The Molecular Spectrum of Carbon Dioxide
THE value of the specific heat of carbon dioxide indicates a triangular molecule. Bjerrum (Deutsch. Phys. Ges., 16, 737, 1914) has made a study of this molecule and has decided that the atomic nuclei lie at the corners of an isosceles triangle the apex angle of which is either 145° or 40°.6. Denniso...
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description | THE value of the specific heat of carbon dioxide indicates a triangular molecule. Bjerrum (Deutsch. Phys. Ges., 16, 737, 1914) has made a study of this molecule and has decided that the atomic nuclei lie at the corners of an isosceles triangle the apex angle of which is either 145° or 40°.6. Dennison (Phil. Mag. (7), 1, 195, 1926) decides in favour of the former angle. Such a model, according to these authors, should be characterised by three fundamental vibrational frequencies. Each tries to associate the three well-known bands of absorption at 14.66µ, 4.25µ and 2.73µ with these predicted frequencies. The model does not anticipate a fourth weak band which I found at 2.02µ (Phys. Rev., 26, 469, 1925), especially since this is not harmonic with any of the other three. |
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Bjerrum (Deutsch. Phys. Ges., 16, 737, 1914) has made a study of this molecule and has decided that the atomic nuclei lie at the corners of an isosceles triangle the apex angle of which is either 145° or 40°.6. Dennison (Phil. Mag. (7), 1, 195, 1926) decides in favour of the former angle. Such a model, according to these authors, should be characterised by three fundamental vibrational frequencies. Each tries to associate the three well-known bands of absorption at 14.66µ, 4.25µ and 2.73µ with these predicted frequencies. The model does not anticipate a fourth weak band which I found at 2.02µ (Phys. 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Bjerrum (Deutsch. Phys. Ges., 16, 737, 1914) has made a study of this molecule and has decided that the atomic nuclei lie at the corners of an isosceles triangle the apex angle of which is either 145° or 40°.6. Dennison (Phil. Mag. (7), 1, 195, 1926) decides in favour of the former angle. Such a model, according to these authors, should be characterised by three fundamental vibrational frequencies. Each tries to associate the three well-known bands of absorption at 14.66µ, 4.25µ and 2.73µ with these predicted frequencies. The model does not anticipate a fourth weak band which I found at 2.02µ (Phys. Rev., 26, 469, 1925), especially since this is not harmonic with any of the other three.</description><subject>Humanities and Social Sciences</subject><subject>letter</subject><subject>multidisciplinary</subject><subject>Science</subject><issn>0028-0836</issn><issn>1476-4687</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>1926</creationdate><recordtype>article</recordtype><recordid>eNptz81KxDAUBeAgCtZR8Amky3FRvUnaJF3K-AsjLhzX5SZzqx06zZC0oG9vpQ5uXJ3Nx-Ecxs45XHGQ5ppzA0YgHLCE51pluTL6kCUAwmRgpDpmJzFuAKDgOk_YfPVB6bNvyQ0thvR1R64Pwzb1dbrAYH2X3jb-s1nTKTuqsY109psz9nZ_t1o8ZsuXh6fFzTJzIi_6jMgJiWidBsCyFGBrUThZSjRccFuOk4SxEvVaG2ltaS1aUqUgpaxUhZEzNp96XfAxBqqrXWi2GL4qDtXPw2r_cKSXE40j6d4pVBs_hG5c95-9mGyH_RDor3QPvgG6oFiw</recordid><startdate>19260717</startdate><enddate>19260717</enddate><creator>ELLIS, JOSEPH W</creator><general>Nature Publishing Group UK</general><scope>AAYXX</scope><scope>CITATION</scope></search><sort><creationdate>19260717</creationdate><title>The Molecular Spectrum of Carbon Dioxide</title><author>ELLIS, JOSEPH W</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c245t-eec23aabc700a9920bf25c393a8121b947628b3a7d783bb9bbabe692e66b36583</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>1926</creationdate><topic>Humanities and Social Sciences</topic><topic>letter</topic><topic>multidisciplinary</topic><topic>Science</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>ELLIS, JOSEPH W</creatorcontrib><collection>CrossRef</collection><jtitle>Nature (London)</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>ELLIS, JOSEPH W</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>The Molecular Spectrum of Carbon Dioxide</atitle><jtitle>Nature (London)</jtitle><stitle>Nature</stitle><date>1926-07-17</date><risdate>1926</risdate><volume>118</volume><issue>2959</issue><spage>82</spage><epage>83</epage><pages>82-83</pages><issn>0028-0836</issn><eissn>1476-4687</eissn><abstract>THE value of the specific heat of carbon dioxide indicates a triangular molecule. Bjerrum (Deutsch. Phys. Ges., 16, 737, 1914) has made a study of this molecule and has decided that the atomic nuclei lie at the corners of an isosceles triangle the apex angle of which is either 145° or 40°.6. Dennison (Phil. Mag. (7), 1, 195, 1926) decides in favour of the former angle. Such a model, according to these authors, should be characterised by three fundamental vibrational frequencies. Each tries to associate the three well-known bands of absorption at 14.66µ, 4.25µ and 2.73µ with these predicted frequencies. The model does not anticipate a fourth weak band which I found at 2.02µ (Phys. Rev., 26, 469, 1925), especially since this is not harmonic with any of the other three.</abstract><cop>London</cop><pub>Nature Publishing Group UK</pub><doi>10.1038/118082a0</doi><tpages>2</tpages></addata></record> |
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title | The Molecular Spectrum of Carbon Dioxide |
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