Buy article online - an online subscription or single-article purchase is required to access this article.
In the title compound, C
7H
4ClNO
4, the molecules form centrosymmetric dimers through O—H
O hydrogen bonds. The dimers are connected by C—H
O hydrogen bonds to form molecular tapes. Disorder of the H atom in the O—H
O hydrogen bond is suggested.
Supporting information
CCDC reference: 227903
Key indicators
- Single-crystal X-ray study
- T = 297 K
- Mean (C-C) = 0.002 Å
- R factor = 0.033
- wR factor = 0.087
- Data-to-parameter ratio = 13.4
checkCIF/PLATON results
No syntax errors found
Alert level A
PLAT052_ALERT_1_A (Proper) Absorption Correction Method Missing .. ?
Alert level B
PLAT222_ALERT_3_B Large Non-Solvent H Ueq(max)/Ueq(min) ... 4.66 Ratio
| Author Response: see _publ_section_comment
|
Alert level C
PLAT057_ALERT_3_C Correction for Absorption Required RT(exp) = 1.15
PLAT355_ALERT_3_C Long O-H Bond (0.82A) O2 - H4 = 1.04 Ang.
PLAT417_ALERT_2_C Short Inter D-H..H-D H4 .. H4 = 2.10 Ang.
1 ALERT level A = In general: serious problem
1 ALERT level B = Potentially serious problem
3 ALERT level C = Check and explain
0 ALERT level G = General alerts; check
1 ALERT type 1 CIF construction/syntax error, inconsistent or missing data
1 ALERT type 2 Indicator that the structure model may be wrong or deficient
3 ALERT type 3 Indicator that the structure quality may be low
0 ALERT type 4 Improvement, methodology, query or suggestion
Data collection: MSC/AFC Diffractometer Control Software
(Molecular Structure Corporation, 1990); cell refinement: MSC/AFC Diffractometer Control Software; data reduction: TEXSAN for Windows (Molecular Structure Corporation, 1997-1999); program(s) used to solve structure: SIR92 (Altomare et al. 1994); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: ORTEP-3 (Farrugia, 1997); software used to prepare material for publication: TEXSAN for Windows.
Crystal data top
C7H4ClNO4 | F(000) = 408.00 |
Mr = 201.57 | Dx = 1.694 Mg m−3 |
Monoclinic, P21/c | Mo Kα radiation, λ = 0.71073 Å |
Hall symbol: -P 2ybc | Cell parameters from 25 reflections |
a = 7.404 (3) Å | θ = 11.8–12.4° |
b = 5.6695 (9) Å | µ = 0.46 mm−1 |
c = 19.144 (3) Å | T = 297 K |
β = 100.42 (2)° | Prismatic, colorless |
V = 790.4 (4) Å3 | 0.50 × 0.45 × 0.20 mm |
Z = 4 | |
Data collection top
Rigaku AFC-5R diffractometer | 1458 reflections with I > 2σ(I) |
Radiation source: Rigaku rotating anode | Rint = 0.011 |
Graphite monochromator | θmax = 27.5°, θmin = 2.2° |
ω–2θ scans | h = −1→9 |
Absorption correction: ψ scan (North et al., 1968) | k = 0→7 |
Tmin = 0.839, Tmax = 0.914 | l = −24→24 |
2234 measured reflections | 3 standard reflections every 97 reflections |
1815 independent reflections | intensity decay: 3.3% |
Refinement top
Refinement on F2 | Primary atom site location: structure-invariant direct methods |
Least-squares matrix: full | Secondary atom site location: difference Fourier map |
R[F2 > 2σ(F2)] = 0.033 | All H-atom parameters refined |
wR(F2) = 0.087 | w = 1/[σ2(Fo2) + (0.0175P)2 + 0.37P] where P = (Fo2 + 2Fc2)/3 |
S = 1.06 | (Δ/σ)max = 0.001 |
1815 reflections | Δρmax = 0.27 e Å−3 |
135 parameters | Δρmin = −0.19 e Å−3 |
0 restraints | Extinction correction: SHELXL97, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4 |
0 constraints | Extinction coefficient: 0.022 (2) |
Special details top
Experimental. The scan width was (1.68 + 0.30tanθ)° with an ω scan speed of 6° per minute
(up to 3 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. All e.s.d.'s (except the e.s.d. in the dihedral angle between two l.s. planes)
are estimated using the full covariance matrix. The cell e.s.d.'s are taken
into account individually in the estimation of e.s.d.'s in distances, angles
and torsion angles; correlations between e.s.d.'s in cell parameters are only
used when they are defined by crystal symmetry. An approximate (isotropic)
treatment of cell e.s.d.'s is used for estimating e.s.d.'s involving l.s.
planes. |
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 >
σ(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 | x | y | z | Uiso*/Ueq | |
Cl | −0.10139 (7) | 0.37469 (9) | 0.68248 (3) | 0.04677 (17) | |
O1 | 0.28058 (19) | −0.4635 (3) | 0.51224 (8) | 0.0511 (4) | |
O2 | 0.52851 (18) | −0.2484 (3) | 0.55339 (8) | 0.0499 (4) | |
O3 | 0.4487 (2) | 0.4707 (3) | 0.69530 (8) | 0.0578 (4) | |
O4 | 0.2740 (2) | 0.3787 (3) | 0.77033 (8) | 0.0562 (4) | |
N | 0.3218 (2) | 0.3616 (3) | 0.71286 (8) | 0.0383 (4) | |
C1 | 0.2472 (2) | −0.1339 (3) | 0.58417 (9) | 0.0322 (4) | |
C2 | 0.3319 (2) | 0.0424 (3) | 0.62893 (9) | 0.0318 (4) | |
C3 | 0.2254 (2) | 0.1895 (3) | 0.66192 (9) | 0.0311 (4) | |
C4 | 0.0348 (2) | 0.1732 (3) | 0.64910 (9) | 0.0322 (4) | |
C5 | −0.0482 (2) | −0.0042 (3) | 0.60515 (10) | 0.0372 (4) | |
C6 | 0.0570 (3) | −0.1580 (3) | 0.57377 (10) | 0.0369 (4) | |
C7 | 0.3579 (2) | −0.2939 (3) | 0.54748 (9) | 0.0354 (4) | |
H1 | 0.458 (3) | 0.065 (3) | 0.6390 (10) | 0.035 (5)* | |
H2 | −0.179 (3) | −0.016 (4) | 0.5960 (11) | 0.049 (6)* | |
H3 | 0.001 (3) | −0.277 (4) | 0.5440 (10) | 0.043 (6)* | |
H4 | 0.592 (6) | −0.377 (7) | 0.528 (2) | 0.163 (17)* | |
Atomic displacement parameters (Å2) top | U11 | U22 | U33 | U12 | U13 | U23 |
Cl | 0.0395 (3) | 0.0464 (3) | 0.0569 (3) | 0.0088 (2) | 0.0154 (2) | −0.0081 (2) |
O1 | 0.0406 (7) | 0.0521 (8) | 0.0612 (9) | −0.0039 (7) | 0.0105 (7) | −0.0268 (7) |
O2 | 0.0350 (7) | 0.0506 (9) | 0.0665 (9) | −0.0040 (6) | 0.0157 (6) | −0.0220 (7) |
O3 | 0.0561 (9) | 0.0504 (9) | 0.0658 (10) | −0.0214 (7) | 0.0082 (8) | −0.0084 (7) |
O4 | 0.0517 (8) | 0.0719 (11) | 0.0453 (8) | −0.0004 (8) | 0.0097 (7) | −0.0244 (8) |
N | 0.0347 (8) | 0.0341 (8) | 0.0440 (9) | 0.0018 (7) | 0.0016 (6) | −0.0072 (7) |
C1 | 0.0326 (8) | 0.0328 (9) | 0.0315 (8) | 0.0007 (7) | 0.0062 (7) | −0.0020 (7) |
C2 | 0.0278 (8) | 0.0331 (9) | 0.0343 (9) | 0.0004 (7) | 0.0048 (7) | −0.0016 (7) |
C3 | 0.0326 (8) | 0.0296 (8) | 0.0303 (8) | −0.0011 (7) | 0.0039 (7) | −0.0010 (7) |
C4 | 0.0327 (8) | 0.0325 (9) | 0.0331 (8) | 0.0037 (7) | 0.0107 (7) | 0.0019 (7) |
C5 | 0.0277 (8) | 0.0440 (10) | 0.0402 (10) | −0.0032 (8) | 0.0070 (7) | −0.0030 (8) |
C6 | 0.0348 (9) | 0.0385 (10) | 0.0374 (9) | −0.0064 (8) | 0.0064 (7) | −0.0071 (8) |
C7 | 0.0335 (9) | 0.0371 (9) | 0.0353 (9) | 0.0008 (7) | 0.0052 (7) | −0.0047 (7) |
Geometric parameters (Å, º) top
Cl—C4 | 1.7215 (18) | C2—C3 | 1.377 (2) |
C7—O1 | 1.252 (2) | C3—C4 | 1.391 (2) |
C7—O2 | 1.274 (2) | C4—C5 | 1.382 (3) |
N—O3 | 1.222 (2) | C5—C6 | 1.378 (3) |
N—O4 | 1.219 (2) | C2—H1 | 0.93 (2) |
N—C3 | 1.470 (2) | C5—H2 | 0.95 (2) |
C1—C2 | 1.390 (2) | C6—H3 | 0.93 (2) |
C1—C6 | 1.392 (3) | O2—H4 | 1.04 (4) |
C1—C7 | 1.482 (2) | | |
| | | |
Cl···O4i | 3.282 (2) | O3···C7iv | 3.091 (3) |
Cl···O4ii | 3.321 (2) | O3···O4v | 3.084 (3) |
O1···O2iii | 2.624 (2) | O4···C5ii | 3.219 (3) |
O3···C1iv | 3.260 (3) | C6···C6vi | 3.322 (3) |
| | | |
O1—C7—O2 | 123.54 (17) | C2—C3—C4 | 121.70 (16) |
O1—C7—C1 | 119.15 (16) | C2—C3—N | 117.19 (15) |
O2—C7—C1 | 117.30 (16) | C4—C3—N | 121.09 (15) |
C7—O2—H4 | 110 (2) | C5—C4—C3 | 118.77 (16) |
O4—N—O3 | 124.85 (16) | C5—C4—Cl | 118.86 (14) |
O4—N—C3 | 117.80 (16) | C3—C4—Cl | 122.29 (14) |
O3—N—C3 | 117.29 (15) | C6—C5—C4 | 120.10 (17) |
C2—C1—C6 | 119.38 (16) | C6—C5—H2 | 120.7 (13) |
C2—C1—C7 | 120.37 (16) | C4—C5—H2 | 119.2 (13) |
C6—C1—C7 | 120.25 (16) | C5—C6—C1 | 120.83 (17) |
C3—C2—C1 | 119.10 (16) | C5—C6—H3 | 120.2 (13) |
C3—C2—H1 | 117.4 (12) | C1—C6—H3 | 119.0 (13) |
C1—C2—H1 | 123.5 (12) | | |
| | | |
C6—C1—C2—C3 | −0.1 (3) | N—C3—C4—Cl | 8.5 (2) |
C7—C1—C2—C3 | 179.55 (16) | C3—C4—C5—C6 | −1.3 (3) |
C1—C2—C3—C4 | −3.0 (3) | Cl—C4—C5—C6 | 175.54 (14) |
C1—C2—C3—N | 175.53 (15) | C4—C5—C6—C1 | −1.7 (3) |
O4—N—C3—C2 | −132.61 (18) | C2—C1—C6—C5 | 2.4 (3) |
O3—N—C3—C2 | 44.7 (2) | C7—C1—C6—C5 | −177.20 (17) |
O4—N—C3—C4 | 45.9 (2) | C2—C1—C7—O1 | 174.02 (17) |
O3—N—C3—C4 | −136.79 (18) | C6—C1—C7—O1 | −6.3 (3) |
C2—C3—C4—C5 | 3.7 (3) | C2—C1—C7—O2 | −6.5 (3) |
N—C3—C4—C5 | −174.78 (16) | C6—C1—C7—O2 | 173.11 (18) |
C2—C3—C4—Cl | −173.02 (14) | | |
Symmetry codes: (i) −x, y−1/2, −z+3/2; (ii) −x, y+1/2, −z+3/2; (iii) −x+1, −y−1, −z+1; (iv) x, y+1, z; (v) −x+1, y+1/2, −z+3/2; (vi) −x, −y, −z+1. |
Hydrogen-bond geometry (Å, º) top
D—H···A | D—H | H···A | D···A | D—H···A |
O2—H4···O1iii | 1.04 (4) | 1.60 (4) | 2.624 (2) | 169 (4) |
C5—H2···O2vii | 0.95 (2) | 2.54 (2) | 3.406 (3) | 150.8 (18) |
Symmetry codes: (iii) −x+1, −y−1, −z+1; (vii) x−1, y, z. |
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.