Ultraslow Water-Mediated Transmembrane Interactions Regulate the Activation of A2A Adenosine Receptor  Yoonji Lee, Songmi Kim, Sun Choi, Changbong Hyeon 

Slides:



Advertisements
Similar presentations
Volume 107, Issue 9, Pages (November 2014)
Advertisements

Voltage-Dependent Hydration and Conduction Properties of the Hydrophobic Pore of the Mechanosensitive Channel of Small Conductance  Steven A. Spronk,
Analysis and Evaluation of Channel Models: Simulations of Alamethicin
Volume 109, Issue 7, Pages (October 2015)
Membrane-Induced Structural Rearrangement and Identification of a Novel Membrane Anchor in Talin F2F3  Mark J. Arcario, Emad Tajkhorshid  Biophysical.
Wenjun Zheng, Han Wen, Gary J. Iacobucci, Gabriela K. Popescu 
Pedro R. Magalhães, Miguel Machuqueiro, António M. Baptista 
Volume 100, Issue 10, Pages (May 2011)
Vishwanath Jogini, Benoît Roux  Biophysical Journal 
Retinal Conformation Changes Rhodopsin’s Dynamic Ensemble
Volume 83, Issue 3, Pages (September 2002)
Jing Han, Kristyna Pluhackova, Tsjerk A. Wassenaar, Rainer A. Böckmann 
Sonya M. Hanson, Simon Newstead, Kenton J. Swartz, Mark S.P. Sansom 
Volume 90, Issue 1, Pages (January 2006)
Supriyo Bhattacharya, Nagarajan Vaidehi  Biophysical Journal 
Monika Sharma, Alexander V. Predeus, Nicholas Kovacs, Michael Feig 
How Does a Voltage Sensor Interact with a Lipid Bilayer
Coupling of Retinal, Protein, and Water Dynamics in Squid Rhodopsin
Liqiang Dai, Holger Flechsig, Jin Yu  Biophysical Journal 
Brittny C. Davis, Jodian A. Brown, Ian F. Thorpe  Biophysical Journal 
Volume 90, Issue 1, Pages (January 2006)
Analysis and Evaluation of Channel Models: Simulations of Alamethicin
Volume 98, Issue 8, Pages (April 2010)
A Molecular Dynamics Study of Ca2+-Calmodulin: Evidence of Interdomain Coupling and Structural Collapse on the Nanosecond Timescale  Craig M. Shepherd,
Molecular-Dynamics Simulations of the ATP/apo State of a Multidrug ATP-Binding Cassette Transporter Provide a Structural and Mechanistic Basis for the.
Yuno Lee, Philip A. Pincus, Changbong Hyeon  Biophysical Journal 
“DFG-Flip” in the Insulin Receptor Kinase Is Facilitated by a Helical Intermediate State of the Activation Loop  Harish Vashisth, Luca Maragliano, Cameron F.
Raf-1 Cysteine-Rich Domain Increases the Affinity of K-Ras/Raf at the Membrane, Promoting MAPK Signaling  Shuai Li, Hyunbum Jang, Jian Zhang, Ruth Nussinov 
A Gating Mechanism of the Serotonin 5-HT3 Receptor
Calcium Enhances Binding of Aβ Monomer to DMPC Lipid Bilayer
Comparative Molecular Dynamics Simulation Studies of Protegrin-1 Monomer and Dimer in Two Different Lipid Bilayers  Huan Rui, Jinhyuk Lee, Wonpil Im 
Volume 102, Issue 9, Pages (May 2012)
Volume 24, Issue 6, Pages (June 2016)
Volume 106, Issue 6, Pages (March 2014)
Firdaus Samsudin, Alister Boags, Thomas J. Piggot, Syma Khalid 
Marcos Sotomayor, Klaus Schulten  Biophysical Journal 
Sundeep S. Deol, Peter J. Bond, Carmen Domene, Mark S.P. Sansom 
Zara A. Sands, Alessandro Grottesi, Mark S.P. Sansom 
Histone Acetylation Regulates Chromatin Accessibility: Role of H4K16 in Inter- nucleosome Interaction  Ruihan Zhang, Jochen Erler, Jörg Langowski  Biophysical.
Volume 107, Issue 5, Pages (September 2014)
Volume 95, Issue 9, Pages (November 2008)
Investigating Lipid Composition Effects on the Mechanosensitive Channel of Large Conductance (MscL) Using Molecular Dynamics Simulations  Donald E. Elmore,
Activation of the Edema Factor of Bacillus anthracis by Calmodulin: Evidence of an Interplay between the EF-Calmodulin Interaction and Calcium Binding 
Grischa R. Meyer, Justin Gullingsrud, Klaus Schulten, Boris Martinac 
Volume 103, Issue 5, Pages (September 2012)
Cholesterol Modulates the Dimer Interface of the β2-Adrenergic Receptor via Cholesterol Occupancy Sites  Xavier Prasanna, Amitabha Chattopadhyay, Durba.
Volume 107, Issue 9, Pages (November 2014)
Velocity-Dependent Mechanical Unfolding of Bacteriorhodopsin Is Governed by a Dynamic Interaction Network  Christian Kappel, Helmut Grubmüller  Biophysical.
Insight into Early-Stage Unfolding of GPI-Anchored Human Prion Protein
Dynamics of the BH3-Only Protein Binding Interface of Bcl-xL
Open-State Models of a Potassium Channel
Volume 114, Issue 1, Pages (January 2018)
Ion-Induced Defect Permeation of Lipid Membranes
Robust Driving Forces for Transmembrane Helix Packing
Coupling of S4 Helix Translocation and S6 Gating Analyzed by Molecular-Dynamics Simulations of Mutated Kv Channels  Manami Nishizawa, Kazuhisa Nishizawa 
Mechanism of Anionic Conduction across ClC
Chris Neale, Henry D. Herce, Régis Pomès, Angel E. García 
Molecular Dynamics Simulations of the Rotary Motor F0 under External Electric Fields across the Membrane  Yang-Shan Lin, Jung-Hsin Lin, Chien-Cheng Chang 
Molecular Dynamics Simulations of Hydrophilic Pores in Lipid Bilayers
OmpT: Molecular Dynamics Simulations of an Outer Membrane Enzyme
Matthieu Chavent, Elena Seiradake, E. Yvonne Jones, Mark S.P. Sansom 
Volume 114, Issue 2, Pages (January 2018)
Sebastian Fritsch, Ivaylo Ivanov, Hailong Wang, Xiaolin Cheng 
Chze Ling Wee, David Gavaghan, Mark S.P. Sansom  Biophysical Journal 
Interactions of the Auxilin-1 PTEN-like Domain with Model Membranes Result in Nanoclustering of Phosphatidyl Inositol Phosphates  Antreas C. Kalli, Gareth.
Volume 78, Issue 6, Pages (June 2000)
Volume 98, Issue 4, Pages (February 2010)
Volume 111, Issue 9, Pages (November 2016)
Volume 98, Issue 3, Pages (February 2010)
The NorM MATE Transporter from N
Presentation transcript:

Ultraslow Water-Mediated Transmembrane Interactions Regulate the Activation of A2A Adenosine Receptor  Yoonji Lee, Songmi Kim, Sun Choi, Changbong Hyeon  Biophysical Journal  Volume 111, Issue 6, Pages 1180-1191 (September 2016) DOI: 10.1016/j.bpj.2016.08.002 Copyright © 2016 Biophysical Society Terms and Conditions

Figure 1 Water molecules in the TM region. (A) The number of water molecules occupying the TM regions as a function of time in the apo (black), agonist-bound (red), and antagonist-bound (blue) forms. On the left depicted is a snapshot of water permeating through the TM region. (B) Probability density map of water ρ(r) at each three-dimensional grid point r (0 ≤ ρ(r)Δr ≤ 1 with the grid cell volume of Δr = ΔxΔyΔz = 1 Å × 1 Å × 1 Å) calculated for the apo, agonist-bound, and antagonist-bound states based on the final 200 ns of simulation. Two-dimensional slices of ρ(r) were calculated using the VolMap plugin in the software VMD (http://www.ks.uiuc.edu/Research/vmd/). To see this figure in color, go online. Biophysical Journal 2016 111, 1180-1191DOI: (10.1016/j.bpj.2016.08.002) Copyright © 2016 Biophysical Society Terms and Conditions

Figure 2 Water flux through the transmembrane region. The number of water molecules traversing the TM domain as a function of time (EC → IC, solid lines; IC → EC, dashed lines). Water fluxes (j) through the receptor, calculated using the slope from linear fits to the data over the interval 400 < t < 1200 ns, are j ≈ 30 (antagonist), 20 (apo), and 10 μs−1 (agonist). To see this figure in color, go online. Biophysical Journal 2016 111, 1180-1191DOI: (10.1016/j.bpj.2016.08.002) Copyright © 2016 Biophysical Society Terms and Conditions

Figure 3 Relaxation kinetics of water mapped on A2A AR structure. (A) Location of the microswitches. (B) Time correlation functions of water from six key residues are fitted to multiexponential functions (see the Supporting Material). (C) Average relaxation time of water from various regions (TM, ECL, and ICL) in the apo (black), agonist-bound (red), and antagonist-bound (blue) forms. The extracellular view of the TM helices is shown on the left. TM1, TM2, and TM7, which have much longer relaxation time in the agonist-bound form, are marked in red. (D–F) Water relaxation time (τ) from each residue in (D) the apo, (E) the agonist-bound, and (F) the antagonist-bound forms. The TM regions are shaded in gray, and the positions of microswitches are marked with cyan dots. The receptor structures are colored based on the τ-values. To see this figure in color, go online. Biophysical Journal 2016 111, 1180-1191DOI: (10.1016/j.bpj.2016.08.002) Copyright © 2016 Biophysical Society Terms and Conditions

Figure 4 Water occupation map of the TM channel. (A) The channel formed across the TM domain of each receptor state using the 250 snapshots from 1000 to 1200 ns for the apo form, and from 600 to 800 ns for the agonist-bound and antagonist-bound forms, at which the highest water flux is observed. The channel surfaces, calculated using the program HOLE (55), are colored to visualize the channel radius (red (r < 1.15 Å), green (r = 1.15 ∼ 2.30 Å), and blue (r > 2.3 Å)). Channel radii (r) along the z axis are shown on the right with a different color for each frame. (B) Water occupancy maps along the axis perpendicular to the bilayer, calculated for the simulations of the apo (top), agonist- (middle), and antagonist-bound forms (bottom). The positions of two hydrophobic layers (HL1 and HL2) are marked with red arrows. The position of the lipid headgroup is in cyan lines on the map. A magnified view of the water occupation map for 600 ≲ t ≲ 800 ns is provided. On the right, the apo structure is displayed with the key microswitches. To see this figure in color, go online. Biophysical Journal 2016 111, 1180-1191DOI: (10.1016/j.bpj.2016.08.002) Copyright © 2016 Biophysical Society Terms and Conditions

Figure 5 Configuration of ionic-lock and Y288 associated with water flux gating. (A) Time traces probing the dynamics of three major structural motifs, i.e., ionic-lock (DRY motif), W2466.48 of CWxP, and Y2887.53 of NPxxY. From the top shown are the distances between R1023.50 and E2286.30 (ionic-lock), and between R1023.50 and Y2887.53, and the dihedral angles of W2466.48 and Y2887.53 for the apo (black), agonist-bound (red), and antagonist-bound (blue) forms. The histograms on the right are drawn using data with t > 400 ns. (B) The configurations of R1023.50, E2286.30, and Y2887.53 in the inactive and active states. The ionic lock (R102-E228) in the inactive form is disrupted in the active form, allowing R102 to form a contact with Y288. The passage of water from the IC domain is blocked by this change in the active form. The helix 7 is illustrated with the transparent band in purple. To see this figure in color, go online. Biophysical Journal 2016 111, 1180-1191DOI: (10.1016/j.bpj.2016.08.002) Copyright © 2016 Biophysical Society Terms and Conditions

Figure 6 Water flux map of A2A AR. Schematics of the water flux map (apo, agonist-bound, and antagonist-bound forms from the left to the right) are drawn based on the water dynamics from Movie S1, Movie S2, and Movie S3. The major and minor paths of water flux are depicted in solid and dashed lines, respectively. The key microswitches are depicted in sticks, and the residues of the three major structural motifs, i.e., R1023.50 of DRY, W2466.48 of CWxP, and Y2887.53 of NPxxY, are enclosed in the boxes. In the agonist-bound form, the microswitches (N241.50, D522.50, N2807.45, N2847.49, and S2817.46) in TM1, 2, and 7 form a water cluster and block the water flux. The breakage of the ionic-lock brings R1023.50 closer to Y2887.53 in TM7, blocking the entry of water from the IC domain. To see this figure in color, go online. Biophysical Journal 2016 111, 1180-1191DOI: (10.1016/j.bpj.2016.08.002) Copyright © 2016 Biophysical Society Terms and Conditions

Figure 7 Allosteric interface extended by water-mediated interactions. (A) Betweenness centralities calculated with (CBw) and without (CBo) water-mediated interaction for each receptor state. Water-free contact between two residues is defined if any heavy atom in one residue is within 4 Å from other residue; water-mediated contact between two residues is defined if a water oxygen is shared by two residues within 3.5 Å. (B) ΔCB (≡ CBw − CBo ) for each state. Large values of ΔCB are identified around the TM7 helix in the agonist-bound active state (red arrow). (C) Regions with CBw > 0.07 (corresponding to the top 10% of CB values, blue mesh, and blue arrows in (A)) and ΔCB > 0.03 (magenta surface in (C) and a magenta arrow in (B)) are demarcated on the structure of the active state. The microswitch residues are depicted as spheres. To see this figure in color, go online. Biophysical Journal 2016 111, 1180-1191DOI: (10.1016/j.bpj.2016.08.002) Copyright © 2016 Biophysical Society Terms and Conditions