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In contrast to Se[CH2C(O)OH]2 versus S[CH2C(O)OH]2, the title compound, Se[CH2CH2C(O)OH]2 or C6H10O4Se, is structurally quite similar to its sulfur analogue. The mol­ecule has twofold symmetry. The C-Se-C bond angle is 96.48 (8)° and the Se-C bond lengths are 1.9610 (14) Å. The shortest Se...O intermolecular distance is 3.5410 (11) Å. The O...O distances in the carboxyl­ic acid dimers are 2.684 (2) Å. The temperature dependence of the IR spectrum suggests tautomerism in the solid state.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S0108270100021077/os1132sup1.cif
Contains datablocks global, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108270100021077/os1132Isup2.hkl
Contains datablock I

CCDC reference: 163918

Computing details top

Data collection: SMART (Bruker, 1999); cell refinement: SAINT (Bruker, 1998); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 1990); program(s) used to refine structure: SHELXTL (Sheldrick, 1997); molecular graphics: SHELXTL; software used to prepare material for publication: SHELXTL.

3,3'-Selenobis(propionic acid) top
Crystal data top
C6H10O4Se? # Insert any comments here.
Mr = 225.10Dx = 1.859 Mg m3
Orthorhombic, PbcnMelting point: 148° C K
Hall symbol: -P 2n 2abMo Kα radiation, λ = 0.71073 Å
a = 8.5981 (3) ÅCell parameters from 8192 reflections
b = 5.1355 (2) Åθ = 2.2–33.2°
c = 18.2159 (7) ŵ = 4.63 mm1
V = 804.33 (5) Å3T = 253 K
Z = 4Flat prism, colourless
F(000) = 4480.33 × 0.25 × 0.07 mm
Data collection top
Bruker AXS SMART 2K CCD
diffractometer
1481 independent reflections
Radiation source: normal focus sealed tube1149 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.023
ω scansθmax = 33.2°, θmin = 2.2°
Absorption correction: numerical
(SHELXTL; Sheldrick 1997)
h = 1313
Tmin = 0.296, Tmax = 0.724k = 77
13334 measured reflectionsl = 2626
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)] = 0.023H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.061 w = 1/[σ2(Fo2) + (0.0307P)2 + 0.1506P]
where P = (Fo2 + 2Fc2)/3
S = 1.15(Δ/σ)max < 0.001
1481 reflectionsΔρmax = 0.43 e Å3
56 parametersΔρmin = 0.54 e Å3
1 restraintExtinction correction: SHELXTL (Sheldrick, 1997), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.0075 (9)
Special details top

Experimental. ? #Insert any special details here.

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
Se0.00000.18817 (4)0.25000.02676 (8)
O10.07447 (15)0.8829 (2)0.07928 (6)0.0362 (3)
O20.13517 (14)0.7398 (3)0.01856 (7)0.0379 (3)
H20.114 (3)0.858 (4)0.0087 (12)0.052 (6)*
C10.06493 (16)0.4425 (3)0.17578 (8)0.0258 (3)
H1A0.14550.36710.14520.039*
H1B0.10790.59480.19990.039*
C20.07177 (16)0.5231 (3)0.12815 (8)0.0282 (3)
H2A0.15480.58460.15970.042*
H2B0.10990.37080.10230.042*
C30.03509 (17)0.7322 (3)0.07267 (9)0.0247 (3)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Se0.03895 (13)0.02022 (10)0.02111 (11)0.0000.00105 (8)0.000
O10.0414 (6)0.0361 (6)0.0310 (6)0.0112 (5)0.0049 (5)0.0081 (5)
O20.0415 (6)0.0388 (6)0.0333 (6)0.0074 (5)0.0118 (5)0.0142 (5)
C10.0266 (6)0.0274 (7)0.0234 (6)0.0015 (6)0.0004 (5)0.0031 (5)
C20.0265 (6)0.0308 (7)0.0273 (7)0.0005 (6)0.0003 (5)0.0075 (6)
C30.0269 (6)0.0254 (6)0.0218 (6)0.0026 (5)0.0011 (5)0.0002 (5)
Geometric parameters (Å, º) top
Se—C1i1.9610 (14)C2—H2A0.9700
Se—C11.9610 (14)C2—H2B0.9700
C1—C21.518 (2)O1—C31.225 (2)
C1—H1A0.9700O2—C31.3091 (18)
C1—H1B0.9700O2—H20.804 (19)
C2—C31.508 (2)
C1i—Se—C196.48 (8)C3—C2—H2A108.6
C3—O2—H2109.9 (16)C1—C2—H2A108.6
C2—C1—Se110.80 (10)C3—C2—H2B108.6
C2—C1—H1A109.5C1—C2—H2B108.6
Se—C1—H1A109.5H2A—C2—H2B107.6
C2—C1—H1B109.5O1—C3—O2124.11 (15)
Se—C1—H1B109.5O1—C3—C2123.02 (14)
H1A—C1—H1B108.1O2—C3—C2112.84 (13)
C3—C2—C1114.52 (12)
C1i—Se—C1—C287.04 (10)C1—C2—C3—O122.4 (2)
Se—C1—C2—C3176.08 (11)C1—C2—C3—O2159.64 (14)
Symmetry code: (i) x, y, z+1/2.
Selected torsion angles (°) for S(CH2CH2C(O)OH)2 (Prout &amp; Hernandez-Cassou, 1982) top
C1-S-C1-C285.0 (2)
S-C1-C2-C3-176.0 (2)
C1-C2-C3-O121.6 (2)
C1-C2-C3-O2-160.6 (2)
 

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