The black crystalline compound N,Nꢀ-ethylenebis(salicylidene-
iminato)nitrosylcobalt [(NO)Co(Salen)] was obtained and its ESR
(Fig. S1†) and IR (Fig. S2†) spectra were compared with those of
an authentic sample.
Dr S. Mukhopadhyay and Dr S. Kulkarni (Vlife Sciences Tech-
nologies Pvt. Ltd., Pune, India) for their contributions to the DFT
calculations.
In a separate reaction the effluent gas coming out from the vent
was passed through a cannula into a freshly prepared aqueous
solution of glutathione–cobalamine (0.4 mmol cobalamine and
4 mmol glutathione were mixed in 20 cm3 distilled water and
phosphate buffer was used to make the solution of pH = 7). A
colour change from violet to brown was observed indicating the
cobalamine–NO adduct formation which was further followed by
UV-Visible spectral changes (Fig. 2).
Similarly the effluent gas coming out from the vent was also
passed through a cannula to a freshly prepared aqueous solution
of myoglobin (Mb). The formation of the Mb–NO adduct was
confirmed by UV-Visible spectroscopy (Fig. 3).
References
1 (a) B. A. Averill, Chem. Rev., 1996, 96, 2951; (b) I. M. Wasser, S. de
Vries, P. Moe¨nne-Loccoz, I. Schro¨der and K. D. Karlin, Chem. Rev.,
2002, 102, 1201.
2 M. T. Gladwin, J. Clin. Invest., 2004, 113, 19.
3 (a) K. Cosby, K. S. Partovi, J. H. Crawford, R. P. Patel, C. D. Reiter, S.
Martyr, B. K. Yang, M. A. Waclawiw, G. Zalos, X. Xu, K. T. Huang, H.
Shields, D. B. Kim-Shapiro, A. N. Schechter, R. O. Cannon and M. T.
Gladwin, Nat. Med., 2003, 12, 1498 and references therein; (b) S. Shiva,
X. Wang, L. A. Ringwood, X. Xu, S. Yuditskaya, V. Annavajjhala, H.
Miyajima, N. Hogg, Z. L. Harris and M. T. Gladwin, Nat. Chem. Biol.,
2006, 2, 486; (c) D. Fukumara, S. Kashiwagi and R. K. Jain, Nat. Rev.
Cancer, 2006, 6, 521; (d) N. Finney, Nat. Chem. Biol., 2006, 2, 349.
4 A. Webb, R. Bond, P. McLean, R. Uppal, N. Benjamin and A.
Ahluwalia, Proc. Natl. Acad. Sci. USA, 2004, 101, 13683.
5 A. Butler and R. Nicholson, in Life, Death and Nitric Oxide, Royal
Society of Chemistry, Cambridge, 2003.
Spectroscopic identification of SafH–NO
6 N. S. Bryan, T. Rassaf, R. E. Maloney, C. M. Rodriguez, F. Saijo, J. R.
Rodriguez and M. Feelisch, Proc. Natl. Acad. Sci. USA, 2004, 101,
4308.
7 Data for Biochemical Research, ed. R. M. C. Dawson, D. C. Elliot,
W. H. Elliot and K. M. Jones, Oxford University Press, New York,
1969, pp. 438–439.
The reduction of nitrite in the U-tube was carried out as mentioned
above and the UV-Visible spectra of both the aqueous layers were
monitored (Fig. S3†). For isolation of the solid after 120 min
reaction the left hand aqueous phase was taken to dryness, the solid
residue extracted with dichloromethane and the dichloromethane
layer taken to dryness to give a very small amount (< 0.5 mg) of
an orange solid. The IR (CHCl3), ESR (CH2Cl2, 77 K) and mass
spectrum (in methanol, ion-spray) and of this solid were recorded
and shown in Fig. 4, 5 and 6, respectively.
8 S. Bhaduri, N. S. Gupta, G. K. Lahiri and P. Mathur, Organometallics,
2004, 23, 3733.
9 S. Bhaduri, P. Mathur, P. Payra and K. Sharma, J. Am. Chem. Soc.,
1998, 120, 12127.
10 S. Bhaduri and K. Sharma, J. Chem. Soc., Chem. Commun., 1992, 21,
1593.
11 G. Longoni and P. Chini, J. Am. Chem. Soc., 1976, 98, 7225.
12 N. S. Gupta, P. Mathur, M. Doble and S. Bhaduri, Inorg. Chim. Acta,
2006, 359, 3895.
Methodology for the DFT calculations
13 A. Earnshaw, P. C. Hewlett and L. F. Larkworthy, J. Chem. Soc., 1965,
The optimized geometries of all the MBH, SafH and their
corresponding NO adducts have been obtained by using the hybrid
density functional method (B3LYP)16 (three parameter Becke’s
exchange energy functional along with correlational functional
due to Lee, Yang and Parr). Specifically, for the closed shell
geometries of MBH and SafH, the B3LYP method has been
used and for all open shell geometries of free NO and all MBH–
NO and SafH–NO adducts, the UB3LYP method (unrestricted
open shell calculations) has been utilized. The basis set used
in these calculations is 6–31G* in which all core electrons have
been explicitly considered. The vibrational frequencies and zero
point corrected energies (ZPE) of all the optimized structures have
been obtained. All the calculations have been performed using the
program Gaussian 98.17
4718.
14 (a) D. Zheng and R. L. Birke, J. Am. Chem. Soc., 2001, 123, 4637; (b) D.
Zheng and R. L. Birke, J. Am. Chem. Soc., 2002, 124, 9066.
15 (a) B. O. Fernandez, I. M. Lorkovic and P. C. Ford, Inorg. Chem., 2004,
43, 5393; (b) A. K. Patra and P. K. Mascharak, Inorg. Chem., 2003, 42,
7363.
16 (a) D. Becke, Phys. Rev. A, 1988, 38, 3098; (b) C. Lee, W. Yang and
R. G. Parr, Phys. Rev. B, 1988, 37, 785; (c) A. D. Becke, J. Chem. Phys.,
1993, 98, 5648.
17 M. J. Frisch, G. W. Trucks, H. B. Schlegel, G. E. Scuseria, M. A.
Robb, J. R. Cheeseman, V. G. Zakrzewski, J. A. Montgomery, Jr., R. E.
Stratmann, J. C. Burant, S. Dapprich, J. M. Millam, A. D. Daniels,
K. N. Kudin, M. C. Strain, O. Farkas, J. Tomasi, V. Barone, M.
Cossi, R. Cammi, B. Mennucci, C. Pomelli, C. Adamo, S. Clifford,
J. Ochterski, G. A. Petersson, P. Y. Ayala, Q. Cui, K. Morokuma,
P. Salvador, J. J. Dannenberg, D. K. Malick, A. D. Rabuck, K.
Raghavachari, J. B. Foresman, J. Cioslowski, J. V. Ortiz, A. G. Baboul,
B. B. Stefanov, G. Liu, A. Liashenko, P. Piskorz, I. Komaromi, R.
Gomperts, R. L. Martin, D. J. Fox, T. Keith, M. A. Al-Laham, C. Y.
Peng, A. Nanayakkara, M. Challacombe, P. M. W. Gill, B. Johnson, W.
Chen, M. W. Wong, J. L. Andres, C. Gonzalez, M. Head-Gordon, E. S.
Replogle and J. A. Pople, GAUSSIAN 98, Revision A.11, Gaussian,
Inc., Pittsburgh PA, 2001.
Acknowledgements
Financial support received from Reliance Industries Lim-
ited, Mumbai, India is gratefully acknowledged. We thank
2598 | Dalton Trans., 2007, 2594–2598
This journal is
The Royal Society of Chemistry 2007
©