Buy article online - an online subscription or single-article purchase is required to access this article.
Download citation
Download citation
link to html
rac-2,3-Di­bromo­succinic acid, C4H4Br2O4, is the product of the electrophilic addition of bromine to maleic acid. Whereas the carboxyl groups and the bromo ligands are in a gauche arrangement with respect to each other, the tertiary H atoms attached to the central C atoms are in a trans arrangement. The hydroxyl groups form hydrogen bonds with the carbonyl O atoms of neighbouring mol­ecules.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S0108270100010611/qd0022sup1.cif
Contains datablocks I, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108270100010611/qd0022Isup2.hkl
Contains datablock I

CCDC reference: 150744

Computing details top

Data collection: SMART (Siemens, 1995); cell refinement: SMART; data reduction: SAINT (Siemens, 1995); program(s) used to solve structure: SHELXS97 (Sheldrick, 1990); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997).

rac-Dibromosuccinic acid top
Crystal data top
C4H4Br2O4F(000) = 520
Mr = 275.89Dx = 2.462 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
a = 12.725 (4) ÅCell parameters from 512 reflections
b = 6.167 (1) Åθ = 1–20°
c = 10.228 (2) ŵ = 10.84 mm1
β = 111.98 (1)°T = 173 K
V = 744.3 (3) Å3Block, colourless
Z = 40.30 × 0.20 × 0.15 mm
Data collection top
Siemens CCD three-circle
diffractometer
1517 independent reflections
Radiation source: fine-focus sealed tube1356 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.073
ω scansθmax = 26.4°, θmin = 3.7°
Absorption correction: empirical (using intensity measurements)
(SADABS; Sheldrick, 1996)
h = 1515
Tmin = 0.090, Tmax = 0.193k = 77
12264 measured reflectionsl = 1212
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.031H-atom parameters constrained
wR(F2) = 0.081 w = 1/[σ2(Fo2) + (0.0464P)2 + 0.0831P]
where P = (Fo2 + 2Fc2)/3
S = 1.12(Δ/σ)max = 0.001
1517 reflectionsΔρmax = 1.16 e Å3
94 parametersΔρmin = 0.72 e Å3
0 restraintsExtinction correction: SHELXL97, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.0049 (8)
Special details top

Experimental. Coverage of the unique set is 100% complete to at least 26.5° in θ. Crystal decay was monitored by repeating the initial frames at the end of data collection and analyzing the duplicate reflections.

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
xyzUiso*/Ueq
C10.1415 (3)0.6347 (5)0.3116 (3)0.0143 (6)
O110.0819 (2)0.7357 (4)0.2070 (2)0.0184 (5)
O120.1182 (2)0.6008 (4)0.4248 (2)0.0179 (5)
H120.05620.66020.41470.021*
C20.2521 (3)0.5281 (5)0.3219 (3)0.0151 (7)
H20.26090.38660.37260.018*
Br20.37350 (3)0.72428 (6)0.43050 (4)0.02705 (17)
C30.2551 (3)0.4903 (5)0.1764 (3)0.0151 (7)
H30.25960.63270.13200.018*
Br30.38534 (3)0.31078 (7)0.18868 (4)0.02555 (17)
C40.1500 (3)0.3680 (5)0.0830 (3)0.0137 (7)
O410.0902 (2)0.2691 (4)0.1308 (2)0.0194 (5)
O420.1328 (2)0.3889 (4)0.0520 (2)0.0183 (5)
H420.07430.31970.10060.022*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.0092 (16)0.0152 (14)0.0161 (16)0.0031 (13)0.0021 (13)0.0023 (12)
O110.0120 (13)0.0243 (12)0.0149 (11)0.0031 (10)0.0005 (10)0.0022 (9)
O120.0128 (13)0.0236 (12)0.0193 (12)0.0056 (10)0.0084 (10)0.0029 (9)
C20.0076 (16)0.0218 (16)0.0142 (15)0.0011 (13)0.0022 (13)0.0014 (12)
Br20.0105 (2)0.0422 (3)0.0257 (2)0.00744 (16)0.00359 (17)0.01437 (16)
C30.0074 (16)0.0220 (17)0.0162 (15)0.0036 (13)0.0047 (13)0.0017 (12)
Br30.0101 (2)0.0407 (3)0.0236 (2)0.00869 (14)0.00387 (17)0.00464 (14)
C40.0059 (16)0.0169 (15)0.0172 (15)0.0048 (12)0.0030 (13)0.0007 (12)
O410.0114 (13)0.0262 (13)0.0205 (12)0.0059 (10)0.0057 (11)0.0022 (10)
O420.0143 (13)0.0240 (12)0.0125 (11)0.0026 (10)0.0001 (10)0.0008 (9)
Geometric parameters (Å, º) top
C1—O111.225 (4)C3—C41.521 (4)
C1—O121.315 (4)C3—Br31.957 (3)
C1—C21.520 (4)C3—H31.0000
O12—H120.8400C4—O411.212 (4)
C2—C31.522 (4)C4—O421.321 (4)
C2—Br21.950 (3)O42—H420.8400
C2—H21.0000
O11—C1—O12125.4 (3)C4—C3—C2110.6 (3)
O11—C1—C2122.3 (3)C4—C3—Br3106.5 (2)
O12—C1—C2112.2 (3)C2—C3—Br3110.8 (2)
C1—O12—H12109.5C4—C3—H3109.6
C1—C2—C3111.1 (2)C2—C3—H3109.6
C1—C2—Br2106.7 (2)Br3—C3—H3109.6
C3—C2—Br2110.3 (2)O41—C4—O42125.9 (3)
C1—C2—H2109.6O41—C4—C3122.3 (3)
C3—C2—H2109.6O42—C4—C3111.8 (3)
Br2—C2—H2109.6C4—O42—H42109.5
O11—C1—C2—C321.2 (4)C1—C2—C3—Br3170.5 (2)
O12—C1—C2—C3157.4 (3)Br2—C2—C3—Br371.4 (2)
O11—C1—C2—Br299.1 (3)C2—C3—C4—O4117.5 (4)
O12—C1—C2—Br282.3 (3)Br3—C3—C4—O41103.0 (3)
C1—C2—C3—C452.7 (4)C2—C3—C4—O42161.1 (3)
Br2—C2—C3—C4170.8 (2)Br3—C3—C4—O4278.5 (3)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O12—H12···O41i0.841.872.702 (3)172
O42—H42···O11ii0.841.912.706 (3)159
Symmetry codes: (i) x, y+1/2, z+1/2; (ii) x, y+1, z.
 

Subscribe to Acta Crystallographica Section C: Structural Chemistry

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