&nbsp;342. A number of detections have been made towards the end of confirming the temperature dependence of the abundance ratio of [HNC]/[HCN]. A strong fit between temperature and the abundance ratio would allow observers to [[Spectroscopy|spectroscopically]] detect the ratio and then extrapolate the temperature of the environment, thus gaining great insight into the environment of the species. The abundance ratio of rare isotopes of HNC and HCN along the OMC-1 varies by more than an order of magnitude in warm regions versus cold regions.<ref>{{cite journal|author=Goldsmith, P. F.|display-authors=etal|year=1986|title=Variations in the HCN/HNC Abundance Ratio in the Orion Molecular Cloud|journal=Astrophysical Journal|volume=310|issue=|pages=383–391|bibcode=1986ApJ...310..383G|doi=10.1086/164692}}</ref> In 1992, the abundances of HNC, HCN, and deuterated analogs along the OMC-1 ridge and core were measured and the temperature dependence of the abundance ratio was confirmed.<ref name=Schilke1992 /> A survey of the W&nbsp;3 Giant Molecular Cloud in 1997 showed over 24 different molecular isotopes, comprising over 14 distinct chemical species, including HNC, HN<sup>13</sup>C, and H<sup>15</sup>NC. This survey further confirmed the temperature dependence of the abundance ratio, [HNC]/[HCN], this time ever confirming the dependence of the isotopomers.<ref>{{cite journal|author1=Helmich, F. P.|author2=van Dishoeck, E. F.|year=1997|title=Physical and chemical variations within the W3 star-forming region|journal=Astronomy and Astrophysics|volume=124|issue=2|pages=205–253|bibcode=1997A&AS..124..205H|doi=10.1051/aas:1997357}}</ref> These are not the only detections of importance of HNC in the interstellar medium. In 1997, HNC was observed along the TMC-1 ridge and its abundance relative to HCO<sup>+</sup> was found to be constant along the ridge—this led credence to the reaction pathway that posits that HNC is derived initially from HCO<sup>+</sup>.<ref name="Pratap1997" /> One significant astronomical detection that demonstrated the practical use of observing HNC occurred in 2006, when abundances of various nitrogenous compounds (including HN<sup>13</sup>C and H<sup>15</sup>NC) were used to determine the stage of evolution of the protostellar core Cha-MMS1 based on the relative magnitudes of the abundances.<ref name="Tennekes2006" /> On 11 August 2014, astronomers released studies, using the [[Atacama Large Millimeter Array|Atacama Large Millimeter/Submillimeter Array (ALMA)]] for the first time, that detailed the distribution of [[Hydrogen cyanide|HCN]], HNC, [[Formaldehyde|H<sub>2</sub>CO]], and [[dust]] inside the [[Coma (cometary)|comae]] of [[comet]]s [[C/2012 F6 (Lemmon)]] and [[Comet ISON|C/2012 S1 (ISON)]].<ref name="NASA-20140811">{{cite web |last=Zubritsky |first=Elizabeth |last2=Neal-Jones |first2=Nancy |title=RELEASE 14-038 - NASA's 3-D Study of Comets Reveals Chemical Factory at Work |url=http://www.nasa.gov/press/2014/august/goddard/nasa-s-3-d-study-of-comets-reveals-chemical-factory-at-work |date=11 August 2014 |work=[[NASA]] |accessdate=12 August 2014 }}</ref><ref name="AJL-20140811">{{cite journal |author=Cordiner, M.A.|title=Mapping the Release of Volatiles in the Inner Comae of Comets C/2012 F6 (Lemmon) and C/2012 S1 (ISON) Using the Atacama Large Millimeter/Submillimeter Array |url=http://iopscience.iop.org/2041-8205/792/1/L2/article |date=11 August 2014 |journal=[[The Astrophysical Journal]] |volume=792 |pages=L2 |number=1 |doi=10.1088/2041-8205/792/1/L2 |accessdate=12 August 2014 |display-authors=etal|arxiv=1408.2458|bibcode=2014ApJ...792L...2C}}</ref> == See also == * [[Isocyanide]] == External links == * [http://webbook.nist.gov/cgi/cbook.cgi?ID=6914-07-4 Hydrogen isocyanide on NIST Chemistry WebBook] ==References== {{reflist}} {{Hydrogen compounds}} {{Molecules detected in outer space}} {{DEFAULTSORT:Hydrogen Isocyanide}} [[Category:Hydrogen compounds]] [[Category:Isocyanides]] [[Category:Zwitterions]]'
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'@@ -71,28 +71,5 @@ The study of HNC is a relatively simple pursuit, and this is one of the greatest motivations for its study. Aside from having its ''J''&nbsp;=&nbsp;1→0 transition in a clear portion of the atmospheric window, as well as having numerous isotopomers also available for easy study, and in addition to having a large dipole moment that makes observations particularly simple, HNC is, in its molecular nature, a quite simple molecule. This makes the study of the reaction pathways that lead to its formation and destruction a good means of obtaining insight to the workings of these reactions in space. Furthermore, the study of the tautomerization of HNC to HCN (and vice versa), which has been studied extensively, has been suggested as a model by which more complicated isomerization reactions can be studied.<ref name="Bentley1993" /><ref>{{cite journal|author=Skurski, P.|display-authors=etal|year=2001|title=''Ab initio'' electronic structure of HCN<sup>−</sup> and HNC<sup>−</sup> dipole-bound anions and a description of electron loss upon tautomerization|journal=J. Chem. Phys.|volume=114|issue=17|page=7446|bibcode=2001JChPh.114.7443S|doi=10.1063/1.1358863}}</ref><ref>{{cite journal|author1=Jakubetz, W.|author2=Lan, B. L.|year=1997|title=A simulation of ultrafast state-selective IR-laser-controlled isomerization of hydrogen cyanide based on global 3D ab initio potential and dipole surfaces|journal=Chem. Phys.|volume=217|issue=2–3|pages=375–388|bibcode=1997CP....217..375J|doi=10.1016/S0301-0104(97)00056-6}}</ref> -==Chemistry in the interstellar medium== - -HNC is found primarily in dense molecular clouds, though it is ubiquitous in the interstellar medium. Its abundance is closely linked to the abundances of other nitrogen-containing compounds.<ref name="Turner1997">{{cite journal|author=Turner, B. E.|display-authors=etal|year=1997|title=The Physics and Chemistry of Small Translucent Molecular Clouds. VIII. HCN and HNC|journal=Astrophysical Journal|volume=483|issue=1|pages=235–261|bibcode=1997ApJ...483..235T|doi=10.1086/304228}}</ref> HNC is formed primarily through the [[dissociative recombination]] of [[HCNH+|HNCH<sup>+</sup>]] and H<sub>2</sub>NC<sup>+</sup>, and it is destroyed primarily through ion-neutral reactions with {{chem|H|3|+}} and C<sup>+</sup>.<ref name="Hiraoka2006">{{cite journal|author=Hiraoka, K.|display-authors=etal|year=2006|title=How are CH<sub>3</sub>OH, HNC/HCN, and NH<sub>3</sub> Formed in the Interstellar Medium?|url=|journal=AIP Conf. Proc.|volume=855|issue=|pages=86–99|doi=10.1063/1.2359543}}</ref><ref>{{cite journal|author=Doty, S. D.|display-authors=etal|year=2004|title=Physical-chemical modeling of the low-mass protostar IRAS 16293-2422|journal=Astronomy and Astrophysics|volume=418|issue=3|pages=1021–1034|arxiv=astro-ph/0402610|bibcode=2004A&A...418.1021D|doi=10.1051/0004-6361:20034476}}</ref> Rate calculations were done at 3.16&nbsp;×&nbsp;10<sup>5</sup> years, which is considered early time, and at 20&nbsp;K, which is a typical temperature for dense molecular clouds.<ref>{{Cite web|url=http://udfa.net/|title=The UMIST Database for Astrochemistry|last=|first=|date=|website=|archive-url=|archive-date=|dead-url=|access-date=}}</ref><ref>{{cite journal|author=Millar, T. J.|display-authors=etal|year=1997|title=The UMIST database for astrochemistry 1995|journal=Astronomy and Astrophysics Supplement Series|volume=121|issue=|pages=139–185|doi=10.1051/aas:1997118|arxiv=1212.6362|bibcode=1997A&AS..121..139M}}</ref> - -{| border="1" cellpadding="5" cellspacing="0" -|- -! colspan="7" style="text-align:center;"| '''Formation Reactions''' -|- -| style="text-align:center;"| '''Reactant 1''' || '''Reactant 2''' || '''Product 1''' || '''Product 2''' || '''Rate constant''' || '''Rate/[H<sub>2</sub>]<sup>2</sup>''' || '''Relative Rate''' -|- -| HCNH<sup>+</sup> || e<sup>−</sup> || HNC || H || {{val|9.50e-8}} || {{val|4.76e-25}} || 3.4 -|- -| H<sub>2</sub>NC<sup>+</sup> || e<sup>−</sup> || HNC || H || {{val|1.80e-7}} || {{val|1.39e-25}} || 1.0 -|- -! colspan="7" style="text-align:center;"| '''Destruction Reactions''' -|- -| style="text-align:center;"| '''Reactant 1''' || '''Reactant 2''' || '''Product 1''' || '''Product 2''' || '''Rate constant''' || '''Rate/[H<sub>2</sub>]<sup>2</sup>''' || '''Relative Rate''' -|- -| {{chem|H|3|+}} || HNC || HCNH<sup>+</sup> || H<sub>2</sub> || {{val|8.10e-9}} || {{val|1.26e-24}} || 1.7 -|- -| C<sup>+</sup> || HNC || C<sub>2</sub>N<sup>+</sup> || H || {{val|3.10e-9}} || {{val|7.48e-25}} || 1.0 -|} - -These four reactions are merely the four most dominant, and thus the most significant in the formation of the HNC abundances in dense molecular clouds; there are dozens more reactions for the formation and destruction of HNC. Though these reactions primarily lead to various protonated species, HNC is linked closely to the abundances of many other nitrogen containing molecules, for example, NH<sub>3</sub> and CN.<ref name="Turner1997" /> The abundance HNC is also inexorably linked to the abundance of HCN, and the two tend to exist in a specific ratio based on the environment.<ref name="Hiraoka2006" /> This is because the reactions that form HNC can often also form HCN, and vice versa, depending on the conditions in which the reaction occurs, and also that there exist isomerization reactions for the two species. +Hajj ==Astronomical detections== '
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[ 0 => '==Chemistry in the interstellar medium==', 1 => false, 2 => 'HNC is found primarily in dense molecular clouds, though it is ubiquitous in the interstellar medium. Its abundance is closely linked to the abundances of other nitrogen-containing compounds.<ref name="Turner1997">{{cite journal|author=Turner, B. E.|display-authors=etal|year=1997|title=The Physics and Chemistry of Small Translucent Molecular Clouds. VIII. HCN and HNC|journal=Astrophysical Journal|volume=483|issue=1|pages=235–261|bibcode=1997ApJ...483..235T|doi=10.1086/304228}}</ref> HNC is formed primarily through the [[dissociative recombination]] of [[HCNH+|HNCH<sup>+</sup>]] and H<sub>2</sub>NC<sup>+</sup>, and it is destroyed primarily through ion-neutral reactions with {{chem|H|3|+}} and C<sup>+</sup>.<ref name="Hiraoka2006">{{cite journal|author=Hiraoka, K.|display-authors=etal|year=2006|title=How are CH<sub>3</sub>OH, HNC/HCN, and NH<sub>3</sub> Formed in the Interstellar Medium?|url=|journal=AIP Conf. Proc.|volume=855|issue=|pages=86–99|doi=10.1063/1.2359543}}</ref><ref>{{cite journal|author=Doty, S. D.|display-authors=etal|year=2004|title=Physical-chemical modeling of the low-mass protostar IRAS 16293-2422|journal=Astronomy and Astrophysics|volume=418|issue=3|pages=1021–1034|arxiv=astro-ph/0402610|bibcode=2004A&A...418.1021D|doi=10.1051/0004-6361:20034476}}</ref> Rate calculations were done at 3.16&nbsp;×&nbsp;10<sup>5</sup> years, which is considered early time, and at 20&nbsp;K, which is a typical temperature for dense molecular clouds.<ref>{{Cite web|url=http://udfa.net/|title=The UMIST Database for Astrochemistry|last=|first=|date=|website=|archive-url=|archive-date=|dead-url=|access-date=}}</ref><ref>{{cite journal|author=Millar, T. J.|display-authors=etal|year=1997|title=The UMIST database for astrochemistry 1995|journal=Astronomy and Astrophysics Supplement Series|volume=121|issue=|pages=139–185|doi=10.1051/aas:1997118|arxiv=1212.6362|bibcode=1997A&AS..121..139M}}</ref>', 3 => false, 4 => '{| border="1" cellpadding="5" cellspacing="0"', 5 => '|-', 6 => '! colspan="7" style="text-align:center;"| '''Formation Reactions'''', 7 => '|-', 8 => '| style="text-align:center;"| '''Reactant 1''' || '''Reactant 2''' || '''Product 1''' || '''Product 2''' || '''Rate constant''' || '''Rate/[H<sub>2</sub>]<sup>2</sup>''' || '''Relative Rate'''', 9 => '|-', 10 => '| HCNH<sup>+</sup> || e<sup>−</sup> || HNC || H || {{val|9.50e-8}} || {{val|4.76e-25}} || 3.4', 11 => '|-', 12 => '| H<sub>2</sub>NC<sup>+</sup> || e<sup>−</sup> || HNC || H || {{val|1.80e-7}} || {{val|1.39e-25}} || 1.0', 13 => '|-', 14 => '! colspan="7" style="text-align:center;"| '''Destruction Reactions'''', 15 => '|-', 16 => '| style="text-align:center;"| '''Reactant 1''' || '''Reactant 2''' || '''Product 1''' || '''Product 2''' || '''Rate constant''' || '''Rate/[H<sub>2</sub>]<sup>2</sup>''' || '''Relative Rate'''', 17 => '|-', 18 => '| {{chem|H|3|+}} || HNC || HCNH<sup>+</sup> || H<sub>2</sub> || {{val|8.10e-9}} || {{val|1.26e-24}} || 1.7', 19 => '|-', 20 => '| C<sup>+</sup> || HNC || C<sub>2</sub>N<sup>+</sup> || H || {{val|3.10e-9}} || {{val|7.48e-25}} || 1.0', 21 => '|}', 22 => false, 23 => 'These four reactions are merely the four most dominant, and thus the most significant in the formation of the HNC abundances in dense molecular clouds; there are dozens more reactions for the formation and destruction of HNC. Though these reactions primarily lead to various protonated species, HNC is linked closely to the abundances of many other nitrogen containing molecules, for example, NH<sub>3</sub> and CN.<ref name="Turner1997" /> The abundance HNC is also inexorably linked to the abundance of HCN, and the two tend to exist in a specific ratio based on the environment.<ref name="Hiraoka2006" /> This is because the reactions that form HNC can often also form HCN, and vice versa, depending on the conditions in which the reaction occurs, and also that there exist isomerization reactions for the two species.' ]
Whether or not the change was made through a Tor exit node (tor_exit_node)
false
Unix timestamp of change (timestamp)
1562654104