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5
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37049086431
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This may be why there is only one current candidate for a natural Diels-Alderase enzyme: (a) Oikawa, H.; Katayama, K.; Suzuki, Y.; Ichihara, A. Chem. Commun. 1995, 1321. (b) Oikawa, H.; Kobayashi, T.; Katayama, K.; Suzuki, Y.; Ichihara, A. J. Org. Chem. 1998, 63, 8748.
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20
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0032549776
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The X-ray crystal structures for complexes between an antibody and a transition state analogue and an inhibitor have been recently reported. (a) Romesberg, F. E.; Spiller, B.; Schultz, P. G.; Stevens, R. C. Science 1998, 279, 1929. (b) Heine, A.; Stura, E. A.; Yli-Kauhaluoma, J. T.; Gao, C.; Deng, Q.; Beno, B. R.; Houk, K. N.; Janda, K. D.; Wilson, I. A. Science 1998, 279, 1934.
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21
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0032549734
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The X-ray crystal structures for complexes between an antibody and a transition state analogue and an inhibitor have been recently reported. (a) Romesberg, F. E.; Spiller, B.; Schultz, P. G.; Stevens, R. C. Science 1998, 279, 1929. (b) Heine, A.; Stura, E. A.; Yli-Kauhaluoma, J. T.; Gao, C.; Deng, Q.; Beno, B. R.; Houk, K. N.; Janda, K. D.; Wilson, I. A. Science 1998, 279, 1934.
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Deng, Q.5
Beno, B.R.6
Houk, K.N.7
Janda, K.D.8
Wilson, I.A.9
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23
-
-
0342793375
-
-
note
-
5 suggest that the accelerated reaction in the presence of such cyclic-metalloporphyrin hosts occurs inside the cavity of the host.
-
-
-
-
24
-
-
4244033876
-
-
2+ cations, and could account for the low acceleration rate (of only 2-fold) observed with monomer 8.
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(1992)
Chem. Rev.
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Kagan, H.B.1
Riant, O.2
-
27
-
-
0028967377
-
-
(c) As each of the porphyrin units in hosts 4-7 can bind the reactants inside or outside the cavity, only a small fraction of bound host is the reactive complex (host + the two reactants inside the cavity) which leads to accelerated product formation. Therefore, the acceleration rates shown in Table 1 underestimate the true ability of such hosts to accelerate the Diels-Alder reaction inside the cavity of the host. The kinetic and stoichiometric aspects of the Diels-Alder reaction in the presence of cyclic-metalloporphyrin hosts have been thoroughly discussed elsewhere: Wylie, R. S.; Sanders, J. K. M. Tetrahedron 1995, 51, 513.
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Tetrahedron
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Wylie, R.S.1
Sanders, J.K.M.2
-
28
-
-
0343227949
-
-
note
-
(a) Because of the poor quality of the diffraction data, it cannot be proved unequivocally that disordered solvent is not present in the crystal structure of the 6-3 complex.
-
-
-
-
29
-
-
0343663563
-
-
note
-
(b) However, as 3 occupies a substantial part of the cavity of 6. clearly seen in Figure 3c and more so in the space-filling model of the 6-3 complex (not shown), the Diels-Alder product 3 is poorly solvated (if at all) inside the cavity of 6.
-
-
-
-
30
-
-
0342793373
-
-
note
-
(c) In addition, it is likely that even if solvent is trapped in the space left in this cavity there will still be fewer molecules of solvent + ligand 3 in the cavity in the case of the 6-3 complex (Figure 3c) than in the cavity of the free host 6 (see Figures 2 and 3a).
-
-
-
-
31
-
-
0029894444
-
-
In some systems, displacement of solvent molecules has been suggested as the driving force for binding and acceleration: (a) Kang, J.; Rebek, J., Jr. Nature 1996, 382, 239. (b) See also ref 6c.
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(1996)
Nature
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Kang, J.1
Rebek J., Jr.2
-
32
-
-
0029894444
-
-
See also ref 6c
-
In some systems, displacement of solvent molecules has been suggested as the driving force for binding and acceleration: (a) Kang, J.; Rebek, J., Jr. Nature 1996, 382, 239. (b) See also ref 6c.
-
-
-
-
33
-
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0342792848
-
-
note
-
(a) The possible geometries of 3 were explored by a Monte-Carlo conformational search and were optimized. The most stable structure for 3 has the same conformation for the oxazine ring and the same type of inversion about the nitrogen atom in this ring, as was found in the 6·3 crystal structure.
-
-
-
-
34
-
-
0343227442
-
-
note
-
(b) The computational method used in this work is described in the Experimental and Computational Procedures section.
-
-
-
-
35
-
-
33748615619
-
-
(a) Anderson, H. L.; Bashall, A.; Henrick, K.; McPartlin, M.; Sanders, J. K. M. Angew. Chem., Int. Ed. Engl. 1994, 33, 429.
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Anderson, H.L.1
Bashall, A.2
Henrick, K.3
McPartlin, M.4
Sanders, J.K.M.5
-
39
-
-
0343663043
-
-
note
-
(a) As the two porphyrin units in 6 and in the 6·3 complex are qualitatively not offset relative to each other (see Figure 3b,d), this angle is truly describing the degree of leaning toward or away from the cavity of the two porphyrin units in the host.
-
-
-
-
40
-
-
0342357816
-
-
note
-
(b) The same is also true for 7 (Figure 4).
-
-
-
-
41
-
-
0001057603
-
-
Menger, F. M.; Ding, J.; Barragan, V. J. Org. Chem. 1998, 63, 7578.
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J. Org. Chem.
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Menger, F.M.1
Ding, J.2
Barragan, V.3
-
42
-
-
0343227436
-
-
note
-
(a) This could be seen by examining molecular models.
-
-
-
-
43
-
-
0342792843
-
-
note
-
(b) Due to the lack of high-quality Zn⋯N parameters in force field packages that we know of, we do not present here a calculated structure for the 6·12 complex. Obviously, these type of complexes are too large for high-level molecular orbital calculations with current computational resources available to us.
-
-
-
-
44
-
-
0032790258
-
-
For the geometry of hydrogen bonding see: (a) Allen, F. H.; Motherwell, W. D. S.; Raithby, P. R.; Shields, G. P.; Taylor, R. New J. Chem. 1999, 23, 25. (b) Jeffrey, G. A.; Saenger, W. Hydrogen Bonding in Biological Structures; Springer-Verlag: Berlin, 1991.
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(1999)
New J. Chem.
, vol.23
, pp. 25
-
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Allen, F.H.1
Motherwell, W.D.S.2
Raithby, P.R.3
Shields, G.P.4
Taylor, R.5
-
45
-
-
0032790258
-
-
Springer-Verlag: Berlin
-
For the geometry of hydrogen bonding see: (a) Allen, F. H.; Motherwell, W. D. S.; Raithby, P. R.; Shields, G. P.; Taylor, R. New J. Chem. 1999, 23, 25. (b) Jeffrey, G. A.; Saenger, W. Hydrogen Bonding in Biological Structures; Springer-Verlag: Berlin, 1991.
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(1991)
Hydrogen Bonding in Biological Structures
-
-
Jeffrey, G.A.1
Saenger, W.2
-
46
-
-
0343663039
-
-
note
-
As the precision in the location of hydrogen atoms is less than that for oxygen atoms, we present the O⋯O distances.
-
-
-
-
47
-
-
0343663038
-
-
note
-
Unfortunately, many attempts to obtain single crystals suitable for X-ray crystallography for the 7·3 complex were not successful.
-
-
-
-
48
-
-
0342792840
-
-
note
-
Obviously, entropic factors due to different desolvation processes for binding 3 to hosts 6 vs 7 could also partially contribute to the binding constants measured between these hosts and the Diels-Alder product 3: It is likely that in solution host 7 would contain more solvent molecules in its cavity than the smaller host 6. Therefore, this could lead to a different entropic gain due to solvent release upon binding of 3 in the cavity of 6 vs 7 (see text above). However, this does not have to be always the case, as having more solvent molecules in a larger cavity does not necessarily ensure that more solvent molecules will be displaced by the ligand. The desolvation process upon binding of ligands inside the cavity of host molecules is a complex phenomenon and, therefore, only some possible qualitative aspects of this problem are discussed here.
-
-
-
-
50
-
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0042041206
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Rappé, A. K.; Casewit, C. J.; Colwell, K. S.; Goddard, W. A., III; Skiff, W. M. J. Am. Chem. Soc. 1992, 114, 10024.
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Casewit, C.J.2
Colwell, K.S.3
Goddard W.A. III4
Skiff, W.M.5
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51
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0031484182
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Cernik, R. J.; Clegg, W.; Catlow, C. R. A.; Bushnell-Wye, G.; Flaherty, J. V.; Greaves, G. N.; Hamichi, M.; Borrows, I. D.; Taylor, D. J.; Teat, S. J. J. Synchrotron Radiat. 1997, 4, 279.
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Clegg, W.2
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Flaherty, J.V.5
Greaves, G.N.6
Hamichi, M.7
Borrows, I.D.8
Taylor, D.J.9
Teat, S.J.10
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0002589481
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Clegg, W.; Elsegood, M. R. J.; Teat, S. J.; Redshaw C.; Gibson, V. C. J. Chem. Soc., Dalton Trans. 1998, 3037.
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J. Chem. Soc., Dalton Trans.
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Clegg, W.1
Elsegood, M.R.J.2
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Redshaw, C.4
Gibson, V.C.5
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84977289324
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G. M. Sheldrick, SADABS, program for scaling and correction of area detector data; University of Göttingen, 1997 (based on the method of Blessing: Blessing, R. H. Acta Crystallogr. Sect A 1995, 51, 33).
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