Buy article online - an online subscription or single-article purchase is required to access this article.
Download citation
Download citation
link to html
The structure of the title compound, C9H10N2O6S, has been determined as part of an ongoing investigation into the preparation of N-allyl-substituted amino acids suitable for alkene cross-metathesis reactions in the generation of combinatorial libraries. The conformational structure is determined by intra- and intermolecular N—H...O and C—H...O hydrogen-bonding interactions.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536805000784/nc6016sup1.cif
Contains datablocks global, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536805000784/nc6016Isup2.hkl
Contains datablock I

CCDC reference: 263692

Key indicators

  • Single-crystal X-ray study
  • T = 295 K
  • Mean [sigma](C-C) = 0.005 Å
  • R factor = 0.050
  • wR factor = 0.206
  • Data-to-parameter ratio = 12.5

checkCIF/PLATON results

No syntax errors found



Alert level C PLAT340_ALERT_3_C Low Bond Precision on C-C bonds (x 1000) Ang ... 5
0 ALERT level A = In general: serious problem 0 ALERT level B = Potentially serious problem 1 ALERT level C = Check and explain 0 ALERT level G = General alerts; check 0 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 0 ALERT type 2 Indicator that the structure model may be wrong or deficient 1 ALERT type 3 Indicator that the structure quality may be low 0 ALERT type 4 Improvement, methodology, query or suggestion

Computing details top

Data collection: MSC/AFC7 Diffractometer Control Software for Windows (Molecular Structure Corporation, 1999); cell refinement: MSC/AFC7 Diffractometer Control Software for Windows; data reduction: TEXSAN for Windows (Molecular Structure Corporation, 2001); program(s) used to solve structure: TEXSAN for Windows; program(s) used to refine structure: TEXSAN for Windows and SHELXL97 (Sheldrick, 1997); molecular graphics: PLATON (Spek, 2001) and ORTEP-3 (Farrugia, 1997); software used to prepare material for publication: TEXSAN for Windows and PLATON.

N-(2-Nitrophenylsulfonyl)glycine methyl ester top
Crystal data top
C9H10N2O6SF(000) = 568
Mr = 274.26Dx = 1.579 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.7107 Å
Hall symbol: -P 2ybcCell parameters from 25 reflections
a = 19.805 (3) Åθ = 12.6–15.8°
b = 7.988 (2) ŵ = 0.30 mm1
c = 7.369 (2) ÅT = 295 K
β = 98.18 (2)°Prism, colorless
V = 1153.9 (5) Å30.50 × 0.30 × 0.30 mm
Z = 4
Data collection top
Rigaku AFC-7R
diffractometer
Rint = 0.035
Radiation source: Rigaku rotating-anodeθmax = 25.0°, θmin = 2.8°
Graphite monochromatorh = 1123
ω–2θ scansk = 09
2280 measured reflectionsl = 88
2037 independent reflections3 standard reflections every 150 reflections
1621 reflections with I > 2σ(I) intensity decay: 0.3%
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.050Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.206H-atom parameters constrained
S = 1.09 w = 1/[σ2(Fo2) + (0.1367P)2 + 0.8688P]
where P = (Fo2 + 2Fc2)/3
2037 reflections(Δ/σ)max < 0.001
163 parametersΔρmax = 0.40 e Å3
0 restraintsΔρmin = 0.56 e Å3
Special details top

Experimental. The scan width was (1.79 + 0.30tanθ)° with an ω scan speed of 16° per minute (up to 4 scans to achieve I/σ(I) > 10). Stationary background counts were recorded at each end of the scan, and the scan time:background time ratio was 2:1.

Geometry. Bond distances, angles etc. have been calculated using the rounded fractional coordinates. All e.s.d.'s are estimated from the variances of the (full) variance-covariance matrix. The cell e.s.d.'s are taken into account in the estimation of distances, angles and torsion angles

Refinement. Refinement of F2 against ALL reflections. The weighted R-factor wR and goodness of fit S are based on F2, conventional R-factors R are based on F, with F set to zero for negative F2. The threshold expression of F2 > 2σ(F2) is used only for calculating R-factors(gt) etc. and is not relevant to the choice of reflections for refinement. R-factors based on F2 are statistically about twice as large as those based on F, and R-factors based on ALL data will be even larger.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
S10.26243 (4)0.50077 (10)0.93936 (12)0.0373 (3)
O10.13296 (18)0.6575 (4)1.0531 (5)0.0650 (11)
O20.05205 (17)0.6008 (5)0.8356 (6)0.0808 (14)
O30.23320 (16)0.6311 (4)0.8198 (4)0.0580 (10)
O40.31893 (14)0.4074 (4)0.8945 (4)0.0561 (10)
O50.40773 (16)0.7240 (4)1.0891 (5)0.0626 (11)
O60.46370 (13)0.5366 (3)1.2802 (4)0.0492 (9)
N10.28386 (15)0.5743 (4)1.1414 (4)0.0433 (10)
N20.10259 (16)0.5631 (4)0.9403 (5)0.0474 (11)
C10.19546 (17)0.3520 (4)0.9502 (4)0.0304 (9)
C20.12700 (18)0.3902 (4)0.9360 (5)0.0356 (10)
C30.0775 (2)0.2660 (6)0.9238 (6)0.0493 (12)
C40.0976 (2)0.1003 (5)0.9307 (6)0.0526 (14)
C50.1653 (2)0.0596 (5)0.9479 (5)0.0483 (14)
C60.2140 (2)0.1844 (4)0.9570 (5)0.0404 (11)
C70.34658 (19)0.5296 (5)1.2533 (5)0.0413 (11)
C80.40842 (19)0.6104 (4)1.1944 (5)0.0397 (11)
C90.5291 (2)0.6045 (6)1.2505 (8)0.0651 (18)
H10.261600.657901.170700.0690*
H30.030700.294300.911600.0630*
H40.065200.013300.922900.0640*
H50.178800.054700.954800.0580*
H60.261000.155000.967800.0480*
H7A0.343700.562501.377000.0520*
H7B0.351500.412301.248200.0520*
H9A0.527400.628701.122700.0780*
H9B0.563500.525201.286600.0780*
H9C0.537300.704301.318600.0780*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
S10.0389 (6)0.0343 (6)0.0395 (6)0.0076 (3)0.0084 (4)0.0030 (3)
O10.075 (2)0.0358 (16)0.081 (2)0.0085 (15)0.0001 (17)0.0085 (15)
O20.050 (2)0.075 (2)0.109 (3)0.0242 (17)0.0174 (19)0.006 (2)
O30.067 (2)0.0490 (16)0.0551 (17)0.0197 (14)0.0009 (14)0.0187 (14)
O40.0439 (15)0.0622 (19)0.0663 (19)0.0108 (13)0.0216 (13)0.0237 (15)
O50.0591 (18)0.0516 (18)0.073 (2)0.0089 (14)0.0044 (15)0.0255 (16)
O60.0413 (15)0.0371 (14)0.0674 (18)0.0000 (11)0.0016 (13)0.0082 (13)
N10.0393 (17)0.0395 (18)0.0493 (18)0.0017 (13)0.0003 (13)0.0136 (14)
N20.0436 (18)0.0396 (18)0.059 (2)0.0051 (15)0.0069 (15)0.0021 (16)
C10.0333 (17)0.0296 (16)0.0282 (15)0.0031 (13)0.0042 (12)0.0022 (12)
C20.0384 (18)0.0327 (18)0.0356 (17)0.0014 (14)0.0052 (14)0.0007 (14)
C30.040 (2)0.056 (2)0.052 (2)0.0110 (18)0.0072 (16)0.0018 (19)
C40.066 (3)0.043 (2)0.050 (2)0.025 (2)0.0123 (19)0.0033 (18)
C50.073 (3)0.0294 (19)0.042 (2)0.0084 (18)0.0062 (18)0.0022 (16)
C60.050 (2)0.0320 (18)0.0395 (18)0.0020 (15)0.0076 (15)0.0026 (15)
C70.042 (2)0.0376 (18)0.0436 (19)0.0057 (15)0.0033 (16)0.0025 (15)
C80.046 (2)0.0290 (17)0.0433 (19)0.0016 (15)0.0039 (15)0.0001 (15)
C90.040 (2)0.055 (3)0.099 (4)0.006 (2)0.005 (2)0.010 (3)
Geometric parameters (Å, º) top
S1—O31.432 (3)C2—C31.389 (6)
S1—O41.422 (3)C3—C41.381 (6)
S1—N11.601 (3)C4—C51.368 (6)
S1—C11.791 (3)C5—C61.382 (5)
O1—N21.216 (5)C7—C81.502 (5)
O2—N21.212 (5)C3—H30.9458
O5—C81.193 (5)C4—H40.9421
O6—C81.322 (5)C5—H50.9507
O6—C91.449 (5)C6—H60.9523
N1—C71.435 (5)C7—H7A0.9581
N2—C21.465 (5)C7—H7B0.9433
N1—H10.8450C9—H9A0.9573
C1—C61.387 (5)C9—H9B0.9405
C1—C21.379 (5)C9—H9C0.9437
S1···O13.075 (4)O5···H7Avi2.5289
S1···O53.431 (3)O6···H9Cx2.7517
O1···S13.075 (4)N1···O13.040 (5)
O1···O32.813 (5)N1···O52.805 (4)
O1···N13.040 (5)N1···O3iii2.941 (4)
O1···C5i3.387 (5)N2···O32.903 (5)
O1···C5ii3.369 (5)C3···O2xi3.253 (6)
O1···O3iii3.090 (5)C4···O2xi3.314 (6)
O2···C4iv3.314 (6)C5···O1xii3.387 (5)
O2···C3iv3.253 (6)C5···O1v3.369 (5)
O3···N22.903 (5)C5···O3ii3.254 (5)
O3···O12.813 (5)C7···O5iii3.257 (5)
O3···C5v3.254 (5)C8···O43.089 (5)
O3···N1vi2.941 (4)C8···O5iii3.197 (5)
O3···O1vi3.090 (5)C9···O4vii3.335 (5)
O4···C83.089 (5)C7···H6ii2.8823
O4···C9vii3.335 (5)H1···O12.5717
O5···S13.431 (3)H1···O3iii2.1307
O5···N12.805 (4)H3···O22.5600
O5···C7vi3.257 (5)H3···O2xi2.7466
O5···C8vi3.197 (5)H3···O2viii2.7797
O1···H5i2.6117H4···O2xi2.8724
O1···H12.5717H5···O1xii2.6117
O2···H4iv2.8724H5···O3ii2.8183
O2···H3iv2.7466H6···O42.4185
O2···H32.5600H6···C7v2.8823
O2···H3viii2.7797H6···H7Av2.5417
O3···H1vi2.1307H7A···O5iii2.5289
O3···H5v2.8183H7A···H6ii2.5417
O4···H7B2.5947H7B···O42.5947
O4···H62.4185H7B···O4ii2.8805
O4···H9Bvii2.8942H9A···O52.4680
O4···H7Bv2.8805H9B···O5x2.6084
O5···H9Bix2.6084H9B···O4vii2.8942
O5···H9A2.4680H9C···O52.8697
O5···H9C2.8697H9C···O6ix2.7517
O3—S1—O4120.06 (18)N1—C7—C8113.7 (3)
O3—S1—N1109.64 (17)O6—C8—C7108.9 (3)
O3—S1—C1105.83 (17)O5—C8—O6125.6 (4)
O4—S1—N1107.18 (17)O5—C8—C7125.5 (4)
O4—S1—C1105.93 (17)C2—C3—H3120.58
N1—S1—C1107.58 (15)C4—C3—H3120.40
C8—O6—C9117.2 (3)C3—C4—H4120.96
S1—N1—C7122.4 (3)C5—C4—H4118.72
O1—N2—O2124.4 (4)C4—C5—H5119.85
O1—N2—C2117.8 (3)C6—C5—H5120.07
O2—N2—C2117.8 (3)C1—C6—H6119.44
C7—N1—H1119.36C5—C6—H6119.56
S1—N1—H1116.66N1—C7—H7A108.34
C2—C1—C6117.9 (3)N1—C7—H7B108.07
S1—C1—C6116.6 (3)C8—C7—H7A108.57
S1—C1—C2125.2 (3)C8—C7—H7B108.80
N2—C2—C1122.1 (3)H7A—C7—H7B109.32
N2—C2—C3116.3 (3)O6—C9—H9A108.48
C1—C2—C3121.6 (3)O6—C9—H9B109.40
C2—C3—C4119.0 (4)O6—C9—H9C109.01
C3—C4—C5120.3 (4)H9A—C9—H9B109.69
C4—C5—C6120.1 (4)H9A—C9—H9C109.38
C1—C6—C5121.0 (4)H9B—C9—H9C110.83
O3—S1—N1—C7138.5 (3)O2—N2—C2—C1139.5 (4)
O4—S1—N1—C76.7 (3)S1—C1—C2—C3172.2 (3)
C1—S1—N1—C7106.9 (3)S1—C1—C6—C5173.7 (3)
O3—S1—C1—C231.3 (3)C6—C1—C2—N2175.8 (3)
O3—S1—C1—C6142.6 (3)C6—C1—C2—C31.7 (5)
O4—S1—C1—C2159.8 (3)S1—C1—C2—N210.3 (5)
O4—S1—C1—C614.1 (3)C2—C1—C6—C50.7 (5)
N1—S1—C1—C285.8 (3)C1—C2—C3—C41.6 (6)
N1—S1—C1—C6100.2 (3)N2—C2—C3—C4176.0 (4)
C9—O6—C8—C7176.1 (3)C2—C3—C4—C50.5 (6)
C9—O6—C8—O53.1 (6)C3—C4—C5—C60.5 (6)
S1—N1—C7—C874.4 (4)C4—C5—C6—C10.4 (6)
O1—N2—C2—C3134.6 (4)N1—C7—C8—O513.4 (5)
O1—N2—C2—C143.1 (5)N1—C7—C8—O6167.4 (3)
O2—N2—C2—C342.9 (5)
Symmetry codes: (i) x, y+1, z; (ii) x, y+1/2, z+1/2; (iii) x, y+3/2, z+1/2; (iv) x, y+1/2, z+3/2; (v) x, y+1/2, z1/2; (vi) x, y+3/2, z1/2; (vii) x+1, y+1, z+2; (viii) x, y+1, z+2; (ix) x+1, y+1/2, z+5/2; (x) x+1, y1/2, z+5/2; (xi) x, y1/2, z+3/2; (xii) x, y1, z.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N1—H1···O10.842.573.040 (5)116
N1—H1···O3iii0.842.132.941 (4)160
C6—H6···O40.952.422.824 (5)105
C7—H7A···O5iii0.962.533.257 (5)133
Symmetry code: (iii) x, y+3/2, z+1/2.
 

Subscribe to Acta Crystallographica Section E: Crystallographic Communications

The full text of this article is available to subscribers to the journal.

If you have already registered and are using a computer listed in your registration details, please email support@iucr.org for assistance.

Buy online

You may purchase this article in PDF and/or HTML formats. For purchasers in the European Community who do not have a VAT number, VAT will be added at the local rate. Payments to the IUCr are handled by WorldPay, who will accept payment by credit card in several currencies. To purchase the article, please complete the form below (fields marked * are required), and then click on `Continue'.
E-mail address* 
Repeat e-mail address* 
(for error checking) 

Format*   PDF (US $40)
   HTML (US $40)
   PDF+HTML (US $50)
In order for VAT to be shown for your country javascript needs to be enabled.

VAT number 
(non-UK EC countries only) 
Country* 
 

Terms and conditions of use
Contact us

Follow Acta Cryst. E
Sign up for e-alerts
Follow Acta Cryst. on Twitter
Follow us on facebook
Sign up for RSS feeds