Thermodynamics of unpaired terminal nucleotides on short RNA helixes correlates with stacking at helix termini in larger RNAs.

Free energies for stacking of unpaired nucleotides (dangling ends) at the termini of oligoribonucleotide Watson-Crick helixes (DeltaG(0)37,stack) depend on sequence for 3' ends but are always small for 5' ends. Here, these free energies are correlated with stacking at helix termini in a database of 34 RNA structures determined by X-ray crystallography and NMR spectroscopy. Stacking involving GA pairs is considered separately. A base is categorized as stacked by its distance from (相似文献   

Recognition of nucleic acid bases and base-pairs by hydrogen bonding to amino acid side-chains

Sequence-specific protein-nucleic acid recognition is determined, in part, by hydrogen bonding interactions between amino acid side-chains and nucleotide bases. To examine the repertoire of possible interactions, we have calculated geometrically plausible arrangements in which amino acids hydrogen bond to unpaired bases, such as those found in RNA bulges and loops, or to the 53 possible RNA base-pairs. We find 32 possible interactions that involve two or more hydrogen bonds to the six unpaired bases (including protonated A and C), 17 of which have been observed. We find 186 "spanning" interactions to base-pairs in which the amino acid hydrogen bonds to both bases, in principle allowing particular base-pairs to be selectively targeted, and nine of these have been observed. Four calculated interactions span the Watson-Crick pairs and 15 span the G:U wobble pair, including two interesting arrangements with three hydrogen bonds to the Arg guanidinum group that have not yet been observed. The inherent donor-acceptor arrangements of the bases support many possible interactions to Asn (or Gln) and Ser (or Thr or Tyr), few interactions to Asp (or Glu) even though several already have been observed, and interactions to U (or T) only if the base is in an unpaired context, as also observed in several cases. This study highlights how complementary arrangements of donors and acceptors can contribute to base-specific recognition of RNA, predicts interactions not yet observed, and provides tools to analyze proposed contacts or design novel interactions.     

Diversity of base-pair conformations and their occurrence in rRNA structure and RNA structural motifs

In addition to the canonical base-pairs comprising the standard Watson-Crick (C:G and U:A) and wobble U:G conformations, an analysis of the base-pair types and conformations in the rRNAs in the high-resolution crystal structures of the Thermus thermophilus 30S and Haloarcula marismortui 50S ribosomal subunits has identified a wide variety of non-canonical base-pair types and conformations. However, the existing nomenclatures do not describe all of the observed non-canonical conformations or describe them with some ambiguity. Thus, a standardized system is required to classify all of these non-canonical conformations appropriately. Here, we propose a new, simple and systematic nomenclature that unambiguously classifies base-pair conformations occurring in base-pairs, base-triples and base-quadruples that are associated with secondary and tertiary interactions. This system is based on the topological arrangement of the two bases and glycosidic bonds in a given base-pair. Base-pairs in the internal positions of regular secondary structure helices usually form with canonical base-pair groups (C:G, U:A, and U:G) and canonical conformations (C:G WC, U:A WC, and U:G Wb). In contrast, non-helical base-pairs outside of regular structure helices usually have non-canonical base-pair groups and conformations. In addition, many non-helical base-pairs are involved in RNA motifs that form a defined set of non-canonical conformations. Thus, each rare non-canonical conformation may be functionally and structurally important. Finally, the topology-based isostericity of base-pair conformations can rationalize base-pair exchanges in the evolution of RNA molecules.     

Characterization of base-pair opening in deoxynucleotide duplexes using catalyzed exchange of the imino proton

Using nuclear magnetic resonance line broadening, longitudinal relaxation and magnetization transfer from water, we have measured the imino proton exchange times in the duplex form of the 10-mer d-CGCGATCGCG and in seven other deoxy-duplexes, as a function of the concentration of exchange catalysts, principally ammonia. All exchange times are catalyst dependent. Base-pair lifetimes are obtained by extrapolation to infinite concentration of ammonia. Lifetimes of internal base-pairs are in the range of milliseconds at 35 degrees C and ten times more at 0 degrees C. Lifetimes of neighboring pairs are different, hence base-pairs open one at a time. Lifetimes of d(G.C) are about three times longer than those of d(A.T). The nature of neighbors usually has little effect, but lifetime anomalies that may be related to sequence and/or structure have been observed. In contrast, there is no anomaly in the A.T base-pair lifetimes of d-CGCGA[TA]5TCGCG, a model duplex of poly[d(A-T)].poly[d(A-T)]. The d(A.T) lifetimes are comparable to those of r(A.U) that we reported previously. End effects on base-pair lifetimes are limited to two base-pairs. The low efficiency of exchange catalysts is ascribed to the small dissociation constant of the deoxy base-pairs, and helps to explain why exchange catalysis had been overlooked in the past. This resulted in a hundredfold overestimation of base-pair lifetimes. Cytosine amino proteins have been studied in the duplex of d-CGm5CGCG. Exchange from the closed base-pair is indicated. Hence, the use of an amino exchange rate to evaluate the base-pair dissociation constant would result in erroneous, overestimated values. Catalyzed imino proton exchange is at this time the safest and most powerful, if not the only probe of base-pair kinetics. We propose that the single base-pair opening event characterized here may be the only mode of base-pair disruption, at temperatures well below the melting transition.     

Proton exchange and base-pair lifetimes in a deoxy-duplex containing a purine-pyrimidine step and in the duplex of inverse sequence

Using proton relaxation and magnetization transfer from water we have measured the imino proton exchange kinetics in two dodecadeoxynucleotide duplexes. One is formed by the self-complementary sequence 5'-d(C-C-T-T-T-C-G-A-A-A-G-G), the other by the inverse sequence. The imino proton exchange rates are found to depend on the concentration of ammonia or imidazole, acting as basic catalysts of proton exchange. Extrapolation of exchange times to infinite catalyst concentration yields the base-pair lifetimes, for instance 40 milliseconds for the central G.C base-pair of the 5'-d(C-C-T-T-T-C-G-A-A-A-G-G) duplex and four milliseconds for its A.T neighbour, at 15 degrees C. These results differ markedly from those reported by other laboratories for similar deoxy compounds. An explanation of the discrepancy has been proposed recently. Differences between base-pair lifetimes indicate that opening is not co-operative. From the catalyst efficiency relative to exchange from isolated nucleosides, we estimate the dissociation constant of each base-pair, e.g. 0.3 x 10(-6) and 1.5 x 10(-5) at 15 degrees C, for the same G.C and A.T base-pairs. The lifetime and dissociation constant of corresponding base-pairs of the two duplexes are similar, except for the central G.C base-pair. This correlates with differences in the solution structures reported by others. We have completed the assignments of the imino protons and of the six cytosine amino protons of the 5'-d(G-G-A-A-A-G-C-T-T-T-C-C) 12-mer. A new base-pair numbering scheme is proposed.     

Inosine.adenine base pairs in a B-DNA duplex.

The structure of the synthetic deoxydodecamer d(C-G-C-I-A-A-T-T-A-G-C-G) has been determined by single crystal X-ray diffraction techniques at 2.5A resolution. The refinement converged with a crystallographic residual, R = 0.19 and the location of 64 solvent molecules. The sequence crystallises as a B-DNA helix with 10 Watson-Crick base-pairs (4 A.T. and 6 G.C) and 2 inosine.adenine (I.A) pairs. The present work shows that in the purine.purine base-pairs the adenine adopts syn orientation with respect to the furanose moiety while the inosine is in the trans (anti) orientation. Two hydrogen bonds link the I.A. base-pair, one between N-1(I) and N-7(A), the other between O-6(I) and N-6(A). This bulky purine.purine base-pair is incorporated in the double helix at two positions with little distortion of either local or global conformation. The pairing observed in this study is presented as a model for I.A base-pairs in RNA codon-anticodon interactions and may help explain the thermodynamic stability of inosine containing base-pairs. Conformational parameters and base stacking interactions are presented and where appropriate compared with those of the native compound, d(C-G-C-G-A-A-T-T-C-G-C-G) and with other studies of oligonucleotides containing purine.purine base-pairs.     

Genetic conversion of G.C base-pairs to A.U base-pairs in a transfer RNA

The cloverleaf stem segments of the suppressor gene of bacteriophage T4 tRNA(Gln) contain ten G.C and ten A.U base-pairs. To gain a better appreciation of the G.C base-pair requirement, we isolated multiple mutants of this suppressor gene in which base-pairs of G.C were replaced by A.U. One active suppressor gene contained only A.U base-pairs on the anticodon stem, indicating that G.C base-pairs in this region of tRNA(Gln) are not essential for function. In contrast, replacement was not possible at two base-pairs on the D stem and at one base-pair on the T stem.     

Singly and bifurcated hydrogen-bonded base-pairs in tRNA anticodon hairpins and ribozymes.

The tRNA anticodon loops always comprise seven nucleotides and is involved in many recognition processes with proteins and RNA fragments. We have investigated the nature and the possible interactions between the first (32) and last (38) residues of the loop on the basis of the available sequences and crystal structures. The data demonstrate the conservation of a bifurcated hydrogen bond interaction between residues 32 and 38, located at the stem/loop junction. This interaction leads to the formation of a non-canonical base-pair which is preserved in the known crystal structures of tRNA/synthetase complexes. Among the tRNA and tDNA sequences, 93 % of the 32.38 oppositions can be assigned to two families of isosteric base-pairs, one with a large (86 %) and the other with a much smaller (7 %) population. The remainder (7 %) of the oppositions have been assigned to a third family due to the lack of evidence for assigning them into the first two sets. In all families, the Y32.R38 base-pairs are not isosteric upon reversal (like the sheared G.A or wobble G.U pairs), explaining the strong conservation of a pyrimidine at position 32. Thus, the 32.38 interaction extends the sequence signature of the anticodon loop beyond the conserved U-turn at position 33 and the usually modified purine at position 37. A comparison with other loops containing both a singly hydrogen-bonded base-pair and a U-turn suggests that the 32.38 pair could be involved in the formation of a base triple with a residue in a ribosomal RNA component. It is also observed that two crystal structures of ribozymes (hammerhead and leadzyme) present similar base-pairs at the cleavage site.     

The conformational variability of an adenosine.inosine base-pair in a synthetic DNA dodecamer.

A crystal structure analysis of the synthetic deoxydodecamer d(CGCAAATTIGCG) which contains two adenosine.inosine (A.I) mispairs has revealed that, in this sequence, the A.I base-pairs adopt a A(anti).I(syn) configuration. The refinement converged at R = 0.158 for 2004 reflections with F greater than or equal to 2 sigma(F) in the range 7.0-2.5A for a model consisting of the DNA duplex and 71 water molecules. A notable feature of the structure is the presence of an almost complete spine of hydration spanning the minor groove of the whole of the (AAATTI)2 core region of the duplex. pH-dependent ultraviolet melting studies have suggested that the base-pair observed in the crystal structure is, in fact, a protonated AH+ (anti).I(syn) species and that the A.I base-pairs in the sequence studied display the same conformational variability as A.G mispairs in the sequence d(CGCAAATTGGCG). The AH+(anti).I(syn) base-pair predominates below pH 6.5 and an A(anti).I(anti) mispair is the major species present between pH 6.5 and 8.0. The protonated base-pairs are held together by two hydrogen bonds one between N6(A) and O6(I) and the other between N1(A) and N7(I). This second hydrogen bond is a direct result of the protonation of the N1 of adenosine. The ultraviolet melting studies indicate that the A(anti).I(anti) base-pair is more stable than the A(anti).G(anti) base-pair but that the AH+(anti).I(syn) base pair is less stable than its AH+(anti).G(syn) analogue. Possible reasons for this observation are discussed.     

Identity elements required for enzymatic formation of N2,N2-dimethylguanosine from N2-monomethylated derivative and its possible role in avoiding alternative conformations in archaeal tRNA

Here, we have investigated the specificity of purified recombinant tRNA:m(2)(2)G10 methyltransferase of Pyrococcus abyssi ((Pab)Trm-m(2)(2)G10 enzyme). This archaeal enzyme catalyses mono- and dimethylation of the N(2)-exocyclic amino group of guanine at position 10 of several tRNA species. Our results indicate that only few identity elements are required for the efficient formation of m(2)(2)G10. They are composed of a G10.U25 wobble base-pair in the dihydrouridine arm (D-arm) and a four nucleotide variable loop (V-loop) within a canonical three-dimensional (3D) structure. The types of base-pairs in the D-arm or amino acid acceptor stem are also important for the enzymatic reaction, but appear to affect only the rate of tRNA methylation. However, in tRNA species harbouring a G10-C25 Watson-Crick base-pair and/or five nucleotide V-loop, only m(2)G10 is produced. To impair the monomethylation reaction, drastic amputation in the T-arm is required. Our observations contrast with those reported earlier for the identity elements required for a remotely related Pyrococcus furiosus Trm-m(2)(2)G26 enzyme (alias (Pfu)Trm1) that also catalyses the two step formation of m(2)(2)G but at position 26 in several tRNA species. In this case, a G10-C25 base-pair together with the five nucleotide V-loop were shown to be required for efficient formation of m(2)(2)G26. Thus, in the Pyrococcus genus, the major identity elements that preclude formation of m(2)(2)G at positions 10 or 26 in tRNA are mutually exclusive. Therefore, the Trm-m(2)(2)G10 and Trm-m(2)(2)G26 enzymes have evolved independently towards different specificities. In addition, identity elements for m(2)/m(2)(2)G10 formation in archaeal tRNA are different from the ones required for m(2)G10 formation in eukaryal tRNA. We propose that archaeal tRNA:m(2)(2)G10 methyltransferases, unlike the orthologous eukaryal tRNA:m(2)G10 methyltransferases, evolved towards m(2)(2)G10 specificity due to the possible requirement of preventing formation of alternative structures in G/C rich archaeal tRNA species.     

Solution structure of a DNA double helix incorporating four consecutive non-Watson-Crick base-pairs

A series of DNA 21-mers containing a variety of the 4 x 4 internal loop sequence 5'-CAAG-3'/3'-ACGT-5' were studied using nuclear magnetic resonance (NMR) methodology and distance geometry (DG)/molecular dynamics (MD) approaches. Such oligomers exhibit excellent resolution in the NMR spectra and reveal many unusual NOEs (nuclear Overhauser effect) that allow for the detailed characterization of a DNA hairpin incorporating a track of four different non-Watson-Crick base-pairs in the stem. These include a wobble C.A base-pair, a sheared A.C base-pair, a sheared A.G base-pair, and a wobble G.T base-pair. Significantly different twisting angles were observed between the base-pairs in internal loop that results with excellent intra-strand and inter-strand base stacking within the four consecutive mismatches and the surrounding canonical base-pairs. This explains why it melts at 52 degrees C even though five out of ten base-pairs in the stem adopt non-Watson-Crick pairs. However, the 4 x 4 internal loop still fits into a B-DNA double helix very well without significant change in the backbone torsion angles; only zeta torsion angles between the tandem sheared base-pairs are changed to a great extent from the gauche(-) domain to the trans domain to accommodate the cross-strand base stacking in the internal loop. The observation that several consecutive non-canonical base-pairs can stably co-exist with Watson-Crick base-pairs greatly increases the limited repertoire of irregular DNA folds and reveals the possibility for unusual structural formation in the functionally important genomic regions that have potential to become single-stranded.     

Molecular and crystal structure of d(CGCGmo4CG): N4-methoxycytosine.guanine base-pairs in Z-DNA

The base analogue N4-methoxycytosine (mo4C) is ambivalent in its hydrogen-bonding potential, since it forms stable base-pairs with both adenine and guanine in oligomer duplexes. To investigate the base-pair geometry, the structure of d(CGCGmo4CG) has been determined by single-crystal X-ray diffraction techniques. The d(CGCGmo4CG)2 crystallized in a left-handed double helical structure (Z-type). Refinement using 2559 reflections between 10 and 1.7 A converged with a final R = 0.181 (Rw = 0.130) including 68 solvent molecules. The orthorhombic crystals are in the space group P2(1)2(1)2(1), with cell dimensions a = 18.17 A, b = 30.36 A, c = 43.93 A. The mo4C.G base-pair is of the wobble type, with mo4C in the imino form, and the methoxy group in the syn configuration.     

Contribution of opening and bending dynamics to specific recognition of DNA damage

Guanine-uracil (G.U) wobble base-pairs are a detrimental lesion in DNA. Previous investigations have shown that such wobble base-pairs are more prone to base-opening than the normal G.C base-pairs. To investigate the sequence-dependence of base-pair opening we have performed 5ns molecular dynamics simulations on G.U wobble base-pairs in two different sequence contexts, TGT/AUA and CGC/GUG. Furthermore, we have investigated the effect of replacing the guanine base in each sequence with a fluorescent guanine analogue, 6-methylisoxanthopterin (6MI). Our results indicate that each sequence opens spontaneously towards the major groove in the course of the simulations. The TGT/AUA sequence has a greater proportion of structures in the open state than the CGC/GUG sequence. Incorporation of 6MI yields wobble base-pairs that open more readily than their guanine counterparts. In order of increasing open population, the sequences are ordered as CGC相似文献   

Molecular dynamics of the frame-shifting pseudoknot from beet western yellows virus: the role of non-Watson-Crick base-pairing, ordered hydration, cation binding and base mutations on stability and unfolding.

Molecular dynamics simulations of the frame-shifting pseudoknot from beet western yellows virus (BWYV, NDB file UR0004) were performed with explicit inclusion of solvent and counterions. In all, 33 ns of simulation were carried out, including 10 ns of the native structure with protonation of the crucial cytosine residue, C8(N3+). The native structure exhibited stable trajectories retaining all Watson-Crick and tertiary base-pairs, except for fluctuations or transient disruptions at specific sites. The most significant fluctuations involved the change or disruption of hydrogen-bonding between C8(N3+) and bases G12, A25, and C26, as well as disruption of the water bridges linking C8(N3+) with A25 and C26. To increase sampling of rare events, the native simulation was continued at 400 K. A partial, irreversible unfolding of the molecule was initiated by slippage of C8(N3+) relative to G12 and continued by sudden concerted changes in hydrogen-bonding involving A23, A24, and A25. These events were followed by a gradual loss of stacking interactions in loop 2. Of the Watson-Crick base-pairs, only the 5'-terminal pair of stem 1 dissociated at 400 K, while the trans sugar-edge/sugar-edge A20.G4 interaction remained surprisingly stable. Four additional room-temperature simulations were carried out to obtain insights into the structural and dynamic effects of selected mutations. In two of these, C8 was left unprotonated. Considerable local rearrangements occurred that were not observed in the crystal structure, thus confirming N3-protonation of C8 in the native molecule. We also investigated the effect of mutating C8(N3+) to U8, to correlate with experimental and phylogenetic studies, and of changing the G4 x C17 base-pair to A4 x U17 to weaken the trans sugar-edge interaction between positions 4 and 20 and to test models of unfolding. The simulations indicate that the C8 x G12 x C26 base-triple at the junction is the most labile region of the frame-shifting pseudoknot. They provide insights into the roles of the other non-Watson-Crick base-pairs in the early stages of unfolding of the pseudoknot, which must occur to allow readthrough of the message by the ribosome. The simulations revealed several critical, highly ordered hydration sites with close to 100 % occupancies and residency times of individual water molecules of up to 5 ns. Sodium cation coordination sites with occupancies above 50 % were also observed.     

IncN plasmid replicon. A deletion and subcloning analysis

A DNA segment of approximately 2000 base-pairs bounded by restriction enzyme sites for PvuII and containing the minimal replicon of an N group plasmid was characterized. A natural derivative of this miniplasmid was found to have undergone a deletion within one of two tandem iteron families, the group I iterons. Further analysis showed that all plasmid-determined functions essential for stable maintenance in Escherichia coli were localized to a contiguous region of DNA of 1019 nucleotides that excludes entirely these iterons. However, the loss of these iterons led to an increase in plasmid copy number. This indicates that members of the group I iteron-family have a role in determining plasmid copy number perhaps by titrating a plasmid-specified trans-acting product. The 2000 base-pair segment contains six open reading frames of 40 or more amino acid residues. The essential segment contains a 368 nucleotide region that must be present in cis and within which there are three "GATC" sequences and a putative Escherichia coli DnaA protein-binding sequence (dnaA box). An interesting feature is that the cis-acting region is present entirely within a presumptive rep gene. The essential segment contains four open reading frames, only one of which has an Escherichia coli canonical ribosome-binding site. The 2000 base-pair miniplasmid has two separable regions determining N group plasmid incompatibility.     

Substituent effects on the binding of ethidium and its derivatives to natural DNA

The binding of eight ethidium derivatives to short (approximately 35 base-pair), random sequence DNA has been investigated using 1H-NMR. At 35 degrees C, all drugs cause upfield shifts of the DNA imino proton resonances characteristic of intercalative binding to DNA, but the line shapes vary significantly with the nature of the drug. The results confirm our previous proposal that removal of the amino group at position-3, but not at position-8, on the parent ethidium shortens the lifetime of the intercalative state (less than 1-2 ms at 35 degrees C). These results suggest that hydrogen-bonding interactions with the 3-NH2 group are involved in stabilization of the drug-DNA complex or that changes in charge distribution that accompany removal of the 3-NH2 group reduce the complex stability. The magnitude of the shift of the drug-DNA spectra indicates a slight preference for binding of the drugs adjacent to G X C base-pairs.     

The crystal structure of N4-methylcytosine.guanosine base-pairs in the synthetic hexanucleotide d(CGCGm4CG).

The structure of d(CGCGm4CG) were m4C = N4-methylcytosine has been determined by crystallographic methods. The crystals are multifaced prisms, with orthorhombic space group P2(1)2(1)2(1) and unit cell dimensions of a = 17.98, b = 30.77 and c = 44.75A. The asymmetric unit consists of one duplex of hexanucleotide and 49 waters. The R-factor is 0.189 for 1495 reflections with F > or = sigma(F) to a resolution limit of 1.8A. The double helix has a Z-DNA type structure which appears to be intermediate in structure to the two previously characterised structure types for Z-DNA hexamers. The two m4C.G base-pairs adopt structures that are very similar to those of the equivalent base-pairs in the structure of the native sequence d(CGCGCG) except for the presence of the methyl groups which are trans to the N3 atoms of their parent nucleotides and protrude into the solvent region. The introduction of the modified base-pairs into the d(CGCGCG) duplex appears to have a minimal effect on the overall base-pair morphology of the Z-DNA duplex.     

Crystal structure and stability of a DNA duplex containing A(anti).G(syn) base-pairs

The synthetic dodecanucleotide d(CGCAAATTGGCG) has been analysed by single-crystal X-ray diffraction techniques and the structure refined to R = 0.16 and 2.25 A resolution, with the location of 94 solvent molecules. The sequence crystallizes as a full turn of a B-DNA helix with ten Watson-Crick base-pairs and two adenine-guanine mispairs. The analysis clearly shows that the mismatches are of the form A(anti).G(syn). Thermal denaturation studies indicate that the stability of the duplex is strongly pH dependent, with a maximum at pH 5.0, suggesting that the base-pair is stabilized by protonation. Three different arrangements have been observed for base-pairs between guanine and adenine and it is likely that A.G mismatch conformation is strongly influenced by dipole-dipole interactions with adjacent base-pairs.     

Conserved structural features are found upstream from the three co-ordinately regulated discoidin I genes of Dictyostelium discoideum

The discoidin I genes of Dictyostelium form a small, co-ordinately regulated multigene family. We have sequenced and compared the upstream regions of the DiscI-alpha, -beta and -gamma genes. For the most part the upstream regions of the three genes are non-homologous. The upstream sequences of the beta and gamma genes are exceedingly A + T-rich, while those of the alpha gene are less so. All three genes have a relatively G + C-rich region 20 to 40 base-pairs in length, found approximately 200 base-pairs 5' to the messenger RNA start site. This G + C-rich region 5' to the beta and gamma genes is flanked by short inverted repeats. Within this region, there is an 11 base-pair exact homology between the alpha and gamma genes, and a less perfect homology between these genes and the beta gene. The homology is flanked at a short distance by interspersed G and T residues. The gamma gene is greater than 90% A + T for greater than 800 base-pairs upstream. Further upstream there is a G + C-rich region that is also found inverted approximately 3.5 X 10(3) base-pairs away. The gamma and beta genes are tandemly linked, and the entire approximately 500 base-pair intergene region between the 3' end of the gamma gene and the 5' end of the beta gene is A + T-rich (approximately 90%) with the exception of the homology region 5' to the gamma gene. We demonstrate also the presence of a discoidin I pseudogene fragment having only 139 base-pairs of discoidin homology with greater than 8% mismatch. It is flanked upstream by five 39 base-pair G + C-rich repeats, and downstream by sequences that are extremely A + T-rich. We discuss the possible significance of the conserved G + C-rich structures on discoidin I gene expression.     

Contacts between Tet repressor and tet operator revealed by new recognition specificities of single amino acid replacement mutants.

We have analyzed the DNA binding properties of Tet-repressor mutants with single amino acid residue replacements at eight positions within the alpha-helix-turn-alpha-helix DNA-binding motif. A saturation mutagenesis of Gln38, Pro39, Thr40, Tyr42, Trp43 and His44 in the second alpha-helix was performed; in addition, several substitutions of Thr27 and Arg28 in the first alpha-helix were constructed. The abilities of these mutant repressors to bind a set of 16 operator variants were determined and revealed 23 new binding specificities. All repressor mutants with DNA-binding activity were inducible by tetracycline, while mutants lacking binding activity were trans-dominant over the wild-type. All mutant proteins were present at the same intracellular steady-state concentrations as the wild-type. These results suggest the structural integrity of the mutant repressors. On the basis of the new recognition specificities, five contacts between a repressor monomer and each operator half-site and the chemical nature of these repressor-operator interactions are proposed. We suggest that Arg28 contacts guanine of the G.C base-pair at operator position 2 with two H-bonds, Gln38 binds adenine of the A.T base-pair at position 3 with two H-bonds, and the methyl group of Thr40 participates in a van der Waals' contact with cytosine of the G.C base-pair at position 6 of tet operator. A previously unrecognized type of interaction is proposed for Pro39, which inserts its side-chain between the methyl groups of the thymines of T.A and A.T base-pairs at positions 4 and 5. Computer modeling of these proposed contacts reveals that they are possible using the canonical structures of the helix-turn-helix motif and B-DNA. These contacts suggest an inverse orientation of the Tet repressor helix-turn-helix with respect to the operator center as compared with non-inducible repressor-operator complexes, and are supported by similar contacts of other repressor-operator complexes.