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. 2014 Nov;21(11):962-968.
doi: 10.1038/nsmb.2899. Epub 2014 Oct 5.

Structure and mechanism of action of the BRCA2 breast cancer tumor suppressor

Affiliations

Structure and mechanism of action of the BRCA2 breast cancer tumor suppressor

Taha Shahid et al. Nat Struct Mol Biol. 2014 Nov.

Abstract

Mutations in BRCA2 increase susceptibility to breast, ovarian and prostate cancers. The product of human BRCA2, BRCA2 protein, has a key role in the repair of DNA double-strand breaks and interstrand cross-links by RAD51-mediated homologous recombination. Here, we present a biochemical and structural characterization of full-length (3,418 amino acid) BRCA2, alone and in complex with RAD51. We show that BRCA2 facilitates nucleation of RAD51 filaments at multiple sites on single-stranded DNA. Three-dimensional EM reconstructions revealed that BRCA2 exists as a dimer and that two oppositely oriented sets of RAD51 molecules bind the dimer. Single-stranded DNA binds along the long axis of BRCA2, such that only one set of RAD51 monomers can form a productive complex with DNA and establish filament formation. Our data define the molecular mechanism by which this tumor suppressor facilitates RAD51-mediated homologous-recombinational repair.

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Figures

Figure 1
Figure 1. 3D reconstruction of BRCA2 and identification of domains
(a) Surface view of the 3D reconstruction. Two halves were colored yellow and cyan, representing two potential monomers although the exact boundary is unknown. (b-g) Antibody labeling against C-terminal Flag tag (b-d) and BRC repeats (e-g). In (b) and (e), raw particles with antibody are circled. (c) and (f) Reprojections along the same orientations of (b) and (e). (d) and (g) 3D reconstructions viewed along the same directions as (b) and (e), with antibody locations represented by spheres. (h) and (i) Top and side views of BRCA2 with antibody locations colored (Flag tag- blue, BRC – magenta). Magnification bars in all single particle images represent 100 Å.
Figure 2
Figure 2. 3D reconstruction of BRCA2-RAD51 complex
(a) and (b) Side and top surface views of the 3D reconstruction. (c) Antibody labeling against RAD51. Left: individual particles with antibody circled. Middle: corresponding reprojections from the BRCA2-RAD51 reconstruction. Right: surface view along the same direction with antibody locations indicated with spheres. (d) Cylinders representing antibody locations defined from individual particles (upper). These intersect at the density regions on the outer rim connecting the two halves (lower, orange surface).
Figure 3
Figure 3. RAD51 binding to BRCA2
(a) Overlay of BRCA2 dimer (yellow and cyan) and BRCA2-RAD51 (pink mesh) highlighting the differences in their shape. (b) Rearranged BRCA2 dimer fitted into the BRCA2-RAD51 complex. (c) as in (b). Four RAD51 monomers (orange ribbon) were fitted into the additional density in BRCA2-RAD51 not accounted for by BRCA2 density. (d) Four RAD51 monomers, arranged as in filaments. (e) Histogram of mass measurement of BRCA2-RAD51 complex using STEM, showing peaks at 800 kD and 1200 kD, corresponding to BRCA2 dimer and BRA2 dimer binding to 8-10 RAD51.
Figure 4
Figure 4. ssDNA binding of BRCA2 and BRCA2-RAD51 complex
(a) Gel-shift assay showing the binding of BRCA2 to 5′-32P-labeled ssDNA substrates ranging from 20 to 100 nt. DNA was detected by autoradiography. (b) Images of individual particles of BRCA2 bound to gapped DNA (duplex arms are indicated in orange). Magnification bars represent 100 Å. (c-e) Electron microscopic visualization of RAD51-ssDNA filaments, BRCA2-ssDNA complexes, and BRCA2-RAD51-ssDNA complexes, as indicated. (f) Localization of BRCA2 in BRCA2-RAD51-ssDNA complexes by immunogold labeling. (g) Visualization of BRCA2-RAD51 filaments formed with 5′-gold particle labeled ssDNA. Magnification bars represent 100 nm.
Figure 5
Figure 5. Nucleation of RAD51 filaments by BRCA2
(a) and (b) Effect of BRCA2 on the number of RAD51-ssDNA nucleation events, as determined by electron microscopy. Inserts show enlargements of RAD51 filaments. (c-d) Quantification of RAD51-ssDNA filament length (c) and nucleation events (d) in the presence (blue) or absence (orange) of BRCA2, as determined by measurement of images shown in Fig. 4c (n = 314) and 4e (n = 332), n = number of RAD51 filaments. In total, 204 (RAD51-ssDNA) and 149 (BRCA2-RAD51-ssDNA) randomly collected grid areas were quantified. P-values (P < 0.0001) were determined using a two-tailed t test, error bars represent SD. (e) BRCA2-RAD51-ssDNA complexes visualized as multiple distinct filament nucleation sites on the same ssDNA molecule (arrowed). Magnification bars represent 100 nm.
Figure 6
Figure 6. A proposed mode of action for BRCA2 in RAD51 filament nucleation
(a) Crystal structure of RPA bound to 30 nt ssDNA, showing a compact configuration and bending of the ssDNA into a U-shape. DNA binding domains of BRCA2 could adapt similar conformations. The polarity of the ssDNA is indicated. The two RPA molecules, related by 2-fold symmetry, could represent the DNA binding domains in the BRCA2 dimer as indicated below. (b) The DNA binding domains (1,2,3,4) of BRCA2 are depicted in similar conformations as those shown for RPA in (a), such that ssDNA could simultaneously bind to domains 3-4 (OB2-OB3) at the 5′ end (left hand side) of one BRCA2 monomer while domains 1-2 (alpha-helical domain and OB1) at the 3′ end (right hand side) of the second monomer. Two sets of RAD51 molecules bind the BRCA2 dimer in opposing directions. Only one set can be productive in ssDNA binding. (c) Model for filament formation and elongation using multiple BRCA2-RAD51 nucleation sites with BRCA2 acting as a molecular chaperone for RAD51.

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