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Cooperativity of Non-Covalent Interactions
G. Narahari Sastry Centre for Molecular Modeling
Indian Institute of Chemical Technology Hyderabad – 500 607, INDIA
[email protected] http://203.199.182.73/gnsmmg/
79th Annual Meeting of Indian Academy of Sciences Chandigarh, 8 – 10 November 2013
Current Ph.D./Project Students • Neela • Bhaskar Sharma • Richard Prem Kumar • U. Purushotham • Altaf Hussain • Uma Devi • Chinmayee • Ram Vivek • Srikanth • Sirisha Scientists in the Group • Dr. Y. Soujanya • Dr. G. Gayatri • Dr. Swati Pannigrahi • Dr. S.Janardhan • Dr. Anirban
Past Ph.D. Students Dr. U. D. Priyakumar Dr. T.C. Dinadayalane Dr. J. Narashimamoorthy Dr. A. Srinivas Reddy * Dr. P. Srivani Dr. M. Nagaraju Dr. G. Gayatri Dr. Dolly Vijay * Dr. J. Srinivasa Rao Dr. B. Sateesh Dr. R.G. Kulkarni Dr. M. Chourasia Preethi Badrinarayan A. Subha Mahadevi *
Collaborators Dr. G.Madhavi Sastry Dr. Devesh Kumar Prof. H. Sakurai Prof. S.P. de Visser Prof. H. Zipse Prof. A. R. Rao Prof. G. Achaiah Prof. S.R. Gadre Prof. E.D. Jemmis Prof. S.R. Gadre Dr. M. Vairamani Dr. A. Kamal Prof. S. Bapiraju Prof . S. Durga Bhavani
Funding: CSIR, DST, DBT, DAE(BRNS), Indo-German(DST-DAAD), Indo-Japan (INSA-JSPS)
Acknowledgements
Molecules Clusters Crystal structure
Are the properties of the clusters similar to bulk properties of larger aggregates like crystals?
Water: From Clusters to the Bulk 'Water is H2O, hydrogen two parts, oxygen one, but there is also a third thing, that makes it water and nobody knows what it is’ !!
D H Lawrence (1885-1930)
Water clusters are small groupings of water molecules that differ in many ways from bulk water
Unlike bulk water, most of the molecules in a small cluster are on the surface, where they have fewer chemical interactions with other water molecules
Formation of clusters from individual units
Animations from Martin chaplin,s website
Physical properties of such clusters vary according to their relative concentrations
Hydrogen bonded networks and cooperativity
In 1957, Wen et al. were the first to discuss the importance of many-body effects in
water in their description of the cooperativity of hydrogen bonds
Structural aspects of ion-solvent interaction in aqueous solutions: A suggested picture of water structure, Frank, H. S.; Wen, W. Y. Discuss. Faraday. Soc. 1957, 24, 133
They postulated that the formation of hydrogen bonds in water is predominantly a
cooperative phenomenon
“When one bond forms several will form, and when one bond
breaks then, typically a whole cluster will dissolve.”
Proposed resonance scheme for hydrogen bond in water
+
+ + E (kcal/mol)
Formamide units
Formamide chain
Cooperativity in Amide Hydrogen Bonding Chains. Relation between Energy, Position, and H-Bond Chain Length in Peptide and Protein Folding ModelsKobko, N.; Dannenberg J. J. J. Phys. Chem. A 2003, 107, 10389-10395 Cooperativity in Amide Hydrogen Bonding Chains. A Comparison between Vibrational Coupling through Hydrogen Bonds and Covalent Bonds. Implications for Peptide Vibrational SpectraKobko, N.; Dannenberg J. J. J. Phys. Chem. A 2003, 107, 6688-6697
• B3LYP/D95** calculations for linear H-bonded formamide (n = 2 – 15) • Their studies reveal cooperative effect of 200% over dimer particularly those bonds in centre of chain
Studies on Cooperativity in linear formamide chains
Interaction enthalpies for H-bonds organized by H-bond type (k) for chains of the lengths indicated by the symbols
Variation of frequencies and intensities for the H-bonding N-H stretches in formamide chains.
Manifestation of hydrogen bond cooperativity as a function of increasing cluster size
and varying arrangement of molecules is explored using formamide [HCONH2]n (n =
1-10) clusters based on DFT calculations.
Mahadevi, A. S.; Neela, Y. I.; Sastry G. N. J. Chem. Sci. 2012, 124, 35-42
Cooperativity in Formamide Clusters (Structural, Energetic, Spectroscopic)
Cooperativity of Hydrogen Bonding in Acetamide Clusters
How much of cooperativity is a function of size of cluster? , and how much is it
due to individual arrangement? Mahadevi ,A. S.; Neela, Y. I.; Sastry, G. N. Phys. Chem. Chem. Phys. 2011, 13,15211-15220
Cooperativity in Acetamide Clusters
Graphical plot of relative energy (RE in kcal mol-1) versus number of monomers for circular and standard arrangements with respect to (w.r.t) the linear arrangement of acetamide, n=2–15, at the B3LYP/D95** level of theory
As the cluster size increases the relative energy of both circular and standard forms
increases on comparison to the corresponding linear form
Naturally occurring forms of Water Clusters
Ice XI, and its repeating unit Buch, V.; Sandler, P.; Sadlej, J. J. Phys. Chem. B 1998, 102, 8641.
Helical water chain Saha, B. K.; Nangia, A. Chem. Commun. 2005, 3024. Barbour, L. J.; Orr, G. W.; Atwood, J. L.
Nature. 1998, 393, 671.
Supra molecular complex in aqueous medium along with repeating unit of
water here
Ice Ih and its repeating unit Distribution of water at micellar surface mimicking
protein surface
Biological water Materer, N.; Starke, U.; Barbieri, A.; Van Hove, M. A.; Somorjai, G. A.; Kroes, G. J.; Minot, C. J. Phys. Chem. 1995, 99, 6267.
Nandi, N.; Bagchi, B. J. Phys. Chem. B 1997, 101, 10954
Pal, S. K.; Peon, J.; Zewail, A. H. Proc. Natl. Acad. Sci. 2002,
99, 15297 Neela, Y. I.; Mahadevi, A. S.; Sastry G. N. J. Phys. Chem. B 2010, 114, 17162
Encapsulated water wire in peptide
Raghavender U. S.; Aravinda K. S.; Shamala N.; Balaram P J. Am. Chem. Soc. 2010, 132, 1075
Water chains Natarajan, R.; Charmant, J. P. H.; Orpen, A. G.; Davis A. P. Angew. Chem. Int. Ed. 2010, 49, 5125.
Buehler, M. J. Nature Nanotech. 2010, 5, 172-173.
Knowles, T. P. J.; Oppenheim, T. W.; Buell, A. K.; Chirgadze,
D. Y.; Welland M. E. Nature Nanotech. 2010, 5, 204-207
Hydrogen Bond 3Å
βStrand 2nm
Amyloid fibril 8-10nm
Amyloid fibre 100s of nm Amyloid
plaque >100nm
Self assembly of proteins in amyloids: an inspiration to create multifunctional macroscopic materials
G.; Rossetti, A.; Magistrato, A.; Pastore, P. Carloni, J. Chem. Theory Comput. 2010, 6, 1777.
The cooperativity of glutamine
side chains affects both the
directions perpendicular and
parallel to the backbone.
Polyglutamine β-sheet aggregates
a r e a s s o c i a t e d w i t h t h e
derangement of Hunt ington’s
disease.
The effect of cooperativity control
the structure and energetics of the
aggregates.
Studies on Cooperativity in Hydrogen Bonding in polyQ -Sheets
Synergy in Noncovalent Interactions-Important Questions ?
Do they behave differently in the
presence of each other ? Mutual impact
Do their properties vary when several of the same
kind of non-bonded interactions occur
together ? Size Effect
How does this impact supramolecular
assembly ? Aggregation
π π Cation π
Hydrogen Bond
Van der Waals?
Spiny-tail gecko lizard has a total Clining force of over 20N, though the Little Lizard weighs only about 40g!
Glue?
Suction?
Friction?
Capillary Forces?
Claws?
π; π π; π,
π,
Central Dogma in Biology: π-π
Interactions in Molecules
Enonbonded = Eelectrostatic + Einduction + ECT + Edispersion + Eexchange-repulsion
Electrostatic multipole – multipole Induction multipole-induced multipole Dispersion instantaneous multipole-induced multipole CT - charge transfer from donor to acceptor Exchange electron exchange
van der Waals electrostatic
E = Ebend + Estretch + Etorsion + Evan der Waals + Eelectrostatic
Bonded Non-Bonded
Distance dependencies of Non-Covalent Interactions
Chem. Rev., 2013, 113, 2100-2138.
Cation-π interactions 1. Arguably the strongest among different non-bonded interactions
2. Tunability of cation-π interactions is effected by subtle variation of key factors
• Size of π system
• Solvent Effect
• Nature of cation
• Cation-π vs. Cation-σ
• Substituent
• Counter-Ion
3. Cooperativity of cation-π interactions with other non-bonded interactions
4. Significant impact in several fields including chemistry, biology, material science,
nanosystems, host guest interaction, catalysis and reaction mechanisms…
5. Potential application in developing scoring functions and drug design
Exploring the Coexistence of M-π and π-π Interactions in Biology and Chemistry
Reddy. A. S.; Vijay, D.; Sastry, G. M.; Sastry, G. N. J. Phys. Chem. B, 2006, 110, 2479 Reddy. A. S.; Vijay, D.; Sastry, G. M.; Sastry, G. N. J. Phys. Chem. B, 2006, 110, 10206
Two key non-covalent forces namely cation-π and π-π, which govern the macromolecular structure, work in concert
Table: π-π interactions Interaction Energies (in kcal/mol) of the Various Benzene Dimers in the Presence of Metal Ion
Cooperativity – Its Universality
Cooperativity
Important Questions ??? Unambiguous
quantitative measure in large system with
multiple kinds of weak interactions
Biological Context
Supramolecular Assembly Catalysis
Potential Applications (design of novel material)
Synonymous Terminology Non-Additivity Synergy Cooperativity
Our contribution to the concept of cooperativity A clear and unambiguous measure for cooperativity in ternary systems
J. Phys. Chem. B, 2006, 110, 2479 J. Phys. Chem. B, 2006, 110, 10206
J. Phys. Chem. B, 2008, 112, 8863 Chem. Phys. Lett, 2010, 485,235 Cation-π and hydrogen bonding Cation-π and π-π
J. Phys. Chem. B, 2010 , 114, 17162; J. Chem. Phys. 2010, 133, 164308; Phys. Chem. Chem. Phys. 2011, 13,15211 ; J. Chem. Sci. 2012, 124, 35
Coexistence of Cation and π- π interactions
NAME METHODOLOGY Morokuma
Analysis Eint = ES + PL + EX + CT + MIX (Kitaura, K.; Morokuma, K. Int. J. Quantum Chem. 1976, 10, 325: Zhu, W.; Luo, X.; Puah, C. M.; Tan, X.; Shen, J.; Gu, J.; Chen, K.; Jiang, H. J. Phys. Chem. A 2004, 108, 4008 )
ES = Electrostatic, PL = Polarization, EX = Exchange, CT = Charge Transfer, MIX = cross
(SAPT) Symmetry Adopted
Perturbation Theory
Eint = E(1)es+E (1)
exch+E (2) ind+E (2) exch –ind +E (2) disp+ E (2) exch - disp+δHFint
= Ees+ Eexch +Eind+Edisp (Jeziorski, B.; Moszynski, R.; Szalewicz, K. Chem. Rev 1994,94, 1887: Kim,
D.; Tarakeshwar, P.; Kim, K. S. J. Phys.Chem. A 2004,108, 1250)
E(1)es = Electrostatic, E (1)
exch= 1st order valance repulsion due to pauli exclusion, E (2) ind= 2nd order energy gain resulting from induction interaction, E (2) exch –ind = Repulsion change due to electron cloud deformation, E (2) disp = 2nd order dispersion energy, E (2) exch – disp= 2nd order dispersion correction for a coupling between the exchange repulsion and the dispersion interaction.
δHFint = Higher order induction and exchange correction.
(MIPP) Molecular Interaction Potential
Eint= Ee+Evw+Ep ( Lugue, F. J.; Orozco, M.; J. Comput. Chem. 1998, 19, 866: Garau, C.; Frontera, A.; Quinonero, D.; Ballester, P.; Costa, A.; Deya, P. M. Chem. Phys. Lett. 2004, 392, 85) Ee= Electrostatic Evw= Sum of dispersion and repulsion energies Ep= Polarization
Energy Partition Schemes
(BLW-ED) Block-localized wave function
approach
EHF = Edist+ Ees+ Eex+ Epol+ Ect ( Mo, Y.; Gao, J. Chem. Phys 2000, 112, 5530: Mo, Y.; Song, L.; Wu, W.; Zhang, Q. J. Am. Chem. Soc. 2004, 126, 3974)
EMP2 = Edist+ Ees+ Eex+ Epol+ Εct + Ecorr Edist = Geometry distortion, Ees= Electrostatic, Eex= Exchange repulsion, Epol = Polarization, Εct = Charge transfer Ecorr = Electron Correlation
Reduced Variational Space (RVS) Analysis
Energy Decomposition Analysis
Manifestation of cooperativity and the various aspects of the concept
Understanding the role, range and relevance of non-covalent interactions, particularly, h-bonding, cation-π and π-π interactions are of outstanding importance in biology, chemistry, material science and all molecular sciences.
Cooperativity is a fascinating phenomenon, and understanding how it operates and manifests in supramolecular assemblies is interesting in its own right. (Energetic, Structural, Spectral and Functional issues)
Concluding Remarks
"It is certain that all bodies whatsoever, though they have no sense,
yet they have perception; for when one body is applied to another,
there is a kind of election to embrace that which is agreeable, and
to exclude or expel that which is ingrate; and whether the body be
alterant or altered, evermore a perception precedeth operation; for
else all bodies would be like one to another." Francis Bacon
(abou.1620)