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Single-molecule FRET for virology: 20 years of insight into protein structure and dynamics

Published online by Cambridge University Press:  18 May 2023

Danielle Groves
Affiliation:
Warwick Medical School, University of Warwick, Coventry, UK
Christof Hepp
Affiliation:
Biological Physics Research Group, Department of Physics, University of Oxford, Oxford, UK Kavli Institute for Nanoscience Discovery, New Biochemistry Building, University of Oxford, Oxford, UK
Achillefs N. Kapanidis*
Affiliation:
Biological Physics Research Group, Department of Physics, University of Oxford, Oxford, UK Kavli Institute for Nanoscience Discovery, New Biochemistry Building, University of Oxford, Oxford, UK
Nicole C. Robb*
Affiliation:
Warwick Medical School, University of Warwick, Coventry, UK Kavli Institute for Nanoscience Discovery, New Biochemistry Building, University of Oxford, Oxford, UK
*
Corresponding authors: Achillefs N. Kapanidis and Nicole C. Robb; Emails: kapanidis@physics.ox.ac.uk; Nicole.Robb@warwick.ac.uk
Corresponding authors: Achillefs N. Kapanidis and Nicole C. Robb; Emails: kapanidis@physics.ox.ac.uk; Nicole.Robb@warwick.ac.uk
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Abstract

Although viral protein structure and replication mechanisms have been explored extensively with X-ray crystallography, cryo-electron microscopy, and population imaging studies, these methods are often not able to distinguish dynamic conformational changes in real time. Single-molecule fluorescence resonance energy transfer (smFRET) offers unique insights into interactions and states that may be missed in ensemble studies, such as nucleic acid or protein structure, and conformational transitions during folding, receptor–ligand interactions, and fusion. We discuss the application of smFRET to the study of viral protein conformational dynamics, with a particular focus on viral glycoprotein dynamics, viral helicases, proteins involved in HIV reverse transcription, and the influenza RNA polymerase. smFRET experiments have played a crucial role in deciphering conformational changes in these processes, emphasising the importance of smFRET as a tool to help elucidate the life cycle of viral pathogens and identify key anti-viral targets.

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Type
Review
Creative Commons
Creative Common License - CCCreative Common License - BY
This is an Open Access article, distributed under the terms of the Creative Commons Attribution licence (http://creativecommons.org/licenses/by/4.0), which permits unrestricted re-use, distribution and reproduction, provided the original article is properly cited.
Copyright
© The Author(s), 2023. Published by Cambridge University Press
Figure 0

Figure 1. The theory of smFRET. a) A biomolecule that switches between two conformations. A short distance between a donor (green) and acceptor (red) fluorophore gives rise to high FRET, while little or no FRET is observed when the fluorophores are far apart. b) The relationship between the inter-fluorophore distance, R, and the FRET efficiency, E. The Förster radius R0 refers to the distance at which the FRET efficiency is 50%. c) A schematic of confocal smFRET measurements on freely diffusing molecules. d) Example histogram of confocal data generated by plotting the FRET efficiency versus the stoichiometry for each fluorescent burst of photons. Stoichiometry is calculated using alternating-laser excitation (Kapanidis et al., 2004), which allows identification of doubly labelled molecules. e) A schematic of total internal reflection fluorescence (TIRF) smFRET measurements on immobilised molecules. When light strikes the glass-water interface at a sufficiently high angle - greater than the critical angle (Ɵc) - it is totally internally reflected. When the angle of incidence is greater than the critical angle light in totally internally reflected. f) Example time trace showing FRET from an immobilised molecule. Clear anti-correlations in donor–acceptor fluorescence are characteristic of FRET dynamics.

Figure 1

Figure 2. Viral glycoproteins have a common architecture. Viral surface glycoproteins often have similar trimer structures. Each protomer consists of a surface facing binding domain and a transmembrane fusion subunit. a) HIV-1 Env contains 3 protomers of gp120 (receptor-binding subunit) and gp41 (transmembrane subunit); left: crystal structure of BG505 SOSIP gp140 mimic of the Env ectodomain (pdb: 4NCO)16 where each protomer is distinguished by shades of purple, right: schematic. b) The full crystalised H5N1 influenza HA and schematic illustrate a trimer of HA1 and HA2 domains (pdb: 2FK0) (Stevens et al., 2006). c) The ectodomain of the Ebola GP without the mucin-like domain consists of a trimer of heterodimers GP1 and GP2 (pdb: 7SWD) (Milligan et al., 2022). d) The SARS-CoV-2 Spike protein also contains a trimer of S1 (receptor-binding domain) and S2 (fusion) subunits (pdb: 6VYB) (Walls et al., 2020).

Figure 2

Figure 3. smFRET analysis reveals conformational states and dynamics of HIV-1 Env. a) Model of Env-mediated membrane fusion. ‘State 1’ (a low-FRET closed state) is thought to represent unliganded Env, while CD4 binding induces a partially open high-FRET conformation (‘state 2’), followed by coreceptor binding which results in the transition to a stabilised open Env, where all 3 protomers are bound to CD4 (intermediate-FRET ‘state 3’). Following CD4 activation fusion of the viral and cellular membranes occurs, leading to virus entry. b) State 1 can also transition into a fourth state (‘state 2A’), representing an off-path semi-open conformation that is highly vulnerable to antibody-dependent cellular cytotoxicity (ADCC). Adapted from (Bruel and Schwartz, 2019).

Figure 3

Figure 4. Schematic model of SARS-CoV-2 spike protein dynamics during ACE2 binding. The spike protein is a trimer consisting of an S1 receptor-binding domain (RBD) and an S2 membrane fusion subunit. S1 binds to the cellular receptor ACE2. smFRET experiments suggest a model whereby the spike transitions from a closed form where all 3 RBDs are facing downwards (FRET ~0.5) to a pre-fusion conformation in which 1 or 2 of the RBDs are rotated to face upwards (intermediate-FRET ~0.3) to a fusion structure where all 3 RBDs face upwards towards ACE2 (FRET ~0.1) (Lu et al., 2020). An off-pathway high-FRET (~0.8) conformation was also observed, which was suggested to aid immune evasion (Lu et al., 2020).

Figure 4

Figure 5. smFRET insights into translocation of the NS3 helicase. a) Structure of NS3 (pdb: 1CU1). The complex consists of the helicase domain (blue), a protease domain (orange), and small viral protein NS4A (cyan), which is needed for protease functionality and membrane binding. b) smFRET was used to demonstrate NS3-mediated repetitive looping on DNA. In the model, NS3 binds at the 5′ partial duplex junction and starts to translocate along the single-stranded DNA until it reaches the 5′ end where a donor dye is positioned. Once NS3 reaches the end, it snaps back to the duplex junction and re-initiates translocation (Lin et al., 2017).

Figure 5

Figure 6. smFRET methodology to investigate the effect of the HIV-1 nucleocapsid (NC) on the stability, conformations, and reactivity of transactivation response (TAR) elements. a) Immobilised TAR DNA with FRET labels (Cy3 on the 5′ end; Cy5 on the 3′ end) and loop structures (L1-L4). ‘B’: Biotin label for surface attachment, ‘C’: closed conformation, ‘Y’: open conformation. The distance between the FRET labels changes upon NC addition, favouring state ‘Y’ (Cosa et al., 2004). b) Experiment on the structural effect of NC on a TAR DNA–RNA duplex (Wang et al., 2009).TAR RNA and DNA anneal in the presence of NC. By washing with buffer, NC is removed from the duplex.

Figure 6

Figure 7. smFRET assay for probing the orientational dynamics of the HIV-1 reverse transcriptase (RT). a) The structure of HIV-1 RT bound to a DNA–DNA substrate (pdb: 1N6Q). RT is a dimer composed of the p66 and p51 (magenta) subunits; p66 contains the DNA polymerase (comprising the fingers (‘F’ cyan), thumb and palm domains (both blue)) and an RNase H subdomain (yellow). Labelling sites for Cy3 are highlighted by green circles. b) smFRET experiments using DNA/DNA duplex templates labelled with Cy5 were used to assess the binding orientation of RT, which suggested that RT binds DNA with the RNase H domain close to the 5′ terminus of the primer. c) Similar to panel (b) but with DNA/RNA duplexes, which suggested that the binding orientation on the RNA primer was the opposite to that on the DNA primer (Liu et al., 2008, 2010; Abbondanzieri et al., 2008).

Figure 7

Figure 8. Insights into influenza replication initiation from smFRET. a) Structural model of the influenza RNAP (PDB code 5MSG) bound to vRNA in a pre-initiation state where the 3′ vRNA is located on the outer surface of the RNAP, or an initiation state where the 3′ vRNA enters the RNAP active site (Robb et al., 2016). b) Model of pre-initiation, initiation, and elongation states on a vRNA template. Upon RNAP binding, the vRNA promoter exists in equilibrium between a pre-initiation state in which the 3′ RNA terminus is bound on the RNAP surface, and an initiation state in which the 3′ RNA is bound in the active site. In the presence of NTPs, the 3′ RNA starts to translocate through the active site during RNA synthesis, resulting in destabilisation of the duplex region. Insights from smFRET experiments are highlighted in red text (Robb et al., 2016). c) Model of initiation states on a cRNA template. Unlike the vRNA promoter, the cRNA promoter exhibited very limited dynamics, in part due to the longer length of the 3′ template strand of the cRNA which allows the cRNA template strand to reach further into the active site (Robb et al., 2019).