addenda and errata\(\def\hfill{\hskip 5em}\def\hfil{\hskip 3em}\def\eqno#1{\hfil {#1}}\)

Journal logoCRYSTALLOGRAPHIC
COMMUNICATIONS
ISSN: 2056-9890

(S,S)-2,2′-(1,2-Ethanediyldi­imino)dibutan-1-ol. Corrigendum

CROSSMARK_Color_square_no_text.svg

aCollege of Chemistry & Environmental Science, Hebei University, Hebei 071002, People's Republic of China, and bSchool of Chemical Engineering and Technology, Tianjin University, Tianjin 300072, People's Republic of China
*Correspondence e-mail: baiguoyi@hotmail.com

(Received 17 September 2006; accepted 14 December 2006; online 20 December 2006)

In the paper by Bai, Zhang, Zhang, Zeng & Li [Acta Cryst. (2006), E62, o2173–o2174], the data relate to the R,R rather than the S,S enantiomer. The revised ellipsoid plot, packing diagram and selected geometrical data are given here.

[Figure 1]
Figure 1
The mol­ecular structure of (I), with the atom-numbering scheme and 30% probability displacement ellipsoids.
[Figure 2]
Figure 2
Packing diagram for (I), with hydrogen bonds shown as dashed lines.

2. Experimental

2.1.2. Data collection
  • Rint = 0.029

2.1.3. Refinement
  • w = 1/[σ2(Fo2) + (0.0546P)2 + 0.0456P] where P = (Fo2 + 2Fc2)/3

  • (Δ/σ)max = 0.002

  • Δρmax = 0.18 e Å−3

  • Δρmin = −0.17 e Å−3

Table 1
Selected geometric parameters (Å, °)

O1—C1 1.419 (3)
C2—N1—C5 115.4 (2)
N1—C2—C1 108.3 (2)
N1—C5—C6 109.7 (2)
O1—C1—C2—N1 −61.4 (3)
N1—C2—C3—C4 −162.1 (3)
N1—C5—C6—N2 173.0 (2)

Table 2
Hydrogen-bond geometry (Å, °)

D—H⋯A D—H H⋯A DA D—H⋯A
O1—H1⋯N2i 0.93 (5) 1.95 (5) 2.877 (3) 174 (3)
O2—H2B⋯N1ii 0.96 (4) 1.82 (4) 2.767 (3) 174 (3)
N1—H1C⋯O2iii 0.85 (3) 2.23 (3) 3.014 (3) 153 (3)
Symmetry codes: (i) [-x+1, y-{\script{1\over 2}}, -z+1]; (ii) [2-x, y+{\script{1\over 2}}, -z+1]; (iii) x-1, y, z.

Supporting information


Computing details top

Data collection: SMART (Bruker, 1997); cell refinement: SAINT (Bruker, 1997); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: SHELXTL (Bruker, 1997); software used to prepare material for publication: SHELXTL.

(S,S)-2,2'-(1,2-Ethanediyldiimino)bis-1-butanol top
Crystal data top
C10H24N2O2F(000) = 228
Mr = 204.31Dx = 1.107 Mg m3
Monoclinic, P21Mo Kα radiation, λ = 0.71073 Å
Hall symbol: P 2ybCell parameters from 1264 reflections
a = 7.157 (3) Åθ = 2.9–25.3°
b = 8.440 (4) ŵ = 0.08 mm1
c = 10.193 (5) ÅT = 294 K
β = 95.631 (8)°Block, colourless
V = 612.7 (5) Å30.22 × 0.20 × 0.10 mm
Z = 2
Data collection top
Bruker SMART-1000 CCD area detector
diffractometer
1318 independent reflections
Radiation source: fine-focus sealed tube1049 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.029
φ and ω scansθmax = 26.3°, θmin = 2.0°
Absorption correction: multi-scan
SADABS (Sheldrick, 1996)
h = 88
Tmin = 0.979, Tmax = 0.992k = 106
3317 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)] = 0.041H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.103 w = 1/[σ2(Fo2) + (0.0546P)2 + 0.0456P]
where P = (Fo2 + 2Fc2)/3
S = 1.07(Δ/σ)max = 0.002
1318 reflectionsΔρmax = 0.18 e Å3
141 parametersΔρmin = 0.17 e Å3
1 restraintAbsolute structure: Friedel pairs merged
Primary atom site location: structure-invariant direct methods
Special details top

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
O10.1972 (3)0.7636 (3)0.6659 (2)0.0496 (6)
H10.145 (5)0.667 (6)0.639 (3)0.074*
O21.3357 (3)1.0029 (3)0.39638 (19)0.0421 (5)
H2B1.376 (4)1.111 (5)0.400 (3)0.063*
N10.5708 (3)0.8209 (3)0.6068 (2)0.0303 (5)
H1C0.481 (4)0.845 (4)0.549 (3)0.036*
N20.9494 (3)0.9540 (3)0.4033 (2)0.0316 (5)
H2A1.036 (4)0.964 (4)0.473 (3)0.038*
C10.3535 (3)0.7352 (3)0.7597 (3)0.0373 (7)
H1A0.39620.62690.75140.045*
H1B0.31620.74890.84800.045*
C20.5125 (3)0.8485 (3)0.7386 (2)0.0319 (6)
H20.61880.81900.80190.038*
C30.4630 (4)1.0212 (4)0.7683 (3)0.0422 (7)
H3A0.55291.09070.73210.051*
H3B0.33981.04520.72440.051*
C40.4627 (6)1.0550 (5)0.9136 (3)0.0697 (11)
H4A0.58031.02250.95900.105*
H4B0.36230.99760.94770.105*
H4C0.44531.16650.92650.105*
C50.7343 (3)0.9135 (3)0.5739 (3)0.0356 (6)
H5A0.83450.90520.64480.043*
H5B0.69981.02430.56340.043*
C60.8011 (4)0.8520 (3)0.4479 (3)0.0348 (6)
H6A0.84920.74520.46190.042*
H6B0.69620.84770.38010.042*
C71.2165 (4)0.9866 (4)0.2782 (2)0.0394 (7)
H7A1.28660.94070.21090.047*
H7B1.17301.09040.24800.047*
C81.0489 (4)0.8826 (3)0.2974 (2)0.0342 (6)
H81.09350.77700.32540.041*
C90.9224 (4)0.8677 (4)0.1694 (3)0.0482 (8)
H9A0.80300.82360.18880.058*
H9B0.89840.97290.13330.058*
C101.0003 (5)0.7663 (6)0.0660 (3)0.0861 (15)
H10A1.04070.66640.10400.129*
H10B1.10520.81910.03340.129*
H10C0.90480.74860.00540.129*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O10.0365 (11)0.0386 (12)0.0726 (14)0.0050 (10)0.0011 (10)0.0063 (11)
O20.0349 (10)0.0396 (12)0.0505 (11)0.0049 (9)0.0030 (8)0.0096 (10)
N10.0256 (10)0.0333 (13)0.0319 (11)0.0017 (10)0.0018 (9)0.0012 (10)
N20.0311 (11)0.0287 (12)0.0356 (12)0.0047 (10)0.0056 (9)0.0016 (10)
C10.0386 (15)0.0332 (16)0.0416 (15)0.0007 (13)0.0120 (12)0.0038 (12)
C20.0333 (13)0.0322 (15)0.0305 (13)0.0050 (12)0.0040 (11)0.0025 (11)
C30.0461 (15)0.0341 (16)0.0472 (16)0.0037 (14)0.0087 (13)0.0033 (14)
C40.095 (3)0.058 (2)0.056 (2)0.019 (2)0.0038 (19)0.0184 (17)
C50.0331 (13)0.0349 (15)0.0393 (14)0.0063 (13)0.0062 (11)0.0039 (12)
C60.0341 (13)0.0305 (14)0.0407 (14)0.0052 (12)0.0081 (12)0.0011 (12)
C70.0369 (14)0.0418 (17)0.0403 (14)0.0066 (13)0.0080 (11)0.0022 (13)
C80.0348 (14)0.0293 (15)0.0395 (14)0.0025 (12)0.0091 (12)0.0013 (12)
C90.0426 (16)0.058 (2)0.0442 (16)0.0096 (16)0.0061 (13)0.0104 (15)
C100.075 (2)0.116 (4)0.070 (2)0.012 (3)0.019 (2)0.045 (3)
Geometric parameters (Å, º) top
O1—C11.419 (3)C4—H4B0.9600
O1—H10.93 (5)C4—H4C0.9600
O2—C71.412 (3)C5—C61.506 (4)
O2—H2B0.96 (4)C5—H5A0.9700
N1—C21.464 (3)C5—H5B0.9700
N1—C51.473 (3)C6—H6A0.9700
N1—H1C0.85 (3)C6—H6B0.9700
N2—C61.473 (3)C7—C81.515 (4)
N2—C81.478 (3)C7—H7A0.9700
N2—H2A0.90 (3)C7—H7B0.9700
C1—C21.518 (4)C8—C91.519 (4)
C1—H1A0.9700C8—H80.9800
C1—H1B0.9700C9—C101.507 (4)
C2—C31.536 (4)C9—H9A0.9700
C2—H20.9800C9—H9B0.9700
C3—C41.508 (4)C10—H10A0.9600
C3—H3A0.9700C10—H10B0.9600
C3—H3B0.9700C10—H10C0.9600
C4—H4A0.9600
C1—O1—H1109 (2)C6—C5—H5A109.7
C7—O2—H2B106.1 (19)N1—C5—H5B109.7
C2—N1—C5115.4 (2)C6—C5—H5B109.7
C2—N1—H1C109.3 (17)H5A—C5—H5B108.2
C5—N1—H1C106.3 (19)N2—C6—C5111.1 (2)
C6—N2—C8113.6 (2)N2—C6—H6A109.4
C6—N2—H2A106.0 (17)C5—C6—H6A109.4
C8—N2—H2A105.8 (16)N2—C6—H6B109.4
O1—C1—C2110.6 (2)C5—C6—H6B109.4
O1—C1—H1A109.5H6A—C6—H6B108.0
C2—C1—H1A109.5O2—C7—C8111.5 (2)
O1—C1—H1B109.5O2—C7—H7A109.3
C2—C1—H1B109.5C8—C7—H7A109.3
H1A—C1—H1B108.1O2—C7—H7B109.3
N1—C2—C1108.3 (2)C8—C7—H7B109.3
N1—C2—C3115.1 (2)H7A—C7—H7B108.0
C1—C2—C3112.3 (2)N2—C8—C7107.6 (2)
N1—C2—H2106.9N2—C8—C9111.8 (2)
C1—C2—H2106.9C7—C8—C9110.5 (2)
C3—C2—H2106.9N2—C8—H8109.0
C4—C3—C2113.3 (3)C7—C8—H8109.0
C4—C3—H3A108.9C9—C8—H8109.0
C2—C3—H3A108.9C10—C9—C8114.7 (3)
C4—C3—H3B108.9C10—C9—H9A108.6
C2—C3—H3B108.9C8—C9—H9A108.6
H3A—C3—H3B107.7C10—C9—H9B108.6
C3—C4—H4A109.5C8—C9—H9B108.6
C3—C4—H4B109.5H9A—C9—H9B107.6
H4A—C4—H4B109.5C9—C10—H10A109.5
C3—C4—H4C109.5C9—C10—H10B109.5
H4A—C4—H4C109.5H10A—C10—H10B109.5
H4B—C4—H4C109.5C9—C10—H10C109.5
N1—C5—C6109.7 (2)H10A—C10—H10C109.5
N1—C5—H5A109.7H10B—C10—H10C109.5
C5—N1—C2—C1175.7 (2)N1—C5—C6—N2173.0 (2)
C5—N1—C2—C357.8 (3)C6—N2—C8—C7170.5 (2)
O1—C1—C2—N161.4 (3)C6—N2—C8—C968.0 (3)
O1—C1—C2—C366.7 (3)O2—C7—C8—N257.3 (3)
N1—C2—C3—C4162.1 (3)O2—C7—C8—C9179.7 (2)
C1—C2—C3—C473.4 (3)N2—C8—C9—C10167.9 (3)
C2—N1—C5—C6169.3 (2)C7—C8—C9—C1072.3 (4)
C8—N2—C6—C5167.6 (2)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O1—H1···N2i0.93 (5)1.95 (5)2.877 (3)174 (3)
O2—H2B···N1ii0.96 (4)1.81 (4)2.767 (3)174 (3)
N1—H1C···O2iii0.85 (3)2.23 (3)3.014 (3)153 (3)
Symmetry codes: (i) x+1, y1/2, z+1; (ii) x+2, y+1/2, z+1; (iii) x1, y, z.
 
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