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The asymmetric unit of the title compound, C30H28N2O4, contains one-half of the centrosymmetric mol­ecule. All bond lengths and angles show normal values. Weak inter­molecular N—H...O hydrogen bonds link mol­ecules related by translation along the a axis into chains.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536807054189/cv2330sup1.cif
Contains datablocks global, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536807054189/cv2330Isup2.hkl
Contains datablock I

CCDC reference: 672822

Key indicators

  • Single-crystal X-ray study
  • T = 293 K
  • Mean [sigma](C-C) = 0.005 Å
  • R factor = 0.069
  • wR factor = 0.207
  • Data-to-parameter ratio = 14.4

checkCIF/PLATON results

No syntax errors found



Alert level C PLAT066_ALERT_1_C Predicted and Reported Transmissions Identical . ? PLAT125_ALERT_4_C No _symmetry_space_group_name_Hall Given ....... ? PLAT152_ALERT_1_C Supplied and Calc Volume s.u. Inconsistent ..... ? PLAT241_ALERT_2_C Check High Ueq as Compared to Neighbors for C2 PLAT241_ALERT_2_C Check High Ueq as Compared to Neighbors for C7 PLAT242_ALERT_2_C Check Low Ueq as Compared to Neighbors for C6 PLAT322_ALERT_2_C Check Hybridisation of H15B in Main Residue . ? PLAT331_ALERT_2_C Small Average Phenyl C-C Dist. C1 -C6 1.37 Ang. PLAT340_ALERT_3_C Low Bond Precision on C-C Bonds (x 1000) Ang ... 5
Alert level G PLAT199_ALERT_1_G Check the Reported _cell_measurement_temperature 293 K PLAT200_ALERT_1_G Check the Reported _diffrn_ambient_temperature . 293 K
0 ALERT level A = In general: serious problem 0 ALERT level B = Potentially serious problem 9 ALERT level C = Check and explain 2 ALERT level G = General alerts; check 4 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 5 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 1 ALERT type 4 Improvement, methodology, query or suggestion 0 ALERT type 5 Informative message, check

Comment top

The acyclic polyether compounds have good complexing ability and high selectivity to metal ions. Of which diamide-type acyclic polyethers have been used successfully as the active materials for ion-selective electrodes and extractants for metal ions (West et al., 1992; Bunzli et al., 1984; Wen et al., 2002). Recently, in our ongoing studies of structures and properties of the rare earth complexes with diamide-type acyclic polyethers (Wen & Zhang, 2007), a new flexible acyclic polyether compound 1,2-ethylenedioxy-bis(N-phenylmethyl-benzamide) (I), was synthesized. Herein we report the synthesis and structural characterization of (I).

The asymmetric part of the title compound contains a half of the centrosymmetric molecule, with the midpoint of the C15—C15ii bond [symmetry code: (ii): 1 - x, 1 - y, -z] located on an invesrion center (Fig. 1). All bond lengths and angles in (I) show normal values (Allen et al., 1987).

In the crystal structure, molecules are linked into chains along a axis by weak N—H···O intermolecular hydrogen bonds (Table 1 and Fig. 2).

Related literature top

The structure of 1,2-ethylenedioxy-bis(N-pyridin-2-ylmethyl-benzamide) was reported by Wen & Zhang (2007). For general background, see: West et al. (1992); Bunzli et al. (1984); Wen et al. (2002); Allen et al. (1987).

Experimental top

1,2-Dichloroethane (0.99 g, 0.01 mol) was added dropwise to a 50 ml of DMF solution containing 2-hydroxy-N-phenylmethyl-benzamide (4.54 g, 0.02 mol), K2CO3 (3 g, 0.02 mol) and KI (0.5 g), and the mixture was stirred at 328 K for 48 h. After cooling to room temperature, the mixture was filtered. DMF was removed from the filtrate under reduced pressure, and the reside was washed by column chromatography (silica gel, C2H5OH:CH3CO2C2H5 = 1:4) resulting in a colourless solid. Colourless single crystals of (I) suitable for X-ray diffraction study were obtained by slow evaporation of an ethanol–DMF (1:1 v/v) solution over a period of 25 d.

Refinement top

All H atoms were located in difference Fourier maps, placed in idealized positions (C—H 0.93–0.98 Å, N—H 0.86 Å) and refined as riding, with Uiso(H) = 1.2 Ueq(C, N).

Computing details top

Data collection: SMART (Siemens, 1996); cell refinement: SAINT (Siemens, 1996); data reduction: SAINT (Siemens, 1996); program(s) used to solve structure: SHELXS97 (Sheldrick, 1997a); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997a); molecular graphics: SHELXTL (Sheldrick, 1997b); software used to prepare material for publication: SHELXTL (Sheldrick, 1997b), PARST (Nardelli, 1995) and PLATON (Spek, 2003).

Figures top
[Figure 1] Fig. 1. The molecular structure of (I) showing 50% probability displacement ellipsoids and the atom numbering scheme [symmetry code: (A) 1 - x, 1 - y, 1 - z].
[Figure 2] Fig. 2. A packing diagram of (I), viewed down the c axis. Hydrogen bonds are indicated by dashed lines.
N,N'-Dibenzyl-2,2'-ethylenedioxydibenzamide top
Crystal data top
C30H28N2O4F(000) = 508
Mr = 480.54Dx = 1.285 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
a = 5.0620 (13) ÅCell parameters from 934 reflections
b = 16.401 (4) Åθ = 2.5–21.0°
c = 15.056 (4) ŵ = 0.09 mm1
β = 96.522 (5)°T = 293 K
V = 1241.9 (6) Å3Block, colourless
Z = 20.42 × 0.11 × 0.05 mm
Data collection top
Siemens SMART 1000 CCD area-detector
diffractometer
2341 independent reflections
Radiation source: fine-focus sealed tube1425 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.035
Detector resolution: 8.33 pixels mm-1θmax = 25.7°, θmin = 1.8°
ω scansh = 65
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
k = 1916
Tmin = 0.989, Tmax = 0.996l = 1817
6638 measured reflections
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)] = 0.069Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.207H-atom parameters constrained
S = 1.12 w = 1/[σ2(Fo2) + (0.1P)2]
where P = (Fo2 + 2Fc2)/3
2341 reflections(Δ/σ)max < 0.001
163 parametersΔρmax = 0.46 e Å3
0 restraintsΔρmin = 0.33 e Å3
Crystal data top
C30H28N2O4V = 1241.9 (6) Å3
Mr = 480.54Z = 2
Monoclinic, P21/cMo Kα radiation
a = 5.0620 (13) ŵ = 0.09 mm1
b = 16.401 (4) ÅT = 293 K
c = 15.056 (4) Å0.42 × 0.11 × 0.05 mm
β = 96.522 (5)°
Data collection top
Siemens SMART 1000 CCD area-detector
diffractometer
2341 independent reflections
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
1425 reflections with I > 2σ(I)
Tmin = 0.989, Tmax = 0.996Rint = 0.035
6638 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0690 restraints
wR(F2) = 0.207H-atom parameters constrained
S = 1.12Δρmax = 0.46 e Å3
2341 reflectionsΔρmin = 0.33 e Å3
163 parameters
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
O20.2700 (4)0.43132 (12)0.04071 (12)0.0539 (6)
C140.1064 (5)0.36654 (17)0.01572 (19)0.0478 (7)
C90.0472 (5)0.33705 (16)0.08071 (19)0.0465 (7)
C80.0383 (6)0.36742 (17)0.1743 (2)0.0490 (7)
N10.1948 (5)0.39077 (16)0.21573 (16)0.0590 (7)
H1A0.33140.38840.18670.071*
O10.2399 (4)0.36622 (16)0.21280 (15)0.0808 (8)
C150.4239 (5)0.46574 (17)0.02322 (18)0.0511 (8)
H15B0.42870.44890.08200.077*
H15C0.30520.48620.07250.077*
C60.3986 (6)0.4961 (2)0.3189 (2)0.0564 (8)
C100.2248 (6)0.27390 (19)0.0563 (2)0.0642 (9)
H10A0.33150.25460.09810.077*
C130.0843 (6)0.3322 (2)0.0687 (2)0.0622 (9)
H13A0.18510.35240.11180.075*
C110.2482 (8)0.2393 (2)0.0265 (3)0.0785 (11)
H11A0.36930.19740.04090.094*
C120.0899 (7)0.2673 (2)0.0889 (3)0.0752 (11)
H12A0.09960.24260.14480.090*
C50.3608 (7)0.5599 (2)0.2607 (2)0.0712 (10)
H5A0.23020.55620.21210.085*
C40.5126 (9)0.6296 (2)0.2724 (3)0.0817 (11)
H4A0.48300.67250.23210.098*
C70.2325 (7)0.4201 (2)0.3075 (2)0.0742 (10)
H7A0.31720.37760.34550.089*
H7B0.05990.43090.32710.089*
C30.7041 (8)0.6360 (3)0.3422 (3)0.0908 (13)
H3A0.80670.68300.34970.109*
C20.7467 (9)0.5735 (3)0.4013 (3)0.1026 (15)
H2A0.87780.57780.44960.123*
C10.5938 (7)0.5033 (2)0.3893 (2)0.0802 (11)
H1B0.62440.46050.42960.096*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O20.0512 (12)0.0616 (13)0.0498 (12)0.0147 (10)0.0101 (9)0.0019 (10)
C140.0360 (16)0.0464 (17)0.0594 (18)0.0058 (13)0.0022 (13)0.0022 (14)
C90.0309 (14)0.0425 (16)0.0642 (18)0.0008 (12)0.0022 (13)0.0092 (14)
C80.0359 (16)0.0505 (17)0.0605 (18)0.0012 (13)0.0054 (14)0.0150 (14)
N10.0405 (15)0.0810 (19)0.0568 (15)0.0144 (13)0.0107 (12)0.0051 (13)
O10.0422 (14)0.125 (2)0.0772 (16)0.0098 (13)0.0160 (12)0.0040 (14)
C150.0481 (17)0.063 (2)0.0423 (15)0.0055 (14)0.0058 (13)0.0110 (13)
C60.0483 (18)0.069 (2)0.0524 (17)0.0021 (15)0.0071 (14)0.0054 (16)
C100.0497 (19)0.0531 (19)0.086 (2)0.0065 (15)0.0081 (17)0.0112 (18)
C130.056 (2)0.071 (2)0.059 (2)0.0062 (17)0.0014 (15)0.0096 (17)
C110.072 (3)0.054 (2)0.104 (3)0.0091 (18)0.013 (2)0.007 (2)
C120.072 (2)0.068 (2)0.079 (2)0.015 (2)0.017 (2)0.024 (2)
C50.066 (2)0.083 (3)0.063 (2)0.0006 (19)0.0006 (17)0.0004 (19)
C40.093 (3)0.067 (2)0.088 (3)0.002 (2)0.018 (2)0.005 (2)
C70.071 (2)0.096 (3)0.056 (2)0.019 (2)0.0081 (17)0.0016 (18)
C30.078 (3)0.070 (3)0.126 (4)0.006 (2)0.015 (3)0.034 (3)
C20.088 (3)0.096 (3)0.113 (4)0.007 (3)0.031 (3)0.038 (3)
C10.084 (3)0.080 (3)0.071 (2)0.006 (2)0.019 (2)0.0083 (19)
Geometric parameters (Å, º) top
O2—C141.373 (3)C10—H10A0.9300
O2—C151.422 (3)C13—C121.394 (5)
C14—C131.383 (4)C13—H13A0.9300
C14—C91.403 (4)C11—C121.380 (5)
C9—C101.393 (4)C11—H11A0.9300
C9—C81.491 (4)C12—H12A0.9300
C8—O11.229 (3)C5—C41.378 (5)
C8—N11.327 (4)C5—H5A0.9300
N1—C71.455 (4)C4—C31.350 (5)
N1—H1A0.8600C4—H4A0.9300
C15—C15i1.491 (5)C7—H7A0.9700
C15—H15B0.9300C7—H7B0.9700
C15—H15C0.9599C3—C21.358 (6)
C6—C51.364 (5)C3—H3A0.9300
C6—C11.369 (4)C2—C11.388 (6)
C6—C71.503 (5)C2—H2A0.9300
C10—C111.362 (5)C1—H1B0.9300
C14—O2—C15118.8 (2)C10—C11—C12119.2 (3)
O2—C14—C13123.4 (3)C10—C11—H11A120.4
O2—C14—C9116.1 (2)C12—C11—H11A120.4
C13—C14—C9120.5 (3)C11—C12—C13120.5 (3)
C10—C9—C14117.7 (3)C11—C12—H12A119.8
C10—C9—C8116.6 (3)C13—C12—H12A119.8
C14—C9—C8125.8 (3)C6—C5—C4121.2 (3)
O1—C8—N1121.7 (3)C6—C5—H5A119.4
O1—C8—C9120.1 (3)C4—C5—H5A119.4
N1—C8—C9118.1 (3)C3—C4—C5120.3 (4)
C8—N1—C7123.7 (3)C3—C4—H4A119.8
C8—N1—H1A118.1C5—C4—H4A119.8
C7—N1—H1A118.1N1—C7—C6113.2 (3)
O2—C15—C15i106.0 (3)N1—C7—H7A108.9
O2—C15—H15B127.0C6—C7—H7A108.9
C15i—C15—H15B127.0N1—C7—H7B108.9
O2—C15—H15C108.6C6—C7—H7B108.9
C15i—C15—H15C110.1H7A—C7—H7B107.7
H15B—C15—H15C56.6C4—C3—C2119.9 (4)
C5—C6—C1117.9 (3)C4—C3—H3A120.1
C5—C6—C7121.8 (3)C2—C3—H3A120.1
C1—C6—C7120.3 (3)C3—C2—C1119.7 (4)
C11—C10—C9122.5 (3)C3—C2—H2A120.1
C11—C10—H10A118.7C1—C2—H2A120.1
C9—C10—H10A118.7C6—C1—C2121.0 (4)
C14—C13—C12119.6 (3)C6—C1—H1B119.5
C14—C13—H13A120.2C2—C1—H1B119.5
C12—C13—H13A120.2
C15—O2—C14—C130.5 (4)C9—C14—C13—C120.7 (4)
C15—O2—C14—C9177.9 (2)C9—C10—C11—C120.3 (5)
O2—C14—C9—C10177.0 (2)C10—C11—C12—C132.5 (5)
C13—C14—C9—C101.4 (4)C14—C13—C12—C112.7 (5)
O2—C14—C9—C82.9 (4)C1—C6—C5—C40.4 (5)
C13—C14—C9—C8178.7 (3)C7—C6—C5—C4179.3 (3)
C10—C9—C8—O131.8 (4)C6—C5—C4—C30.3 (6)
C14—C9—C8—O1148.1 (3)C8—N1—C7—C6134.0 (3)
C10—C9—C8—N1144.3 (3)C5—C6—C7—N144.4 (4)
C14—C9—C8—N135.8 (4)C1—C6—C7—N1135.9 (3)
O1—C8—N1—C72.8 (5)C5—C4—C3—C20.3 (6)
C9—C8—N1—C7178.8 (3)C4—C3—C2—C10.4 (7)
C14—O2—C15—C15i179.5 (3)C5—C6—C1—C20.5 (5)
C14—C9—C10—C111.7 (5)C7—C6—C1—C2179.2 (4)
C8—C9—C10—C11178.4 (3)C3—C2—C1—C60.5 (6)
O2—C14—C13—C12179.0 (3)
Symmetry code: (i) x+1, y+1, z.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N1—H1A···O1ii0.862.192.895 (3)139
Symmetry code: (ii) x+1, y, z.

Experimental details

Crystal data
Chemical formulaC30H28N2O4
Mr480.54
Crystal system, space groupMonoclinic, P21/c
Temperature (K)293
a, b, c (Å)5.0620 (13), 16.401 (4), 15.056 (4)
β (°) 96.522 (5)
V3)1241.9 (6)
Z2
Radiation typeMo Kα
µ (mm1)0.09
Crystal size (mm)0.42 × 0.11 × 0.05
Data collection
DiffractometerSiemens SMART 1000 CCD area-detector
diffractometer
Absorption correctionMulti-scan
(SADABS; Sheldrick, 1996)
Tmin, Tmax0.989, 0.996
No. of measured, independent and
observed [I > 2σ(I)] reflections
6638, 2341, 1425
Rint0.035
(sin θ/λ)max1)0.609
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.069, 0.207, 1.12
No. of reflections2341
No. of parameters163
H-atom treatmentH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.46, 0.33

Computer programs: SMART (Siemens, 1996), SAINT (Siemens, 1996), SHELXS97 (Sheldrick, 1997a), SHELXL97 (Sheldrick, 1997a), SHELXTL (Sheldrick, 1997b), PARST (Nardelli, 1995) and PLATON (Spek, 2003).

Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N1—H1A···O1i0.862.1912.895 (3)139.02
Symmetry code: (i) x+1, y, z.
 

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