Polycarbonyl

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Polycarbonyl, (also known as polymeric-CO, p-CO or poly-CO) is a solid metastable and explosive polymer of carbon monoxide.[1] The polymer is produced by exposing carbon monoxide to high pressures. The structure of the solid appears amorphous, but may include a zig zag of equally spaced CO groups.[2]

Formation

Poly-CO can be produced at pressures of 5.2 GPa. Polymerisation is catalysed by blue light at slightly lower pressures in the δ-phase of solid CO.[3] Another white phase can be made at higher temperatures at 6 or 7 GPa.[1] Poly-CO appears to be a yellow to dark red amorphous phase.[4] Whereas the white phase appears to be crystalline.[1]

R. J. Mills was the first to discover this solid. It was produced in a tungsten carbide anvil. Originally this was thought to be polymeric carbon suboxide, but the formation does not yield any gas byproduct such as carbon dioxide.[5] The yield of the solid can be up to 95%.[6]

Properties

The polymer is stable above about 80K. Below this temperature the ε form of solid molecular CO is formed instead. When the pressure is released the polymer remains stable at atmospheric pressure. The solid dissolves in water, alcohol and acetone.[5] When exposed to the atmosphere it is hydroscopic, becomes gluey, and changes colour, becoming darker.[6] The reaction with water produces carboxylic groups.[7]

[8]

The solid stores a high energy. It can decompose explosively forming glassy carbon and carbon dioxide.[6] The energy density stored can be up to 8 kJ/g. During the decomposition the temperature can be 2500K.[6] The density is 1.65 gcm-3, however most of the solid produced is porous, so the true density is likely to be higher.[6]

Infrared spectroscopy shows bands at 650, 1210, 1440, 1650 and 1760 cm-1. The 1760 band is likely to be due to the -C-(C=O)-C- structure.[3] The 1600 is due to vibration of a C=C double bond.[6]

The solid is electrically insulating with an electronic gap energy of 1.9 eV.[3]

Nuclear magnetic resonance for the material made from 13CO shows sharp resonance at 223 ppm due to ester or lactone attached carbon, and 151 ppm due to C=C double bonds. There is also broad resonance at 109 and 189 ppm. Over time of a few days, the 223 ppm peak reduces and all the other features increase in strength.[6]

Structure

Ideas of the structure include a zig zag chain of CO pointing in opposite directions, or five atom rings connected by CO and C-C bonds. The rings are lactones of tetronic acid: -C:-(C=O)-(C-O-)-(C=O)-O-. Interconnections between the rings are zig zags of CO.[3]

Other ideas of the structure of the solid, include graphitic carbon with carbon dioxide under pressure, and a polymer with this C3O2 monomer: -(C=O)-O-(C-)=C<. Yet other ideas are that the solid is the same as the polymer of carbon suboxide with oxalic anhydride.[9]

References

  1. 1.0 1.1 1.2 Rademacher, N.; L. Bayarjargal, W. Morgenroth, B. Winkler, and J. Ciezak-Jenkins (2011). "Preparation and characterization of solid carbon monoxide at high pressure in the diamond anvil cell". Retrieved 30 May 2013. 
  2. Podeszwa, Rafa?; Rodney J. Bartlett (2003). "Crystal orbital study of polycarbonyl". International Journal of Quantum Chemistry 95 (4-5): 638–642. doi:10.1002/qua.10655. ISSN 0020-7608. 
  3. 3.0 3.1 3.2 3.3 Bernard, Stephane (Feb 1998). "DECOMPOSITION AND POLYMERIZATION OF SOLID CARBON MONOXIDE UNDER PRESSURE". Trieste. Retrieved 30 May 2013. 
  4. Rademacher, Nadine; Lkhamsuren Bayarjargal, Wolfgang Morgenroth, Jennifer Ciezak-Jenkins, Sasha Batyrev, Björn Winkler. "High Pressure Investigations of Liquid and Polymerized CO up to 20 GPa Using Pair Distribution Function Analysis". Retrieved 30 May 2013. 
  5. 5.0 5.1 Mills, R. L.; D. Schiferl, A. I. Katz, B. W. Olinger (1984). "NEW PHASES AND CHEMICAL REACTIONS IN SOLID CO UNDER PRESSURE". Le Journal de Physique Colloques 45 (C8): C8–187–C8–190. doi:10.1051/jphyscol:1984833. ISSN 0449-1947. 
  6. 6.0 6.1 6.2 6.3 6.4 6.5 6.6 Lipp, Magnus J.; William J. Evans, Bruce J. Baer, Choong-Shik Yoo (2005). "High-energy-density extended CO solid". Nature Materials 4 (3): 211–215. doi:10.1038/nmat1321. ISSN 1476-1122. 
  7. Ceppatelli, Matteo; Anton Serdyukov, Roberto Bini, Hans J. Jodl (2009). "Pressure Induced Reactivity of Solid CO by FTIR Studies". The Journal of Physical Chemistry B 113 (19): 6652–6660. doi:10.1021/jp900586a. ISSN 1520-6106. 
  8. Katz, Allen I.; David Schiferl, Robert L. Mills (1984). "New phases and chemical reactions in solid carbon monoxide under pressure". The Journal of Physical Chemistry 88 (15): 3176–3179. doi:10.1021/j150659a007. ISSN 0022-3654. 
  9. Lipp, M.; W. J. Evans, V. Garcia-Baonza, H. E. Lorenzana (1998). "Carbon Monoxide: Spectroscopic Characterization of the High–Pressure Polymerized Phase". Journal of Low Temperature Physics 111 (3/4): 247–256. doi:10.1023/A:1022267115640. ISSN 0022-2291. 

Other reading

  • Batyrev, I. G.; W. D. Mattson, B. M. Rice (2012). "Modeling of Early Stages of Formation of Poly-CO". MRS Proceedings 1405. doi:10.1557/opl.2012.345. ISSN 1946-4274. 
  • Sun, Jian; Dennis D. Klug, Chris J. Pickard, Richard J. Needs (2011). "Controlling the Bonding and Band Gaps of Solid Carbon Monoxide with Pressure". Physical Review Letters 106 (14). doi:10.1103/PhysRevLett.106.145502. ISSN 0031-9007. 
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