Molecular dynamics calculations suggest a conduction mechanism for the M2 proton channel from influenza A virus

The M2 protein of the influenza A virus is activated by low endosomal pH and performs the essential function of proton transfer into the viral interior. The resulting decrease in pH within the virion is essential for the uncoating and further replication of the viral genetic material. The x-ray crystal [Stouffer AL, et al. (2008) Nature 451:596–599] and solution NMR [Schnell JR, Chou JJ (2008) Nature 451:591–595] structures of the transmembrane region of the M2 homo-tetrameric bundle both revealed pores with narrow constrictions at one end, leaving a question as to how protons enter the channel. His-37, which is essential for proton-gating and selective conduction of protons, lies in the pore of the crystallographic and NMR structures. Here, we explore the different protonation states of the His-37 residues of the M2 bundle in a bilayer using molecular dynamics (MD) simulations. When the His-37 residues are neutral, the protein prefers an Openout-Closedin conformation in which the channel is open to the environment on the outside of the virus but closed to the interior environment of the virus. Diffusion of protons into the channel from the outside of the virus and protonation of His-37 residues in the tetramer stabilizes an oppositely gated Closedout-Openin conformation. Thus, protons might be conducted through a transporter-like mechanism, in which the protein alternates between Openout-Closedin and Closedout-Openin conformations, and His-37 is protonated/deprotonated during each turnover. The transporter-like mechanism is consistent with the known properties of the M2 bundle, including its relatively low rate of proton flux and its strong rectifying behavior.

[1]  Xianghong Jing,et al.  Functional studies indicate amantadine binds to the pore of the influenza A virus M2 proton-selective ion channel , 2008, Proceedings of the National Academy of Sciences.

[2]  Huan‐Xiang Zhou,et al.  A secondary gate as a mechanism for inhibition of the M2 proton channel by amantadine. , 2008, The journal of physical chemistry. B.

[3]  S. Cady,et al.  Amantadine-induced conformational and dynamical changes of the influenza M2 transmembrane proton channel , 2008, Proceedings of the National Academy of Sciences.

[4]  J. Chou,et al.  Structure and mechanism of the M2 proton channel of influenza A virus , 2008, Nature.

[5]  Christopher Miller Ion channels: Coughing up flu's proton channels , 2008, Nature.

[6]  R. Fu,et al.  Solid-state 19F NMR spectroscopy reveals that Trp41 participates in the gating mechanism of the M2 proton channel of influenza A virus. , 2008, Journal of the American Chemical Society.

[7]  Vikas Nanda,et al.  Structural basis for the function and inhibition of an influenza virus proton channel , 2008, Nature.

[8]  Gregory A Voth,et al.  Proton transport behavior through the influenza A M2 channel: insights from molecular simulation. , 2007, Biophysical journal.

[9]  W. DeGrado,et al.  Determining the orientation of uniaxially rotating membrane proteins using unoriented samples: a 2H, 13C, AND 15N solid-state NMR investigation of the dynamics and orientation of a transmembrane helical bundle. , 2007, Journal of the American Chemical Society.

[10]  Gregory A Voth,et al.  Multiscale simulation of transmembrane proteins. , 2007, Journal of structural biology.

[11]  R. Lamb,et al.  Influenza virus proton channels , 2006, Photochemical & photobiological sciences : Official journal of the European Photochemistry Association and the European Society for Photobiology.

[12]  Huan‐Xiang Zhou,et al.  Histidines, heart of the hydrogen ion channel from influenza A virus: toward an understanding of conductance and proton selectivity. , 2006, Proceedings of the National Academy of Sciences of the United States of America.

[13]  I. Arkin,et al.  How pH opens a H+ channel: the gating mechanism of influenza A M2. , 2005, Structure.

[14]  Laxmikant V. Kalé,et al.  Scalable molecular dynamics with NAMD , 2005, J. Comput. Chem..

[15]  G. Voth,et al.  A computational study of the closed and open states of the influenza a M2 proton channel. , 2005, Biophysical journal.

[16]  A. Hay,et al.  Differences in conductance of M2 proton channels of two influenza viruses at low and high pH , 2003, The Journal of physiology.

[17]  R. Lamb,et al.  The Gate of the Influenza Virus M2 Proton Channel Is Formed by a Single Tryptophan Residue* , 2002, The Journal of Biological Chemistry.

[18]  Sanguk Kim,et al.  The closed state of a H+ channel helical bundle combining precise orientational and distance restraints from solid state NMR. , 2002, Biochemistry.

[19]  G. Voth,et al.  Molecular dynamics simulation of proton transport through the influenza A virus M2 channel. , 2002, Biophysical journal.

[20]  J Wang,et al.  Structure of the transmembrane region of the M2 protein H+ channel , 2001, Protein science : a publication of the Protein Society.

[21]  Cornelia Schroeder,et al.  Definitive Assignment of Proton Selectivity and Attoampere Unitary Current to the M2 Ion Channel Protein of Influenza A Virus , 2001, Journal of Virology.

[22]  W. DeGrado,et al.  pH-dependent tetramerization and amantadine binding of the transmembrane helix of M2 from the influenza A virus. , 2000, Biochemistry.

[23]  Q Zhong,et al.  Two possible conducting states of the influenza A virus M2 ion channel , 2000, FEBS letters.

[24]  R. Lamb,et al.  Mechanism for Proton Conduction of the M2 Ion Channel of Influenza A Virus* , 2000, The Journal of Biological Chemistry.

[25]  M. Klein,et al.  The M2 channel of influenza A virus: a molecular dynamics study , 1998, FEBS letters.

[26]  Alexander D. MacKerell,et al.  All-atom empirical potential for molecular modeling and dynamics studies of proteins. , 1998, The journal of physical chemistry. B.

[27]  Alexander D. MacKerell,et al.  Molecular dynamics simulation of unsaturated lipid bilayers at low hydration: parameterization and comparison with diffraction studies. , 1997, Biophysical journal.

[28]  R. Lamb,et al.  A functionally defined model for the M2 proton channel of influenza A virus suggests a mechanism for its ion selectivity. , 1997, Proceedings of the National Academy of Sciences of the United States of America.

[29]  G. R. Smith,et al.  The influenza A virus M2 channel: a molecular modeling and simulation study. , 1997, Virology.

[30]  K Schulten,et al.  VMD: visual molecular dynamics. , 1996, Journal of molecular graphics.

[31]  E. De Clercq,et al.  Synthesis and antiviral activity evaluation of some new aminoadamantane derivatives. 2. , 1996, Journal of medicinal chemistry.

[32]  T. Darden,et al.  A smooth particle mesh Ewald method , 1995 .

[33]  B. Wallace,et al.  The pore dimensions of gramicidin A. , 1993, Biophysical journal.

[34]  T. Darden,et al.  Particle mesh Ewald: An N⋅log(N) method for Ewald sums in large systems , 1993 .

[35]  P. Kollman,et al.  Settle: An analytical version of the SHAKE and RATTLE algorithm for rigid water models , 1992 .

[36]  C B Hall,et al.  Genetic basis of resistance to rimantadine emerging during treatment of influenza virus infection , 1988, Journal of virology.

[37]  J. Skehel,et al.  Molecular basis of resistance of influenza A viruses to amantadine. , 1986, The Journal of antimicrobial chemotherapy.

[38]  W. L. Jorgensen,et al.  Comparison of simple potential functions for simulating liquid water , 1983 .

[39]  G. Ciccotti,et al.  Numerical Integration of the Cartesian Equations of Motion of a System with Constraints: Molecular Dynamics of n-Alkanes , 1977 .