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The second polymorph (monoclinic form) of the [Re(NCS){LH(Me)NO}(CO)3] complex, where LH(Me)NO is N-methyl­pyridine-2-carboxamide, has been obtained and structurally characterized by X-ray diffraction and supported by DFT calculations.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S205698901601389X/wm5320sup1.cif
Contains datablock I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S205698901601389X/wm5320Isup2.hkl
Contains datablock I

CCDC reference: 1501544

Key indicators

  • Single-crystal X-ray study
  • T = 100 K
  • Mean [sigma](C-C) = 0.002 Å
  • R factor = 0.011
  • wR factor = 0.025
  • Data-to-parameter ratio = 21.8

checkCIF/PLATON results

No syntax errors found



Alert level C PLAT480_ALERT_4_C Long H...A H-Bond Reported H7 .. S1 .. 2.90 Ang. PLAT480_ALERT_4_C Long H...A H-Bond Reported H10C .. S1 .. 2.98 Ang.
Alert level G PLAT142_ALERT_4_G s.u. on b - Axis Small or Missing .............. 0.00010 Ang. PLAT143_ALERT_4_G s.u. on c - Axis Small or Missing .............. 0.00010 Ang. PLAT153_ALERT_1_G The s.u.'s on the Cell Axes are Equal ..(Note) 0.0001 Ang. PLAT230_ALERT_2_G Hirshfeld Test Diff for S1 -- C11 .. 7.9 s.u. PLAT230_ALERT_2_G Hirshfeld Test Diff for O2 -- C2 .. 6.7 s.u. PLAT232_ALERT_2_G Hirshfeld Test Diff (M-X) Re1 -- N3 .. 8.7 s.u. PLAT232_ALERT_2_G Hirshfeld Test Diff (M-X) Re1 -- C1 .. 10.6 s.u. PLAT232_ALERT_2_G Hirshfeld Test Diff (M-X) Re1 -- C2 .. 13.4 s.u. PLAT232_ALERT_2_G Hirshfeld Test Diff (M-X) Re1 -- C3 .. 11.8 s.u. PLAT910_ALERT_3_G Missing # of FCF Reflection(s) Below Theta(Min) 2 Note PLAT978_ALERT_2_G Number C-C Bonds with Positive Residual Density 5 Note
0 ALERT level A = Most likely a serious problem - resolve or explain 0 ALERT level B = A potentially serious problem, consider carefully 2 ALERT level C = Check. Ensure it is not caused by an omission or oversight 11 ALERT level G = General information/check it is not something unexpected 1 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 7 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 4 ALERT type 4 Improvement, methodology, query or suggestion 0 ALERT type 5 Informative message, check

Computing details top

Data collection: CrysAlis PRO (Agilent, 2014); cell refinement: CrysAlis PRO (Agilent, 2014); data reduction: CrysAlis PRO (Agilent, 2014); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL2014 (Sheldrick, 2015); molecular graphics: Mercury (Macrae et al., 2008); software used to prepare material for publication: publCIF (Westrip, 2010).

Tricarbonyl(N-methylpyridine-2-carboxamide-κ2N1,O)(thiocyanato-κN)rhenium(I) top
Crystal data top
[Re(NCS)(C7H8N2O)(CO)3]F(000) = 872
Mr = 464.46Dx = 2.213 Mg m3
Monoclinic, P21/nMo Kα radiation, λ = 0.71073 Å
a = 8.3456 (1) ÅCell parameters from 49644 reflections
b = 13.3241 (1) Åθ = 3.1–31.3°
c = 12.7011 (1) ŵ = 8.88 mm1
β = 99.284 (1)°T = 100 K
V = 1393.83 (2) Å3Block, yellow
Z = 40.15 × 0.12 × 0.08 mm
Data collection top
Agilent SuperNova Dual Source
diffractometer with an Eos detector
4060 independent reflections
Radiation source: SuperNova (Mo) X-ray Source3921 reflections with I > 2σ(I)
Detector resolution: 16.0131 pixels mm-1Rint = 0.041
ω scansθmax = 30.0°, θmin = 2.9°
Absorption correction: multi-scan
(CrysAlis PRO; Agilent, 2014)
h = 1111
Tmin = 0.629, Tmax = 1.000k = 1818
77774 measured reflectionsl = 1717
Refinement top
Refinement on F20 restraints
Least-squares matrix: fullHydrogen site location: mixed
R[F2 > 2σ(F2)] = 0.011H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.025 w = 1/[σ2(Fo2) + (0.0082P)2 + 0.8572P]
where P = (Fo2 + 2Fc2)/3
S = 1.11(Δ/σ)max = 0.005
4060 reflectionsΔρmax = 0.42 e Å3
186 parametersΔρmin = 0.51 e Å3
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.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Re10.94102 (2)0.61839 (2)0.78536 (2)0.01041 (2)
S10.39614 (5)0.76937 (3)0.72060 (3)0.01731 (8)
O20.81867 (15)0.46596 (9)0.93364 (10)0.0228 (3)
N20.96200 (16)0.75572 (10)0.48766 (10)0.0133 (2)
O11.07960 (14)0.74704 (9)0.97900 (9)0.0203 (2)
C20.86838 (19)0.52386 (12)0.87960 (12)0.0161 (3)
O40.99371 (13)0.71917 (8)0.66237 (8)0.0127 (2)
N10.85068 (15)0.54369 (9)0.63442 (10)0.0125 (2)
O31.27172 (14)0.51162 (9)0.82262 (9)0.0184 (2)
C31.14740 (19)0.55136 (11)0.80679 (11)0.0135 (3)
C11.02572 (18)0.69876 (11)0.90694 (12)0.0145 (3)
C50.7205 (2)0.41062 (12)0.52690 (14)0.0192 (3)
H50.67440.34530.52260.023*
C60.7256 (2)0.46596 (12)0.43525 (13)0.0184 (3)
H60.68110.43960.36730.022*
C80.85873 (18)0.59693 (11)0.54460 (12)0.0120 (3)
C40.78361 (19)0.45171 (11)0.62492 (13)0.0159 (3)
H40.77940.41360.68760.019*
C90.94147 (17)0.69584 (11)0.56703 (11)0.0116 (3)
N30.71182 (16)0.69184 (10)0.75566 (10)0.0149 (2)
C70.79640 (19)0.56049 (12)0.44386 (12)0.0157 (3)
H70.80210.59950.38200.019*
C101.0420 (2)0.85309 (12)0.50654 (13)0.0166 (3)
H10A0.98830.89220.55620.025*
H10B1.03490.88940.43890.025*
H10C1.15630.84300.53720.025*
C110.58131 (19)0.72422 (11)0.74029 (11)0.0130 (3)
H20.921 (3)0.7413 (16)0.4243 (18)0.026 (6)*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Re10.01001 (3)0.01132 (3)0.00967 (3)0.00108 (2)0.00092 (2)0.00183 (2)
S10.01461 (18)0.02173 (19)0.01450 (17)0.00703 (14)0.00096 (13)0.00273 (14)
O20.0222 (6)0.0262 (6)0.0202 (6)0.0021 (5)0.0040 (5)0.0091 (5)
N20.0159 (6)0.0124 (6)0.0111 (6)0.0027 (5)0.0008 (5)0.0007 (4)
O10.0199 (6)0.0212 (6)0.0190 (6)0.0012 (5)0.0009 (5)0.0047 (4)
C20.0129 (7)0.0196 (7)0.0149 (7)0.0029 (6)0.0005 (5)0.0008 (6)
O40.0134 (5)0.0126 (5)0.0117 (5)0.0016 (4)0.0008 (4)0.0012 (4)
N10.0118 (6)0.0120 (6)0.0137 (6)0.0010 (4)0.0023 (5)0.0009 (4)
O30.0155 (5)0.0195 (5)0.0199 (5)0.0041 (4)0.0016 (4)0.0027 (4)
C30.0154 (7)0.0134 (6)0.0115 (6)0.0018 (5)0.0014 (5)0.0008 (5)
C10.0118 (7)0.0156 (7)0.0161 (7)0.0035 (5)0.0027 (5)0.0030 (5)
C50.0205 (8)0.0145 (7)0.0236 (8)0.0067 (6)0.0061 (6)0.0028 (6)
C60.0195 (8)0.0182 (7)0.0180 (7)0.0049 (6)0.0048 (6)0.0053 (6)
C80.0110 (7)0.0118 (6)0.0133 (6)0.0000 (5)0.0022 (5)0.0005 (5)
C40.0171 (7)0.0124 (7)0.0189 (7)0.0015 (5)0.0051 (6)0.0024 (5)
C90.0099 (6)0.0117 (6)0.0131 (6)0.0016 (5)0.0014 (5)0.0011 (5)
N30.0155 (6)0.0155 (6)0.0136 (6)0.0012 (5)0.0021 (5)0.0003 (5)
C70.0179 (7)0.0161 (7)0.0134 (7)0.0021 (6)0.0036 (6)0.0006 (5)
C100.0194 (8)0.0128 (7)0.0170 (7)0.0038 (6)0.0012 (6)0.0022 (5)
C110.0165 (7)0.0121 (6)0.0103 (6)0.0006 (5)0.0011 (5)0.0010 (5)
Geometric parameters (Å, º) top
Re1—C21.9028 (16)O3—C31.1533 (19)
Re1—C11.9180 (16)C5—C41.384 (2)
Re1—C31.9201 (16)C5—C61.384 (2)
Re1—N32.1275 (13)C5—H50.9500
Re1—O42.1583 (10)C6—C71.388 (2)
Re1—N12.1836 (13)C6—H60.9500
S1—C111.6394 (16)C8—C71.389 (2)
O2—C21.1533 (19)C8—C91.494 (2)
N2—C91.3182 (18)C4—H40.9500
N2—C101.4610 (19)N3—C111.158 (2)
N2—H20.84 (2)C7—H70.9500
O1—C11.1494 (19)C10—H10A0.9800
O4—C91.2581 (17)C10—H10B0.9800
N1—C41.3446 (19)C10—H10C0.9800
N1—C81.3542 (18)
C2—Re1—C188.66 (7)C4—C5—H5120.4
C2—Re1—C388.42 (6)C6—C5—H5120.4
C1—Re1—C386.56 (6)C5—C6—C7119.17 (15)
C2—Re1—N392.72 (6)C5—C6—H6120.4
C1—Re1—N395.16 (6)C7—C6—H6120.4
C3—Re1—N3177.96 (5)N1—C8—C7122.06 (14)
C2—Re1—O4171.84 (5)N1—C8—C9112.69 (13)
C1—Re1—O498.26 (5)C7—C8—C9125.25 (13)
C3—Re1—O496.27 (5)N1—C4—C5122.25 (14)
N3—Re1—O482.40 (4)N1—C4—H4118.9
C2—Re1—N198.66 (6)C5—C4—H4118.9
C1—Re1—N1172.54 (6)O4—C9—N2121.26 (14)
C3—Re1—N195.00 (5)O4—C9—C8118.64 (13)
N3—Re1—N183.15 (5)N2—C9—C8120.08 (13)
O4—Re1—N174.33 (4)C11—N3—Re1174.40 (12)
C9—N2—C10121.62 (13)C6—C7—C8118.77 (14)
C9—N2—H2120.5 (15)C6—C7—H7120.6
C10—N2—H2117.6 (15)C8—C7—H7120.6
O2—C2—Re1177.17 (14)N2—C10—H10A109.5
C9—O4—Re1117.61 (9)N2—C10—H10B109.5
C4—N1—C8118.59 (13)H10A—C10—H10B109.5
C4—N1—Re1125.03 (10)N2—C10—H10C109.5
C8—N1—Re1116.34 (10)H10A—C10—H10C109.5
O3—C3—Re1178.12 (13)H10B—C10—H10C109.5
O1—C1—Re1178.53 (13)N3—C11—S1179.00 (14)
C4—C5—C6119.15 (15)
C4—C5—C6—C71.2 (2)C10—N2—C9—O41.8 (2)
C4—N1—C8—C71.7 (2)C10—N2—C9—C8179.84 (13)
Re1—N1—C8—C7176.03 (12)N1—C8—C9—O40.19 (19)
C4—N1—C8—C9177.88 (13)C7—C8—C9—O4179.33 (14)
Re1—N1—C8—C94.44 (16)N1—C8—C9—N2178.59 (13)
C8—N1—C4—C51.1 (2)C7—C8—C9—N20.9 (2)
Re1—N1—C4—C5176.40 (12)C5—C6—C7—C80.6 (2)
C6—C5—C4—N10.4 (2)N1—C8—C7—C60.8 (2)
Re1—O4—C9—N2176.79 (11)C9—C8—C7—C6178.65 (14)
Re1—O4—C9—C84.83 (17)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N2—H2···S1i0.84 (2)2.57 (2)3.3642 (14)158.0 (19)
C7—H7···S1i0.952.903.8255 (16)166
C10—H10C···S1ii0.982.983.8445 (17)148
Symmetry codes: (i) x+1/2, y+3/2, z1/2; (ii) x+1, y, z.
Comparison of selected bond lengths, distances (Å) and angles (°) between the experiments and calculations from three different basis sets for the studied complex(a) top
Triclinic(b)Monoclinic6-31G(d,p)6-31G++(d,p)6-311G++(d,p)
Re1—C11.915 (4)1.9180 (16)1.93281.93061.9329
Re1—C21.901 (4)1.9028 (16)1.90521.90161.9033
Re1—C31.923 (4)1.9201 (16)1.93421.92971.9330
Re1—N12.190 (3)2.1836 (13)2.22722.20792.2049
Re1—O42.159 (2)2.1583 (10)2.24122.22572.2169
Re1—N32.117 (3)2.1275 (13)2.12682.10762.0982
C9—O41.261 (4)1.2581 (17)1.25241.27981.2773
C9—N21.309 (5)1.3182 (18)1.33841.33881.3388
C10—N21.461 (5)1.4610 (19)1.46301.47081.4698
N1···O42.620 (4)2.623 (2)2.66162.64962.6401
N1—Re1—O474.09 (10)74.33 (4)73.1273.4073.32
N1—Re1—N383.91 (12)83.15 (5)81.1681.4081.12
O4—Re1—N381.68 (11)82.40 (5)79.0678.8479.73
C11—N3—Re1167.0 (1)174.4 (1)157.29161.39167.84
N1—Re1—C1170.93 (13)172.55 (6)169.97169.90169.65
O4—Re1—C2168.57 (12)171.84 (6)170.77170.63170.91
N3—Re1—C3174.90 (12)177.96 (6)171.84171.84172.19
Notes: (a)DFT Calculations were carried out by means of GAUSSIAN09 software (Frisch et al., 2009) using the B3LYP functional and the LANL2DZ basis set for the Re atom; (b)data from Lyczko et al. (2015).
 

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