Molecular gyroscope

Supramolecular complex of a chloride ion (in green), cucurbit[5]uril (rotor, in red), and cucurbit[10]uril (stator, in purple),[1] one of the first reported molecular gyroscopes

Molecular gyroscopes are chemical compounds or supramolecular complexes containing a rotor that moves freely relative to a stator, and therefore act as gyroscopes. Though any single bond or triple bond permits a chemical group to freely rotate, the compounds described as gyroscopes may protect the rotor from interactions, such as in a crystal structure with low packing density[2] or by physically surrounding the rotor avoiding steric contact.[3] A qualitative distinction can be made based on whether the activation energy needed to overcome rotational barriers is higher than the available thermal energy. If the activation energy required is higher than the available thermal energy, the rotor undergoes "site exchange", jumping in discrete steps between local energy minima on the potential energy surface. If there is thermal energy sufficiently higher than that needed to overcome the barrier to rotation, the molecular rotor can behave more like a macroscopic freely rotating inertial mass.[2]

A p-Phenylene rotor (red) rotates on two acetylene (black) axles between two m-methoxy-substituted trityl stators (blue)

For example, several studies in 2002 with a p-phenylene rotor found that some structures using variable-temperature (VT) solid-state 13C CPMAS and quadrupolar echo 2H NMR were able to detect a two-site exchange rate of 1.6 MHz (over 106/second at 65 °C), described as "remarkably fast for a phenylene group in a crystalline solid", with steric barriers of 12–14 kcal/mol. However, tert-butyl modification of the rotor increased the exchange rate to over 108 per second at room temperature, and the rate for inertially rotating p-phenylene without barriers is estimated to be approximately 2.4 x 1012 revolutions per second.[2]

Year of publication Rotor Stator Linkage Reference
2002 cucurbit[5]uril cucurbit[10]uril noncovalent [1]
2007 p-phenylene two m-methoxy-substituted trityl groups triple bonds [2]
2007 p-phenylene triply bridged trityl cage triple bonds [4]
2010 halogen-substituted p-phenylene silaalkane chains single bonds [3]
2014 p-phenylene trityl groups bridged by photoactive azobenzene bridge triple bonds [5]

References

  1. 1 2 Day, Anthony I.; Blanch, Rodney J.; Arnold, Alan P.; Lorenzo, Susan; Lewis, Gareth R.; Dance, Ian (2002). "A Cucurbituril-Based Gyroscane: A New Supramolecular Form". Angew. Chem. Int. Ed. 41 (2): 275–277. doi:10.1002/1521-3773(20020118)41:2<275::AID-ANIE275>3.0.CO;2-M.
  2. 1 2 3 4 Tinh-Alfredo V. Khuong, Hung Dang, Peter D. Jarowski, Emily F. Maverick, and Miguel A. Garcia-Garibay (2007). "Rotational Dynamics in a Crystalline Molecular Gyroscope by Variable-Temperature 13C NMR, 2H NMR, X-Ray Diffraction, and Force Field Calculations" (PDF). J. Am. Chem. Soc. 129 (4): 839–845. doi:10.1021/ja064325c.
  3. 1 2 Wataru Setaka, Soichiro Ohmizu, Mitsuo Kira (2010). "Molecular Gyroscope Having a Halogen-substituted p-Phenylene Rotator and Silaalkane Chain Stators". Chemistry Letters 39 (5): 468–469. doi:10.1246/cl.2010.468.
  4. ↑ Jose E. Nuez, Arunkumar Natarajan, Saeed I. Khan, and Miguel A. Garcia-Garibay (2007). "Synthesis of a Triply-Bridged Molecular Gyroscope by a Directed Meridional Cyclization Strategy" (PDF). Org. Lett. 9 (18): 3559–3561. doi:10.1021/ol071379y.
  5. ↑ Patrick Commins and Miguel A. Garcia-Garibay (2014). "Photochromic Molecular Gyroscope with Solid State Rotational States Determined by an Azobenzene Bridge". J. Org. Chem. 79 (4): 1611–1619. doi:10.1021/jo402516n.
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