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In the title mononuclear copper(II) complex, [Cu(C12H17N2O2)(NCS)], the CuII atom is four-coordinated by an NNO-donor set of the tridentate Schiff base ligand and the N atom of a terminal thio­cyanate ligand in a slightly distorted square-planar geometry.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536810009402/ci5055sup1.cif
Contains datablocks global, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536810009402/ci5055Isup2.hkl
Contains datablock I

CCDC reference: 774143

Key indicators

  • Single-crystal X-ray study
  • T = 293 K
  • Mean [sigma](C-C) = 0.007 Å
  • R factor = 0.044
  • wR factor = 0.129
  • Data-to-parameter ratio = 17.9

checkCIF/PLATON results

No syntax errors found



Alert level C PLAT029_ALERT_3_C _diffrn_measured_fraction_theta_full Low ....... 0.97 PLAT242_ALERT_2_C Check Low Ueq as Compared to Neighbors for C13 PLAT341_ALERT_3_C Low Bond Precision on C-C Bonds (x 1000) Ang .. 7 PLAT420_ALERT_2_C D-H Without Acceptor N2 - H2N ... ? PLAT911_ALERT_3_C Missing # FCF Refl Between THmin & STh/L= 0.600 4 PLAT912_ALERT_4_C Missing # of FCF Reflections Above STh/L= 0.600 112
Alert level G PLAT960_ALERT_3_G Number of Intensities with I .LT. - 2*sig(I) .. 2 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 6 ALERT level C = Check and explain 3 ALERT level G = General alerts; check 2 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 2 ALERT type 2 Indicator that the structure model may be wrong or deficient 4 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

Copper(II) complexes with Schiff base ligands have received much attention in coordination chemistry (Rai, 2010; Roy & Manassero, 2010; Rajasekar et al., 2010; Dede et al., 2009). In the present work, we report the the crystal structure of a new copper(II) complex, the title compound, with the Schiff base ligand 2-[(2-ethylaminoethylimino)methyl]-5-methoxyphenolate.

The CuII atom in the title complex is four-coordinated by the NNO donor set of the Schiff base ligand, and the N atom of the terminal thiocyanate ligand, in a square-planar geometry. The coordination bond distances (Table 1) are within normal ranges and comparable to those in related complexes (Roper et al., 1989; Adams et al., 2003).

Related literature top

For CuII complexes with Schiff base ligands, see: Dede et al. (2009); Rai (2010); Rajasekar et al. (2010); Roper et al. (1989). For related structures, see: Adams et al. (2003); Roy & Manassero (2010).

Experimental top

Equimolar quantities (1 mmol each) of 2-hydroxy-4-methoxybenzaldehyde, N-ethylethylenediamine, ammonium thiocyanate, and copper nitrate were mixed and stirred in a methanol-acetonitrile (2:1 v/v) solution at room temperature for 3 h. The solution was allowed to evaporate slowly to give needle-shaped single crystals.

Refinement top

H atoms were placed in geometrically idealized positions and constrained to ride on their parent atoms, with C–H = 0.93–0.97 Å, N–H = 0.91 Å, and Uiso(H) = 1.2Ueq(C,N) and 1.5Ueq(Cmethyl).

Computing details top

Data collection: SMART (Bruker, 1998); cell refinement: SAINT (Bruker, 1998); data reduction: SAINT (Bruker, 1998); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: SHELXTL (Sheldrick, 2008); software used to prepare material for publication: SHELXTL (Sheldrick, 2008).

Figures top
[Figure 1] Fig. 1. The molecular structure of the title compound, showing the atomic numbering. Displacement ellipsoids are drawn at the 50% probability level.
{2-[2-(Ethylamino)ethyliminomethyl]-5-methoxyphenolato}(thiocyanato-κN) copper(II) top
Crystal data top
[Cu(C12H17N2O2)(NCS)]F(000) = 708
Mr = 342.90Dx = 1.533 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ybcCell parameters from 2310 reflections
a = 12.296 (6) Åθ = 2.6–25.0°
b = 10.582 (5) ŵ = 1.61 mm1
c = 12.480 (6) ÅT = 293 K
β = 113.810 (7)°Block cut from needle, blue
V = 1485.7 (12) Å30.30 × 0.27 × 0.27 mm
Z = 4
Data collection top
Bruker SMART CCD area-detector
diffractometer
3282 independent reflections
Radiation source: fine-focus sealed tube2123 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.039
ω scanθmax = 27.5°, θmin = 1.8°
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
h = 1515
Tmin = 0.643, Tmax = 0.670k = 1313
8523 measured reflectionsl = 1610
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)] = 0.044Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.129H-atom parameters constrained
S = 1.00 w = 1/[σ2(Fo2) + (0.0551P)2 + 1.5145P]
where P = (Fo2 + 2Fc2)/3
3282 reflections(Δ/σ)max = 0.001
183 parametersΔρmax = 0.61 e Å3
0 restraintsΔρmin = 0.34 e Å3
Crystal data top
[Cu(C12H17N2O2)(NCS)]V = 1485.7 (12) Å3
Mr = 342.90Z = 4
Monoclinic, P21/cMo Kα radiation
a = 12.296 (6) ŵ = 1.61 mm1
b = 10.582 (5) ÅT = 293 K
c = 12.480 (6) Å0.30 × 0.27 × 0.27 mm
β = 113.810 (7)°
Data collection top
Bruker SMART CCD area-detector
diffractometer
3282 independent reflections
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
2123 reflections with I > 2σ(I)
Tmin = 0.643, Tmax = 0.670Rint = 0.039
8523 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0440 restraints
wR(F2) = 0.129H-atom parameters constrained
S = 1.00Δρmax = 0.61 e Å3
3282 reflectionsΔρmin = 0.34 e Å3
183 parameters
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds 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
Cu10.55890 (4)0.38272 (4)0.94272 (4)0.04744 (18)
N10.6492 (3)0.3114 (3)1.0844 (3)0.0465 (8)
N20.4301 (3)0.2831 (3)0.9449 (3)0.0596 (9)
H2N0.36860.33820.92870.072*
N30.4579 (3)0.4525 (3)0.7995 (3)0.0488 (8)
O10.6770 (2)0.4836 (3)0.9392 (2)0.0543 (7)
O21.0326 (3)0.7210 (3)1.0840 (3)0.0718 (9)
S10.30391 (13)0.57348 (14)0.60132 (10)0.0790 (4)
C10.7807 (3)0.5063 (4)1.0246 (3)0.0460 (9)
C20.8513 (4)0.5995 (4)1.0075 (3)0.0516 (10)
H20.82490.64140.93600.062*
C30.9598 (4)0.6314 (4)1.0944 (4)0.0552 (10)
C40.9978 (5)0.7842 (5)0.9760 (4)0.0858 (17)
H4A0.98770.72400.91520.129*
H4B1.05780.84430.98010.129*
H4C0.92400.82760.95900.129*
C51.0006 (4)0.5683 (5)1.2010 (4)0.0664 (12)
H51.07400.58851.25980.080*
C60.9326 (4)0.4776 (4)1.2183 (4)0.0629 (12)
H60.96050.43651.29040.075*
C70.8217 (4)0.4421 (4)1.1327 (3)0.0480 (9)
C80.7542 (4)0.3458 (4)1.1546 (3)0.0510 (10)
H80.78840.30351.22580.061*
C90.5884 (4)0.2097 (4)1.1177 (4)0.0597 (11)
H9A0.61750.20421.20230.072*
H9B0.60240.12931.08800.072*
C100.4593 (4)0.2402 (4)1.0658 (4)0.0630 (12)
H10A0.41290.16601.06580.076*
H10B0.44210.30621.11060.076*
C110.3850 (5)0.1848 (5)0.8565 (4)0.0792 (15)
H11A0.43790.11260.88190.095*
H11B0.38790.21590.78450.095*
C120.2620 (5)0.1410 (5)0.8301 (4)0.0816 (16)
H12A0.25690.11240.90090.122*
H12B0.24220.07270.77480.122*
H12C0.20740.20950.79760.122*
C130.3932 (4)0.5018 (4)0.7173 (3)0.0459 (9)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Cu10.0569 (3)0.0430 (3)0.0396 (3)0.0019 (2)0.0166 (2)0.00224 (19)
N10.063 (2)0.0397 (17)0.0379 (16)0.0056 (15)0.0213 (15)0.0010 (13)
N20.077 (3)0.0499 (19)0.0485 (19)0.0137 (18)0.0216 (18)0.0024 (15)
N30.055 (2)0.0471 (18)0.0396 (17)0.0061 (16)0.0142 (15)0.0017 (14)
O10.0489 (16)0.0666 (18)0.0378 (14)0.0067 (14)0.0073 (12)0.0121 (12)
O20.0598 (19)0.089 (2)0.0557 (19)0.0252 (18)0.0123 (15)0.0104 (16)
S10.0831 (9)0.1010 (10)0.0463 (6)0.0400 (8)0.0192 (6)0.0180 (6)
C10.046 (2)0.050 (2)0.0409 (19)0.0040 (18)0.0167 (17)0.0023 (17)
C20.048 (2)0.063 (3)0.040 (2)0.002 (2)0.0142 (17)0.0014 (18)
C30.052 (2)0.060 (3)0.051 (2)0.004 (2)0.0181 (19)0.0141 (19)
C40.078 (4)0.106 (4)0.069 (3)0.044 (3)0.024 (3)0.008 (3)
C50.051 (3)0.078 (3)0.054 (3)0.002 (2)0.004 (2)0.007 (2)
C60.063 (3)0.068 (3)0.045 (2)0.010 (2)0.008 (2)0.003 (2)
C70.047 (2)0.050 (2)0.043 (2)0.0092 (19)0.0146 (17)0.0009 (17)
C80.064 (3)0.048 (2)0.038 (2)0.018 (2)0.0180 (19)0.0068 (17)
C90.087 (3)0.044 (2)0.047 (2)0.001 (2)0.025 (2)0.0102 (18)
C100.086 (4)0.052 (2)0.052 (2)0.018 (2)0.029 (2)0.002 (2)
C110.103 (4)0.073 (3)0.065 (3)0.030 (3)0.037 (3)0.011 (3)
C120.078 (3)0.093 (4)0.057 (3)0.029 (3)0.009 (2)0.002 (3)
C130.054 (2)0.046 (2)0.038 (2)0.0007 (19)0.0193 (18)0.0025 (17)
Geometric parameters (Å, º) top
Cu1—O11.817 (3)C4—H4B0.96
Cu1—N11.828 (3)C4—H4C0.96
Cu1—N31.868 (3)C5—C61.346 (6)
Cu1—N21.912 (4)C5—H50.93
N1—C81.286 (5)C6—C71.402 (6)
N1—C91.463 (5)C6—H60.93
N2—C111.453 (6)C7—C81.410 (6)
N2—C101.474 (5)C8—H80.93
N2—H2N0.91C9—C101.488 (6)
N3—C131.139 (5)C9—H9A0.97
O1—C11.313 (4)C9—H9B0.97
O2—C31.346 (5)C10—H10A0.97
O2—C41.409 (6)C10—H10B0.97
S1—C131.610 (4)C11—C121.487 (7)
C1—C21.386 (6)C11—H11A0.97
C1—C71.409 (5)C11—H11B0.97
C2—C31.379 (6)C12—H12A0.96
C2—H20.93C12—H12B0.96
C3—C51.389 (6)C12—H12C0.96
C4—H4A0.96
O1—Cu1—N194.97 (13)C3—C5—H5120.4
O1—Cu1—N388.49 (13)C5—C6—C7122.9 (4)
N1—Cu1—N3176.29 (15)C5—C6—H6118.5
O1—Cu1—N2177.40 (14)C7—C6—H6118.5
N1—Cu1—N286.67 (15)C6—C7—C1117.6 (4)
N3—Cu1—N289.82 (15)C6—C7—C8120.9 (4)
C8—N1—C9120.1 (3)C1—C7—C8121.6 (4)
C8—N1—Cu1126.4 (3)N1—C8—C7125.5 (3)
C9—N1—Cu1113.4 (3)N1—C8—H8117.3
C11—N2—C10114.7 (3)C7—C8—H8117.3
C11—N2—Cu1116.6 (3)N1—C9—C10107.1 (3)
C10—N2—Cu1108.9 (3)N1—C9—H9A110.3
C11—N2—H2N105.2C10—C9—H9A110.3
C10—N2—H2N105.2N1—C9—H9B110.3
Cu1—N2—H2N105.2C10—C9—H9B110.3
C13—N3—Cu1174.4 (3)H9A—C9—H9B108.5
C1—O1—Cu1127.7 (2)N2—C10—C9106.8 (4)
C3—O2—C4118.0 (3)N2—C10—H10A110.4
O1—C1—C2118.0 (3)C9—C10—H10A110.4
O1—C1—C7122.9 (4)N2—C10—H10B110.4
C2—C1—C7119.1 (4)C9—C10—H10B110.4
C3—C2—C1121.3 (4)H10A—C10—H10B108.6
C3—C2—H2119.3N2—C11—C12115.7 (4)
C1—C2—H2119.3N2—C11—H11A108.4
O2—C3—C2124.5 (4)C12—C11—H11A108.4
O2—C3—C5115.7 (4)N2—C11—H11B108.4
C2—C3—C5119.8 (4)C12—C11—H11B108.4
O2—C4—H4A109.5H11A—C11—H11B107.4
O2—C4—H4B109.5C11—C12—H12A109.5
H4A—C4—H4B109.5C11—C12—H12B109.5
O2—C4—H4C109.5H12A—C12—H12B109.5
H4A—C4—H4C109.5C11—C12—H12C109.5
H4B—C4—H4C109.5H12A—C12—H12C109.5
C6—C5—C3119.3 (4)H12B—C12—H12C109.5
C6—C5—H5120.4N3—C13—S1178.8 (4)

Experimental details

Crystal data
Chemical formula[Cu(C12H17N2O2)(NCS)]
Mr342.90
Crystal system, space groupMonoclinic, P21/c
Temperature (K)293
a, b, c (Å)12.296 (6), 10.582 (5), 12.480 (6)
β (°) 113.810 (7)
V3)1485.7 (12)
Z4
Radiation typeMo Kα
µ (mm1)1.61
Crystal size (mm)0.30 × 0.27 × 0.27
Data collection
DiffractometerBruker SMART CCD area-detector
diffractometer
Absorption correctionMulti-scan
(SADABS; Sheldrick, 1996)
Tmin, Tmax0.643, 0.670
No. of measured, independent and
observed [I > 2σ(I)] reflections
8523, 3282, 2123
Rint0.039
(sin θ/λ)max1)0.649
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.044, 0.129, 1.00
No. of reflections3282
No. of parameters183
H-atom treatmentH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.61, 0.34

Computer programs: SMART (Bruker, 1998), SAINT (Bruker, 1998), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008), SHELXTL (Sheldrick, 2008).

Selected bond lengths (Å) top
Cu1—O11.817 (3)Cu1—N31.868 (3)
Cu1—N11.828 (3)Cu1—N21.912 (4)
 

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