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In the title complex, [GaCl3(CH3CN)], the GaIII atom shows a slightly distorted tetra­hedral coordination, with three Cl atoms and one N atom of the acetonitrile as ligands. The Ga atom, one Cl atom, the N atom, both C atoms and one H atom of the acetonitrile mol­ecule are situated on a mirror plane. The crystal packing is stabilized by several weak inter­molecular C—H...Cl hydrogen-bonding contacts.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536807043516/wm2142sup1.cif
Contains datablocks I, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536807043516/wm2142Isup2.hkl
Contains datablock I

CCDC reference: 667186

Key indicators

  • Single-crystal X-ray study
  • T = 173 K
  • Mean [sigma](C-C) = 0.003 Å
  • R factor = 0.017
  • wR factor = 0.042
  • Data-to-parameter ratio = 21.1

checkCIF/PLATON results

No syntax errors found



Alert level B PLAT480_ALERT_4_B Long H...A H-Bond Reported H1 .. CL2 .. 3.34 Ang. PLAT480_ALERT_4_B Long H...A H-Bond Reported H2 .. CL1 .. 3.44 Ang. PLAT480_ALERT_4_B Long H...A H-Bond Reported H2 .. CL2 .. 3.23 Ang.
Alert level C PLAT031_ALERT_4_C Refined Extinction Parameter within Range ...... 2.57 Sigma PLAT063_ALERT_3_C Crystal Probably too Large for Beam Size ....... 0.73 mm PLAT164_ALERT_4_C Nr. of Refined C-H H-Atoms in Heavy-At Struct... 2 PLAT242_ALERT_2_C Check Low Ueq as Compared to Neighbors for Ga1 PLAT390_ALERT_3_C Deviating Methyl C2 X-C-H Bond Angle ...... 117.00 Deg. PLAT480_ALERT_4_C Long H...A H-Bond Reported H1 .. CL1 .. 3.01 Ang. PLAT480_ALERT_4_C Long H...A H-Bond Reported H2 .. CL2 .. 2.90 Ang. PLAT710_ALERT_4_C Delete 1-2-3 or 2-3-4 Linear Torsion Angle ... # 1 CL1 -GA1 -N1 -C1 0.00 0.03 1.555 1.555 1.555 1.555 PLAT710_ALERT_4_C Delete 1-2-3 or 2-3-4 Linear Torsion Angle ... # 2 CL2 -GA1 -N1 -C1 -119.72 0.04 1.555 1.555 1.555 1.555 PLAT710_ALERT_4_C Delete 1-2-3 or 2-3-4 Linear Torsion Angle ... # 3 CL2 -GA1 -N1 -C1 119.72 0.03 7.565 1.555 1.555 1.555 PLAT710_ALERT_4_C Delete 1-2-3 or 2-3-4 Linear Torsion Angle ... # 4 GA1 -N1 -C1 -C2 18.00 0.00 1.555 1.555 1.555 1.555
0 ALERT level A = In general: serious problem 3 ALERT level B = Potentially serious problem 11 ALERT level C = Check and explain 0 ALERT level G = General alerts; check 0 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 1 ALERT type 2 Indicator that the structure model may be wrong or deficient 2 ALERT type 3 Indicator that the structure quality may be low 11 ALERT type 4 Improvement, methodology, query or suggestion 0 ALERT type 5 Informative message, check

Comment top

In the title adduct, the coordination of the Ga atom by the three Cl atoms and the N atom of the acetonitrile ligand can be considered as slightly distorted tetrahedral, with Cl—Ga—N bond angles in the range 104.68 (6)–105.14 (3) ° and Cl—Ga—Cl bond angles in the range 113.371 (17)–113.93 (3) ° (Fig. 1).

The Cs-symmetric molecule exhibits an almost linear Ga—N1—C1—C2 unit (C1—N1—Ga1 = 179.22 (19) °, N1—C1—C2 = 179.9 (3) °), and the H atoms of the methyl group adopt a staggered conformation relative to the Cl atoms.

In the crystal structure, the GaCl3.CH3CN adducts are linked by very weak intermolecular C—H···Cl interactions (Fig. 2, Table).

Related literature top

For related literature, see: Herler et al. (2005).

Experimental top

The title compound was unintentionally obtained as a by-product of an attempted reaction of 4-bis(trimethylsilyl)-amino-1,2,4,3,5-triazadiphosphole GaCl3 adduct (Herler et al., 2005) with Cr(CH3CN)3(CO)3 in CH2Cl2. Recrystallization from a saturated CH2Cl2/Et2O solution at ambient temperature gave colourless needle-like crystals of GaCl3.CH3CN.

Refinement top

All Hydrogen atoms were found from difference Fourier maps and were refined freely.

Structure description top

In the title adduct, the coordination of the Ga atom by the three Cl atoms and the N atom of the acetonitrile ligand can be considered as slightly distorted tetrahedral, with Cl—Ga—N bond angles in the range 104.68 (6)–105.14 (3) ° and Cl—Ga—Cl bond angles in the range 113.371 (17)–113.93 (3) ° (Fig. 1).

The Cs-symmetric molecule exhibits an almost linear Ga—N1—C1—C2 unit (C1—N1—Ga1 = 179.22 (19) °, N1—C1—C2 = 179.9 (3) °), and the H atoms of the methyl group adopt a staggered conformation relative to the Cl atoms.

In the crystal structure, the GaCl3.CH3CN adducts are linked by very weak intermolecular C—H···Cl interactions (Fig. 2, Table).

For related literature, see: Herler et al. (2005).

Computing details top

Data collection: APEX2 (Bruker, 2003); cell refinement: APEX2 (Bruker, 2003); data reduction: SAINT (Bruker, 2003); program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: ORTEP-3 (Farrugia, 1997) and DIAMOND (Brandenburg, 2005); software used to prepare material for publication: SHELXL97 (Sheldrick, 1997).

Figures top
[Figure 1] Fig. 1. Molecular structure of (I), showing the atomic numbering scheme and displacement ellipsoids drawn at the 50% probability level. [Symmetry code: (i) x, -y + 1/2, z.]
[Figure 2] Fig. 2. Part of the packing diagram of (I). Unique C—H···Cl interactions represented by dashed lines are shown for one molecule of (I). Colour code as in Fig. 1. [Symmetry codes: (i) x + 1, y, z; (ii) x + 1/2, y, -z + 1/2; (iii) -x + 1, y - 1/2, -z + 1; (iv) -x + 3/2, -y, z + 1/2; (v) -x + 1, -y, -z + 1.]
(Acetonitrile-κN)trichloridogallium(III) top
Crystal data top
[GaCl3(C2H3N)]F(000) = 416
Mr = 217.12Dx = 1.928 Mg m3
Orthorhombic, PnmaMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ac 2nCell parameters from 4237 reflections
a = 9.1760 (18) Åθ = 5.8–56.4°
b = 7.5100 (15) ŵ = 4.64 mm1
c = 10.857 (2) ÅT = 173 K
V = 748.2 (3) Å3Needle, colourless
Z = 40.73 × 0.12 × 0.09 mm
Data collection top
Bruker–Nonius Apex X8 CCD
diffractometer
1011 independent reflections
Radiation source: sealed tube878 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.037
ω scansθmax = 28.5°, θmin = 2.9°
Absorption correction: multi-scan
(SADABS; Sheldrick, 2004)
h = 1212
Tmin = 0.130, Tmax = 0.660k = 109
11546 measured reflectionsl = 1414
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.017All H-atom parameters refined
wR(F2) = 0.042 w = 1/[σ2(Fo2) + (0.0212P)2 + 0.2025P]
where P = (Fo2 + 2Fc2)/3
S = 1.04(Δ/σ)max < 0.001
1011 reflectionsΔρmax = 0.28 e Å3
48 parametersΔρmin = 0.38 e Å3
0 restraintsExtinction correction: SHELXL, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.0018 (7)
Crystal data top
[GaCl3(C2H3N)]V = 748.2 (3) Å3
Mr = 217.12Z = 4
Orthorhombic, PnmaMo Kα radiation
a = 9.1760 (18) ŵ = 4.64 mm1
b = 7.5100 (15) ÅT = 173 K
c = 10.857 (2) Å0.73 × 0.12 × 0.09 mm
Data collection top
Bruker–Nonius Apex X8 CCD
diffractometer
1011 independent reflections
Absorption correction: multi-scan
(SADABS; Sheldrick, 2004)
878 reflections with I > 2σ(I)
Tmin = 0.130, Tmax = 0.660Rint = 0.037
11546 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0170 restraints
wR(F2) = 0.042All H-atom parameters refined
S = 1.04Δρmax = 0.28 e Å3
1011 reflectionsΔρmin = 0.38 e Å3
48 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
Ga10.41273 (2)0.25000.356223 (19)0.02617 (9)
Cl10.25406 (7)0.25000.50041 (6)0.04725 (17)
Cl20.41187 (5)0.01076 (6)0.24861 (4)0.04570 (13)
N10.60162 (19)0.25000.44199 (18)0.0359 (4)
C10.7096 (2)0.25000.4926 (2)0.0331 (5)
C20.8469 (3)0.25000.5568 (3)0.0437 (6)
H10.926 (5)0.25000.511 (6)0.13 (2)*
H20.861 (3)0.159 (4)0.605 (3)0.106 (10)*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Ga10.02312 (12)0.02984 (13)0.02554 (13)0.0000.00012 (8)0.000
Cl10.0414 (3)0.0532 (3)0.0472 (3)0.0000.0204 (3)0.000
Cl20.0555 (3)0.0393 (2)0.0424 (2)0.00081 (19)0.00219 (17)0.01284 (17)
N10.0290 (9)0.0415 (10)0.0372 (10)0.0000.0038 (8)0.000
C10.0296 (10)0.0345 (11)0.0352 (11)0.0000.0010 (8)0.000
C20.0288 (11)0.0513 (15)0.0512 (16)0.0000.0133 (11)0.000
Geometric parameters (Å, º) top
Ga1—N11.9676 (18)N1—C11.133 (3)
Ga1—Cl12.1379 (7)C1—C21.440 (3)
Ga1—Cl22.1432 (5)C2—H10.88 (5)
Ga1—Cl2i2.1432 (5)C2—H20.87 (3)
N1—Ga1—Cl1104.68 (6)C1—N1—Ga1179.22 (19)
N1—Ga1—Cl2105.14 (3)N1—C1—C2179.9 (3)
Cl1—Ga1—Cl2113.371 (17)C1—C2—H1116 (4)
N1—Ga1—Cl2i105.14 (3)C1—C2—H2115 (2)
Cl1—Ga1—Cl2i113.371 (17)H1—C2—H2103 (3)
Cl2—Ga1—Cl2i113.93 (3)
Cl1—Ga1—N1—C10.00 (3)Cl2i—Ga1—N1—C1119.72 (3)
Cl2—Ga1—N1—C1119.72 (4)Ga1—N1—C1—C2180 (100)
Symmetry code: (i) x, y+1/2, z.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C2—H1···Cl1ii0.88 (5)3.01 (5)3.786 (3)147 (5)
C2—H1···Cl2iii0.88 (5)3.34 (5)3.818 (3)117 (3)
C2—H2···Cl1iv0.87 (3)3.44 (3)3.9172 (10)117 (2)
C2—H2···Cl2v0.87 (3)2.90 (3)3.615 (2)141 (2)
C2—H2···Cl2vi0.87 (3)3.23 (3)3.733 (3)119 (2)
Symmetry codes: (ii) x+1, y, z; (iii) x+1/2, y, z+1/2; (iv) x+1, y1/2, z+1; (v) x+3/2, y, z+1/2; (vi) x+1, y, z+1.

Experimental details

Crystal data
Chemical formula[GaCl3(C2H3N)]
Mr217.12
Crystal system, space groupOrthorhombic, Pnma
Temperature (K)173
a, b, c (Å)9.1760 (18), 7.5100 (15), 10.857 (2)
V3)748.2 (3)
Z4
Radiation typeMo Kα
µ (mm1)4.64
Crystal size (mm)0.73 × 0.12 × 0.09
Data collection
DiffractometerBruker–Nonius Apex X8 CCD
diffractometer
Absorption correctionMulti-scan
(SADABS; Sheldrick, 2004)
Tmin, Tmax0.130, 0.660
No. of measured, independent and
observed [I > 2σ(I)] reflections
11546, 1011, 878
Rint0.037
(sin θ/λ)max1)0.671
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.017, 0.042, 1.04
No. of reflections1011
No. of parameters48
H-atom treatmentAll H-atom parameters refined
Δρmax, Δρmin (e Å3)0.28, 0.38

Computer programs: APEX2 (Bruker, 2003), SAINT (Bruker, 2003), SHELXS97 (Sheldrick, 1997), SHELXL97 (Sheldrick, 1997), ORTEP-3 (Farrugia, 1997) and DIAMOND (Brandenburg, 2005), SHELXL97 (Sheldrick, 1997).

Selected geometric parameters (Å, º) top
Ga1—N11.9676 (18)Ga1—Cl22.1432 (5)
Ga1—Cl12.1379 (7)
N1—Ga1—Cl1104.68 (6)Cl1—Ga1—Cl2113.371 (17)
N1—Ga1—Cl2105.14 (3)Cl2—Ga1—Cl2i113.93 (3)
Symmetry code: (i) x, y+1/2, z.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C2—H1···Cl1ii0.88 (5)3.01 (5)3.786 (3)147 (5)
C2—H1···Cl2iii0.88 (5)3.34 (5)3.818 (3)117 (3)
C2—H2···Cl1iv0.87 (3)3.44 (3)3.9172 (10)117 (2)
C2—H2···Cl2v0.87 (3)2.90 (3)3.615 (2)141 (2)
C2—H2···Cl2vi0.87 (3)3.23 (3)3.733 (3)119 (2)
Symmetry codes: (ii) x+1, y, z; (iii) x+1/2, y, z+1/2; (iv) x+1, y1/2, z+1; (v) x+3/2, y, z+1/2; (vi) x+1, y, z+1.
 

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