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In the title compound, C21H22N4, all three substituents are found in equatorial positions. Intermolecular C—H...N and C—H...π interactions seem to be responsible for the packing.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536803013394/na6244sup1.cif
Contains datablocks global, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536803013394/na6244Isup2.hkl
Contains datablock I

CCDC reference: 217603

Key indicators

  • Single-crystal X-ray study
  • T = 120 K
  • Mean [sigma](C-C) = 0.003 Å
  • R factor = 0.049
  • wR factor = 0.111
  • Data-to-parameter ratio = 17.7

checkCIF results

No syntax errors found

ADDSYM reports no extra symmetry








Comment top

Subsequent to the publication of some coordination compounds with the ligand N-benzyl-N'-carboxymethyl-N,N'-bis(2-pyridylmethyl)-1,2-ethanediamine (Baffert et al., 2003) we have succeeded in crystallizing the ligand precursor 2-phenyl-1,3-bis(2-pyridylmethyl)imidazolidine, (I).

Fig. 1 shows the molecular structure of (I) with atom-numbering scheme. The five-membered ring is in the envelope conformation with the apex on C3 [ϕ2 = 5.6 (2)°, total ring puckering amplitude Q2 = 0.3974 (16) Å (Cremer & Pople, 1975)]. This has a pseudo-mirror that includes the phenyl ring through C3 and orthogonal to the C1—C2 bond. All three substituents are in equatorial positions and the pyridine rings are oriented in a syn fashion i.e. the two N atoms are both pointing in the same direction as the axial hydrogen on C2. The exact orientations of the central ring and substituents is summarized in table 1 by the dihedral angles formed by least-squares planes through the individual rings.

Extensive C—H···π interactions (closest contact 2.79 Å) exist between the aromatic rings. Short contacts include N1···H36i 3.48 Å, N2···H36i 3.07 Å, N11···H34ii 2.90 Å and N21···H2Biii 2.76 Å [symmetry codes: (i) x + 1, y, z; (ii) x − 1/2, y − 1/2, 1/2 − z; (iii) −x, −y, −z]. The former two result in stacking along the a axis of the unit cell.

Experimental top

2-Phenyl-1,3-bis(2-pyridylmethyl)imidazolidine was prepared according to a literature method (Baffert et al., 2003). Colourless block-shaped single crystals suitable were grown by slow evaporation of a dichloromethane solution.

Computing details top

Data collection: SMART (Bruker, 1998); cell refinement: SAINT (Bruker, 2000); data reduction: SAINT; program(s) used to solve structure: SIR97 (Altomare, 1999); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: X-SEED (Barbour, 2001); software used to prepare material for publication: WinGX (Farrugia, 1999).

Figures top
[Figure 1] Fig. 1. View of (I) (50% probability displacement ellipsoids)
(I) top
Crystal data top
C21H22N4F(000) = 704
Mr = 330.43Dx = 1.253 Mg m3
Monoclinic, P21/nMelting point = 415–419 K
Hall symbol: -P 2ynMo Kα radiation, λ = 0.71069 Å
a = 6.003 (5) ÅCell parameters from 22931 reflections
b = 15.175 (5) Åθ = 2.7–26.2°
c = 19.237 (5) ŵ = 0.08 mm1
β = 91.794 (5)°T = 120 K
V = 1751.5 (16) Å3Block, colourless
Z = 40.45 × 0.25 × 0.1 mm
Data collection top
Bruker SMART CCD
diffractometer
2464 reflections with I > 2σ(I)
ω rotation scansRint = 0.083
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
θmax = 27.5°, θmin = 1.7°
Tmin = 0.883, Tmax = 0.992h = 77
20244 measured reflectionsk = 1919
4019 independent reflectionsl = 2424
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)] = 0.049H-atom parameters constrained
wR(F2) = 0.111 w = 1/[σ2(Fo2) + (0.0464P)2 + 0.1083P]
where P = (Fo2 + 2Fc2)/3
S = 1.02(Δ/σ)max < 0.001
4019 reflectionsΔρmax = 0.24 e Å3
227 parametersΔρmin = 0.2 e Å3
0 restraintsExtinction correction: SHELXL97, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.0053 (8)
Crystal data top
C21H22N4V = 1751.5 (16) Å3
Mr = 330.43Z = 4
Monoclinic, P21/nMo Kα radiation
a = 6.003 (5) ŵ = 0.08 mm1
b = 15.175 (5) ÅT = 120 K
c = 19.237 (5) Å0.45 × 0.25 × 0.1 mm
β = 91.794 (5)°
Data collection top
Bruker SMART CCD
diffractometer
4019 independent reflections
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
2464 reflections with I > 2σ(I)
Tmin = 0.883, Tmax = 0.992Rint = 0.083
20244 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0490 restraints
wR(F2) = 0.111H-atom parameters constrained
S = 1.02Δρmax = 0.24 e Å3
4019 reflectionsΔρmin = 0.2 e Å3
227 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.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
C10.2844 (3)0.04647 (11)0.18605 (8)0.0260 (4)
H1A0.19930.00680.19860.031*
H1B0.43460.04340.20870.031*
C20.3002 (3)0.05436 (11)0.10745 (8)0.0236 (4)
H2A0.45750.05940.09390.028*
H2B0.2320.00260.08380.028*
C30.0262 (3)0.15051 (10)0.14702 (8)0.0180 (4)
H30.10540.11020.1430.022*
C110.0466 (3)0.11771 (11)0.27076 (8)0.0216 (4)
H11A0.03820.06170.26920.026*
H11B0.0620.16650.27360.026*
C120.1960 (3)0.11853 (10)0.33514 (8)0.0189 (4)
C130.4076 (3)0.15388 (11)0.33586 (9)0.0231 (4)
H130.46660.17750.29460.028*
C140.5330 (3)0.15462 (11)0.39737 (9)0.0285 (4)
H140.67960.17830.39890.034*
C150.4416 (3)0.12039 (12)0.45635 (9)0.0306 (5)
H150.5230.12040.49950.037*
C160.2294 (3)0.08624 (12)0.45123 (9)0.0308 (5)
H160.1670.06260.4920.037*
C210.0582 (3)0.13274 (11)0.02272 (8)0.0221 (4)
H21A0.04970.18210.020.026*
H21B0.02730.07710.01910.026*
C220.2104 (3)0.13883 (10)0.03784 (8)0.0196 (4)
C230.4226 (3)0.17400 (11)0.03124 (9)0.0236 (4)
H230.48070.19260.01290.028*
C240.5488 (3)0.18162 (11)0.08975 (9)0.0280 (4)
H240.69540.20510.08640.034*
C250.4592 (3)0.15483 (11)0.15283 (9)0.0285 (4)
H250.54110.160.19410.034*
C260.2481 (3)0.12041 (12)0.15444 (9)0.0325 (5)
H260.1870.10170.19810.039*
C310.0492 (3)0.24523 (11)0.14910 (8)0.0182 (4)
C320.1092 (3)0.31028 (11)0.16163 (8)0.0229 (4)
H320.25950.29410.17190.027*
C330.0513 (3)0.39829 (11)0.15932 (9)0.0262 (4)
H330.16110.44230.1680.031*
C340.1676 (3)0.42206 (11)0.14433 (8)0.0276 (4)
H340.20780.48260.14180.033*
C350.3260 (3)0.35831 (11)0.13308 (9)0.0284 (4)
H350.47630.37480.12320.034*
C360.2681 (3)0.26934 (11)0.13606 (8)0.0237 (4)
H360.37940.22540.12910.028*
N10.1676 (2)0.12666 (8)0.20699 (7)0.0189 (3)
N20.1755 (2)0.13554 (8)0.08983 (7)0.0191 (3)
N110.1054 (2)0.08435 (9)0.39190 (7)0.0245 (4)
N210.1221 (3)0.11135 (9)0.09878 (7)0.0277 (4)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.0327 (11)0.0233 (9)0.0219 (9)0.0075 (8)0.0014 (8)0.0004 (8)
C20.0272 (10)0.0214 (9)0.0224 (9)0.0035 (8)0.0029 (8)0.0005 (7)
C30.0197 (9)0.0185 (9)0.0156 (8)0.0028 (7)0.0003 (7)0.0005 (7)
C110.0222 (10)0.0225 (9)0.0200 (9)0.0033 (8)0.0016 (7)0.0001 (7)
C120.0223 (9)0.0160 (8)0.0185 (9)0.0019 (7)0.0022 (7)0.0014 (7)
C130.0263 (10)0.0217 (9)0.0215 (9)0.0014 (8)0.0018 (8)0.0011 (7)
C140.0275 (11)0.0262 (10)0.0316 (11)0.0035 (8)0.0026 (9)0.0079 (8)
C150.0362 (12)0.0333 (11)0.0216 (10)0.0052 (9)0.0071 (9)0.0028 (8)
C160.0425 (12)0.0320 (10)0.0179 (9)0.0015 (9)0.0002 (8)0.0025 (8)
C210.0235 (10)0.0241 (9)0.0185 (9)0.0012 (8)0.0016 (7)0.0010 (7)
C220.0249 (10)0.0158 (9)0.0181 (9)0.0022 (7)0.0000 (7)0.0008 (7)
C230.0256 (10)0.0265 (10)0.0186 (9)0.0008 (8)0.0018 (8)0.0016 (7)
C240.0257 (10)0.0281 (10)0.0302 (10)0.0006 (8)0.0022 (8)0.0090 (8)
C250.0362 (12)0.0264 (10)0.0235 (10)0.0030 (9)0.0099 (9)0.0038 (8)
C260.0450 (13)0.0335 (11)0.0192 (10)0.0034 (10)0.0038 (9)0.0044 (8)
C310.0227 (10)0.0215 (9)0.0106 (8)0.0016 (7)0.0027 (7)0.0010 (7)
C320.0255 (10)0.0234 (9)0.0199 (9)0.0007 (8)0.0015 (7)0.0001 (7)
C330.0342 (11)0.0209 (9)0.0237 (10)0.0058 (8)0.0046 (8)0.0028 (7)
C340.0375 (12)0.0208 (9)0.0253 (10)0.0061 (9)0.0130 (9)0.0014 (8)
C350.0248 (10)0.0305 (11)0.0304 (10)0.0070 (9)0.0085 (8)0.0076 (8)
C360.0227 (10)0.0230 (9)0.0255 (10)0.0029 (8)0.0025 (8)0.0030 (8)
N10.0223 (8)0.0187 (7)0.0157 (7)0.0023 (6)0.0011 (6)0.0005 (6)
N20.0221 (8)0.0194 (7)0.0157 (7)0.0025 (6)0.0004 (6)0.0002 (6)
N110.0306 (9)0.0249 (8)0.0182 (8)0.0011 (7)0.0013 (7)0.0003 (6)
N210.0340 (9)0.0296 (8)0.0196 (8)0.0043 (7)0.0018 (7)0.0044 (6)
Geometric parameters (Å, º) top
C1—N11.467 (2)C21—N21.452 (2)
C1—C21.523 (2)C21—C221.506 (2)
C1—H1A0.99C21—H21A0.99
C1—H1B0.99C21—H21B0.99
C2—N21.476 (2)C22—N211.338 (2)
C2—H2A0.99C22—C231.383 (3)
C2—H2B0.99C23—C241.381 (2)
C3—N11.456 (2)C23—H230.95
C3—N21.459 (2)C24—C251.373 (2)
C3—C311.508 (2)C24—H240.95
C3—H31C25—C261.370 (3)
C11—N11.451 (2)C25—H250.95
C11—C121.506 (2)C26—N211.337 (2)
C11—H11A0.99C26—H260.95
C11—H11B0.99C31—C361.380 (3)
C12—N111.340 (2)C31—C321.387 (2)
C12—C131.379 (3)C32—C331.380 (2)
C13—C141.382 (2)C32—H320.95
C13—H130.95C33—C341.384 (3)
C14—C151.377 (3)C33—H330.95
C14—H140.95C34—C351.369 (2)
C15—C161.376 (3)C34—H340.95
C15—H150.95C35—C361.395 (2)
C16—N111.343 (2)C35—H350.95
C16—H160.95C36—H360.95
N1—C1—C2104.64 (13)C22—C21—H21B108.9
N1—C1—H1A110.8H21A—C21—H21B107.7
C2—C1—H1A110.8N21—C22—C23122.62 (15)
N1—C1—H1B110.8N21—C22—C21115.19 (15)
C2—C1—H1B110.8C23—C22—C21122.14 (15)
H1A—C1—H1B108.9C24—C23—C22118.97 (16)
N2—C2—C1104.28 (13)C24—C23—H23120.5
N2—C2—H2A110.9C22—C23—H23120.5
C1—C2—H2A110.9C25—C24—C23119.08 (17)
N2—C2—H2B110.9C25—C24—H24120.5
C1—C2—H2B110.9C23—C24—H24120.5
H2A—C2—H2B108.9C26—C25—C24117.97 (17)
N1—C3—N2101.65 (13)C26—C25—H25121
N1—C3—C31112.57 (13)C24—C25—H25121
N2—C3—C31111.13 (12)N21—C26—C25124.54 (17)
N1—C3—H3110.4N21—C26—H26117.7
N2—C3—H3110.4C25—C26—H26117.7
C31—C3—H3110.4C36—C31—C32119.16 (16)
N1—C11—C12113.17 (14)C36—C31—C3122.21 (15)
N1—C11—H11A108.9C32—C31—C3118.57 (15)
C12—C11—H11A108.9C33—C32—C31120.81 (17)
N1—C11—H11B108.9C33—C32—H32119.6
C12—C11—H11B108.9C31—C32—H32119.6
H11A—C11—H11B107.8C32—C33—C34119.70 (16)
N11—C12—C13122.69 (16)C32—C33—H33120.2
N11—C12—C11114.87 (15)C34—C33—H33120.2
C13—C12—C11122.43 (15)C35—C34—C33119.93 (17)
C12—C13—C14119.26 (17)C35—C34—H34120
C12—C13—H13120.4C33—C34—H34120
C14—C13—H13120.4C34—C35—C36120.44 (17)
C15—C14—C13118.78 (18)C34—C35—H35119.8
C15—C14—H14120.6C36—C35—H35119.8
C13—C14—H14120.6C31—C36—C35119.92 (16)
C16—C15—C14118.37 (17)C31—C36—H36120
C16—C15—H15120.8C35—C36—H36120
C14—C15—H15120.8C11—N1—C3113.45 (13)
N11—C16—C15123.79 (17)C11—N1—C1114.23 (13)
N11—C16—H16118.1C3—N1—C1105.09 (12)
C15—C16—H16118.1C21—N2—C3112.52 (13)
N2—C21—C22113.40 (14)C21—N2—C2114.10 (13)
N2—C21—H21A108.9C3—N2—C2106.04 (12)
C22—C21—H21A108.9C12—N11—C16117.11 (15)
N2—C21—H21B108.9C26—N21—C22116.82 (16)
N1—C1—C2—N24.15 (18)C3—C31—C36—C35174.81 (15)
N1—C11—C12—N11160.54 (13)C34—C35—C36—C311.3 (3)
N1—C11—C12—C1321.1 (2)C12—C11—N1—C3163.80 (13)
N11—C12—C13—C140.1 (2)C12—C11—N1—C175.77 (17)
C11—C12—C13—C14178.16 (15)N2—C3—N1—C11167.80 (12)
C12—C13—C14—C150.4 (2)C31—C3—N1—C1173.23 (16)
C13—C14—C15—C160.5 (3)N2—C3—N1—C142.33 (15)
C14—C15—C16—N110.1 (3)C31—C3—N1—C1161.30 (13)
N2—C21—C22—N21161.40 (14)C2—C1—N1—C11153.77 (14)
N2—C21—C22—C2321.3 (2)C2—C1—N1—C328.79 (17)
N21—C22—C23—C240.3 (2)C22—C21—N2—C3166.43 (13)
C21—C22—C23—C24176.72 (15)C22—C21—N2—C272.70 (17)
C22—C23—C24—C250.6 (2)N1—C3—N2—C21165.09 (12)
C23—C24—C25—C260.9 (3)C31—C3—N2—C2174.92 (16)
C24—C25—C26—N210.3 (3)N1—C3—N2—C239.70 (15)
N1—C3—C31—C36133.08 (16)C31—C3—N2—C2159.69 (13)
N2—C3—C31—C36113.65 (17)C1—C2—N2—C21146.35 (14)
N1—C3—C31—C3249.73 (19)C1—C2—N2—C321.94 (17)
N2—C3—C31—C3263.54 (18)C13—C12—N11—C160.5 (2)
C36—C31—C32—C331.8 (2)C11—C12—N11—C16177.85 (14)
C3—C31—C32—C33175.52 (14)C15—C16—N11—C120.5 (3)
C31—C32—C33—C340.0 (2)C25—C26—N21—C220.6 (3)
C32—C33—C34—C351.1 (2)C23—C22—N21—C260.9 (2)
C33—C34—C35—C360.5 (3)C21—C22—N21—C26176.36 (15)
C32—C31—C36—C352.4 (2)

Experimental details

Crystal data
Chemical formulaC21H22N4
Mr330.43
Crystal system, space groupMonoclinic, P21/n
Temperature (K)120
a, b, c (Å)6.003 (5), 15.175 (5), 19.237 (5)
β (°) 91.794 (5)
V3)1751.5 (16)
Z4
Radiation typeMo Kα
µ (mm1)0.08
Crystal size (mm)0.45 × 0.25 × 0.1
Data collection
DiffractometerBruker SMART CCD
diffractometer
Absorption correctionMulti-scan
(SADABS; Sheldrick, 1996)
Tmin, Tmax0.883, 0.992
No. of measured, independent and
observed [I > 2σ(I)] reflections
20244, 4019, 2464
Rint0.083
(sin θ/λ)max1)0.649
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.049, 0.111, 1.02
No. of reflections4019
No. of parameters227
H-atom treatmentH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.24, 0.2

Computer programs: SMART (Bruker, 1998), SAINT (Bruker, 2000), SAINT, SIR97 (Altomare, 1999), SHELXL97 (Sheldrick, 1997), X-SEED (Barbour, 2001), WinGX (Farrugia, 1999).

Selected geometric parameters (Å, º) top
C1—N11.467 (2)C2—N21.476 (2)
C1—C21.523 (2)C3—N11.456 (2)
N1—C1—C2104.64 (13)C3—N1—C1105.09 (12)
N2—C2—C1104.28 (13)C3—N2—C2106.04 (12)
N1—C3—N2101.65 (13)
Dihedral angles formed by least-squares planes (°) top
IIIIIIV
I21.97 (8)73.97 (8)70.71 (9)
II84.34 (8)71.65 (9)
III85.44 (9)
Least-squares planes: I N11/C12–C16, II N21/C22–C26, III C31–C36 and IV N1/C1/C2/N2/C3
 

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