Artigo Acesso aberto Revisado por pares

An induced fit mechanism regulates p53 DNA binding kinetics to confer sequence specificity

2011; Springer Nature; Volume: 30; Issue: 11 Linguagem: Inglês

10.1038/emboj.2011.127

ISSN

1460-2075

Autores

Tom J. Petty, Soheila Emamzadah, Lorenzo Costantino, Irina Petkova, Elena S. Stavridi, Jeffery G. Saven, Eric Vauthey, Thanos D. Halazonetis,

Tópico(s)

Epigenetics and DNA Methylation

Resumo

Article26 April 2011free access An induced fit mechanism regulates p53 DNA binding kinetics to confer sequence specificity Tom J Petty Tom J Petty Department of Molecular Biology, University of Geneva, Geneva, Switzerland Genomics and Computational Biology Graduate Group, University of Pennsylvania, Philadelphia, PA, USA Search for more papers by this author Soheila Emamzadah Soheila Emamzadah Department of Molecular Biology, University of Geneva, Geneva, Switzerland Search for more papers by this author Lorenzo Costantino Lorenzo Costantino Department of Molecular Biology, University of Geneva, Geneva, Switzerland Search for more papers by this author Irina Petkova Irina Petkova Department of Physical Chemistry, University of Geneva, Geneva, Switzerland Search for more papers by this author Elena S Stavridi Elena S Stavridi The Wistar Institute, Philadelphia, PA, USAPresent address: Merck-Serono, Geneva, Switzerland Search for more papers by this author Jeffery G Saven Jeffery G Saven Department of Chemistry, University of Pennsylvania, Philadelphia, PA, USA Search for more papers by this author Eric Vauthey Eric Vauthey Department of Physical Chemistry, University of Geneva, Geneva, Switzerland Search for more papers by this author Thanos D Halazonetis Corresponding Author Thanos D Halazonetis Department of Molecular Biology, University of Geneva, Geneva, Switzerland Department of Biochemistry, University of Geneva, Geneva, Switzerland Search for more papers by this author Tom J Petty Tom J Petty Department of Molecular Biology, University of Geneva, Geneva, Switzerland Genomics and Computational Biology Graduate Group, University of Pennsylvania, Philadelphia, PA, USA Search for more papers by this author Soheila Emamzadah Soheila Emamzadah Department of Molecular Biology, University of Geneva, Geneva, Switzerland Search for more papers by this author Lorenzo Costantino Lorenzo Costantino Department of Molecular Biology, University of Geneva, Geneva, Switzerland Search for more papers by this author Irina Petkova Irina Petkova Department of Physical Chemistry, University of Geneva, Geneva, Switzerland Search for more papers by this author Elena S Stavridi Elena S Stavridi The Wistar Institute, Philadelphia, PA, USAPresent address: Merck-Serono, Geneva, Switzerland Search for more papers by this author Jeffery G Saven Jeffery G Saven Department of Chemistry, University of Pennsylvania, Philadelphia, PA, USA Search for more papers by this author Eric Vauthey Eric Vauthey Department of Physical Chemistry, University of Geneva, Geneva, Switzerland Search for more papers by this author Thanos D Halazonetis Corresponding Author Thanos D Halazonetis Department of Molecular Biology, University of Geneva, Geneva, Switzerland Department of Biochemistry, University of Geneva, Geneva, Switzerland Search for more papers by this author Author Information Tom J Petty1,2,‡, Soheila Emamzadah1,‡, Lorenzo Costantino1,‡, Irina Petkova3, Elena S Stavridi4, Jeffery G Saven5, Eric Vauthey3 and Thanos D Halazonetis 1,6 1Department of Molecular Biology, University of Geneva, Geneva, Switzerland 2Genomics and Computational Biology Graduate Group, University of Pennsylvania, Philadelphia, PA, USA 3Department of Physical Chemistry, University of Geneva, Geneva, Switzerland 4The Wistar Institute, Philadelphia, PA, USA 5Department of Chemistry, University of Pennsylvania, Philadelphia, PA, USA 6Department of Biochemistry, University of Geneva, Geneva, Switzerland ‡These authors contributed equally to this work *Corresponding author. Department of Molecular Biology, University of Geneva, 30 Quai Ernest-Ansermet, Geneva 1205, Switzerland. Tel.: +41 22 379 6112; Fax: +41 22 379 6868; E-mail: [email protected] The EMBO Journal (2011)30:2167-2176https://doi.org/10.1038/emboj.2011.127 There is a Have you seen? (June 2011) associated with this Article. PDFDownload PDF of article text and main figures. Peer ReviewDownload a summary of the editorial decision process including editorial decision letters, reviewer comments and author responses to feedback. ToolsAdd to favoritesDownload CitationsTrack CitationsPermissions ShareFacebookTwitterLinked InMendeleyWechatReddit Figures & Info The p53 tumour suppressor gene, the most frequently mutated gene in human cancer, encodes a transcription factor that contains sequence-specific DNA binding and homo-tetramerization domains. Interestingly, the affinities of p53 for specific and non-specific DNA sites differ by only one order of magnitude, making it hard to understand how this protein recognizes its specific DNA targets in vivo. We describe here the structure of a p53 polypeptide containing both the DNA binding and oligomerization domains in complex with DNA. The structure reveals that sequence-specific DNA binding proceeds via an induced fit mechanism that involves a conformational switch in loop L1 of the p53 DNA binding domain. Analysis of loop L1 mutants demonstrated that the conformational switch allows DNA binding off-rates to be regulated independently of affinities. These results may explain the universal prevalence of conformational switching in sequence-specific DNA binding proteins and suggest that proteins like p53 rely more on differences in binding off-rates, than on differences in affinities, to recognize their specific DNA sites. Introduction The most frequently mutated gene in human cancer is p53 (Hollstein et al, 1991; Kan et al, 2010), a gene encoding a sequence-specific DNA binding protein (Kern et al, 1991). The p53 protein is activated in response to DNA damage and then enhances transcription of genes that induce cell-cycle arrest, apoptosis or senescence (Kastan et al, 1991; Kuerbitz et al, 1992; Vogelstein et al, 2000). To explain the high frequency of p53 mutations in human cancer, it has been proposed that activation of oncogenes in precancerous lesions leads to DNA damage, which in turn curtails, in a p53-dependent manner, the macroscopic growth of the lesion (Bartkova et al, 2005; Gorgoulis et al, 2005). According to this model, inactivation of p53 is an important step in the progression of precancerous lesions to cancer, because it allows cancer cells to proliferate despite the presence of oncogene-induced DNA damage (Halazonetis et al, 2008). Given the central role of the p53 protein in human cancer, it is not surprising that significant effort has been devoted towards elucidating its function and structure at the molecular level. These studies have revealed that the full-length p53 protein contains two independently folding domains: a sequence-specific DNA binding domain at the centre of the protein and a homo-tetramerization domain towards the C-terminus (Vogelstein et al, 2000). In addition, p53 contains three unstructured regions: an N-terminal transactivation domain, a linker between the DNA binding and oligomerization domains and a C-terminal basic region (Joerger and Fersht, 2008). Several three-dimensional structures of the DNA binding domain of p53 have been determined both in the presence of specific DNA and in the absence of DNA (Cho et al, 1994; Ho et al, 2006; Malecka et al, 2009; Chen et al, 2010; Kitayner et al, 2006, 2010). All these structures encompass only the DNA binding domain. The most recent structures are derived from crystals containing four DNA binding domains in complex with specific DNA, thereby potentially recapitulating how full-length p53 tetramers recognize DNA (Malecka et al, 2009; Chen et al, 2010; Kitayner et al, 2010). With the exception of one structure, in which the p53 DNA binding domains had been chemically crosslinked to DNA (Malecka et al, 2009), the structures show that sequence-specific DNA binding is not accompanied by conformational changes within the p53 DNA binding domain (Cho et al, 1994; Ho et al, 2006; Chen et al, 2010; Kitayner et al, 2006, 2010). Yet, in the context of practically every other sequence-specific DNA binding protein characterized to date, the interaction with DNA is accompanied by conformational changes (Frankel and Kim, 1991; Alber, 1993; Spolar and Record, 1994). The significance of these conformational changes is not well understood, but their universal prevalence suggests that they may have an important role and raises the question why p53 is an exception. The DNA binding domain of p53 is monomeric in solution and has micromolar affinity for DNA (Weinberg et al, 2005). Because of this, except for the crosslinked p53–DNA complex, all the other studied p53–DNA complexes assembled during crystallization, implying that crystal packing interactions have contributed to their formation and, hence, to their structure. In contrast, p53 polypeptides that encompass both the DNA binding and oligomerization domains have nanomolar affinity for sequence-specific DNA and form stable protein–DNA complexes in solution (Weinberg et al, 2005). We envisioned, therefore, that the three-dimensional structures of such complexes would be much less likely to be affected by crystal packing interactions. We describe here structures of a multidomain p53 oligomer in the presence and absence of DNA. The structures reveal a conformational switch in loop L1, when p53 binds to specific DNA. Analysis of loop L1 mutants further shows that the conformational switch alters the kinetic properties of p53 DNA binding, allowing binding off-rates to be regulated independently of affinities. Since conformational switching is a characteristic of practically all sequence-specific DNA binding proteins (Frankel and Kim, 1991; Alber, 1993; Spolar and Record, 1994), our findings may be broadly relevant. Results Crystallization of a thermostable multidomain p53 protein Our initial attempts to express p53 polypeptides that contained both the DNA binding and oligomerization domains in a soluble form were unsuccessful. To address this problem, we introduced stabilizing amino-acid substitutions in the DNA binding domain of human p53, which, in its wild-type form, has a very low melting temperature (Bullock et al, 1997). The designed substitutions targeted non-conserved residues away from the DNA binding surface and, generally, sampled residues from the repertoire present at that position in p53 proteins from other species (Soussi and May, 1996). The goal of these substitutions was to maximize the contribution of the hydrophobic effect to protein folding. One substitution, Arg209 to Pro, was designed computationally (Zhu et al, 2004). After many rounds of mutagenesis and functional testing, we obtained a stabilized (ST) human p53 DNA binding domain that had the same DNA binding specificity as wild-type p53 and was functional in cells (Figures 1, 2A and B; Supplementary Figures S1–S6). Figure 1.Development of a stabilized human p53 protein. Stabilized proteins were developed via an iterative process of protein design and functional testing allowing the retention of substitutions that enhanced stability. About a hundred generations of stabilized proteins were generated, but, for brevity, only seven generations (ST1–ST7) are presented. The amino-acid substitutions present in the stabilized mutants are shown in Supplementary Figure S3. (A) Functional assay employed for the design of mutants ST1–ST5. Full-length wild-type human p53 and the stabilized mutants ST1–ST5 were translated in vitro using a rabbit reticulocyte lysate transcription/translation system (Promega Corporation). The proteins were then diluted in DNA binding buffer, heated at the indicated temperature for 10 min, returned to room temperature and assayed for binding to [32P]-labelled oligonucleotide BC (Supplementary Figure S1). (B) Assay employed for the design of mutants ST6–ST7. Proteins consisting of residues 94–358 of human p53 with an internal deletion of residues 292–321, containing stabilizing amino-acid substitutions in their DNA binding domains (ST6 or ST7), were expressed in E. coli. The soluble fraction of the E. coli lysate (Input, Inp) was heated for 10 min at the indicated temperature and the fraction that remained soluble was subjected to SDS–polyacrylamide gel electrophoresis and stained with Coomassie Brilliant Blue. (C) List of amino-acid substitutions, using the single letter amino-acid code, present in the DNA binding domain of the stabilized protein ST7 (hereafter referred to as ST). Download figure Download PowerPoint Figure 2.Overall three-dimensional structure of a multidomain p53 oligomer with and without bound DNA. (A) Sequence of the oligonucleotide, containing four contiguous pentamer repeats (a–d), that was crystallized in complex with DNA. (B) DNA binding specificity of the p53CR2 protein, as examined by an electrophoresis mobility shift assay using an oligonucleotide containing a high affinity binding site (BC; Supplementary Figure S1) and variants thereof that differ from BC by having the indicated bases at positions 1, 2, 3, 4 or 5 of the pentamer repeats. The first letter in the name of the variants refers to the base introduced in repeats a and c and the second letter to the base introduced in repeats b and d; − indicates that no substitution was made. (C) Overall three-dimensional structure of p53CR1 in the absence of DNA. The two subunits are labelled A and B. H2, helix 2 of the DNA binding domain; OLIG, oligomerization domain. (D) Overall three-dimensional structure of two p53CR2 dimers bound to DNA. The p53 subunits are labelled A–D. The DNA binding domain of subunit B has the same orientation as the DNA binding domain of subunit A of p53CR1 in panel (C). The DNA has complementary overhangs at each end and formed a pseudo-continuous double helix in the crystal. (E) The structure of the p53CR2–DNA complex rotated by 90o relative to panel (D). The arrows indicate the linkers between the DNA binding and oligomerization domains. Download figure Download PowerPoint For crystallization, we expressed a p53 polypeptide lacking the unstructured N-terminal and C-terminal ends of the protein and most of the linker between the DNA binding and oligomerization domains. Further, two amino-acid substitutions were introduced in the tetramerization domain to convert it to a dimerization domain (Davison et al, 2001). Three p53 proteins modified in this way were studied; they are referred to as p53CR1, p53CR2 and p53CR3 and have deletions of 30, 29 and 28 residues, respectively, in the linker between the DNA binding and oligomerization domains (Supplementary Figure S6). The three-dimensional structure of p53CR1 in the absence of DNA was determined at a resolution of 2.1 Å (Supplementary Table 1). As predicted, the protein crystallized as a dimer (Figure 2C). The stabilized DNA binding domains adopted the same conformation as the wild-type DNA binding domain (Cho et al, 1994). The dimerization domain also adopted the same conformation as the half wild-type tetramerization domain (Lee et al, 1994; Clore et al, 1995; Jeffrey et al, 1995; Davison et al, 2001). The DNA binding domains of the dimer did not interact with one another and it appears that their orientation relative to each other was dictated by crystal packing contacts. The p53CR2 and p53CR3 proteins formed stable complexes with DNA oligonucleotides containing consensus p53 binding sites (Supplementary Figure S7), allowing their three-dimensional structures with DNA to be determined at resolutions of 2.4 and 3.2 Å, respectively (Supplementary Table 1). The two structures were essentially identical (Supplementary Figure S8) and so the description will focus on the higher resolution p53CR2–DNA structure. The overall structure shows two p53CR2 dimers—having in total four DNA binding domains—bound to double-stranded DNA (Figure 2D and E). The DNA molecule contains four contiguous pentamer repeats, which we named a, b, c and d, reflecting their 5′ to 3′ order (Figure 2A). The major groove of each pentamer repeat is recognized by one p53 subunit, which bears the same label (A, B, C and D) as the repeat it contacts. The structure can recapitulate well how a full-length p53 tetramer would bind DNA. Unlike p53CR2, full-length p53 has long linkers between the DNA binding and oligomerization domains, allowing the oligomerization domains of all four subunits to interact with each other (Figure 2E). Validation of the structure While the overall structure of the p53CR2–DNA complex appears grossly similar to the recently described structures of four p53 DNA binding domains in complex with DNA (Malecka et al, 2009; Chen et al, 2010; Kitayner et al, 2010), none of the previous structures can be superimposed on the p53CR2–DNA structure or on each other (Supplementary Figure S9). One of the several differences between the various structures is the intersubunit interface between the DNA binding domains recognizing parallel non-consecutive pentamer repeats, for example, domains B and D. Two main areas of interaction are evident at this interface in the p53CR2–DNA structure (Figure 3A and B). One area, near the bound DNA, is dominated by hydrogen bonds involving Thr123, Thr140, Glu198 and Gly199 from one subunit and Ser94, Ser96, Gln167 and Thr170 from the other subunit. The second area, away from the bound DNA, involves Val225, Gly226, Asp228 from one subunit and Ser99, Lys101, Tyr103, Leu264 and Arg267 from the other subunit. Figure 3.Functional analysis of the p53–p53 contacts at the parallel intersubunit interface. (A) Structure of the p53CR2–DNA complex rotated by 180° relative to Figure 2D. Only parts of subunits B and D are shown. The side chains of the residues that form the parallel intersubunit interface are indicated. (B) Structure of the p53CR2–DNA complex rotated by 90o relative to panel (A). (C) Structure of the p53CR2–DNA complex showing only the N-terminal residues and first β-strand of the DNA binding domain of subunit D and the corresponding segments of the D subunits of the previously determined p53 tetramer structures (sa1, self-assembled 1, pdb 3KMD (Chen et al, 2010); sa2, self-assembled 2, pdb 3IGK (Kitayner et al, 2010); cl, crosslinked, pdb 3EXJ (Malecka et al, 2009)). The structures are superimposed on the basis of the B subunits and only the B subunit of the p53CR2–DNA complex is shown, for clarity. The side chain of Tyr103 (Y103) of all structures and the side chain of one possible phenylalanine rotamer at position 226 (F226) of subunit B are also shown. The orientation is the same as in panel (B). (D) Structure of the p53CR2–DNA complex showing the two other possible rotamers of phenylalanine at position 226 (F226) of subunit B. The orientation is the same as in panel (A). (E) Transcriptional activity of full-length p53 proteins containing the stabilized DNA binding domain and no additional substitutions (wt) or the following substitutions, as indicated: Gly226 to Phe (F226); Arg267 to Ser (S267); the double mutant (F226/S267); or the tumour-derived mutant Arg248 to Gln (Q248). Oligonucleotide BC has contiguous pentamer repeats; oligonucleotide BC.S10 has a 10 base pair insertion between repeats b and c (Supplementary Figure S1). Mean values and standard deviations from three independent experiments are shown. All p53 proteins were expressed at equal levels (Supplementary Figure S10). Download figure Download PowerPoint This second area of interaction is unique to the p53CR2–DNA structure among all the previously described p53 tetramer–DNA structures (Figure 3C; Supplementary Figure S9). Gly226 appears critical for this interface, because glycine's small side chain permits the two subunits to come close to each other. We modelled the common rotamers of phenylalanine at this position. All these rotamers were incompatible with the p53CR2–DNA structure, as they overlapped with the side chains of either Arg267 or Tyr103 from the other subunit (Figure 3C and D). Yet, they were compatible with all the previously determined p53 tetramer structures, which are characterized by larger intersubunit distances (Figure 3C; Supplementary Figure S9). As predicted by the p53CR2–DNA structure, the Gly226 to Phe substitution compromised the ability of full-length p53 to activate transcription from a binding site containing contiguous pentamer repeats and, importantly, substitution of Arg267 with serine acted as a second-site revertant (Figure 3E; Supplementary Figure S10). In contrast, the Gly226 to Phe substitution did not compromise the transcriptional activity of p53 from a DNA site with a 10 base pair insertion between pentamer repeats b and c. This insertion moves p53 domains B and D away from each other and should make p53 tolerant to interface substitutions, as, indeed, was the case. Thus, second-site revertant mutagenesis analysis of the transcriptional activity of full-length p53 in human cells supports the p53CR2–DNA structure described here and not any one of the other previously determined p53 tetramer-DNA structures. DNA binding-induced conformational switch of loop L1 Contrary to the previously determined p53–DNA structures, we observed a conformational switch in loop L1 upon DNA binding. In the subunits contacting the inner repeats (repeats b and c; Figure 2A), loop L1 adopted an extended conformation that was similar to the conformation seen in the absence of DNA and in the previously determined self-assembled p53–DNA structures (Figure 4A; Supplementary Figure S11). In this conformation, Lys120 and Ser121 contacted the DNA. However, in the subunits contacting the outer repeats (repeats a and d), loop L1 adopted a recessed conformation and neither Lys120 nor Ser121 contacted the DNA; instead Arg283 from helix H2 made a DNA contact (Figure 4B). The recessed loop L1 conformation was similar to the one observed in the crosslinked p53 tetramer–DNA structure (Supplementary Figure S12; Malecka et al, 2009) and was also reminiscent of the loop L1 conformation observed in C. elegans p53 in the absence of DNA (Huyen et al, 2004). Figure 4.Conformational changes in p53 and DNA upon sequence-specific DNA binding. (A) The extended conformation of loop L1 of subunits B and C (subunit B is shown as an example). The contacts of residues Lys120 (K120), Ser121 (S121), Cys277 (C277) and Arg280 (R280) with DNA are shown. The side chain of Val122 (V122), which stabilizes the extended conformation of loop L1, is indicated. Bases are referred to by type (A, G, T, C), position in the pentamer repeats (1–5) and pentamer repeat labels (b, c), as shown in Figure 2A. H2, helix 2; L1, loop L1. (B) The recessed conformation of loop L1 of subunits A and D (subunit A is shown as an example). The contacts of residues Cys277 (C277), Arg280 (R280) and Arg283 (R283) with DNA are shown. The crystallographic symmetry-related DNA molecule at the bottom of the image is coloured blue. (C) C1′-C1′ vectors and helical axes for each base pair of the p53-bound DNA. All vectors are coloured according to the oligonucleotide sequence (as shown in Figure 2A). The orientation of the DNA is the same as in Figure 2D. The arrow indicates the DNA helical axis shift at the centre of the p53 binding site. (D) Comparison of the conformations of loop L1 of subunits A and B and of the adjacent DNA backbones. Subunit B and its neighbour DNA backbone are coloured yellow; subunit A and its neighbour DNA are coloured green; the crystallographic symmetry-related DNA next to subunit A is coloured blue. The backbone of an ideal B-form DNA is coloured red. The arrows indicate the 5′ to 3′ direction of each DNA strand. The orientation is the same as in panels (A), (B) and (C). (E) Same elements as shown in panel (D) viewed after a 90o rotation. Only a slab is shown corresponding to the DNA segment with darker colours in panel (D). Helix H2 (not shown) would be above the plane of the paper. Download figure Download PowerPoint In the crosslinked p53–DNA structure, the recessed conformation of loop L1 was present in all four subunits (Supplementary Figure S12) and was attributed to steric interference with the chemical crosslink (Malecka et al, 2009). However, in the p53–CR2 structure, the conformational switch of loop L1 was linked to a 3-Å shift of the DNA helical axis at the centre of the p53 DNA binding site (Figure 4C; Supplementary Figure S13). As a result of this shift, the DNA backbone was displaced away from loop L1 of p53 subunits B and C, providing space to accommodate the extended loop L1 in the major groove of the bound DNA (Figure 4D and E; Supplementary Figures S11 and S14). In contrast, at the edges of the p53 binding site, the DNA helical axis did not shift and loop L1 of subunits A and D adopted a recessed conformation to be able to accommodate to the standard B-form DNA (Figure 4D and E; Supplementary Figure S14). Effect of the loop L1 conformational switch on DNA binding kinetics The observed conformational changes in p53 and DNA in the p53CR2–DNA structure suggest that p53 binds DNA via an induced fit mechanism (Koshland, 1958). Induced fit, as compared with rigid body interactions, may not significantly affect binding affinities, but can have profound effects on binding kinetics (Pape et al, 1999; Johnson, 2008). To illustrate this, we first consider binding of p53 to DNA via a rigid body interaction. Under equilibrium conditions, the dissociation constant KD is equal to the off-rate constant koff divided by the on-rate constant kon (Figure 5A). In the rigid body interaction model, the on-rate constant would be determined by diffusion and electrostatic attraction/repulsion and would be the same irrespective of the DNA sequence (von Hippel and Berg, 1989; Johnson, 2008). Thus, for different DNAs, the off-rate constant would be proportional to the KD, reflecting the fact that high affinity interactions are characterized by long half-lives (Figure 5A). Figure 5.Loop L1 regulates p53 DNA binding off-rates. (A) Equations describing the formation of p53–DNA complexes via a rigid body interaction mechanism. KD, dissociation constant; koff, off-rate constant; kon, on-rate constant. (B) Equations describing the formation of p53–DNA complexes via an induced fit mechanism. p53 (in italics) indicates the DNA-bound conformation. koffo and kono, overall off-rate and on-rate constants, respectively. (C) Scatchard plots for binding of stabilized wild-type p53 (residues 79–393) to specific (sp) DNA (oligonucleotide ABC.4TT, Supplementary Figure S1) and non-specific (ns) DNA (oligonucleotide NS, Supplementary Figure S1) and of the stabilized tumour-derived mutant Gln284 (Q248) to specific DNA. The KD values are indicated in nM. The slope of the fitted lines is equal to −1/KD. v=[p53/DNA]/([p53/DNA]+[DNA]). (D) Plot of the natural logarithm of the concentration (lnC) of the complexes of wild-type p53 with fluorescent-specific (sp) and non-specific (ns) DNA versus time (in s). Excess non-fluorescent competitor DNA was added at time zero. The koff values, which are equal to the slope of the fitted lines, are indicated in s−1. (E) Scatchard plots for binding of stabilized wild-type and loop L1 p53 mutants (residues 79–393) to specific (sp) DNA (oligonucleotide ABC.4TT). F121, Phe121; S122, Ser122; F121/G122, Phe121/Gly122 double mutant. The KD values are indicated in nM. (F) Plot of the natural logarithm of the concentration (lnC) of the complexes of wild-type p53 and p53 loop L1 mutants with fluorescent-specific DNA versus time (in s). Excess non-fluorescent competitor DNA was added at time zero. The koff values are indicated in s−1. Download figure Download PowerPoint In the case of an induced fit mechanism, binding proceeds in two steps (Koshland, 1958). An initial interaction occurs without any conformational change, as described above for rigid body interactions, and then, in a second step, the initial interaction drives a conformational switch that allows a better fit between the protein and DNA (Figure 5B). The constant kon1 is determined by diffusion and electrostatic attraction/repulsion, whereas the constant kon2 is determined by the conformational switch (which may be different for different DNAs and for different p53 proteins; Johnson, 2008). If one considers macroscopic (overall) on-rate and off-rate constants, kono and koffo, respectively, to describe both steps of the reaction, then the dissociation constant KD equals koffo divided by kono (Figure 5B). But because kono depends partially on the conformational switch (which may be different for different DNAs and for different p53 proteins), the koffo values are not proportional to the KD values. Therefore, one can distinguish between rigid body interaction and induced fit mechanisms by measuring KD and koffo values for different p53–DNA complexes. DNA binding affinities of p53 under equilibrium conditions have been previously studied by fluorescence anisotropy; at physiological salt concentrations the reported dissociation constants for high affinity sites were in the range of 1.1–4.2 nM, whereas non-specific DNAs were bound with affinities in the range of 29.8–88.6 nM (Weinberg et al, 2004). The reported small differences in affinities for specific and non-specific DNAs is puzzling, since it makes it difficult to understand how human p53 identifies its specific target sites in a diploid genome containing six billion competing non-specific sites. To study the DNA binding properties of p53, we also relied on fluorescence anisotropy. We employed proteins that span residues 79–393 of human p53. These proteins contained the stabilized DNA binding domain (to prevent denaturation during the experiment). However, unlike the proteins used for crystallization, the proteins used for the DNA binding studies contained a wild-type tetramerization domain, an int

Referência(s)