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© 1995 Oxford University Press 951-961

Footnote

The crystal structure analysis of d(CGCGAASSCGCG) 2 , a synthetic DNA dodecamer duplex containing four 4 ' -thio-2 '-deoxythymidine nucleotides

The crystal structure analysis of d(CGCGAASSCGCG) 2 , a synthetic DNA dodecamer duplex containing four 4 ' -thio-2 '-deoxythymidine nucleotides Titus J. Boggon , E. Louise Hancox 1 , Katherine E. McAuley-Hecht 2 , Bernard A. Connolly 3 , William N. Hunter , Tom Brown 2,+ , Richard T. Walker 1 and Gordon A. Leonard*

Department of Chemistry, University of Manchester, Oxford Road, Manchester M13 9PL, UK , 1 School of Chemistry, University of Birmingham, Birmingham B15 2TT, UK , 2 Department of Chemistry, University of Edinburgh, King's Buildings, West Mains Road, Edinburgh EH9 3JJ, UK and 3 Department of Biochemistry and Genetics, University of Newcastle-upon-Tyne, Newcastle-upon-Tyne NE2 4HH, UK

Received September 19, 1995; Revised and Accepted December 15, 1995

ABSTRACT

The crystal structure refinement of the synthetic dodecamer d(CGCGAASSCGCG), where S = 4 ' -thio- 2 ' -deoxythymidine, has converged at R = 0.201 for 2605 reflections with F > 2 [sigma] ( F ) in the resolution range 8.0-2.4 Å for a model consisting of the dodecamer duplex and 66 water molecules. A comparison of its structure with that of the native dodecamer d(CGCGAATTCGCG) has revealed that the major differences between the two structures is a change in the conformation of the sugar-phosphate backbone in the regions at and adjacent to the positions of the modified nucleosides. Examination of the fine structural parameters for each of the structures reveals that the thiosugars adopt a C3 ' - exo conformation in d(CGCGAASSCGCG), rather than the approximate C1 ' - exo conformation found for the analogous sugars in the structure of d(CGCGAATTCGCG). The observed differences in structure between the two duplexes may help to explain the enhanced resistance to nuclease digestion of synthetic oligonucleotides containing 4 ' -thio-2 ' -deoxynucleotides.

INTRODUCTION

The biological properties of 4'-thionucleosides ( 1 - 5 ), which are sulphur-containing isoelectronic analogues of natural nucleosides (Fig. 1 ), are not always apparent from a comparison with those of the corresponding oxysugar-containing deoxynucleoside. Hence, while ( E )-5-(2-bromovinyl)-2'-deoxyuridine and its sulphur-containing analogue both show potent and selective inhibition of HSV-1 and varicella zoster virus (VZV), the strong antiviral properties of 5-isopropyl- and 5-cyclopropyl-4'-thio-2'-deoxyuridine are markedly different to those of the corresponding natural nucleosides, which show no antiviral activity at all. Similarly, 5-vinyl-2'-deoxyuridine is very toxic, whereas the corresponding 4'-thio analogue shows no toxicity, but is active against HSV-1.

Some of the most interesting properties of pyrimidine 4'-thio-2'-deoxynucleotides are that they are significantly more lipophilic than oxysugar-containing deoxynucleotides and have a much longer serum half-life than normal nucleotides, the latter property arising because they are stable to phosphorolysis. This led to the suggestion that oligonucleotides containing pyrimidine 4'-thio-2'-deoxynucleosides might be useful in the antisense field, especially as structure determination had shown the modified nucleosides to adopt similar conformations to those of the natural nucleosides ( 6 ). Additionally, circular dichroism and ultraviolet melting studies ( 7 ) of thiosugar nucleoside-containing oligonucleotides had shown them to adopt the same overall conformation as the analogous unmodified oligonucleotides and that the duplexes were only slightly less thermodynamically stable.

Experiments involving the synthesis of oligonucleotides containing the Eco RV recognition site revealed that when a 4'-thiothymidine residue was incorporated on the 5'-side of the scissile bond the DNA duplex was resistant to endonuclease attack ( 7 ). The reasons for this were not at all clear, as a crystal structure of the complex between Eco RV and the modified duplex (Kostrewa,D., Hancox,E.L., Walker,R.T., Connolly,B.A. and Winkler,F.K., unpublished results; 8 ) showed that the conformation of the DNA had not significantly changed. However, The Mg 2+ ion required for enzyme activity was not present in the structure.


Figure 1 . Representations of ( a ) 2'-deoxythymidine-5'-phosphate and ( b ) its isoelectronic analogue 4'-thio-2'-deoxythymidine-5'-phosphate (S).


As part of a continuing investigation into the structures and biological properties of oligonucleotides containing 4'-thio-2'- deoxynucleosides we report here the results of an X-ray structural analysis of the self-complementary dodecamer d(CGCGAASSCGCG), where S = 4'-thio-2'-deoxythymidine (Fig. 1 ). The observed structure is compared with that of the native dodecamer d(CGCGATTCGCG) ( 9 ) and the structural reasons for the resistance of 4'-thiosugar-containing oligonucleotides to endonuclease attack are explored.


Figure 2 . ( a ) The final calculated electron density (2 F obs - F calc , [alpha] calc ; grey chicken wire) for one of the A.S base pairs in the structure of d(CGCGAASSCGCG). The nucleotides are depicted as sticks with the following atom colouring scheme: carbon, yellow; nitrogen, blue; oxygen, red; sulphur, green; phosphorus, yellow. The electron density is contoured at approximately one standard deviation (SD) from the r.m.s. level found in the unit cell. For clarity solvent molecules have not been shown. ( b ) A close-up of the final calculated electron density for the sugar-phosphate backbone in the region of one of the 4'-thiosugars. Two contour levels are shown: 1 SD from the r.m.s. level (grey) and 2.75 SD from the r.m.s. level (brown). Note the spherical, high level density at the sulphur position of the 4'-thio sugar when compared with the density for the unmodified sugar shown.


MATERIALS AND METHODS

Chemical synthesis

The oligonucleotide was synthesized (10 [mu]M scale) using an Applied Biosystems 381A DNA synthesizer. The modified deoxynucleoside phosphoramidite ( 7 ) was introduced at the fifth position of the synthesis as previously described ( 7 ). The synthesis and purification of the oligodeoxynucleotide was achieved under standard conditions.

Crystallization, X-ray data collection and structure refinement

Thin, colourless, needle-shaped crystals were grown at ambient temperature in sitting drops which contained the dodecanucleotide (0.5 mM), sodium cacodylate buffer (14 mM, pH 6.0), magnesium chloride (17 mM), spermine tetrahydrochloride (1 mM) and 2-methyl-2,4-pentanediol (MPD) (17% v/v), which were diffused against external reservoirs containing 50% aqueous MPD. Two such crystals were then mounted in thin-walled glass capillaries for X-ray data collection. Data from the first of these, which had dimensions of 1.0 * 0.05 * 0.05 mm, was collected at [lambda] = 0.882 Å on station PX9.6 at the Synchrotron Radiation Source, Daresbury Laboratory, to a resolution limit of 2.35 Å using a 18 cm MAR Research image plate detector and 17 4o oscillation frames, each exposed for 120 s. This data was later supplemented by a set collected from a bigger crystal (1.5 * 0.15 * 0.15 mm) to a resolution limit of 2.5 Å on a Rigaku RU200 rotating anode generator ([lambda] = 1.5418 Å) operating at 50 kV, 140 mA and equipped with a RAXIS IIc image plate system. This latter data set was collected on 39 3o oscillation frames, each of which were exposed to X-rays for 1 h. All the data was processed using the program MOSFLM (version 5.20) ( 10 ), then scaled, merged and reduced using programs from the CCP4 suite of programs ( 11 ) to yield a total of 2820 unique reflections with R sym = 0.065 to a resolution of 2.4 Å and a multiplicity of 6.3.

Orthorhombic unit cell dimensions of a = 24.99 Å, b = 40.36 Å, c = 65.99 Å and space group P2 1 2 1 2 1 suggested that the structure of d(CGCGAASSCGCG) is isomorphous with that of the native dodecamer d(CGCGAATTCGCG) ( 9 ). The initial stage of the structure refinement therefore consisted of rigid body minimization, against the observed data, of the structure of the native dodecamer stripped of solvent molecules and with sulphur atoms replacing oxygen atoms where necessary. This procedure, as with the rest of the refinement, was carried out using the program X-PLOR ( 12 , 13 ) and converged with R = 0.333 for the 2605 reflections with F > 2[sigma]( F ) in the resolution range 8.0-2.4 Å. The refinement then continued, using the same data, with a round of simulated annealing-based minimization. This consisted of initial energy minimization of the model followed by a slow cooling procedure (initial temperature 1000 K, final temperature 300 K, temperature decrement 25 K, time step 0.5 fs) and one round (120 cycles) of Powell minimization. Throughout this procedure and for subsequent rounds of refinement the dictionary of restraints used was that provided with X-PLOR and modified to include C-S bond length and C-S-C bond angle values for 4'-thio-2'-deoxy-thymidine, which were taken from Dyson et al. ( 3 ). It should be noted that the values used for dihedral angles and improper angles in the modified nucleoside were those already in place for 2'-deoxythymidine.


Figure 3 . A least squares superposition of the structure of d(CGCGAASSCGCG) (black sticks) and the 1BNA structure of d(CGCGAATTCGCG) (red sticks). Note that the positions of the bases remains almost constant and that major differences between the two structures are confined to the conformation of the sugar-phosphate backbone in the vicinity of the modified nucleosides.

At this stage R had been reduced to 0.258. Both electron density (2 F o - F c , [alpha] calc ) and difference density maps ( F o - F c , [alpha] calc ) were then calculated using the CCP4 suite of programs ( 11 ) and displayed and examined on a graphics workstation using the program O ( 14 ). Modifications to the model were then made in order to improve its fit to the electron density and a number of potential solvent molecules were added to the model. Solvent molecules were added only if they appeared with approximately spherical density in both electron density and difference density maps and had good hydrogen bonding geometry with other atoms already included in the model. Discrimination of potential peaks on the difference maps was greatly aided by the use of the program WATERSHED (Bond,C.S., personal communication). The refinement then consisted of several rounds, each of which consisted of 40 cycles of positional refinement, 20 cycles of temperature factor (individual, restrained isotropic) minimization, map calculation and examination, model manipulation and the addition of new solvent molecules coupled with the checking of those already incorporated into the model.

The refinement procedure was deemed to have converged when no further solvent molecules could be added to the model and no further manual manipulation of the model was required. At this point the R factor was 0.201 for the 2605 reflections with F > 2[sigma]( F ) in the resolution range 8.0-2.4 Å for a model consisting of the dodecanucleotide (486 atoms) and 66 solvent molecules, each of which was modelled as an oxygen atom. The data used in the refinement represents 89% of the total theoretical data available between the resolution limits stated, ~50% for the range 2.5-2.4 Å. The final model has root mean square (r.m.s.) deviations from ideality of 0.018 Å for bond lengths and 3.53o for bond angles. The average temperature factors for the phosphate groups, deoxyribose groups, bases and solvent molecules are 44.2 Å 2 , 35.0 Å 2 , 24.4 Å 2 and 61.4 Å 2 respectively. The fit of the model to the final calculated electron density is generally excellent (Fig. 2 ), although there are occasional discontinuities in the sugar-phosphate backbone. Both observed structure factor data and the final refined coordinates have been deposited with the Brookhaven Protein Databank (PDB) ( 15 ) and have been assigned the accession code 233d.

RESULTS AND DISCUSSION

In the structure of the modified dodecamer the nucleotides are labelled C1-G12 on strand 1 and C13-G24 on strand 2, both in the 5' -> 3' direction. The 66 solvent molecules are labelled HOH25-HOH91.

As indicated by nucleotide sequence, unit cell parameters and space group, the structure of d(CGCGAASSCGCG) is isomorphous with that of the native dodecamer ( 9 ). The parameters that define global double helical conformation do not differ significantly between the two structures. A least squares superposition of the two double helices (Fig. 3 ) shows the r.m.s. difference in atomic positions between the two structures to be 0.49 Å and also suggests that the global conformation of the two structures is extremely similar. However, a closer inspection of the two superposed structures reveals that incorporation of the four 4'-thiosugar moieties into the sequence has led to some significant differences in the local structure of the two duplexes. This view is supported by an examination of Figure 4 . Figure 4 a shows the difference in position for every atom in the two duplexes. As can be seen, on each of the two strands the deviation in atomic position remains fairly constant until one reaches a point in the vicinity of the 4'-thio-2'-deoxythymidine residues, when the deviations increase to a maximum before falling away to background level. Although the magnitudes of the positional differences are somewhat greater on strand 1 than strand 2, in both cases the distribution is rather symmetrical, which indicates that these deviations are real and not artefacts of the refinement procedure. Figure 4 b shows that for an average deviation per nucleotide the differences in position reach their peak for residues S8 and S20, which are the second of the two modified nucleotides on strands 1 and 2 respectively.

The above analysis refers to the superposition of the modified dodecamer onto the coordinate set 1BNA ( 9 ) as deposited in the PDB. There have been several other determinations of the structure of d(CGCGAATTCGCG), either at low temperature (deposition 2BNA in the PDB; 17 ) or using different refinement techniques (depositions 7BNA, 9BNA in the PDB; 18 , 19 ). The refined structure of d(CGCGAASSCGCG) has been superimposed on each of these coordinate sets (Figure 4 a), yielding similar results to those found when the structure of d(CGCGAASSCGCG) is superimposed in the original 1BNA coordinate set. This is further evidence that the differences we observe between the structure of d(CGCGAASSCGCG) and that of the native doecamer are real. Moreover, when the coordinate sets 2BNA, 7BNA and 9BNA are superimposed on those of 1BNA (Fig. 4 c) there is no significant increase in the r.m.s. deviations of the sugar atoms in nucleotides 7, 8, 19 and 20 when compared with the rest of the atoms, although, inexplicably, for the 1BNA versus 9BNA superposition anomalously large deviations occur for the C6 and M5 atoms of nucleotides 7, 8, 19 and 20.

Incorporation of the 4'-thiosugars into the sequence does not greatly affect the positions of the bases when both the modified and native structures are compared (Fig. 3 ), but rather they induce a change in the conformation of the sugar-phosphate backbone in the vicinity of the modified sugars. Indeed, the greatest deviations in the positions of the atoms in the modified and native (1BNA) dodecamers occurs in the phosphodiester linkages on the 5'-side of the thiosugars themselves (Fig. 5 )


Figure 4 . ( a ) A plot of the r.m.s. differences in the positions of the atoms in d(CGCGAASSCGCG) and d(CGCGAATTCGCG) resulting from a superposition of the modified and the 1BNA, 2BNA, 7BNA and 9BNA native structures. The atoms on strand 1 are numbered from 1 to 243, those on strand 2 from 244 to 486. ( b ) A plot showing the average r.m.s. deviation per residue resulting from the least squares superposition of the modified and the 1BNA native structures. In this figure the residues are numbered from 1 to 12 for both strands in the 5' -> 3' direction. ( c ) A plot of the r.m.s. differences in atomic position following the superposition of the 2BNA, 7BNA and 9BNA coordinate sets of d(CGCGAATTCGCG) on the 1BNA coordinate set. In both this figure and Figure 7, 233d refers to the refined coordinates of d(CGCGAASSCGCG) as deposited in the PDB.


Figure 5 . A schematic representation of the sugar-phosphate backbone of d(CGCGAASCGCG) in the region of the 4'-thio-2'-deoxythymidine moieties showing the average deviation (in Å) between each atom and its counterpart in the 1BNA structure of the native d(CGCGAATTCGCG).

There are few other differences in structure between d(CGCGAASSCGCG) and its native analogue. However, there is an increase in helical rise at base step 6 (Fig. 6 a) in the modified duplex which is coupled with a decrease in helical twist at the same base step (Fig. 6 b). As the base step in question is the 5'-ApS-3' step it would appear that this local change in conformation of the duplex is a direct result of the incorporation of sulphur into each strand.

Examination (Table 1 ) of cross-strand phosphorus-phosphorus distances in d(CGCGAASSCGCG) appears to suggest that compared with d(CGCGAATTCGCG) the width of the minor groove increases in the vicinity of the 4'-thionucleotides. This is sensible, in that in order to accommodate the larger 4'-thio'-2'- deoxyribose groups cross-strand phosphate groups will tend to be further apart. However, if we define minor groove width by measuring cross-strand O4'-O4', O4'-S4' or S4'-S4' distances (Table 2 ) we can see that in d(CGCGAASSCGCG) there appears to be a slight narrowing of the minor groove with respect to that in d(CGCGATTCGCG). In the region of the 4-thiosugars it is tempting to say that this apparent narrowing of the groove is due to the increased van der Waals radius of sulphur compared with oxygen. However, as the narrowing is observed at all points at which the minor groove is measured, it may be that it is a result of the refinement procedure used. Given that the average difference in minor groove width is only 0.5 Å, it is probable that incorporation of 4-thiosugars into this oligonucleotide has not significantly modified the accessibility of the floor of the minor groove and that potential protein-DNA interactions in this area are unlikely to be affected.

Table 3 details the values of the sugar-phosphate backbone torsion angles in the structures of both the modified and native dodecamers. It shows that there are a number of differences in the torsion angle values for the two structures, particularly in the regions containing the 4'-thiosugars (residues S7, S8, S19 and S20). Although there is no real consistency in the differences over both strands, there is a suggestion of an increase in the value of the torsion angle [delta] for the residues which have 4'-thiosugars. This is indicative of a change in the sugar conformations of the modified residues on going from the native to the modified duplex. This indication is supported if one examines the deoxyribose pseudorotation phase angles ( P ) in the structure of d(CGCGAASSCGCG) (Table 1 ).

For all the modified sugars the average value of P is 197o, which is close to those values (178o and 180o) found in the crystal structures of two 4'-thio-2'-deoxynucleosides ( 3 ), but much higher than the average value of P (116o) found for the analogous residues in the crystal structure of d(CGCGAATTCGCG) ( 9 ). The values of P suggest ( 19 ) that the 4'-thiosugars have a conformation close to C 3' - exo , rather than the approximate C 1' - exo found for the analogous sugars in the native structure.

This observation is supported if we compare the pseudorotaion angles in d(CGCGAASSCGCG) with those in the 2BNA ( 16 ), 7BNA ( 17 ) and 9DNA ( 18 ) native structures (Fig. 7 a). In each case the pseudorotation angle for the modified sugars is greater than those of the analagous sugars in the native dodecamer, regardless of the refinement technique used or the temperature at which the native structure was determined. Moreover, the values of the pseudorotation angles in the 2BNA, 7BNA and 9BNA native structures closely mimic those of the 1BNA structure (Fig. 7 a).

A surprising observation in the structure of d(CGCGAASSCGCG) is that the sugar puckering amplitude ([tau]) of the 4'-thio-2'-deoxyribose groups appears to be generally lower than those for the analagous sugars in the structures of the native oligonucleotide (Fig. 7 b). The cause of our suprise is that one might reasonably expect that in 4'-thiosugars the increase in the length of the C-S bonds with respect to the C-O bonds in unmodified sugars would lead to an increase in the sugar puckering amplitude. Indeed, such an increase is observed if one compares [tau] in the structures of 4'-thiothymidine (47.9o) and ( E )-5-(2-bromovinyl)-2'-deoxy-4'- thiouridine (48.6o) ( 3 ) with that of free thymidine (37.8o) ( 20 ).


Figure 6 . Comparison of individual values of ( a ) helical rise and ( b ) helical twist in the structures of d(CGCGAASSCGCG) ([diamonds]) and the 1BNA structure of d(CGCGAATTCGCG) (+).


Table 1 A comparison of cross-strand phosphorus-phosphorus distances (Å) which define minor groove width in d(CGCGAASSCGCG) and d(CGCGA- ATTCGCG) (1BNA)

d(CGCGAATTCGCG)

d(CGCGAASSCGCG)

P5-P24

8.7

8.9

P6-P23

7.2

7.2

P7-P22

5.3

5.2

P8-P21

4.2

4.9

P9-P20

4.0

5.2

P10-P19

3.1

4.1

P11-P18

5.2

5.2

P12-P17

5.1

4.9

In order to take into account the van der Waals radius of a phosphate group the distance quoted is that measured less 5.8 Å.

Table 2 A comparison of cross-strand O4'-O4', O4'-S4' and S4'-S4' distances (Å) which define minor groove width in d(CGCGAASSCGCG) and the 1BNA structure of d(CGCGAATTCGCG)

d(CGCGAATTCGCG)

d(CGCGAASSCGCG)

O4'(4)-O4'(24)

7.0

6.8

O4'(5)-O4'(23)

6.9

6.0

O4'(6)-O4'(22)

5.9

6.1

S4'(7)-O4'(21) a

4.6

4.1

S4'(8)-S4'(20) a

4.3

3.7

O4'(9)-S4'(19) a

3.7

3.2

O4'(10)-O4'(18)

4.7

4.4

O4'(11)-O4'(17)

4.5

3.8

O4'(12)-O4'(16)

5.9

6.3

In order to take into account the van der Waals radii of the atoms the distances quoted are those measured less 2.8, 3.25 and 3.7 Å respectively. a In d(CGCGAATTCGCG) the S4' atoms are, in fact, O4' atoms


Figure 7 . Comparisons of the values of ( a ) pseudorotation angle and ( b ) sugar puckering amplitude ([tau]) found in the structure of d(CGCGAASSCGCG) and in the 1BNA, 2BNA, 7BNA and 9BNA structures of d(CGCGAATTCGCG).


Do the observed differences between the native and the modified oligonucleotide structures help to explain the resistance to digestion by restriction endonucleases of oligonucleotides containing 4'-thiosugars? The extremely high specificity of restriction enzymes is due to two major types of interaction between the enzyme and its cognate DNA sequence ( 19 ). These are: (i) direct readout of the base sequence of the cognate DNA resulting from interactions between the enzyme and the major groove functional groups of the DNA; (ii) indirect readout of the base sequence of the cognate DNA which occurs via interactions between the endonuclease and the sugar-phosphate backbone of the DNA. In addition to these modes of inducing sequence specificity there are also non-sequence-specific interactions between the protein and the sugar-phosphate backbone of the DNA which usually help to increase the overall binding affinity of the DNA for the protein.

In some cases these interactions can only occur if there is a distortion of the DNA sequence from the canonical B-form and it had been suggested ( 7 ) that the presence of thiosugars in oligonucleotides would `rigidify' them and mean that the sequences could not undergo the distortion required for them to be good substrates for their restriction endonuclease. However, analysis of the structure of Eco RV endonuclease complexed with a thiosugar-modified cognate DNA sequence (Kostrewa,D., Hancox,E.L., Walker,R.T., Connolly,B.A. and Winkler,F.K., unpublished results) has shown that the DNA adopts the same kinked structure observed in the complex of the endonuclease with an unmodified cognate DNA sequence ( 8 ), but, crucially, that the Mg 2+ ion, which is an absolute requirement for endonuclease activity, is not present.

Table 3 . Sugar-phosphate backbone and glycosyl torsion angles, pseudorotation phase angles ( P ) and sugar puckering amplitudes ([tau]) for the structures of d(CGCGAASSCGCG) and d(CGCGAATTCGCG) (1BNA)
Residue

[alpha]

[beta]

[gamma]

[delta]

[epsilon]

[zeta]

[chi]

P

[tau]

C1

154

172

213

200

272

181

50

174

157

218

216

255

161

60

G2

312

152

36

144

207

221

248

147

43

295

170

40

128

174

262

249

140

43

C3

312

134

58

83

199

260

215

42

46

298

172

59

98

183

272

225

93

39

G4

312

163

49

159

199

215

268

175

42

297

180

57

155

205

208

268

167

52

A5

304

164

49

147

198

248

250

166

37

317

143

53

119

180

268

234

129

48

A6

286

171

56

119

186

267

247

133

34

287

180

66

121

174

272

238

127

52

S7

273

171

66

138

261

175

288

178

27

303

181

52

99

174

274

232

101

49

S8

69

229

195

151

205

214

262

218

30

301

174

64

109

170

271

234

116

51

C9

56

132

318

159

198

256

266

181

36

302

180

61

129

203

266

241

141

49

G10

292

183

40

156

265

145

281

179

42

293

169

47

143

257

150

270

146

58

C11

286

145

45

147

200

258

251

166

42

286

139

56

136

198

271

235

148

50

G12

287

177

51

97

262

102

35

279

176

57

111

248

113

54

C13

57

156

251

193

238

163

43

56

137

201

234

232

153

45

G14

298

137

43

145

203

218

248

141

46

309

164

49

122

178

267

244

128

47

C15

316

129

62

82

200

262

226

48

43

297

169

61

86

175

262

226

68

45

G16

298

157

73

123

151

283

248

146

27

291

171

73

136

174

262

245

149

42

A17

286

198

58

151

195

213

252

158

42

303

190

54

146

177

263

254

169

45

A18

56

181

282

193

225

200

254

205

44

303

186

48

130

174

259

251

146

45

S19

297

132

48

141

238

217

286

194

37

302

173

60

109

179

272

228

116

49

S20

285

129

68

134

197

265

267

199

24

301

179

55

122

179

266

240

129

52

C21

278

196

53

126

191

264

258

139

34

301

185

45

110

183

274

246

114

44

G22

292

180

41

156

240

172

288

176

42

293

179

50

150

260

171

271

156

54

C23

304

161

28

133

189

245

260

176

32

289

138

45

113

186

263

235

117

46

G24

310

143

55

73

223

24

44

295

171

47

79

225

35

48

Values for d(CGCGAASSCGCG) are given on the first line and for d(CGCGAATTCGCG) on the second line in italic. All angles are in degrees. All parameters were calculated using the NEWHEL92 program distrubuted by R.E.Dickerson through the Brookhaven Protein Data Bank (15).

This observation, coupled with the fact that our analysis of the structure of d(CGCGAASSCGCG) reveals that the major effect of incorporation of 4'-thio-2'-deoxyribose groups into a DNA duplex is to change its backbone conformation, suggests the following reasons for the resistance to nuclease digestion of oligonucleotides containing 4'-thiosugars. (i) Changes in the backbone conformation result in the enzyme being able to bind less well to the modified DNA than to its unmodified cognate sequence, thus causing a reduction in activity of the endonuclease; (ii) changes in backbone conformation resulting from DNA modification cause a reduction in Mg 2+ ion binding, which again would result in a reduction in the activity of the enzyme. The decision as to which, if either, of these two hypotheses is correct would require further analysis of the structures of 4'-thiosugar-modified DNAs, both in isolation and, more importantly, complexed to their specific restriction endonucleases.

We conclude with the observation that the inclusion of 4'-deoxy-2'-thiothymidine into DNA has a small, but detectable, effect on the backbone conformation of a DNA duplex. On occasions this may appear to be of little significance, but should it be associated with the conferring of increased nuclease resistance or increased lipophicity it may make such oligodeoxynucleotides candidates for antisense molecules.

ACKNOWLEDGEMENTS

This work was supported by the United Kingdom Engineering and Physical Sciences Research Council, the Biotechnology and Biology Science Research Council and the Wellcome Trust. We are grateful to the Wellcome Foundation for financial support (to ELH). We thank Drs Miroslav Papiz and Pierre Rizkallah of the Synchrotron Radiation Source, Daresbury Laboratory, for the allocation of contingency beam time, part of which was used to collect the data described here. TB wishes to thank the Royal Society of Edinburgh for a Caledonian Research Fellowship.

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* To whom correspondence should be addressed

+ Present address: Department of Chemistry, University of Southampton, Highfield, Southampton SO19 5NH, UK
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