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doi.org/10.1002/cplu.202000590
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byproduct 3 was obtained to enable the current study. TOF MS ES
Acknowledgements
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(m/z) [M]+ calculated for C13H23N2O2, 239.1760, found 239.1756. H
NMR (CDCl3, 300 MHz): δ ppm 3.99 (t, 2H), 3.76 (m, 7H), 3.70 (t, 2H),
3.06 (d, 2H), 2.85 (t, 2H), 2.20 (m, 2H), 1.84 (m, 6H); 13C NMR (CDCl3,
125 MHz):δ ppm 171.08, 167.63, 55.87, 52.25, 49.67, 49.64, 47.36,
33.09, 29.27, 28.52, 25.97, 23.02, 20.15.
The authors gratefully acknowledge financial support from the
National Science Foundation CAREER program (award CHE-
1352239) and from Wesleyan University.
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General procedure for byproduct reactions with thiolate. Sodium
hydride was added to a round-bottom flask under inert atmosphere
followed by the addition of anhydrous CDCl3. The solution was
Conflict of Interest
°
cooled down to 0 C using an ice bath and methyl 3-mercaptopro-
pionate was added to the NaH solution dropwise. The mixture was
The authors declare no conflict of interest.
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allowed to stir for 2 h at 0 C. An equimolar amount of the aza-
Michael nucleophile byproduct (1–3) was added to a separate
round-bottom flask under inert atmosphere. A minimal amount of
dry CDCl3 was added, and the resulting solution was taken up by
Keywords: click chemistry
· density functional theory ·
nucleophiles · reaction mechanisms · thiol-Michael reactions
°
syringe and transferred dropwise to the NaH mixture at 0 C. The
combined reaction was stirred and allowed to warm to room
temperature overnight. The reaction mixture was passed through a
short pad of Celite, concentrated under reduced pressure, and
dried further under high vacuum. The residue was diluted with
CDCl3 and analyzed by 1H NMR spectroscopy.
[1] a) D. P. Nair, M. Podgórski, S. Chatani, T. Gong, W. Xi, C. R. Fenoli, C. N.
Bowman Chem. Mater. 2014, 26, 724–744; b) A. B. Lowe Polym. Chem.
2014, 5, 4820–4870.
[2] a) H. C. Kolb, M. G. Finn, K. B. Sharpless Angew. Chem. Int. Ed. 2001, 40,
2004–2021; Angew. Chem. 2001, 113, 2056–2075; b) C. E. Hoyle, C. N.
Bowman Angew. Chem. Int. Ed. 2010, 49, 1540–1573; Angew. Chem.
2010, 122, 1584–1617; c) P. Espeel, F. E. Du Prez Macromolecules, 2015,
48, 2–14.
[3] a) M. Podgórski, S. Chatani, C. N. Bowman Macromol. Rapid Commun.
2014, 35, 1497–1502; b) S. Martens, J. O. Holloway, F. E. Du Prez Macro-
mol. Rapid Commun. 2017, 38, 1700469.
[4] a) X. Ma, Q. Sun, Z. Zhou, E. Jin, J. Tang, E. Van Kirk, W. J. Murdoch, Y.
Shen Polym. Chem. 2013, 4, 812–819; b) S. Chatani, M. Podgórski, C.
Wang, C. N. Bowman Macromolecules 2014, 47, 4894–4900; c) Z. Zhang,
S. Feng, J. Zhang Macromol. Rapid Commun. 2016, 37, 318–322; d) S. H.
Frayne, R. M. Stolz, B. H. Northrop Org. Biomol. Chem. 2019, 17, 7878–
7883.
[5] a) D. P. Nair, N. B. Cramer, J. C. Gaipa, M. K. McBride, E. M. Matherly, R. R.
McLeod, R. Shandas, C. N. Bowman Adv. Funct. Mater. 2012, 22, 1502–
1510; b) S. Chatani, C. Wang, M. Podgórski, C. N. Bowman Macro-
molecules 2014, 47, 4949–4954; c) W. Xi, A. Aguirre-Soto, C. J. Kloxin,
J. W. Stansbury, C. N. Bowman Macromolecules, 2014, 47, 6159–6165.
[6] a) M. P. Lutolf, J. A. Hubbell Biomacromolecules 2003, 4, 713–722; b) S. C.
Rizzi, J. A. Hubbell Biomacromolecules 2005, 6, 1226–1238; c) X. Sui, L.
van Ingen, M. A. Hempenius, G. J. Vancso Macromol. Rapid Commun.
2010, 31, 2059–2063; d) S. P. Zustiak, J. B. Leach Biomacromolecules
2010, 11, 1348–1357; e) K. Peng, I. Tomatsu, B. van den Broek, C. Cui,
A. V. Korobko, J. van Noort, A. H. Meijer, H. P. Spaink, A. Kros Soft Matter
2011, 7, 4881–4887; f) L. Maleki, U. Edlund, A.-C. Albertsson Biomacro-
molecules 2015, 16, 667–674; g) N. G. Moon, A. M. Pekkanen, T. E. Long,
T. N. Showalter, B. Libby Polymer 2017, 125, 66–75.
[7] a) C. Wang, S. Chatani, M. Podgórski, C. N. Bowman Polym. Chem. 2015,
6, 3758–3763; b) D. Konetski, A. Baranek, S. Mavila, X. Zhang, C. N.
Bowman Soft Matter 2018, 14, 7645–7652.
[8] a) T. H. Ho, M. Levere, J.-C. Soutif, V. Montembault, S. Pascual, L.
Fontaine Polym. Chem. 2011, 2, 1258–1260; b) W. Tang, M. L. Becker,
M. J. Matos, B. L. Oliveira, N. Martínez-Sáez, I. S. Albuquerque, E. Perkins,
F. Corzana, A. C. B. Burtoloso, G. Jiménez-Osés, G. J. L. Bernardes Nat.
Commun. 2016, 7, 13128; d) Y. Sun, H. Liu, L. Cheng, S. Zhu, C. Cai, T.
Yang, L. Yang, P. Ding Polym. Int. 2018, 67, 25–31.
The quantities used for thiolate reactions with nucleophile by-
products 1–3 were as follows: DMAP nucleophile byproduct 1
(28.9 mg, 0.1 mmol) was mixed with sodium hydride (60%
dispersion in oil) (4.0 mg, 0.1 mmol) and methyl 3-mercaptopropio-
nate (11 μL, 0.1 mmol). MIM nucleophile byproduct 2 (24.9 mg,
0.1 mmol) was mixed with sodium hydride (60% dispersion in oil)
(4.0 mg, 0.1 mmol) and methyl 3-mercaptopropionate (11 μL,
0.1 mmol). DBU nucleophile byproduct 3 (42.7 mg, 0.13 mmol) was
mixed with sodium hydride (60% dispersion in oil) (5.4 mg,
0.13 mmol) and methyl 3-mercaptopropionate (15 μL, 0.13 mmol).
Each reaction resulted in the formation of symmetric thiodipropio-
nate 4.
Computational Modeling
Computational investigations were performed using the Gaussian16
suite of programs.[14] Structures of stationary points along each
reaction mechanism were each subjected to a conformational
search by scanning all freely rotating torsional angles at the B3LYP/
6-31G(d)[15] level to locate approximate global energy minimum
structures. The optimal structure of each stationary point was then
optimized to full convergence at the B3LYP/6-31+G(d) level of
theory. Approximate transition state geometries were located by
scanning along the reaction coordinate(s) corresponding to bond
breakage/formation. Each approximate transition state geometry
was then subjected to a Berney transition state optimized to full
convergence. Transition states were distinguished as having a
single imaginary vibrational frequency, whereas all minima had
only real vibrational frequencies. Prior computational modeling of
thiol-Michael reactions by Houk,[11a] Qi,[11c] and Northrop[11d,12] has
shown that geometry optimization at the B3LYP/6-31+G(d) level
followed by single-point energy calculations using the M06-2X
functional[16] with a large basis set provides reaction energetics that
agree well with CBS-QB3 benchmarks. Reaction and transition state
enthalpies and free energies reported herein were therefore
calculated at the M06-2x/6-311+G(2d,p)//B3LYP/6-31+G(d) level.
Reaction energetics were obtained at 298.15 K, 1.0 atm pressure,
and in a PCM model[17] of CHCl3 and DMSO solvents.
[9] a) H. Seto, M. Takara, C. Yamashita, T. Murakami, T. Hasegawa, Y.
Hoshino, Y. Miura ACS Appl. Mater. Interfaces 2012, 4, 5125–5133; b) R.
Tedja, A. H. Soeriyadi, M. R. Whittaker, M. Lin, C. Marquis, C. Boyer, T. P.
Davis, R. Amal Polym. Chem. 2012, 3, 2743–2751.
[10] a) J. W. Chan, C. E. Hoyle, A. B. Lowe, M. Bowman Macromolecules 2010,
43, 6381–6388; b) G.-Z. Li, R. K. Randev, A. H. Soeriyadi, G. Rees, C. Boyer,
Z. Tong, T. P. Davis, C. R. Becer, D. M. Haddleton Polym. Chem. 2010, 1,
1196–1204; c) W. Xi, C. Wang, C. J. Kloxin, C. N. Bowman ACS Macro Lett.
2012, 1, 811–814; d) L.-T. Nguyen, M. T. Gokmen, F. E. Du Prez Polym.
Chem. 2013, 4, 5527–5536; e) S. Chatani, D. P. Nair, C. N. Bowman Polym.
Chem. 2013, 4, 1048–1055; f) S. H. Frayne, R. R. Murthy, B. H. Northrop J.
Org. Chem. 2017, 82, 7946–7956; g) S. Huang, J. Sinha, M. Podgórski, X.
Zhang, M. Claudino, C. N. Bowman Macromolecules 2018, 51, 5979–
5988.
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