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The title compound, [TiZr(C5H11NO2)3(C3H7O)2], contains three methyl­imino­diethano­late ligands, two in different [mu]-oxo bridging coordination modes and one bound only to the Ti atom. The Ti and Zr atoms have distorted octahedral and pentagonal-bipyramidal coordinations, respectively, which share edges. As well as some conformational disorder in the carbon chains, there is chemical disorder at one Ti site, with a mix of n- and isopropanolate ligands.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S0108270102015275/ta1389sup1.cif
Contains datablocks global, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108270102015275/ta1389Isup2.hkl
Contains datablock I

CCDC reference: 197320

Comment top

The title compound, (I), was prepared as part of a study of possible precursor compounds for zirconium titanates and lead zirconate titanate (PZT). An X-ray analysis was required as the chemical structure was not unambiguously determined by other techniques (Kemmitt, Al-Salim & Gainsford, 2002). \sch

The crystal structure of (I) (Fig. 1) consists of independent [TiZr(MDEA)3(n-propanolato)1.6(iso-propanolato)0.4] molecules (MDEA is methyliminodiethanolate) with only weak intermolecular contacts, e.g. C33A—H332···O22i with C···O 3.476 (9) Å [symmetry code: (i) 1/2 - x, 1/2 + y, 1/2 - z]. Within the complex, there is one weak intramolecular C15—H15B···O22 hydrogen-bond contact, with C···O 3.280 (5) Å and C—H···O 148°. For clarity, Fig. 1 shows only the major conformation rings (suffix A) and the major (60% occupancy) n-propanolate ligand bound to the Ti atom at the O41 site.

The Ti atom is in a typical distorted octahedral coordination environment, while the Zr is seven-coordinate, highly distorted from bipyramidal-pentagonal symmetry. The Ti···Zr distance of 3.459 (1) Å is considerably longer than the values of 3.413 and 3.4117 (12) Å found in the oxo-linked titanium and zirconium pinacolate complexes reported by Zechmann et al. (1998) [Cambridge Structural Database (CSD; Allen & Kennard, 1993) refcodes JARSUQ and JARWEE]. The latter are the only two µ-oxo-bridged Ti···Zr complexes found in the CSD.

Both of the MDEA ligands bound to the Zr in (I) have one O atom bridging the two metal centres. One adopts a facial conformation, as previously observed by Kemmitt, Al-Salim & Gainsford (1999), while the other is meridionally bound (see examples in Sevast'yanov et al., 2001). The latter MDEA ligand, with its flattened conformation, has Zr—N 2.397 (3) Å, which is shorter than the usual facial (twist) conformation length (Zr—N21) of 2.443 (3) Å. A comparable twist Zr—N distance of 2.427 Å is found in the complex {N,N-bis[2-(mesitylamido)ethyl]methylamine}zirconium (Schrock et al., 2000).

The Zr—O distances in (I) are similar to those found in JARSUQ and JARWEE, which have distances to the µ O atom of 2.135 (3), 2.178 (4), 2.174 (5) and 2.164 (5) Å, compared with 2.182 (2) and 2.222 (2) Å in (I). The Ti—O lengths of the bound iso-propanolate ligand in JARSUQ and JARWEE [mean 1.791 (5) Å] are identical to that for the n-propanolate ligand in (I) [1.786 (3) Å]. This suggests that the mixture of iso- and n-propanolate ligands bound to the Ti atom through oxygen (site O41) found by model trials is, structurally speaking, a reasonable possibility (see Experimental).

The third MDEA ligand is bound only to the Ti atom, adopting the facially bound conformation with a Ti—N distance of 2.346 (3) Å, slightly shorter than the values of 2.380 (3) and 2.401 (2) Å found in [Ti3(MDEA)2(1,3-propanolate)4] (hereinafter KEMM1; Kemmitt, Gainsford & Robson-Marsden, 2002), and the maxiumum of 2.422 (2) Å observed in [Ti(MDEA)2] (Kemmitt, Al-Salim et al., 1999). The folding in the MDEA is normal, with N—C—C—O dihedral angles of 44.9 (5) and 37.0 (4)° (for the A conformations), compared with means of 43.8 and 30.7° in KEMM1.

All the Ti—O(MDEA) bond lengths are similar to those found previously. The Ti—O(MDEA) mean in (I) is 1.883 (3) Å, which is comparable with the range 1.848–1.878 Å found in KEMM1, and the usually longer bridging bonds (2.014 and 2.067 Å) compare with mean values observed in related compounds of 2.107 Å (Kemmitt, Al-Salim & Gainsford, 1999) and 2.103 Å (Sevast'yanov et al., 2001).

The O atoms bound to the Ti atom (O11, O12, O21 and O31) are planar, with an average deviation of 0.024 (3) Å, and the Ti atom is 0.279 (1) Å from the plane. This plane makes an angle of 10.3 (1)° with the plane through the four approximately planar atoms O21, O31, O32 and N31 (average deviation out of the plane 0.08 Å) bound to Zr; atoms Zr and N21 are 0.022 (2) and 0.446 (5) Å, respectively, from this plane.

Experimental top

Titanium tetra-iso-propoxide (mass?, 21 mmol) and zirconium tetra-n-propoxide (mass?, 21 mmol) were added to N-methyldiethoxoamine (mass?, 42 mmol) in anhydrous benzene at room temperature. The mixture was stirred at 323 K under an inert atmosphere for 1 h, and the solvent was then evaporated at 323–343 K under vacuum to give a viscous material. This was dissolved in anhydrous benzene (2 ml), from which approximately cubic colourless crystals of (I) separated out (ca 30% yield).

Refinement top

The H atoms on atoms C31 and C34 were positionally refined. Other H atoms were placed in calculated positions, with C—H = 0.98–0.99 Å. Subsequently, all H atoms were constrained, with Uiso(H) = 1.2Ueq of their parent atom. Is this added text correct? There was conformational disorder in one methyliminodiethanolate ligand and the n-propanolate ligand bound to Zr. Chemical disorder (iso/n-propanolate) was modelled for the ligand bound to Ti; full details are given in the archived CIF. No H atoms were included for the poorly ordered iso-propanolate C atoms.

Computing details top

Data collection: SMART (Siemens, 1996); cell refinement: SMART; data reduction: SAINT (Siemens, 1996) and SADABS (Sheldrick, 1996); program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: ORTEP-3 in WinGX (Farrugia, 1997, 1999); software used to prepare material for publication: SHELXL97.

Figures top
[Figure 1] Fig. 1. A view of the molecular structure of (I) with the atom-numbering scheme. Displacement ellipsoids are drawn at the 30% probability level. H atoms, minor conformers and the iso-propanolate ligand at O41 (see text) have been omitted for clarity.
bis(µ-methyliminodiethanolato-1κ3O,N,O';1:2κ2O)(methyliminodiethanolato- 2κ3O,N,O')dipropanolato-1κO,2κO-titanium(IV)zirconium(IV) top
Crystal data top
[TiZr(C5H11NO2)3(C3H7O)2]F(000) = 2560
Mr = 608.74Dx = 1.451 Mg m3
Monoclinic, C2/cMo Kα radiation, λ = 0.71073 Å
Hall symbol: -C 2ycCell parameters from 5093 reflections
a = 31.172 (10) Åθ = 2.6–25.8°
b = 10.407 (3) ŵ = 0.71 mm1
c = 19.116 (6) ÅT = 163 K
β = 116.002 (3)°Cubic block, colourless
V = 5574 (5) Å30.30 × 0.27 × 0.25 mm
Z = 8
Data collection top
Make Model CCD area-detector
diffractometer
5613 independent reflections
Radiation source: fine-focus sealed tube3723 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.056
Detector resolution: 8.192 pixels mm-1θmax = 26.4°, θmin = 2.1°
ϕ and ω scansh = 3835
Absorption correction: multi scan
(Blessing, 1995)
k = 1212
Tmin = 0.686, Tmax = 0.837l = 823
19935 measured reflections
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)] = 0.043H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.104 w = 1/[σ2(Fo2) + (0.0537P)2]
where P = (Fo2 + 2Fc2)/3
S = 0.95(Δ/σ)max < 0.001
5613 reflectionsΔρmax = 0.60 e Å3
272 parametersΔρmin = 0.59 e Å3
1 restraintExtinction correction: SHELXL97 (Sheldrick, 1997), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.00051 (7)
Crystal data top
[TiZr(C5H11NO2)3(C3H7O)2]V = 5574 (5) Å3
Mr = 608.74Z = 8
Monoclinic, C2/cMo Kα radiation
a = 31.172 (10) ŵ = 0.71 mm1
b = 10.407 (3) ÅT = 163 K
c = 19.116 (6) Å0.30 × 0.27 × 0.25 mm
β = 116.002 (3)°
Data collection top
Make Model CCD area-detector
diffractometer
5613 independent reflections
Absorption correction: multi scan
(Blessing, 1995)
3723 reflections with I > 2σ(I)
Tmin = 0.686, Tmax = 0.837Rint = 0.056
19935 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0431 restraint
wR(F2) = 0.104H atoms treated by a mixture of independent and constrained refinement
S = 0.95Δρmax = 0.60 e Å3
5613 reflectionsΔρmin = 0.59 e Å3
272 parameters
Special details top

Experimental. Crystal decay was monitored by repeating the initial 10 frames at the end of the data collection and analyzing duplicate reflections. The standard 0.8 mm diameter collimator was used.

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. Conformational and chemical disorder was modelled as follows. The meridional MDEA ligand bound to Zr had two alternative conformations (A/B) for atoms C32, C33 and C35, with final occupancies 0.549 (3)/0.451 (3) and a common U of 0.0459 (9) Å2. The n-propanolate ligand bound to Zr was modelled in two conformations (A/B) to give final occupancies 0.641 (9)/0.359 (9) and a common U of 0.063 (1) Å2. Chemical disorder for the propanolate ligand(s) bound to Ti was finally modelled by one n-propanolate (atoms C41A, C42A and C43A, and their bound H atoms) with a common occupancy of 0.60 (1) and a common U of 0.075 (2) Å2, and iso-propanolate `atoms' (C41B, C42B, C41C, C4OC, C42C and C43C) corresponding to two conformations, with individual occupancies refined so that the total carbon occupancy for all 9 C atoms, C41A···C43C, summed to 3 (SHELXL97 SUMP); the latter six atoms had a common U which refined to 0.085 (4) Å2. The final difference map peaks (<0.59 e %A-3) around the disorder model atoms (e.g. C41A) correspond to expected anisotropic thermal motion or unresolved H atoms.

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*/UeqOcc. (<1)
Zr0.144893 (12)0.16988 (3)0.229178 (17)0.02441 (12)
Ti0.12749 (2)0.05976 (6)0.38555 (3)0.02994 (18)
O110.17559 (9)0.0289 (3)0.48695 (13)0.0399 (7)
O120.07409 (8)0.0297 (2)0.38118 (13)0.0333 (6)
O210.09844 (8)0.0593 (2)0.26841 (12)0.0268 (6)
O220.16483 (8)0.0005 (2)0.19769 (12)0.0293 (6)
O310.17928 (8)0.1157 (2)0.35186 (12)0.0312 (6)
O320.15633 (9)0.2626 (3)0.14312 (13)0.0395 (7)
O410.11001 (11)0.2137 (3)0.40551 (15)0.0484 (7)
O510.10897 (9)0.3216 (2)0.23668 (14)0.0385 (6)
N110.14742 (11)0.1567 (3)0.38172 (15)0.0336 (8)
N210.07596 (9)0.0930 (3)0.11375 (14)0.0248 (7)
N310.22118 (11)0.2733 (3)0.29057 (16)0.0350 (7)
C110.20113 (15)0.0867 (4)0.5120 (2)0.0457 (10)*
H11A0.21010.10030.56790.055*
H11B0.23070.08260.50500.055*
C120.17035 (15)0.1963 (4)0.4650 (2)0.0470 (11)*
H12A0.19010.27400.47170.056*
H12B0.14570.21650.48270.056*
C130.10037 (14)0.2187 (4)0.3384 (2)0.0455 (10)*
H13A0.10320.31260.34800.055*
H13B0.08870.20400.28190.055*
C140.06535 (14)0.1612 (4)0.3661 (2)0.0405 (10)*
H14B0.03230.17400.32560.049*
H14A0.06870.20580.41390.049*
C150.17881 (17)0.1859 (4)0.3446 (2)0.0579 (13)
H15A0.20980.14390.37360.070*
H15B0.16420.15430.29090.070*
H15C0.18340.27910.34460.070*
C210.04910 (12)0.0584 (3)0.21554 (18)0.0288 (8)*
H21A0.03550.14580.21050.035*
H21B0.03140.00010.23450.035*
C220.04510 (12)0.0125 (4)0.13766 (18)0.0300 (9)
H22A0.05510.07850.14170.036*
H22B0.01150.01850.09790.036*
C230.09775 (12)0.0160 (3)0.07250 (18)0.0284 (8)*
H23A0.11120.07400.04620.034*
H23B0.07300.03800.03240.034*
C240.13695 (13)0.0689 (4)0.12996 (19)0.0339 (9)
H24A0.12260.14410.14340.041*
H24B0.15740.10060.10600.041*
C250.04734 (13)0.1986 (3)0.0624 (2)0.0343 (9)*
H25A0.03300.24980.08960.041*
H25B0.02210.16220.01490.041*
H25C0.06810.25350.04870.041*
C310.22580 (17)0.1581 (5)0.4045 (3)0.0467 (11)*
H31A0.2180 (14)0.216 (4)0.431 (2)0.056*
H31B0.2433 (14)0.086 (4)0.418 (2)0.056*
C340.19340 (18)0.3481 (5)0.1581 (3)0.0528 (12)*
H34A0.1828 (14)0.432 (4)0.157 (2)0.063*
H34B0.2105 (14)0.331 (4)0.125 (2)0.063*
C32A0.2531 (3)0.1927 (8)0.3558 (4)0.0459 (8)*0.549 (3)
H3210.28280.24000.38820.055*0.549 (3)
H3220.26170.11360.33600.055*0.549 (3)
C33A0.2375 (3)0.2943 (8)0.2308 (4)0.0459 (8)*0.549 (3)
H3310.24860.21270.21770.055*0.549 (3)
H3320.26410.35680.24900.055*0.549 (3)
C35A0.2156 (3)0.4056 (7)0.3219 (4)0.0459 (8)*0.549 (3)
H3510.20280.39420.36000.055*0.549 (3)
H3520.19380.45890.27880.055*0.549 (3)
H3530.24690.44770.34690.055*0.549 (3)
C41A0.0716 (4)0.2724 (11)0.4108 (5)0.075 (2)*0.598 (12)
H4110.04890.20350.40750.090*0.598 (12)
H4120.05550.32630.36380.090*0.598 (12)
C42A0.0784 (5)0.3517 (12)0.4771 (7)0.075 (2)*0.598 (12)
H4210.09290.30240.52630.090*0.598 (12)
H4220.04790.38970.47140.090*0.598 (12)
C43A0.1146 (4)0.4614 (10)0.4735 (6)0.075 (2)*0.598 (12)
H4310.14720.42730.49590.090*0.598 (12)
H4320.11340.53690.50320.090*0.598 (12)
H4330.10510.48590.41920.090*0.598 (12)
C51A0.0743 (3)0.4172 (8)0.2235 (5)0.0635 (11)*0.641 (9)
H5110.07940.45730.27350.076*0.641 (9)
H5120.04210.37830.19990.076*0.641 (9)
C52A0.0782 (3)0.5224 (8)0.1670 (5)0.0635 (11)*0.636 (6)
H5210.10790.57240.19480.076*0.636 (6)
H5220.08000.47950.12210.076*0.636 (6)
C53A0.0371 (3)0.6101 (8)0.1386 (4)0.0635 (11)*0.636 (6)
H5310.00830.56330.10400.076*0.636 (6)
H5320.04270.68100.10990.076*0.636 (6)
H5330.03280.64440.18290.076*0.636 (6)
C32B0.2349 (3)0.2871 (9)0.3725 (5)0.0459 (8)*0.451 (3)
H3230.21600.35650.38120.055*0.451 (3)
H3240.26910.31020.40010.055*0.451 (3)
C33B0.2165 (3)0.3904 (9)0.2463 (5)0.0459 (8)*0.451 (3)
H3330.24810.43020.26110.055*0.451 (3)
H3340.19580.45310.25590.055*0.451 (3)
C35B0.2587 (3)0.1866 (9)0.2800 (5)0.0459 (8)*0.451 (3)
H3540.28960.23050.30140.055*0.451 (3)
H3550.24830.16970.22450.055*0.451 (3)
H3560.26180.10510.30750.055*0.451 (3)
C41B0.1301 (18)0.346 (5)0.435 (3)0.085 (5)*0.163 (11)
C42B0.0836 (17)0.429 (4)0.441 (3)0.085 (5)*0.163 (11)
C51B0.0938 (6)0.4480 (15)0.2063 (9)0.0635 (11)*0.359 (9)
H5130.09550.45670.15600.076*0.359 (9)
H5140.11580.51210.24280.076*0.359 (9)
C52B0.0453 (4)0.4744 (10)0.1949 (6)0.0635 (11)*0.364 (6)
H5230.04570.47270.24690.076*0.364 (6)
H5240.02540.40110.16530.076*0.364 (6)
C53B0.0195 (4)0.5948 (10)0.1552 (6)0.0635 (11)*0.364 (6)
H5340.03840.67000.18240.076*0.364 (6)
H5350.01160.59790.15610.076*0.364 (6)
H5360.01500.59510.10110.076*0.364 (6)
C41C0.092 (3)0.340 (7)0.413 (4)0.085 (5)*0.115 (14)
C4OC0.123 (2)0.322 (5)0.470 (3)0.085 (5)*0.130 (14)
C42C0.1429 (7)0.437 (2)0.4515 (11)0.085 (5)*0.334 (14)
C43C0.0944 (9)0.366 (3)0.4891 (15)0.085 (5)*0.307 (19)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Zr0.0206 (2)0.0309 (2)0.02144 (16)0.00500 (17)0.00891 (13)0.00285 (15)
Ti0.0327 (4)0.0374 (4)0.0230 (3)0.0036 (3)0.0151 (3)0.0058 (3)
O110.0433 (17)0.0508 (18)0.0245 (12)0.0131 (14)0.0138 (12)0.0079 (12)
O120.0309 (15)0.0438 (17)0.0312 (13)0.0002 (12)0.0191 (11)0.0003 (11)
O210.0182 (13)0.0373 (15)0.0236 (11)0.0056 (11)0.0082 (10)0.0018 (10)
O220.0242 (14)0.0380 (15)0.0254 (12)0.0012 (12)0.0107 (11)0.0044 (11)
O310.0207 (14)0.0444 (16)0.0233 (11)0.0093 (12)0.0050 (10)0.0047 (11)
O320.0348 (16)0.0500 (18)0.0323 (13)0.0197 (14)0.0135 (12)0.0016 (12)
O410.065 (2)0.0452 (18)0.0451 (15)0.0045 (16)0.0338 (15)0.0087 (13)
O510.0378 (16)0.0328 (16)0.0416 (14)0.0037 (13)0.0142 (12)0.0008 (12)
N110.0335 (19)0.044 (2)0.0254 (14)0.0055 (16)0.0150 (14)0.0002 (13)
N210.0202 (16)0.0328 (18)0.0216 (13)0.0007 (14)0.0093 (12)0.0018 (12)
N310.0299 (19)0.039 (2)0.0343 (16)0.0093 (16)0.0126 (14)0.0060 (14)
C150.080 (4)0.059 (3)0.056 (3)0.024 (3)0.048 (3)0.010 (2)
C220.020 (2)0.040 (2)0.0268 (17)0.0053 (17)0.0071 (15)0.0056 (16)
C240.032 (2)0.042 (3)0.0300 (18)0.0020 (19)0.0165 (17)0.0038 (17)
Geometric parameters (Å, º) top
Zr—O511.977 (3)C24—H24B0.9900
Zr—O222.046 (2)C25—H25A0.9800
Zr—O322.068 (2)C25—H25B0.9800
Zr—O312.182 (2)C25—H25C0.9800
Zr—O212.222 (2)C31—C32A1.554 (8)
Zr—N312.397 (3)C31—C32B1.552 (10)
Zr—N212.443 (3)C31—H31A0.89 (4)
Ti—O411.786 (3)C31—H31B0.90 (4)
Ti—O121.877 (2)C34—C33A1.569 (8)
Ti—O111.887 (2)C34—C33B1.579 (10)
Ti—O212.014 (2)C34—H34A0.93 (4)
Ti—O312.067 (2)C34—H34B1.01 (4)
Ti—N112.346 (3)C32A—H3210.9900
O11—C111.406 (5)C32A—H3220.9900
O12—C141.401 (4)C33A—H3310.9900
O21—C211.423 (4)C33A—H3320.9900
O22—C241.402 (4)C35A—H3510.9800
O31—C311.425 (5)C35A—H3520.9800
O32—C341.386 (5)C35A—H3530.9800
O41—C41A1.386 (10)C41A—C42A1.449 (14)
O41—C41C1.46 (6)C41A—H4110.9900
O41—C41B1.52 (5)C41A—H4120.9900
O41—C4OC1.58 (6)C42A—C43A1.629 (18)
O51—C51A1.408 (9)C42A—H4210.9900
O51—C51B1.432 (16)C42A—H4220.9900
N11—C151.471 (4)C43A—H4310.9800
N11—C131.479 (5)C43A—H4320.9800
N11—C121.489 (5)C43A—H4330.9800
N21—C231.481 (4)C51A—C52A1.580 (12)
N21—C251.483 (4)C51A—H5110.9900
N21—C221.491 (4)C51A—H5120.9900
N31—C32B1.438 (9)C52A—C53A1.471 (10)
N31—C33B1.454 (9)C52A—H5210.9900
N31—C33A1.456 (7)C52A—H5220.9900
N31—C32A1.470 (8)C53A—H5310.9800
N31—C35A1.541 (7)C53A—H5320.9800
N31—C35B1.559 (9)C53A—H5330.9800
C11—C121.508 (5)C32B—H3230.9900
C11—H11A0.9900C32B—H3240.9900
C11—H11B0.9900C33B—H3330.9900
C12—H12A0.9900C33B—H3340.9900
C12—H12B0.9900C35B—H3540.9800
C13—C141.528 (5)C35B—H3550.9800
C13—H13A0.9900C35B—H3560.9800
C13—H13B0.9900C41B—C42B1.73 (7)
C14—H14B0.9900C51B—C52B1.46 (2)
C14—H14A0.9900C51B—H5130.9900
C15—H15A0.9800C51B—H5140.9900
C15—H15B0.9800C52B—C53B1.5029
C15—H15C0.9800C52B—H5230.9900
C21—C221.516 (4)C52B—H5240.9900
C21—H21A0.9900C53B—H5340.9800
C21—H21B0.9900C53B—H5350.9800
C22—H22A0.9900C53B—H5360.9800
C22—H22B0.9900C41C—C4OC1.11 (7)
C23—C241.518 (5)C41C—C43C1.45 (7)
C23—H23A0.9900C41C—C42C1.74 (9)
C23—H23B0.9900C4OC—C43C1.20 (6)
C24—H24A0.9900C4OC—C42C1.45 (6)
O51—Zr—O22164.68 (10)N21—C22—H22B109.7
O51—Zr—O3289.19 (10)C21—C22—H22B109.7
O22—Zr—O3289.27 (10)H22A—C22—H22B108.2
O51—Zr—O3198.93 (10)N21—C23—C24110.0 (3)
O22—Zr—O3191.39 (9)N21—C23—H23A109.7
O32—Zr—O31143.18 (9)C24—C23—H23A109.7
O51—Zr—O2185.16 (10)N21—C23—H23B109.7
O22—Zr—O2188.84 (9)C24—C23—H23B109.7
O32—Zr—O21151.06 (9)H23A—C23—H23B108.2
O31—Zr—O2165.74 (8)O22—C24—C23110.2 (3)
O51—Zr—N3194.46 (11)O22—C24—H24A109.6
O22—Zr—N3199.61 (10)C23—C24—H24A109.6
O32—Zr—N3172.55 (10)O22—C24—H24B109.6
O31—Zr—N3171.05 (9)C23—C24—H24B109.6
O21—Zr—N31136.14 (9)H24A—C24—H24B108.1
O51—Zr—N2191.43 (10)N21—C25—H25A109.5
O22—Zr—N2173.29 (9)N21—C25—H25B109.5
O32—Zr—N2179.88 (9)H25A—C25—H25B109.5
O31—Zr—N21135.17 (9)N21—C25—H25C109.5
O21—Zr—N2171.94 (8)H25A—C25—H25C109.5
N31—Zr—N21151.68 (9)H25B—C25—H25C109.5
O41—Ti—O1296.12 (13)O31—C31—C32A107.7 (4)
O41—Ti—O1196.46 (12)O31—C31—C32B107.1 (5)
O12—Ti—O11104.55 (11)C32A—C31—C32B47.3 (4)
O41—Ti—O21102.08 (11)O31—C31—H31A99 (3)
O12—Ti—O2189.51 (10)C32A—C31—H31A123 (3)
O11—Ti—O21155.40 (11)O31—C31—H31B104 (3)
O41—Ti—O3199.61 (12)C32B—C31—H31B130 (3)
O12—Ti—O31157.61 (10)H31A—C31—H31B133 (4)
O11—Ti—O3189.46 (10)O32—C34—C33A106.3 (4)
O21—Ti—O3171.71 (9)O32—C34—C33B110.4 (5)
O41—Ti—N11167.78 (11)O32—C34—H34A110 (3)
O12—Ti—N1176.37 (11)C33A—C34—H34A121 (3)
O11—Ti—N1176.51 (11)O32—C34—H34B112 (2)
O21—Ti—N1187.64 (9)C33B—C34—H34B127 (2)
O31—Ti—N1190.41 (10)H34A—C34—H34B116 (3)
C11—O11—Ti124.9 (2)N31—C32A—C31107.2 (5)
C14—O12—Ti125.6 (2)N31—C32A—H321110.3
C21—O21—Ti127.52 (18)C31—C32A—H321110.3
C21—O21—Zr115.15 (18)N31—C32A—H322110.3
Ti—O21—Zr109.39 (10)C31—C32A—H322110.3
C24—O22—Zr124.8 (2)H321—C32A—H322108.5
C31—O31—Ti124.0 (2)N31—C33A—C34106.1 (5)
C31—O31—Zr123.2 (2)N31—C33A—H331110.5
Ti—O31—Zr108.96 (10)C34—C33A—H331110.5
C34—O32—Zr123.7 (2)N31—C33A—H332110.5
C41A—O41—Ti139.9 (6)C34—C33A—H332110.5
C41B—O41—Ti141.3 (18)H331—C33A—H332108.7
C4OC—O41—Ti144 (2)N31—C35A—H351109.5
C51A—O51—Zr165.0 (4)N31—C35A—H352109.5
C51B—O51—Zr143.2 (7)N31—C35A—H353109.5
C15—N11—C13110.2 (3)O41—C41A—C42A121.1 (9)
C15—N11—C12110.5 (3)O41—C41A—H411107.1
C13—N11—C12111.8 (3)C42A—C41A—H411107.1
C15—N11—Ti117.1 (2)O41—C41A—H412107.1
C13—N11—Ti103.0 (2)C42A—C41A—H412107.1
C12—N11—Ti104.0 (2)H411—C41A—H412106.8
C23—N21—C25109.3 (2)C41A—C42A—C43A101.5 (9)
C23—N21—C22111.5 (3)C41A—C42A—H421111.5
C25—N21—C22109.7 (3)C43A—C42A—H421111.5
C23—N21—Zr103.35 (19)C41A—C42A—H422111.5
C25—N21—Zr113.0 (2)C43A—C42A—H422111.5
C22—N21—Zr109.72 (18)H421—C42A—H422109.3
C32B—N31—C33B117.1 (6)O51—C51A—C52A109.2 (7)
C32B—N31—C33A143.1 (5)O51—C51A—H511109.8
C33B—N31—C32A146.1 (5)C52A—C51A—H511109.8
C33A—N31—C32A114.3 (5)O51—C51A—H512109.8
C33A—N31—C35A108.0 (5)C52A—C51A—H512109.8
C32A—N31—C35A109.3 (4)H511—C51A—H512108.3
C32B—N31—C35B108.5 (5)C53A—C52A—C51A111.5 (7)
C33B—N31—C35B107.4 (5)C53A—C52A—H521109.3
C35A—N31—C35B141.8 (5)C51A—C52A—H521109.3
C32B—N31—Zr109.6 (4)C53A—C52A—H522109.3
C33B—N31—Zr105.5 (4)C51A—C52A—H522109.3
C33A—N31—Zr107.2 (3)H521—C52A—H522108.0
C32A—N31—Zr108.4 (3)N31—C32B—C31108.9 (6)
C35A—N31—Zr109.6 (3)N31—C32B—H323109.9
C35B—N31—Zr108.4 (4)C31—C32B—H323109.9
O11—C11—C12109.1 (3)N31—C32B—H324109.9
O11—C11—H11A109.9C31—C32B—H324109.9
C12—C11—H11A109.9H323—C32B—H324108.3
O11—C11—H11B109.9N31—C33B—C34105.7 (6)
C12—C11—H11B109.9N31—C33B—H333110.6
H11A—C11—H11B108.3C34—C33B—H333110.6
N11—C12—C11108.0 (3)N31—C33B—H334110.6
N11—C12—H12A110.1C34—C33B—H334110.6
C11—C12—H12A110.1H333—C33B—H334108.7
N11—C12—H12B110.1N31—C35B—H354109.5
C11—C12—H12B110.1N31—C35B—H355109.5
H12A—C12—H12B108.4H354—C35B—H355109.5
N11—C13—C14108.6 (3)N31—C35B—H356109.5
N11—C13—H13A110.0H354—C35B—H356109.5
C14—C13—H13A110.0H355—C35B—H356109.5
N11—C13—H13B110.0O41—C41B—C42B105 (4)
C14—C13—H13B110.0O51—C51B—C52B111.7 (13)
H13A—C13—H13B108.3O51—C51B—H513109.3
O12—C14—C13110.5 (3)C52B—C51B—H513109.3
O12—C14—H14B109.5O51—C51B—H514109.3
C13—C14—H14B109.5C52B—C51B—H514109.3
O12—C14—H14A109.5H513—C51B—H514107.9
C13—C14—H14A109.5C51B—C52B—C53B121.6 (8)
H14B—C14—H14A108.1C51B—C52B—H523106.9
N11—C15—H15A109.5C53B—C52B—H523106.9
N11—C15—H15B109.5C51B—C52B—H524106.9
H15A—C15—H15B109.5C53B—C52B—H524106.9
N11—C15—H15C109.5H523—C52B—H524106.7
H15A—C15—H15C109.5C52B—C53B—H534109.5
H15B—C15—H15C109.5C52B—C53B—H535109.5
O21—C21—C22107.3 (3)H534—C53B—H535109.5
O21—C21—H21A110.3C52B—C53B—H536109.5
C22—C21—H21A110.3H534—C53B—H536109.5
O21—C21—H21B110.3H535—C53B—H536109.5
C22—C21—H21B110.3C43C—C41C—O41114 (4)
H21A—C21—H21B108.5O41—C41C—C42C105 (5)
N21—C22—C21109.8 (3)C43C—C4OC—C42C102 (4)
N21—C22—H22A109.7C43C—C4OC—O41122 (4)
C21—C22—H22A109.7C42C—C4OC—O41113 (4)
O41—Ti—O11—C11173.9 (3)O32—Zr—N21—C2553.4 (2)
O12—Ti—O11—C1175.9 (3)O31—Zr—N21—C25139.7 (2)
O21—Ti—O11—C1147.2 (4)O21—Zr—N21—C25120.0 (2)
O31—Ti—O11—C1186.5 (3)N31—Zr—N21—C2566.6 (3)
N11—Ti—O11—C114.1 (3)O51—Zr—N21—C2287.3 (2)
O41—Ti—O12—C14179.4 (3)O22—Zr—N21—C2291.5 (2)
O11—Ti—O12—C1482.3 (3)O32—Zr—N21—C22176.2 (2)
O21—Ti—O12—C1477.3 (3)O31—Zr—N21—C2216.9 (3)
O31—Ti—O12—C1444.9 (4)O21—Zr—N21—C222.9 (2)
N11—Ti—O12—C1410.4 (3)N31—Zr—N21—C22170.5 (2)
O41—Ti—O21—C2166.8 (3)O51—Zr—N31—C32B72.8 (5)
O12—Ti—O21—C2129.4 (3)O22—Zr—N31—C32B113.3 (4)
O11—Ti—O21—C21155.2 (3)O32—Zr—N31—C32B160.6 (5)
O31—Ti—O21—C21163.0 (3)O31—Zr—N31—C32B25.1 (4)
N11—Ti—O21—C21105.8 (3)O21—Zr—N31—C32B14.8 (5)
O41—Ti—O21—Zr80.19 (13)N21—Zr—N31—C32B174.2 (4)
O12—Ti—O21—Zr176.35 (11)O51—Zr—N31—C33B54.1 (4)
O11—Ti—O21—Zr57.9 (3)O22—Zr—N31—C33B119.8 (4)
O31—Ti—O21—Zr16.06 (10)O32—Zr—N31—C33B33.6 (4)
N11—Ti—O21—Zr107.28 (11)O31—Zr—N31—C33B152.0 (4)
O51—Zr—O21—C2165.2 (2)O21—Zr—N31—C33B141.8 (4)
O22—Zr—O21—C21100.7 (2)N21—Zr—N31—C33B47.3 (5)
O32—Zr—O21—C2114.3 (3)O51—Zr—N31—C33A109.5 (4)
O31—Zr—O21—C21167.3 (2)O22—Zr—N31—C33A64.4 (4)
N31—Zr—O21—C21156.6 (2)O32—Zr—N31—C33A21.8 (4)
N21—Zr—O21—C2127.9 (2)O31—Zr—N31—C33A152.6 (4)
O51—Zr—O21—Ti86.23 (12)O21—Zr—N31—C33A162.8 (3)
O22—Zr—O21—Ti107.88 (11)N21—Zr—N31—C33A8.1 (5)
O32—Zr—O21—Ti165.71 (16)O51—Zr—N31—C32A126.6 (4)
O31—Zr—O21—Ti15.84 (10)O22—Zr—N31—C32A59.5 (4)
N31—Zr—O21—Ti5.18 (18)O32—Zr—N31—C32A145.6 (4)
N21—Zr—O21—Ti179.33 (13)O31—Zr—N31—C32A28.7 (3)
O51—Zr—O22—C2410.8 (5)O21—Zr—N31—C32A39.0 (4)
O32—Zr—O22—C2473.4 (3)N21—Zr—N31—C32A132.0 (4)
O31—Zr—O22—C24143.4 (2)O51—Zr—N31—C35A7.4 (3)
O21—Zr—O22—C2477.7 (2)O22—Zr—N31—C35A178.6 (3)
N31—Zr—O22—C24145.6 (2)O32—Zr—N31—C35A95.2 (3)
N21—Zr—O22—C246.2 (2)O31—Zr—N31—C35A90.5 (3)
O41—Ti—O31—C3175.1 (3)O21—Zr—N31—C35A80.2 (3)
O12—Ti—O31—C31150.9 (3)N21—Zr—N31—C35A108.8 (4)
O11—Ti—O31—C3121.4 (3)O51—Zr—N31—C35B168.9 (4)
O21—Ti—O31—C31174.8 (3)O22—Zr—N31—C35B5.0 (4)
N11—Ti—O31—C3197.9 (3)O32—Zr—N31—C35B81.2 (4)
O41—Ti—O31—Zr83.33 (13)O31—Zr—N31—C35B93.2 (4)
O12—Ti—O31—Zr50.7 (3)O21—Zr—N31—C35B103.4 (4)
O11—Ti—O31—Zr179.79 (12)N21—Zr—N31—C35B67.5 (4)
O21—Ti—O31—Zr16.32 (10)Ti—O11—C11—C1228.4 (4)
N11—Ti—O31—Zr103.70 (12)C15—N11—C12—C1186.9 (4)
O51—Zr—O31—C3193.5 (3)C13—N11—C12—C11150.0 (3)
O22—Zr—O31—C3197.9 (3)Ti—N11—C12—C1139.5 (3)
O32—Zr—O31—C317.2 (4)O11—C11—C12—N1144.9 (4)
O21—Zr—O31—C31174.0 (3)C15—N11—C13—C14166.6 (3)
N31—Zr—O31—C311.8 (3)C12—N11—C13—C1470.2 (4)
N21—Zr—O31—C31165.3 (3)Ti—N11—C13—C1440.9 (3)
O51—Zr—O31—Ti65.15 (13)Ti—O12—C14—C1310.6 (4)
O22—Zr—O31—Ti103.49 (12)N11—C13—C14—O1237.0 (4)
O32—Zr—O31—Ti165.87 (13)Ti—O21—C21—C22160.8 (2)
O21—Zr—O31—Ti15.38 (9)Zr—O21—C21—C2253.8 (3)
N31—Zr—O31—Ti156.83 (14)C23—N21—C22—C21144.1 (3)
N21—Zr—O31—Ti36.04 (18)C25—N21—C22—C2194.5 (3)
O51—Zr—O32—C3485.0 (3)Zr—N21—C22—C2130.2 (3)
O22—Zr—O32—C34110.3 (3)O21—C21—C22—N2154.0 (4)
O31—Zr—O32—C3418.9 (4)C25—N21—C23—C24165.1 (3)
O21—Zr—O32—C34163.5 (3)C22—N21—C23—C2473.3 (3)
N31—Zr—O32—C349.9 (3)Zr—N21—C23—C2444.5 (3)
N21—Zr—O32—C34176.6 (3)Zr—O22—C24—C2317.0 (4)
O12—Ti—O41—C41A6.2 (7)N21—C23—C24—O2243.1 (4)
O11—Ti—O41—C41A111.7 (7)Ti—O31—C31—C32A179.2 (4)
O21—Ti—O41—C41A84.6 (7)Zr—O31—C31—C32A23.7 (5)
O31—Ti—O41—C41A157.8 (7)Ti—O31—C31—C32B129.5 (4)
N11—Ti—O41—C41A57.5 (10)Zr—O31—C31—C32B25.9 (5)
O21—Ti—O41—C41B105 (3)Zr—O32—C34—C33A37.0 (5)
N11—Ti—O41—C41B112 (3)Zr—O32—C34—C33B14.3 (6)
O22—Zr—O51—C51A10.5 (18)Zr—N31—C32A—C3149.3 (5)
O32—Zr—O51—C51A73.8 (17)O31—C31—C32A—N3147.7 (6)
O31—Zr—O51—C51A142.3 (17)C32B—C31—C32A—N3149.6 (6)
O21—Zr—O51—C51A77.8 (17)C32B—N31—C33A—C34138.9 (8)
N31—Zr—O51—C51A146.2 (17)C33B—N31—C33A—C3451.9 (6)
N21—Zr—O51—C51A6.0 (17)C32A—N31—C33A—C34165.0 (5)
O22—Zr—O51—C51B86.0 (11)C35A—N31—C33A—C3473.2 (6)
O32—Zr—O51—C51B1.7 (11)C35B—N31—C33A—C34145.8 (7)
O31—Zr—O51—C51B142.3 (11)Zr—N31—C33A—C3444.8 (5)
O21—Zr—O51—C51B153.3 (11)O32—C34—C33A—N3152.7 (6)
N31—Zr—O51—C51B70.8 (11)Ti—O41—C41A—C42A131.0 (9)
N21—Zr—O51—C51B81.5 (11)O41—C41A—C42A—C43A58.8 (13)
O41—Ti—N11—C15157.2 (6)C51B—O51—C51A—C52A13.1 (11)
O12—Ti—N11—C15149.8 (3)Zr—O51—C51A—C52A83.0 (18)
O11—Ti—N11—C15101.3 (3)O51—C51A—C52A—C53A168.5 (6)
O21—Ti—N11—C1559.7 (3)C33B—N31—C32B—C31166.2 (6)
O31—Ti—N11—C1511.9 (3)C33A—N31—C32B—C31130.2 (8)
O41—Ti—N11—C1381.7 (6)C32A—N31—C32B—C3152.0 (6)
O12—Ti—N11—C1328.7 (2)C35A—N31—C32B—C31148.3 (8)
O11—Ti—N11—C13137.6 (2)C35B—N31—C32B—C3172.1 (7)
O21—Ti—N11—C1361.4 (2)Zr—N31—C32B—C3146.1 (7)
O31—Ti—N11—C13133.1 (2)O31—C31—C32B—N3146.7 (7)
O41—Ti—N11—C1235.0 (7)C32A—C31—C32B—N3151.8 (6)
O12—Ti—N11—C1288.1 (2)C32B—N31—C33B—C34171.1 (6)
O11—Ti—N11—C1220.8 (2)C33A—N31—C33B—C3451.3 (6)
O21—Ti—N11—C12178.1 (2)C32A—N31—C33B—C34129.9 (8)
O31—Ti—N11—C12110.2 (2)C35A—N31—C33B—C34152.7 (8)
O51—Zr—N21—C23153.61 (19)C35B—N31—C33B—C3466.6 (7)
O22—Zr—N21—C2327.61 (18)Zr—N31—C33B—C3448.9 (6)
O32—Zr—N21—C2364.7 (2)O32—C34—C33B—N3143.8 (7)
O31—Zr—N21—C23102.2 (2)C33A—C34—C33B—N3150.3 (6)
O21—Zr—N21—C23122.0 (2)Ti—O41—C41B—C42B175.1 (15)
N31—Zr—N21—C2351.5 (3)Zr—O51—C51B—C52B140.2 (8)
O51—Zr—N21—C2535.5 (2)O51—C51B—C52B—C53B173.0 (5)
O22—Zr—N21—C25145.7 (2)

Experimental details

Crystal data
Chemical formula[TiZr(C5H11NO2)3(C3H7O)2]
Mr608.74
Crystal system, space groupMonoclinic, C2/c
Temperature (K)163
a, b, c (Å)31.172 (10), 10.407 (3), 19.116 (6)
β (°) 116.002 (3)
V3)5574 (5)
Z8
Radiation typeMo Kα
µ (mm1)0.71
Crystal size (mm)0.30 × 0.27 × 0.25
Data collection
DiffractometerMake Model CCD area-detector
diffractometer
Absorption correctionMulti scan
(Blessing, 1995)
Tmin, Tmax0.686, 0.837
No. of measured, independent and
observed [I > 2σ(I)] reflections
19935, 5613, 3723
Rint0.056
(sin θ/λ)max1)0.626
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.043, 0.104, 0.95
No. of reflections5613
No. of parameters272
No. of restraints1
H-atom treatmentH atoms treated by a mixture of independent and constrained refinement
Δρmax, Δρmin (e Å3)0.60, 0.59

Computer programs: SMART (Siemens, 1996), SMART, SAINT (Siemens, 1996) and SADABS (Sheldrick, 1996), SHELXS97 (Sheldrick, 1997), SHELXL97 (Sheldrick, 1997), ORTEP-3 in WinGX (Farrugia, 1997, 1999), SHELXL97.

Selected geometric parameters (Å, º) top
Zr—O511.977 (3)Ti—O411.786 (3)
Zr—O222.046 (2)Ti—O121.877 (2)
Zr—O322.068 (2)Ti—O111.887 (2)
Zr—O312.182 (2)Ti—O212.014 (2)
Zr—O212.222 (2)Ti—O312.067 (2)
Zr—N312.397 (3)Ti—N112.346 (3)
Zr—N212.443 (3)
O51—Zr—O3198.93 (10)O21—Zr—N31136.14 (9)
O32—Zr—O31143.18 (9)O31—Zr—N21135.17 (9)
O22—Zr—O2188.84 (9)O21—Zr—N2171.94 (8)
O32—Zr—N3172.55 (10)O12—Ti—N1176.37 (11)
O31—Zr—N3171.05 (9)O11—Ti—N1176.51 (11)
O11—Ti—O21—Zr57.9 (3)O31—Ti—O21—Zr16.06 (10)
 

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