DNAmediateddisassemblyofhRad51and hRad52
proteins andrecruitmentofhRad51tossDNAby hRad52
Vasundhara M. Navadgi, Ashish Shukla, Rahul Kumar Vempati and Basuthkar J. Rao
Department of Biological Sciences, Tata Institute of Fundamental Research, Mumbai, India
Human Rad51 protein (hRad51), a homologue of
Escherichia coli RecA performs the fundamental role
of homologous pairing and strand exchange during
homologous recombination and double-strand break
repair [1,2]. Rad51 and Rad52 colocalize in distinct
nuclear foci in response toDNA damage [3]. Yeast
rad52 mutants show extensive degradation of the
DNA double-strand break ends suggesting that Rad52
is critically involved in stable maintenance of chromo-
somal integrity [4]. Cytological studies indicate that
Rad52 is required for Rad51 foci formation during
meiosis [5] and chromatin immunoprecipitation assays
demonstrated the requirement of Rad52 for association
of yeast Rad51 to HO induced double strand break
site at the MATa locus in vivo [6,7]. Biochemically,
Rad52 stimulates the strand exchange activity of
Rad51 [8–10] and is shown to displace Replication
Protein A (RPA) [11,12] and stabilize the Rad51-
single-stranded (ssDNA) filament [13].
hRad51 andhRad52 form ring-shaped structures
like other recombination proteins RecA, RecT, human
Dmc1 and b protein from bacteriophage k [14–18].
Rad51 and RecA bind DNA as helical filaments
whereas their meiosis specific homologue Dmc1 and
archaeal recombinase, RadA proteins, form stacked
octameric rings on DNA in the absence of ATP and as
helical filaments in the presence of ATP [18–20]. The
crystal structure of Pyrococcus furiosus Rad51 reveals
that it forms a biheptameric ring [21]. High-resolution
crystal structural description of human Rad51, human
Rad52 and human Dmc1 has delineated the complex-
ity of homologous-pairing as well as the inter-subunit
interaction domains [18,21–24]. Structural studies with
both Rad51 and RecA suggest two distinct oligomeric
states of these proteins: rings and DNA-bound helical
forms [21,25]. Light scattering studies on RecA assem-
bly have suggested that under some solution conditions
free protein filament assembly effectively competes
with RecA assembly on ssDNA [26,27]. This property
of RecA seems to be evolutionarily conserved as
archaeal RadA also forms long helical filaments even
in the absence ofDNAand the protein assembles into
Keywords
DNA binding; homologous
recombination;oligomerization; Rad51;
Rad52
Correspondence
B.J. Rao, Department of Biological
Sciences, Tata Institute of Fundamental
Research, Homi Bhabha Road, Colaba,
Mumbai 400 005, India
Fax: +91 22 22782606 ⁄ 22782255
Tel: +91 22 22804545 Extn: 2606
(Received 1 October 2005, accepted
10 November 2005)
doi:10.1111/j.1742-4658.2005.05058.x
Purified human Rad51 and Rad52 proteins exhibit multiple oligomeric
states, in vitro. Single-stranded DNA (ssDNA) renders high molecular
weight aggregates of both proteins into smaller and soluble forms that
include even the monomers. Consequently, these proteins that have a pro-
pensity to interact with each other’s higher order forms by themselves, start
interacting with monomeric forms in the presence of ssDNA, presumably
reflecting the steps of protein assembly on DNA. In the same conditions,
DNA binding assays reveal hRad52-mediated recruitmentofhRad51 on
ssDNA. Put together, these studies hint at DNA-induced disassembly of
higher-order forms of Rad51 and Rad52 proteins as steps that precede
protein assembly during hRad51 presynapsis on DNA, in vitro.
Abbreviations
ATPcS, Adenosine 5¢-O-(3-thiotriphosphate); hRad51, human Rad51; hRad52, human Rad52; ssDNA, single-stranded DNA.
FEBS Journal 273 (2006) 199–207 ª 2005 The Authors Journal compilation ª 2005 FEBS 199
shorter and thicker nucleoprotein filaments when
ssDNA is added [28]. Tumour suppressors BRCA2
and p53 interact with the oligomerization domain of
Rad51 [24,29,30], and RPA is shown to inhibit the
higher order self association ofhRad52 rings [31] sug-
gesting that oligomerization of Rad51 and Rad52 is
regulated by other molecules to control their activity.
In this work, we have studied the oligomeric states
of hRad51andhRad52 in the presence and absence of
ssDNA. Our studies indicate that human Rad51, like
its bacterial homologue RecA exists in multiple aggre-
gation states [14,32]. DNA seems to dissociate the
higher order structures of both hRad51and hRad52.
hRad52 interacts specifically with higher oligomeric
states ofhRad51 in the absence of DNA, but with
hRad51 monomers when ssDNA is present. These
results are rationalized through a model where we pro-
pose that the interaction between hRad52and hRad51
monomers in the presence ofDNA might be related to
the steps of protein recruitment during hRad51 pre-
synapsis on ssDNA.
Results and discussion
hRad51 is a 37-kDa protein whereas hRad52 is a
55-kDa protein. Both of the proteins are known to
exist in oligomeric forms [15,20–23]. Here, we describe
the changes associated with the aggregation states of
hRad51 andhRad52 in the presence of 121-mer
ssDNA andhRad52mediated assembly of the
ssDNA–hRad51 complex. The changes in the protein
aggregation states were monitored by three different
readouts: native PAGE, centrifugation assays, and
analyses of hydrodynamic radii changes by dynamic
light scattering (DLS).
ssDNA-induced disassemblyof higher oligomeric
forms of hRad51
A fixed amount ofhRad51 (7.5 lm) was incubated
with ssDNA (0–22 lm) as described in Experimental
procedures and analysed by native gel electrophoresis
(Fig. 1A) and centrifugation assays (Fig. 1B). hRad51
migrated as a highly aggregated form (several hun-
dred kDa complexes) that barely entered into the
gel. Only a faint signal was detectable at the mono-
mer position (based on the mobility of standard
molecular weight markers) (lane 1, Fig. 1A). In the
presence of ssDNA, the level of monomers increased
(compare lanes 2–4 with lane 1, Fig. 1A). In these
gel conditions, even though ssDNAand hRad51
were migrating close to each other, there was enough
difference between the two to discern an increase in
the monomer level. Using 5¢
32
P-labelled ssDNA, we
mapped the positions of protein–DNA complexes in
this gel system (data not shown; compare Fig. 4).
Based on this comparison, the protein–DNA com-
plexes that entered into the gel mapped to the posi-
tion indicated by the asterisk in Fig. 1A. The
ssDNA mediated increase in monomer level remained
essentially unchanged in the presence of nucleotide
cofactors ADP, ATP or ATPcS (compare lanes 6–8,
10–12, 14–16 with of 2–4, respectively, Fig. 1A).
However, the signals associated with protein–DNA
complexes (position indicated by asterisk) appear to
diminish and that of higher oligomeric forms that
enter into the gel (as labelled in Fig. 1A) appear to
increase in sets containing nucleotide cofactors. This
trend is consistent with ATP induced effects reported
earlier, where much larger forms ofhRad51 are dis-
aggregated into oligomeric complexes equivalent to
3–8 protein monomers [33].
In order to trap the oligomeric forms that do not
enter the gel, we used centrifugation assays. Following
the assay, we recovered a fraction of the protein in the
pellet (lane 1, Fig. 1B) and the remainder in the super-
natant (lane 5). In the presence of ssDNA, the protein
fraction that was pelletable became fully soluble, as no
signal was recovered in the pellet (lanes 2–4). This
effect suggested that addition ofssDNA renders pellet-
able forms of protein aggregates into smaller and more
soluble forms. Consequently, the resultant ssDNA–
protein complexes formed (see Fig. 5) are soluble as
they are recovered in the supernatant fraction of the
assay. Both of the assays suggested that addition of
ssDNA facilitates significant level of disaggregation in
hRad51.
To reconfirm the DNAmediated disaggregation of
hRad51, we analysed the hydrodynamic radii (R
h
)of
hRad51 as a function ofssDNA using dynamic light
scattering studies. Monomodal distribution of R
h
val-
ues (in nm) vs. intensity is plotted as histograms where
the observed R
h
distribution (10–80 nm range) is
grouped into categories (a–d) for easy comparison
between samples (Fig. 1C). It is to be noted that under
these conditions, buffer components as well as naked
ssDNA in solution hardly scatter any light, thereby
yielding no detectable DLS signal in this R
h
range.
The free protein showed a distribution of R
h
ranging
from 30 to 80 nm sizes (grouped as b, c and d in
Fig. 1C). Upon ssDNA addition, the distribution shif-
ted towards smaller R
h
values (10–20 nm size, grouped
as a) with a concomitant drop in the levels of larger
ones (grouped as c and d). As a result, at the highest
concentration of DNA, the distribution revealed a high
preponderance of smaller protein particles and reduced
Disassembly andrecruitmentofhRad51andhRad52proteins V. M. Navadgi et al.
200 FEBS Journal 273 (2006) 199–207 ª 2005 The Authors Journal compilation ª 2005 FEBS
level of larger ones, thereby corroborating the effect of
ssDNA induced disaggregation of hRad51.
DNA/ATP induced changes in hRad51
We tested whether DNA induced disaggregation of
protein leads to changes in the pattern of limited pro-
teolysis ofhRad51by trypsin, where the extent of pro-
tease attacks is a function of both conformational as
well as overall organizational changes in the target
protein system. Comparison revealed that hRad51 is
relatively more protected in the presence of ssDNA
than in its absence (compare lanes 4 and 5 with lanes
2 and 3, respectively, Fig. 1D). This effect might
arise either due to steric hindrance imparted by ssDNA
binding or to changes in protein configuration ⁄
conformation following ssDNA binding or a combina-
tion of both. ATP has been shown to induce changes
in hRad51 such that accessibility to protease attacks is
altered [33]. We observed that ATP induced change
was somewhat different from that induced by ssDNA
(compare lane 3 with lane 4). Note the increase in
small sized proteolytic product (indicated by arrow-
head 3) with the concurrent decrease in large fragment
(indicated by arrowhead 1) in the ATP lane (lane 3).
However compared to the control (lane 2), presence of
ATP results in an increase in the larger fragment (indi-
cated by arrowhead 2, lane 3). The appearance of large
fragments in the presence of ATP (compare lane 3
with lane 2) or ssDNA (compare lanes 4 and 5 with
lanes 2and 3, respectively) hint that these binders
induce discernable changes in hRad51 organization.
A
B
CD
Fig. 1. DNA induced solublization of Human Rad51 protein. (A) Native gel assay to visualize oligomeric state of hRad51. hRad51 (7.5 lM)
was incubated with 0, 7.5, 15 and 22 l
M oligo PUC+ in buffer containing 30 mM Tris ⁄ HCl pH 7.5, 1 mM MgCl
2
,20mM KCl and 1 mM DTT
either in the absence of nucleotide cofactors (lanes 1–4) or in the presence of 1 m
M ADP (lanes 5–8), 1 mM ATP (lanes 9–12), 1 mM ATPcS
(lanes 13–16) and analysed by native PAGE ( 6% acrylamide) followed by silver staining. (B) Centrifugation assay. hRad51 was incubated
with varying concentrations ofDNA as described in (A) in the absence of any nucleotide cofactors and later subjected to centrifugation and
the resulting pellet and supernatant were analysed by SDS PAGE followed by silver staining. (C) Dynamic light scattering to study the effect
of DNA on hydrodynamic radius (R
h
) of hRad51. hRad51 (1 lM) was incubated with 0, 1, 3, 4 and 5 l M of oligo PUC+ (in the absence of any
nucleotide cofactor) followed by the measurement of hydrodynamic radius of the protein molecules. Monomodal distribution of R
h
values (in
nm) vs. intensity is plotted as histograms where groupings a–d depicts 10–80 nm range distribution. (D) Partial proteolysis experiment to
analyse DNA induced conformational changes on hRad51 protein. hRad51 (25 l
M) was incubated in binding buffer in the absence (lanes 2
and 3) or presence of 75 l
M ssDNA (lanes 4 and 5) and 1 mM ATP (lanes 3 and 5) for 1 h at 37 °C and then subjected to partial digestion
with trypsin (Sigma, Munich, Germany) (50 lgÆmL
)1
) for 1 min. The reaction was quenched by Laemmli buffer and analysed by SDS ⁄ PAGE
(20% acrylamide), followed by silver staining. Lane 6 consists of only ssDNA.
V. M. Navadgi et al. DisassemblyandrecruitmentofhRad51andhRad52 proteins
FEBS Journal 273 (2006) 199–207 ª 2005 The Authors Journal compilation ª 2005 FEBS 201
DNA-induced disassemblyof higher oligomeric
forms of hRad52
A similar effect of disaggregation byssDNA was also
observed with hRad52 protein. In the absence of
ssDNA, hRad52 protein appeared to be so highly
aggregated that it hardly entered into the gel (lane 5,
Fig. 2A) and was mostly in the pellet fraction following
a centrifugation assay (lane 1, Fig. 2B). Aggregation of
hRad52 appears to be highly salt sensitive and in the
present assay conditions with 20 mm KCl, the protein
remains highly aggregated. The addition ofssDNA ren-
dered the protein into forms that not only entered into
the gel, but also migrated as the monomeric form. This
effect was further evidenced by the complete recovery
of the protein in the supernatant fraction, as a function
of added ssDNA (lanes 7 and 8, Fig. 2B).
Protein aggregation/disaggregation changes vs.
ionic effects
In order to assess whether ssDNA induced diaggrega-
tion ofhRad52 ⁄ hRad51proteins reflects anionic effects
contributed by ssDNA, we tested another relevant anion
ATP and compared with its counter-cation Mg
2+
in the
same assays. A titration with varying ATP concentra-
tions had no effect on hRad52 sedimentation properties.
Most protein that was in pellet fraction of the assay
remained so even after the addition of 5 mm ATP
(Fig. 3A), suggesting that anionic ATP had no effect on
protein aggregation. As a control, we compared hRad51
protein in the same assay. ATP, a known modulator of
hRad51 function, caused protein disaggregation, as evi-
denced by significant recovery ofhRad51 in the super-
natant fraction of the assay (Fig. 3A). This effect is
consistent with an increase in the level of higher oligo-
meric forms of protein that enter into the gel due to
ATP (compare lane 9 with lane 1, Fig. 1A). However,
unlike with ssDNA where the entire protein fraction
was rendered soluble by 7.5–15 lm nucleotide concen-
tration ofDNA (Fig. 1B), only a fraction of protein
sample became soluble with as high as 5 mm ATP
(Fig. 3A), suggesting that the effects were distinct and
not related to general ionic conditions in the assay. This
conclusion was further strengthened when the protein
aggregation was tested as a function of Mg
2+
. In the
same assay, Mg
2+
titration rendered hRad52 highly sol-
uble, whereas hRad51 was highly insoluble (Fig. 3B). A
significant fraction of pelletable hRad52 was recovered
in the supernatant fraction following Mg
2+
treatment,
indicating that the protein was subject to solublization
not only byssDNA (Fig. 2A and B), but also by Mg
2+
(Fig. 3B), a common effect facilitated by oppositely
charged ionic species. On the other hand, hRad51 exhib-
ited a behaviour opposite to that ofhRad52by under-
going high level of aggregation, which is akin to that
of E. coli RecA aggregation induced by Mg
2+
observed
earlier [32]. These studies indicate that hRad52 ⁄ hRad51
disaggregation ⁄ aggregation properties assayed here
reflect genuine modulations rendered byssDNA ⁄
ATP ⁄ Mg
2+
, etc. rather than nonspecific ionic effects in
solution conditions.
hRad52 protein selectively interacts with higher
oligomeric forms ofhRad51 in the absence of
DNA
As seen in earlier experiment, hRad51 exhibited
multiple oligomeric forms (lane 1, Fig. 4A) whereas
hRad52 was in an aggregated state and hardly entered
into the gel (lane 5, Fig. 4A). hRad51 (10 lm) was
A
B
Fig. 2. DNA induced solublization of Human Rad52 protein. (A)
Native gel to visualize oligomeric state of hRad52. hRad52 (10 l
M)
was incubated with 0, 10, 20 and 30 l
M (lanes 1–4) oligo PUC+ in
buffer containing 30 m
M Tris pH 7.5, 1 mM MgCl
2
,20mM KCl and
1m
M DTT and analysed by native PAGE (6% acrylamide) followed
by silver staining. (B) Centrifugation assay. hRad52 was incubated
with varying concentrations ofDNA as described in (A) and later
subjected to centrifugation and the samples analysed by SDS
PAGE followed by silver staining.
Disassembly andrecruitmentofhRad51andhRad52proteins V. M. Navadgi et al.
202 FEBS Journal 273 (2006) 199–207 ª 2005 The Authors Journal compilation ª 2005 FEBS
incubated with increasing concentrations of hRad52
(0–10 lm) in the absence of ssDNA; this led to a grad-
ual and selective disappearance of higher oligomeric
states of hRad51, whereas the smaller forms of
hRad51 were largely unaffected (lanes 2–4, Fig. 4A).
At the highest concentration of hRad52, most of
higher oligomeric forms ofhRad51 were converted
into large complexes that did not enter the gel
(Fig. 4A). These complexes were present in the pellet
fraction in a centrifugation assay (data not shown).
Earlier studies had shown that yeast Rad51 and Rad52
also form large complexes that elute much earlier than
individual proteins in gel filtration chromatography
experiment [34].
Recruitment ofhRad51tossDNA targets: the role
of hRad52
We addressed this issue by analysing the status of sol-
uble forms ofhRad51 protein as a function of increas-
ing hRad52 protein in the presence of ssDNA. As
expected, native gel analyses revealed DNA (25 lm)
induced ‘monomerization’ ofhRad51 protein (10 lm)
(compare lanes 2 and 7 with lanes 1 and 6, respect-
ively, Fig. 4B). In this native gel assay conditions, the
‘monomerized’ form ofhRad52 essentially comigrates
with that ofhRad51 monomer (compare lanes 2 and 7
with lane 11, Fig. 4B). Interestingly, addition of
hRad52 protein led to a measurable depletion rather
than a cumulative increase in the monomer signal of
both proteins (compare lanes 5 and 10 with 2–4 and
7–9, respectively, Fig. 4B). This was concomitantly
associated with the rise of a signal at high molecular
weight region in the gel (at asterisk position in lanes
5 and 10). This was observed both with and without
ATP.
In parallel, we studied protein binding to 5¢
32
P-
labelled ssDNAof 121-mer (used in the previous
experiments) and analysed the complex formation by
native gel electrophoresis. Increasing concentration of
hRad51 led to the generation of protein–DNA com-
plexes. The complexes formed at low protein concen-
trations were presumably smaller in size and hence
entered into the gel (small protein–DNA complexes,
Fig. 5) and those at high protein concentrations were
much larger and retained at the top of the gel (large
protein–DNA complexes). Moreover, there appeared
to be a precursor–product relationship between the
small and large complexes, where the appearance of
large complexes was concomitantly associated with the
disappearance of small ones. To assess the role of
hRad52 on hRad51 binding, we performed gel shift
analyses of complexes at a limiting amount of hRad51
(1 lm) in the presence of increasing levels of hRad52.
The control experiment revealed that in these condi-
tions, the hRad52 protein by itself showed only margi-
nal binding (lanes 10 and 11). In the set containing
hRad51 protein, addition ofhRad52 protein converted
free DNA as well as ‘small protein–DNA complexes’
(lane 7) into much ‘larger complexes’ (lanes 8 and 9,
Fig. 5). Comparison of gel-shifted complexes in lanes 8
and 9 with those in lanes 3, 4 and 5 reveals that the
A
B
Fig. 3. Aggregation ⁄ disaggregation ofhRad51 ⁄ hRad52proteins vs. ionic effects. (A) hRad51 (10 lM) andhRad52 (10 lM) were incubated in
buffer (30 m
M Tris ⁄ HCl pH 7.5, 1 mM MgCl
2
,20mM KCl, 1 mM DTT) containing varying concentrations of ATP, for 30 min at 37 °C, followed
by centrifugation and analyses of pellet ⁄ supernatant fractions by SDS PAGE. (B) In separate sets, hRad51 (10 l
M) or hRad52 (10 lM) was
incubated in buffer (30 m
M Tris ⁄ HCl pH 7.5, 20 mM KCl, 1 mM DTT) containing varying concentrations of MgCl
2
for 30 min at 37 °C, fol-
lowed by centrifugation and analyses of pellet ⁄ supernatant fractions by SDS PAGE.
V. M. Navadgi et al. DisassemblyandrecruitmentofhRad51andhRad52 proteins
FEBS Journal 273 (2006) 199–207 ª 2005 The Authors Journal compilation ª 2005 FEBS 203
presence ofhRad52 renders much better binding of
hRad51 tossDNA even at lower concentrations of the
latter, thereby implying that hRad52 plays a role in
the recruitmentofhRad51to ssDNA.
The results described in this study help us to under-
stand the transitions associated with the oligomeric
states ofhRad51andhRad52proteins in the presence
of ssDNAand relate them to their DNA binding
activity. The observation that hRad51 protein in its
DNA-unbound form, exits in higher oligomeric forms,
poses a mechanistic challenge as to how such struc-
tures transform into right-handed helical filaments
during ⁄ following DNA binding. Whether higher oligo-
meric states of protein are directly recruited to DNA
or much smaller forms of the protein are generated
prior to active assembly, is an open question. Our
results suggest that transient contacts ofDNA strands
with either protein create an effect of ‘protein disaggre-
gation’. It is important to note that all the effects
uncovered in the present study are from in vitro analy-
ses and it is not clear how these effects may relate to
the situations in vivo, the mechanistic description of
which is not very clear at present.
A large body of experimental evidence available in
the literature suggests that Rad52 functions as a stimu-
lator of Rad51 mediated recombination [8–10], and it
has been postulated that these effects of Rad52 are lar-
gely due to its role as a recruiter of Rad51 to DNA.
Our study extends this hypothesis further by showing
that the recruitmentof hRad51, mediatedby hRad52,
might encompass steps where the two proteins together
undergo large-scale disaggregation in the presence of
ssDNA, followed by interaction between the two at
the level of monomeric forms, leading to an active faci-
litated assembly of protein–DNA complexes. We want
to end with a note of caution: we believe that purified
hRad52 ⁄ hRad51 system is a highly complex organiza-
tion and is difficult to probe by high-resolution analy-
ses at its equilibrium state. We believe that the simple
biochemical readouts used in the current study have
A
B
Fig. 4. Effect ofDNA on the interaction of hRad51–hRad52. (A)
hRad52 selectively interacts with higher oligomeric forms of
hRad51 in the absence of DNA. Rad51 (10 l
M) was incubated with
0, 2.5, 5.0 and 10 l
M (lanes 1–4) ofhRad52 in binding buffer (see
Experimental procedures) containing 50 m
M KCl at 37 °C for 1 h
and analysed by native PAGE (6% acrylamide) followed by silver
staining. Lane 5 contains 10 l
M hRad52 alone. (B) hRad52 interacts
with hRad51 monomers in the presence of DNA. hRad51 (10 l
M)
was incubated with 0, 2, 4 and 10 l
M (lanes 2–5 and 7–10) of
hRad52 in the presence of 25 l
M oligo PUC+ in binding buffer con-
taining 50 m
M KCl either in the absence (lane 1–5) or presence of
1m
M ATP (lane 6–10) and analysed by native PAGE (6% acryl-
amide) followed by silver staining. Lane 1 and 6 has hRad51
(10 l
M) without DNAand lane 11 had hRad52 (10 lM) with DNA.
The position of asterisk indicates the formation of large complex in
the presence of hRad51, hRad52and ssDNA.
Fig. 5. hRad51 binding tossDNA in the presence of hRad52.
32
P
labelled oligo PUC+ (1 l
M) was incubated with 0, 1, 2, 3, 6 lM
hRad51 (lanes 1–5) in the absence ofhRad52and 1 lM hRad51
with 0, 0.25 and 0.50 l
M hRad52 (lanes 6–9). Lanes 10 and 11 con-
tain DNA samples incubated with hRad52 alone. Samples were
resolved by native PAGE (6% acrylamide) and the gel was scanned
using a PhosphorImager.
Disassembly andrecruitmentofhRad51andhRad52proteins V. M. Navadgi et al.
204 FEBS Journal 273 (2006) 199–207 ª 2005 The Authors Journal compilation ª 2005 FEBS
provided some useful clues on important organiza-
tional changes that ensue in protein during their
recruitment to ssDNA. However the results are limited
by the resolution limits imposed by the assays.
Experimental procedures
Materials
T4 polynucleotide kinase, ATP, ADP were from Amersham
life Sciences (Piscataway, NJ, USA). ATPcS was obtained
from Roche-Molecular Biochemicals (Mannheim, Germany).
Ni–NTA agarose beads were from Qiagen (Hiden,
Germany). Oligonucleotides were from DNA technology
(Aarhus, Denmark).
DNA substrate
The sequence of the 121-mer ssDNA substrate
PUC+, used in this study was: 5¢—TTTCCCAGTCACGA
CGTTGTAAAACGACGGCCAGTGCCAAGCTTGCAT
GCCTGCAGGTCGACTCTAGAGGATCCCCGGGTAC
CGAGCTCGAATTCGTAATCATGGTCATAGCTGTTT
CCT—3¢. DNA concentrations are expressed as total nucleo-
tide concentrations. The oligonucleotide used in the current
study was more than 90% pure, as assessed by 8 m urea-
containing denaturing PAGE. End labelling of oligonucleo-
tides was carried out as described earlier [35].
Purification ofhRad51and hRad52
The hRad52 overexpressing clone was obtained from Steve
West (Cancer Research UK, London, UK, earlier ICRF,
London, UK). Protein was purified as described [35]. The
hRad51 overexpression plasmid was obtained from Hitoshi
Kurumizaka (Wako, Saitama, Japan) and purified as
described [36].
Centrifugation assay
Reaction mixtures containing DNAand protein (as des-
cribed in the figure legends) were incubated in binding
buffer [30 mm Tris ⁄ HCl pH 7.5, 1 mm MgCl
2
,1mm di-
thiothreitol (DTT)] at 37 °C for 1 h. Samples were subjec-
ted to centrifugation at 14 000 r.p.m. for 10 min. The
supernatant and pellet were separated and heated in
Laemmli buffer at 90 °C for 10 min and analysed by
SDS ⁄ PAGE (10% acrylamide), followed by silver staining.
Native polyacrylamide gel electrophoresis
of proteins
Varying concentrations of Rad51, Rad52 andDNA were
incubated in specific conditions (as described in the figure
legends) at 37 °C for 1 h. Samples were subjected to native
PAGE (6% acrylamide) in TBE buffer at 200 V for 3 h at
room temperature (25 °C). Subsequently the proteins were
visualized by silver staining.
DNA binding by gel-shift assays
Labelled DNA substrate was incubated with various con-
centrations ofhRad51andhRad52 (as described in the fig-
ure legends) in a binding buffer (30 mm Tris ⁄ HCl pH 7.5,
1mm MgCl
2
,1mm DTT, 100 lgÆmL
)1
BSA) at 37 °C for
1 h. DNA–protein complexes were analysed by native
PAGE (6% acrylamide) in TBE buffer at 200 V for 3 h at
room temperature (25 °C). The radioactivity in the gels
was quantified by ImageQuant software on a Phosphor-
Imager (Molecular Dynamics, Piscataway, NJ, USA).
Dynamic light scattering
Measurement of hydrodynamic radius
Dynamic light scattering experiments were performed at
22 °C on a DynaPro-MS800 dynamic light scattering instru-
ment (Protein Solutions Inc., VA, USA). Buffer solutions
were filtered carefully through 20-nm filters (Whatman Ano-
disc 13) to remove dust particles. The particulate matter, if
any, in the DNAand protein samples, were removed by sub-
jecting the samples to centrifugation (14 000 r.p.m) at 4 °C
for 10 min. hRad51 (1 lm) was incubated with different con-
centrations ofDNA (as mentioned in the legends) in a 50-lL
reaction buffer (30 mm Tris ⁄ HCl pH 7.5, 1 mm MgCl
2
,
1mm DTT) in the absence of any nucleotide cofactor for 10–
15 min in a quartz cuvette followed by DLS analysis. It was
ascertained that the buffer system was free of particles as
reflected by very low R
h
(0.1–0.2 nm) values associated with
it. The data were analysed using Dynamics software, which
reported the hydrodynamic radii (R
h
) for monomodal distri-
butions as defined by a baseline from 0.9 to 1.001.
Acknowledgements
We thank Steve West, Cancer Research, UK, and
Hitoshi Kurumizaka, Japan for hRad52and hRad51
overexpression clones, respectively.
References
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. DNA mediated disassembly of hRad51 and hRad52
proteins and recruitment of hRad51 to ssDNA by hRad52
Vasundhara M. Navadgi,. with the aggregation states of
hRad51 and hRad52 in the presence of 121-mer
ssDNA and hRad52 mediated assembly of the
ssDNA hRad51 complex. The changes