DNA bending induced by high mobility group proteins studied by fluorescence resonance energy transfer.

The HMG domains of the chromosomal high mobility group proteins homologous to the vertebrate HMG1 and HMG2 proteins preferentially recognize distorted DNA structures. DNA binding also induces a substantial bend. Using fluorescence resonance energy transfer (FRET), we have determined the changes in the end-to-end distance consequent on the binding of selected insect counterparts of HMG1 to two DNA fragments, one of 18 bp containing a single dA(2) bulge and a second of 27 bp with two dA(2) bulges. The observed changes are consistent with overall bend angles for the complex of the single HMG domain with one bulge and of two domains with two bulges of approximately 90-100 degrees and approximately 180-200 degrees, respectively. The former value contrasts with an inferred value of 150 degrees reported by Heyduk et al. (1) for the bend induced by a single domain. We also observe that the induced bend angle is unaffected by the presence of the C-terminal acidic region. The DNA bend of approximately 95 degrees observed in the HMG domain complexes is similar in magnitude to that induced by the TATA-binding protein (80 degrees), each monomeric unit of the integration host factor (80 degrees), and the LEF-1 HMG domain (107 degrees). We suggest this value may represent a steric limitation on the extent of DNA bending induced by a single DNA-binding motif.     

The DNA bend angle and binding affinity of an HMG box increased by the presence of short terminal arms.

The HMG box of human LEF-1 (hLEF-1, formerly TCF1alpha) has been expressed in four forms: a parent box of 81 amino acids and constructs having either a 10 amino acid C-terminal extension, a 9 amino acid N-terminal extension, or both. These four species have been compared for DNA binding and bending ability using a 28 bp recognition sequence from the TCR alpha-chain enhancer. In the bending assay, whereas the parent box and that with the N-terminal extension bent the DNA by 57/58 degrees, the box extended at the C-terminus bent the DNA by 77/78 degrees, irrespective of the presence or absence of the N-terminal extension. A 6- fold increase in DNA affinity also resulted from addition of both terminal extensions. These observations redefine the functional boundaries of the HMG box. The structure of a mouse LEF-1/DNA complex recently published [Love et al. (1995) Nature 376, 791-795] implies that the higher DNA affinity and in particular the increased bend angle observed are consequences, at least in part, of the C-terminal extension spanning the major groove on the inside of the DNA bend.     

Interaction of human SRY protein with DNA: A molecular dynamics study

Molecular dynamics simulations have been conducted to study the interaction of human sex-determining region Y (hSRY) protein with DNA. For this purpose, simulations of the hSRY high mobility group (HMG) domain (hSRY-HMG) with and without its DNA target site, a DNA octamer, and the DNA octamer alone have been carried out, employing the NMR solution structure of hSRY-HMG–DNA complex as a starting model. Analyses of the simulation results demonstrated that the interaction between hSRY and DNA was hydrophobic, just a few hydrogen bonds and only one water molecule as hydrogen-bonding bridge were observed at the protein–DNA interface. These two hydrophobic cores in the hSRY-HMG domain were the physical basis of hSRY-HMG–DNA specific interaction. They not only maintained the stability of the complex, but also primarily caused the DNA deformation. The salt bridges formed between the positive-charged residues of hSRY and phosphate groups of DNA made the phosphate electroneutral, which was advantageous for the deformation of DNA and the formation of a stable complex. We predicted the structure of hSRY-HMG domain in the free state and found that both hSRY and DNA changed their conformations to achieve greater complementarity of geometries and properties during the binding process; that is, the protein increased the angle between its long and short arms to accommodate the DNA, and the DNA became bent severely to adapt to the protein, although the conformational change of DNA was more severe than that of the hSRY-HMG domain. The sequence specificity and the role of residue Met9 are also discussed. Proteins 31:417–433, 1998. © 1998 Wiley-Liss, Inc.     

Solution structure of an A-tract DNA bend

The solution structure of a DNA dodecamer d(GGCAAAAAACGG)/d(CCGTTTTTTGCC) containing an A-tract has been determined by NMR spectroscopy with residual dipolar couplings. The structure shows an overall helix axis bend of 19 degrees in a geometry consistent with solution and gel electrophoresis experiments. Fourteen degrees of the bending occurs in the GC regions flanking the A-tract. The remaining 5 degrees is spread evenly over its six AT base-pairs. The A-tract is characterized by decreasing minor groove width from the 5' to the 3' direction along the A strand. This is a result of propeller twist in the AT pairs and the increasing negative inclination of the adenine bases at the 3' side of the run of adenine bases. The four central thymine bases all have negative inclination throughout the A-tract with an average value of -6.1 degrees. Although this negative inclination makes the geometry of the A-tract different from all X-ray structures, the proton on N6 of adenine and the O4 of thymine one step down the helix are within distance to form bifurcated hydrogen bonds. The 5' bend of 4 degrees occurs at the junction between the GC flank and the A-tract through a combination of tilt and roll. The larger 3' bend, 10 degrees, occurs in two base steps: the first composed of tilt, -4.1 degrees, and the second a combination of tilt, -4.2 degrees, and roll, 6.0 degrees. This second step is a direct consequence of the change in inclination between an adjacent cytosine base, which has an inclination of -12 degrees, and the next base, a guanine, which has 3 degrees inclination. This bend is a combination of tilt and roll. The large change in inclination allows the formation of a hydrogen bond between the protons of N4 of the 3' cytosine and the O6 of the next 3' base, a guanine, stabilizing the roll component in the bend. These structural features differ from existing models for A-tract bends.For comparison, we also determined the structure of the control sequence, d(GGCAAGAAACGG)/d(CCGTTTCTTGCC), with an AT to GC transition in the center of the A-tract. This structure has no negative inclination in most of the bases within the A-tract, resulting in a bend of only 9 degrees. When ligated in phase, the control sequence has nearly normal mobility in gel electrophoresis experiments.     

Lrp, a major regulatory protein in Escherichia coli, bends DNA and can organize the assembly of a higher-order nucleoprotein structure.

Lrp (Leucine-responsive regulatory protein) is a global regulatory protein that controls the expression of many operons in Escherichia coli. One of those operons, ilvIH, contains six Lrp binding sites located within a several hundred base pair region upstream of the promoter region. Analysis of the binding of Lrp to a set of circularly permuted DNA fragments from this region indicates that Lrp induces DNA bending. The results of DNase I footprinting experiments suggest that Lrp binding to this region facilitates the formation of a higher-order nucleoprotein structure. To define more precisely the degree of bending associated with Lrp binding, one or two binding sites were separately cloned into a pBend vector and analyzed. Lrp induced a bend of approximately 52 degrees upon binding to a single binding site, and the angle of bending is increased to at least 135 degrees when Lrp binds to two adjacent sites. Lrp-induced DNA bending, and a natural sequence-directed bend that exists within ilvIH DNA, may be architectural elements that facilitate the assembly of a nucleoprotein complex.     

Cpf1 protein induced bending of yeast centromere DNA element I.

The centromere complex is a multicomponent structure essential for faithful chromosome transmission. Here we show that the S. cerevisiae centromere protein Cpf1 bends centromere DNA element I (CDEI) with the bend angle ranging from 66 degrees to 71 degrees. CDEI DNA sequences that carry point mutations which lead to reduced Cpf1 binding affinity and in vivo centromere activity are still able to show bending. The Cpf1 induced bend is directed towards the major groove with the bend centre located in CDEI. An intrinsic bend cannot replace the Cpf1 induced DNA bend for in vivo centromere function. An in vivo phasing experiment suggests that both the distance and the correct spatial arrangement of the CDEI/Cpf1 complex to CDEII and CDEIII are important for optimal centromere function.     

Conformational changes induced by a single amino acid substitution in the trans-membrane domain of Vpu: implications for HIV-1 susceptibility to channel blocking drugs

The channel-forming trans-membrane domain of Vpu (Vpu TM) from HIV-1 is known to enhance virion release from the infected cells and is a potential target for ion-channel blockers. The substitution of alanine at position 18 by a histidine (A18H) has been shown to render HIV-1 infections susceptible to rimantadine, a channel blocker of M2 protein from the influenza virus. In order to describe the influence of the mutation on the structure and rimantadine susceptibility of Vpu, we determined the structure of A18H Vpu TM, and compared it to those of wild-type Vpu TM and M2 TM. Both isotropic and orientationally dependent NMR frequencies of the backbone amide resonance of His18 were perturbed by rimantadine, and those of Ile15 and Trp22 were also affected, suggesting that His18 is the key residue for rimantadine binding and that residues located on the same face of the TM helix are also involved. A18H Vpu TM has an ideal, straight alpha-helix spanning residues 6-27 with an average tilt angle of 41 degrees in C14 phospholipid bicelles, indicating that the tilt angle is increased by 11 degrees compared to that of wild-type Vpu TM. The longer helix formed by the A18H mutation has a larger tilt angle to compensate for the hydrophobic mismatch with the length of the phospholipids in the bilayer. These results demonstrate that the local change of the primary structure plays an important role in secondary and tertiary structures of Vpu TM in lipid bilayers and affects its ability to interact with channel blockers.     

A Stochastic Model for Helix Bending in B-DNA

Abstract

Bending in double-helical B-DNA apparently occurs only by rolling adjacent base pairs over one another along their long axes. The lifting apart of ends that would be required by tilt or wedge angle contributions is too costly in free energy and does not occur. Roll angles at base steps can be positive (compression of major groove) or negative (compression of minor groove); with the former somewhat easier.

Individual steps may advance or oppose the overall direction of bend, or make lateral excursions, but the result of this series of “random roll” steps is the production of a net bending in the helix axis. Because the natural roll points for bending in a given plane occur every 5 base pairs, one would expect that double-helical DNA wrapped around a nucleosome core would exhibit bends with the same periodicity. Alternate bends might be particularly acute where the major groove faced the nucleosome core and was compressed against it.

The “annealed kinking” model proposed by Fratini et al. (J. Biol. Chem. 257, 14686 (1982) was suggested from the observation that a major bend at a natural roll point is flanked by decreasing roll angles at the steps to either side, as though local strain was being minimized by somewhat blurring the bend out rather than keeping it localized. The random walk model suggested in this paper would describe this as a decreased roll angle as the helix step rotates toward a direction perpendicular to the overall bend. Bending of DNA is seen to be a more stochastic process than had been suspected. Detailed analysis of every helix step reveals both side excursions and backward or retrograde motion, as in any random walk situation. Yet these isolated steps counteract one another, to leave behind a residuum of overall bending in a specific direction.     

DNA bending: the prevalence of kinkiness and the virtues of normality.

DNA bending in 86 complexes with sequence-specific proteins has been examined using normal vector plots, matrices of normal vector angles between all base pairs in the helix, and one-digit roll/slide/twist tables. FREEHELIX, a new program especially designed to analyze severely bent and kinked duplexes, generates the foregoing quantities plus local roll, tilt, twist, slide, shift and rise parameters that are completely free of any assumptions about an overall helix axis. In nearly every case, bending results from positive roll at pyrimidine-purine base pair steps: C-A (= T-G), T-A, or less frequently C-G, in a direction that compresses the major groove. Normal vector plots reveal three well-defined types of bending among the 86 examples: (i) localized kinks produced by positive roll at one or two discrete base pairs steps, (ii) three-dimensional writhe resulting from positive roll at a series of adjacent base pairs steps, or (iii) continuous curvature produced by alternations of positive and negative roll every 5 bp, with side-to-side zig-zag roll at intermediate position. In no case is tilt a significant component of the bending process. In sequences with two localized kinks, such as CAP and IHF, the dihedral angle formed by the three helix segments is a linear function of the number of base pair steps between kinks: dihedral angle = 36 degrees x kink separation. Twenty-eight of the 86 examples can be described as major bends, and significant elements in the recognition of a given base sequence by protein. But even the minor bends play a role in fine-tuning protein/DNA interactions. Sequence-dependent helix deformability is an important component of protein/DNA recognition, alongside the more generally recognized patterns of hydrogen bonding. The combination of FREEHELIX, normal vector plots, full vector angle matrices, and one-digit roll/slide/twist tables affords a rapid and convenient method for assessing bending in DNA.     

Angle and locus of the bend induced by the msp I DNA methyltransferase in a sequence-specific complex with DNA.

Bending of DNA induced by M.Msp I, one of the m5C-DNA methyltransferases, has been investigated using circular permutation analysis. The M.Msp I MTase induced sharp bends in DNA containing its recognition sequence 5'-CCGG-3'which was estimated to be 142+/-4 degrees and 132+/-4 degrees for circularly permuted DNA fragments of 127 and 1459 bp respectively. The bend centre was found to be asymmetric with respect to the CCGG sequence and appeared to exclude the 'target cytosine'. An estimate of approximately 15 kcal/mol was obtained for the free energy associated with M.Msp I-induced DNA bending.     

The DNA sequence specificity of HMG boxes lies in the minor wing of the structure.

To establish the basis of sequence-specific DNA recognition by HMG boxes we separately transferred the minor and major wings from the sequence-specific HMG box of TCF1 alpha into their equivalent position in the non-sequence-specific box 2 of HMG1. Thus chimera THT1 contains the minor wing (of 11 N-terminal and 25 C-terminal residues) from the HMG box of TCF1 alpha and the major wing (the 45 residue central section) from HMG1 box 2, whilst the situation is reversed in chimera HTH1. The structural integrity of the two chimeric proteins was established by CD, NMR and their binding to four-way junction DNA. Gel retardation and circular permutation assays showed that only chimera THT1, containing the TCF1 alpha minor wing, formed a sequence-specific complex and bent the DNA. The bend angle was estimated to be 59 degrees for chimera THT1 and 52 degrees for the HMG box of TCF1 alpha. Our results, in combination with mutagenesis and other data, suggests a model for the DNA binding of HMG boxes in which the N-terminal residues and part of helix 1 contact the minor groove on the outside of a bent DNA duplex.     

DNA binding and bending properties of the post-meiotically expressed Sry-related protein Sox-5.

Sox-5 is one of a family of genes which show homology to the HMG box region of the testis determining gene SRY. We have used indirect immunofluorescence to show that Sox-5 protein is localized to the nucleus of post-meiotic round spermatids in the mouse testis. In vitro footprinting and gel retardation assays demonstrate that Sox-5 binds specifically to the sequence AACAAT with moderately high affinity (Kd of approximately 10(-9) M). Moreover, interaction of Sox-5 with its target DNA induces a significant bend in the DNA, characteristic of HMG box proteins. Circular dichroism spectroscopy of the Sox-5 HMG box and its specific complex with DNA shows an alteration in the DNA spectrum, perhaps as a consequence of DNA bending, but none in the protein spectrum on complex formation. The dependence of the change in the CD spectrum with protein to DNA ratio demonstrates the formation of a 1:1 complex. Analysis of the structure of the Sox-5 HMG box by 2D NMR suggests that both the location of helical secondary structure as well as the tertiary structure is similar to that of HMG1 box 2.