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Cross-saturation and transferred cross-saturation experiments

Published online by Cambridge University Press:  29 April 2014

Takumi Ueda
Affiliation:
Graduate School of Pharmaceutical Sciences, The University of Tokyo, Hongo, Tokyo 113-0033, JapanPrecursory Research for Embryonic Science and Technology, Japan Science and Technology Agency, Chiyoda-ku 102-0075, Japan
Koh Takeuchi
Affiliation:
Molecular Profiling Research Center, National Institute of Advanced Industrial Science and Technology, Aomi, Koto-ku, Tokyo 135-0064, Japan
Noritaka Nishida
Affiliation:
Graduate School of Pharmaceutical Sciences, The University of Tokyo, Hongo, Tokyo 113-0033, Japan
Pavlos Stampoulis
Affiliation:
Graduate School of Pharmaceutical Sciences, The University of Tokyo, Hongo, Tokyo 113-0033, Japan
Yutaka Kofuku
Affiliation:
Graduate School of Pharmaceutical Sciences, The University of Tokyo, Hongo, Tokyo 113-0033, Japan
Masanori Osawa
Affiliation:
Graduate School of Pharmaceutical Sciences, The University of Tokyo, Hongo, Tokyo 113-0033, Japan
Ichio Shimada*
Affiliation:
Graduate School of Pharmaceutical Sciences, The University of Tokyo, Hongo, Tokyo 113-0033, Japan
*
*Author for Correspondence: Graduate School of Pharmaceutical Sciences, The University of Tokyo, Hongo, Bunkyo-ku, Tokyo 113-0033, Japan. Tel: +(81) (3) 3815 6540; Fax: +(81) (3) 3815 6540; Email: shimada@iw-nmr.f.u-tokyo.ac.jp
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Abstract

Structural analyses of protein–protein interactions are required to reveal their functional mechanisms, and accurate protein–protein complex models, based on experimental results, are the starting points for drug development. In addition, structural information about proteins under physiologically relevant conditions is crucially important for understanding biological events. However, for proteins such as those embedded in lipid bilayers and transiently complexed with their effectors under physiological conditions, structural analyses by conventional methods are generally difficult, due to their large molecular weights and inhomogeneity. We have developed the cross-saturation (CS) method, which is an nuclear magnetic resonance measurement technique for the precise identification of the interfaces of protein–protein complexes. In addition, we have developed an extended version of the CS method, termed transferred cross-saturation (TCS), which enables the identification of the residues of protein ligands in close proximity to huge (>150 kDa) and heterogeneous complexes under fast exchange conditions (>0.1 s−1). Here, we discuss the outline, basic theory, and practical considerations of the CS and TCS methods. In addition, we will review the recent progress in the construction of models of protein–protein complexes, based on CS and TCS experiments, and applications of TCS to in situ analyses of biologically and medically important proteins in physiologically relevant states.

Information

Type
Review Article
Copyright
Copyright © Cambridge University Press 2014 
Figure 0

Fig. 1.Schematic diagrams of the CS method.

Figure 1

Fig. 2.Schematic diagrams of the TCS method.

Figure 2

Fig. 3.Schematic diagrams of the samples used in TCS experiments. Protein I is deuterated, and water with a low proton concentration is used as the solvent. Under these conditions, the spatial configurations of the protons of each isotopomer in protein I can be highly variable.

Figure 3

Fig. 4.Model spin system used in the simulation study. (a) Basic structure of the model spin system. Protein I is composed of three exchangeable protons, L1, L2, and L3 (open circles) placed linearly with 3 Å spacing. Protein II is composed of non-exchangeable protons (closed circles) placed at 3 Å -spaced grid points in a cube. The distance between the L1 proton and the closest proton of protein II is set to 5 Å. (b) CPK model of the model spin system. The total number of protons in protein II is 133. The protons of proteins I and II are colored gray and white, respectively.

Figure 4

Fig. 5.Schematic representations of ASCS methods. (a) The ASCS method. Protein II molecules are amino acids, X, Y, and Z selectively 1H-labeled in a 2H-background on each panel, respectively, whereas protein I is labeled in the same way as in conventional CS. The amide protons affected by the rf-irradiation on the ligand are depicted as H1, H2, H3, and H4. (b) Combinatorial approach to determine the proximal residue pairs. The CS-source residues can be identified by combining several ASCS results, based on the spatial complementarity of the CS-source candidates and the amide protons affected by the rf-irradiation.

Figure 5

Fig. 6.CS from YUH1 to Ub. (a) Conventional CS experiment using unlabeled YUH1. Residues 7–11, 36, 40–42, 47, and 69–76 of Ub were significantly affected by the rf-irradiation. (b) CS experiment using uniformly 2H-labeled YUH1. No Ub residue was affected by the rf-irradiation. (c) Ala, (d) Leu, (e) Pro, (f) Tyr, (g) Met, (h) Phe, and (i) Arg-selective CS experiments. (c–f and i) ASCS experiments were performed at 30°C with irradiation for 1.5 s. Numbers show Ub residues affected by the rf-irradiation. (g and h) ASCS experiments were performed at 10°C with irradiation for 4.5 s. Asterisks indicate the Ub residues within 4–5 Å from the 1H-labeled amino-acid residues of YUH1.

Figure 6

Fig. 7.Identification of proximal residues on Ub and YUH1 by ASCS. (a) Left: Amide protons affected by the rf-irradiation (red spheres) in four ASCS experiments. The Ub backbone is shown as a blue tube model. Right: Candidates of residues on YUH1 proximal to Ub residues affected by the rf-irradiation. Ala, Pro, Tyr, and Leu are colored pink, red, orange, and green, respectively. (b) The residue proximal to the residues affected by the rf-irradiation on the crystal structure of Ub–YUH1.

Figure 7

Fig. 8.Model building of a protein–protein complex satisfying the ASCS results. (a) Initial structures for the simulated annealing calculations. Green spheres represent the centers of mass for 42 candidates of Ub. The initial structures of Ub generated from the 1st and 34th pair list are shown and colored red and blue, respectively. The YUH1 and Ub of the reference complex are shown and colored light blue and orange, respectively. The C-terminal Cα atoms of Ub are displayed as space-filled models. (b) Relationship between the EASCS values and the RMSDtotal values of Ub, determined using the simulated annealing procedure. The open circle represents the EASCS value calculated from the reference complex. The dashed line represents EASCS=15.4 kcal mol−1. (c) Complex structure of YUH1 and Ub. YUH1 and Ub of the complex with the lowest EASCS value are shown and colored blue and red, respectively. The YUH1 and Ub of the complex after equilibration in explicit water are shown and colored green and purple, respectively. Furthermore, the YUH1 and Ub of the reference complex are shown and colored light blue and orange, respectively. The YUH1 of the model complex is superimposed on the YUH1 of the reference structure.

Figure 8

Fig. 9.Gβγ-binding interface on GIRKCP. (a) Mapping of the affected residues in the TCS experiment on a single subunit of the GIRKCP structure (PDB code 1N9P). The residues with large intensity reduction ratios and small but significant intensity reduction ratios are colored red and orange, respectively. In the surface representations (center and right), proline residues and residues with no data are colored black and gray, respectively, because they lacked CS data. (b) Mapping of the affected residues in the TCS experiment on two adjacent subunits of a GIRKCP tetramer (white and cyan), viewed from the outside (left) and the inside (right) of the pore, with the same color code as in (a). (c) Important residues for the interaction between GIRKCP and Gβγ. (Upper) Surface representations of Gα (right) and Gβγ (left), viewed from the contacting surfaces in the crystal structure of the Gαβγ complex (PDB code 1GOT). The residues involved in the intermolecular interaction between Gα and Gβγ, within a distance of 4 Å in the Gαβγ complex structure, are colored according to their side chain properties: hydrophobic, hydrophilic, acidic, and basic residues are green, yellow, red, and blue, respectively. The interacting residues between the N-terminal helix of Gα and Gβγ are labeled in gray. The important residues of Gβγ for GIRK binding, identified by mutational analyses, are labeled with asterisks. The region of the Gβγ-binding site on Gα (the Gβγ-binding motif), composed of a hydrophobic area flanked by two acidic residues, and the interacting surface on Gβγ are enclosed in circles. (Lower) The Gβγ-binding surface of GIRK, determined by TCS experiments, on the GIRKCP structure, colored according to the side chain properties. The similar Gβγ-binding motif to that found on the Gα surface in the upper panel is circled and enlarged, where the residues without TCS information are also labeled in black and blue, for the residues from one subunit colored in white and the other subunit, colored cyan, respectively.

Figure 9

Fig. 10.Binding mode of Gβγ-and GIRK. (a) The residues with large intensity reductions and small but significant reductions upon addition of Gβγ in the chemical shift perturbation experiments, mapped on the surface of a single subunit of the GIRKCP structure and colored red and orange, respectively. Proline residues and residues with no data are colored black and gray, respectively. (b) Mapping of the residues with significant intensity reductions clustered in the interface on the outside surface of the two neighboring subunits of GIRKCP (left), and mapping of the other residues, which are not exposed to the outside surface, on two neighboring subunits of GIRKCP viewed from the inside of the pore (right), with the same color scheme as in (a). The buried residues are labeled with dashed lines. (c) Interacting residues between the CP and TM regions of the chimeric channel. (Left) Backbone structure of the chimeric channel of KirBac1.3 and GIRK1 (PDB code 2QKS). Two neighboring subunits are shown from the outside, and are colored gray and cyan, respectively. The regions lacking electron density are depicted by dashed lines. The interface between the CP and TM regions is boxed, and the residues in G-loop (the loop between the H and I strands of one subunit), proximal to those in the TM region of the same and adjacent subunits within 4 Å, are depicted by stick models. (Right, upper) Enlarged view of the interface between the CP and TM regions boxed in the left panel. The residue numbers are labeled according to those of GIRK1. (Right, lower) Schematic drawing of the interface between the CP and TM regions of the chimeric channel, shown in (b). The residue pairs within 4 Å of each other are connected by green lines. The following are the shortest distances between the inter- and intra-subunit residues: intersubunit, 4.0 Å (Phe72 (CE2) –Thr305 (CG2)), 4.0 Å (Thr73 (OG1) –Thr305 (OG1)), 3.7 Å (Ile182 (CG2) –Thr305 (O)), and 2.6 Å (Gln186 (NE2)–Thr305 (O)); and intrasubunit, 3.4 Å (Ser185 (O)–Thr306 (OG1)), 3.1 Å (Ser185 (O)–Met308 (CG)), 3.7 Å (Gln186 (NE2)–Met308 (CE)), 3.6 Å (Pro187 (CB)–Val303 (CG2)), and 3.8 Å (Pro187 (CG)–Cys310 (CB)). The positions of the Cα atoms are depicted as red dots, except for those of the residues with significant chemical shift perturbations, which are indicated as yellow dots.

Figure 10

Fig. 11.Direct interactions between GIRKCP-L and Gαi3, revealed by TCS. (a) Mapping of the affected residues in the TCS experiment from GIRKCP-L to Gαi3 is shown on the Gα structure (PDB code 1GIA). The affected residues are colored red on the Gα structure, whereas residues with no data, including proline residues, are colored black. The αA, αB, α2, and α3 helices are colored green. (b) Mapping of the affected residues in the TCS experiment from Gαi3 to GIRKCP-L on a single subunit of the GIRKCP-L tetramer. Residues 371–386 are depicted by gray tubes. The affected residues are colored red on the GIRKCP-L structure, whereas residues with no data, including proline residues, are colored black. The αA helix is colored green in the ribbon diagrams. (c) Mapping of the affected residues (colored red) in the TCS experiment on two adjacent subunits of a GIRKCP-L tetramer (white and gray), viewed from the outside (left) and the inside (right) of the tetramer.

Figure 11

Fig. 12.PRE results of the interaction between GIRKCP-L and Gαi3. Mapping of the affected residues in the PRE experiment using HexaIII-I82C-MTSL (a, left) and HexaIII-S153C-MTSL (b, left), respectively, on a single subunit of the GIRKCP-L structure. The affected residues are colored red. Proline residues and residues with no data are colored black. (Right) Mapping of the spin-labeled site of Gαi3 on the structure of Gα.

Figure 12

Fig. 13.Proposed model of Gα(GTP) and the cytoplasmic region of the GIRK complex. (a, Left) Two adjacent subunits of a GIRKCP-L tetramer, viewed from the inside of the tetramer, are depicted by a ribbon diagram, and a homology model of Gαi3 is shown in a surface representation. The nitrogen atoms of the GIRKCP-L residues identified in the TCS experiments, and the residues with PRE effects from the MTSL modification of I82C on the helical domain of Gαi3, are shown as red and magenta balls, respectively. The α2/α3 residues of Gαi3 identified in the TCS experiments are colored blue. (Center and right) Binding model of Gαi3(GTP) and the cytoplasmic region of GIRK1 (PDB code 1N9P), obtained with the HADDOCK software. Only the two adjacent subunits of the GIRK tetramer are shown, from the inside of the tetramer. (b) Model of the Gα-GIRK-Gβγ ternary complex. (Left) The nitrogen atoms of the Gβγ-binding residues on GIRK1 are mapped as magenta balls on the complex model of Gα and the GIRK tetramer. (Right) Ternary complex model of Gα-GIRK-Gβγ. Gβ and Gγ are colored magenta and violet, respectively. The residues involved in the intermolecular interactions between Gα and Gβγ, within a distance of 4 Å in the Gαi1(GDP)β1γ2 (PDB code 1GP2) structure, are colored orange. (c) GIRK- and RGS-binding sites on Gα. The GIRK-binding residues identified in this study are colored red, and the residues involved in the intermolecular interaction between Gα and RGS, within a distance of 4 Å in the Gαi1(GDP/Mg2+/AlF4−) – RGS4 complex structure (PDB code 1AGR), are colored green. The overlapping residues, Lys209 and His213, are colored blue.

Figure 13

Fig. 14.Identification of the oligomer interface of CCL5 by CS experiments. Surface representation of the CCL5 tetramer model. The residues involved in the dimer–dimer contacts (residues 26–29, 33, 34, 66, and 67), and the monomer–monomer contacts (residues 6–10) are colored red and orange, respectively.

Figure 14

Fig. 15.Identification of the fibril seeds-binding site in β2-microglobulin. (a) Scheme of two-step fibril formation by β2m. (b) Profiles of TCS experiments performed in the presence (blue bars) and the absence (black diamonds) of fibril. The intensity ratios of signals with and without RF irradiation (Isat/Inon-sat) are plotted. The red circle indicates the residues that showed significant R2 relaxation dispersion.

Figure 15

Fig. 16.CXCR4–SDF-1 interaction revealed by methyl-TCS experiments. (a) Results of the methyl-TCS experiments performed in the absence of AMD3100. The SDF-1 structure (PDB code 1VMC) is shown in a CPK representation. Isoleucine, leucine, and valine residues are colored according to the reduction ratios (RR) originating from the specific interactions, as follows. Red: RR>0.150. Light red: 0.150>RR>0.110. Orange: 0.110>RR>0.100. Cyan: RR<0.100. For the leucine and valine residues, the larger RR of their two methyl resonances was utilized. (b) Results of the methyl-TCS experiments performed in the presence of AMD3100. Red: RR>0.125. Light red: 0.125>RR>0.100. Orange: 0.100>RR>0.075. Cyan: RR<0.075. The other details are the same as in (a). (c) Schematic diagram of the two-step mechanism for the SDF-1–CXCR4 interaction. The 1st-step interaction between the SDF-1 β-sheet, 50s-loop, and N-loop, and the CXCR4 extracellular region facilitates the rapid binding and efficient anchoring of SDF-1 on the extracellular side of CXCR4. The SDF-1 N-terminus is highly dynamic even in this state, which is used to search for the binding cavities buried within the TM helices. Consequently, the 2nd-step interaction between the SDF-1 N-terminus and the CXCR4 TM region occurs, and the SDF-1 N-terminus triggers the conformational changes in the CXCR4 TM to induce G-protein signaling.

Figure 16

Fig. 17.Interaction between CCR5–rHDL and MIP-1α variant. (a and b) Stability of the solubilized CCR5. Normalized SPR responses for 2D7 antibody binding to CCR5 in DDM micelles, immediately after solubilization (dotted line) and after a 24 h incubation at 4°C (solid line) are shown in (a). Responses were normalized for the amount of captured CCR5. Relative values of the responses for 2D7 antibody binding of CCR5 in DDM micelles (immediately after solubilization=100%) over time are shown in (b). (c) Schematic representation of the preparation of CCR5–rHDL. CCR5 embedded in Sf9 cell membranes was solubilized, immediately reconstituted into rHDL, and subsequently purified using the His-tag and the 1D4-tag in MSP and CCR5, respectively. (d) Normalized SPR responses for the binding of the 2D7 antibody to CCR5-rHDL, immediately after preparation (dotted line) and after a 24 h incubation at 4°C (solid line). Responses were normalized for the amount of captured CCR5-rHDL. (e) SPR analyses of the interaction between the MIP-1α variant and CCR5-rHDL. Overlay plots of the sensorgrams obtained for the interaction between 0.33 and 13.2 μM of the MIP-1α variant and the immobilized CCR5-rHDL. (f) Determination of the CCR5 binding interface on MIP-1α by methyl-TCS experiments. Mapping of the affected residues in the TCS experiment with CCR5-rHDL are colored orange on the MIP-1α structure (PDB code 1B53). Glu57, whose mutations were identified in SNPs involved in HIV-1 infection, is also colored red.

Figure 17

Fig. 18.Determination of the interface residues of Pc for cyt b6f or PSI by TCS. (a) Distribution of the hydrophobic and acidic patches in spinach Pc (PDB code 1YLB). The surface of Pc is transparent, and the copper atom and the ribbon diagram are simultaneously displayed. The residues in the hydrophobic and acidic patches that were proposed to be responsible for the electron transport in previous mutational analyses are labeled, and colored green and red, respectively. (b,g) TCS experiments with excess amounts of Pc relative to (b,c) PSI and cyt b6f embedded in thylakoid vesicles, (d,e) solubilized PSI, or (f,g) solubilized b6f. Panels (b), (d), and (f) are schematic diagrams of the experiments. Panels (c), (e), and (g) are maps of the residues affected by the rf-irradiation in the TCS experiments. The residues with signal intensity reduction ratios >0.3 and within the 0.2–0.3 range are colored red and pink, respectively. Proline residues and residues with intensity reductions that were not determined, because of low signal intensity or spectral overlap, are white. The surface of Pc is transparent, and the copper atom and the ribbon diagram are simultaneously displayed. The molecular diagrams were generated with Web Lab Viewer Pro (Molecular Simulations, Inc.).

Figure 18

Fig. 19.Schematic views of the interaction modes in the Pc–PSI and Pc–cyt b6f complexes.

Figure 19

Fig. 20.Interaction of CERT PH domain with PI4P-embedded membrane. (a) Ribbon representation of the CERT PH domain, with magnification of the basic groove. The side chains of the basic and aromatic residues in the basic groove and the protruding part of the β1/β2 region are displayed as blue and green sticks, respectively. (b) Electrostatic potential surface of the CERT PH domain. Negative and positive electrostatic surfaces are colored red and blue, respectively. (c) Mapping of the residues that were significantly perturbed by the titration of diC4–PI4P on the surface representation of the CERT PH domain structure. The side chains of the residues with Δδ>0.2 and 0.1–0.2 ppm chemical shift perturbation are indicated by red and orange surfaces, respectively. (d) Schematic representation of the TCS experiment using PI4P-embedded liposomes. The proton resonances originating from the lipid head group were saturated by radiofrequency irradiation, and this saturation was transferred to the residues in the CERT PH domain that were proximal to the PI4P-embedded liposome. (e) Mapping of the residues affected by the TCS on the surface of the CERT PH domain. The side chains of the residues with signal intensity reduction ratios >0.4 and 0.3–0.4 are indicated by red and orange surfaces, respectively. (f) Proposed mechanism of PH domain-mediated CERT translocation to the Golgi apparatus. I, Unbound state of the CERT PH domain. II, Weakly bound CERT PH domain. A non-specific electrostatic interaction occurs between the basic groove in the CERT PH domain and the surface of the phospholipid membrane. III, Orientation of the CERT PH domain for high affinity interaction. The specific high affinity interaction with the PI4P-embedded membrane is shown.

Figure 20

Fig. 21.Interaction of p47phox PX domain with PI(3,4)P2-embedded membrane. (a) Ribbon representation of the p47phox PX domain. The bound diC4–PI3P2 is displayed in a ball-and-stick representation. (b) Left: Ribbon representation of the p47phox PX domain, with mapping of residues displaying strong intensity reductions in the TCS experiment with PI(3,4)P2-containing liposomes. Right: Mapping of residues displaying strong intensity reductions in the TCS experiment with PI(3,4)P2-containing liposomes on the surface of the crystal structure of p47phox PX. Residues are color-coded according to their intensity reduction (IR), with red for strong (IR>0.3) and orange for moderate (0.25c) Schematic representation of the TCS experiment using PI(3,4)P2-embedded liposomes. The proton resonances originating from the lipid head group were saturated by radiofrequency irradiation, and this saturation was transferred to the residues in the p47phox PX domain that were proximal to the PI(3,4)P2-embedded liposome. (d) Mapping of residues displaying strong diC4–PI(3,4)P2-induced chemical shift perturbations onto a ribbon representation of the crystal structure of the p47phox PX domain. Normalized chemical shift changes were calculated based on the equation Δδ=((ΔδH)2+(ΔδN/5)2)1/2. Residues that showed strong (Δδ>0.2 ppm) and moderate (0.12 ppm<Δδ<0.2 ppm) normalized chemical shift changes are colored red and orange, respectively.

Figure 21

Fig. 22.Interaction of EEA1 FYVE domain with PI3P-embedded rHDL. (a) Schematic representation of the TCS experiment using PI3P-embedded rHDL. The proton resonances originating from the lipids were saturated by radiofrequency irradiation, and the saturation was transferred to the residues in the EEA1 FYVE domain that were proximal to the PI3P-embedded rHDL. (b) Mapping of the residues affected by the TCS on the surface of the EEA1 FYVE domain. Residues with differences in the reduction ratio (ΔRR) values larger than 0.10, and within the 0.06–0.10 range are indicated by red and orange surfaces, respectively. The ΔRR value was calculated by the following equation: ΔRR=RRPI3P–rHDL−RRPI-free–rHDL, where RRPI3P–rHDL and RRPI-free–rHDL were obtained from (Iunsat−Isat)/Iunsat in the presence of PI3P–rHDL and PI-free rHDL. (c) Model for the complex of EEA1 FYVE domain bound to PI3P-embedded in the membrane. The residues on the EEA1 FYVE domain affected in both the TCS and PRE (green), only in TCS (blue), and only in PRE (yellow) experiments are mapped on the surface of EEA1 FYVE domain. The Ins(1,3)P2 bound to EEA1 FYVE is depicted by a stick model, and the residues that were not analyzed in either TCS or PRE experiments are colored black. Lipid molecules within the membrane are schematically shown, with the phosphate and choline head groups depicted as orange and blue spheres, respectively.

Figure 22

Fig. 23.Determination of binding sites in CG1 for endogenous MTs by in-cell TCS. (a) Schematic representation of the method to introduce the target proteins into mammalian cells by SLO. (b) Schematic of the gel-encapsulated bioreactor system for the long-term in-cell NMR measurements. (c) Time-dependent changes of intracellular ATP concentration monitored by 31P NMR signals of the β P atom of ATP, with (red) and without (blue) the bioreactor. The medium injection was stopped at 5 h (arrow). The error bar is based on the signal-to-noise ratio for each spectrum. (d) The results of the in-cell TCS experiments, mapped on the CG1 structure (PDB code, 2CP5) according to the intensity reduction ratio. Red and light green spheres indicate intensity reduction ratios greater or less than 0.5, respectively, and black spheres represent methyl groups for which TCS data were unavailable. (e) The putative MT-binding region of CG1 indicated by a previous in vitro study. Hydrophobic and basic residues are colored green and blue, respectively.