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The second polymorph of the compound 2,4,6-tris­(4-pyridyl)-1,3,5-triazine (TPT) is reported, TPT-II, which crystallizes in space group I2/a. Its higher density and more efficient space filling indicate the lower entropy of TPT-II, while its slightly lower melting point indicates its weaker intermolecular interactions. The conditions of the crystallization experiments for TPT-I and TPT-II are the dominant factors that determine the final crystalline products. The crystals of TPT-II are long needles. They exhibit bending behaviour along the crystallographic b direction when a mechanical force is imposed perpendicular to it, and regain their original shape after the external stress is removed. The elasticity of the single crystals is interpreted in terms of intermolecular interactions and an energy framework analysis.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S2052520619012514/rm5020sup1.cif
Contains datablock I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520619012514/rm5020Isup2.hkl
Contains datablock I

pdf

Portable Document Format (PDF) file https://doi.org/10.1107/S2052520619012514/rm5020sup3.pdf
Additional tables and figures

CCDC reference: 1944221

Computing details top

Data collection: CrysAlis PRO 1.171.39.46e (Rigaku OD, 2018); cell refinement: CrysAlis PRO 1.171.39.46e (Rigaku OD, 2018); data reduction: CrysAlis PRO 1.171.39.46e (Rigaku OD, 2018); program(s) used to solve structure: ShelXT (Sheldrick, 2015); program(s) used to refine structure: SHELXL (Sheldrick, 2015); molecular graphics: Olex2 (Dolomanov et al., 2009); software used to prepare material for publication: Olex2 (Dolomanov et al., 2009).

(I) top
Crystal data top
0.67(C18H12N6)F(000) = 1296
Mr = 208.22Dx = 1.485 Mg m3
Monoclinic, I2/aMo Kα radiation, λ = 0.71073 Å
a = 21.3047 (16) ÅCell parameters from 2299 reflections
b = 3.7345 (2) Åθ = 2.2–28.1°
c = 35.1825 (19) ŵ = 0.10 mm1
β = 93.364 (6)°T = 100 K
V = 2794.4 (3) Å3Needle, colourless
Z = 120.84 × 0.08 × 0.03 mm
Data collection top
XtaLAB AFC12 (RINC): Kappa single
diffractometer
3387 independent reflections
Radiation source: Rotating-anode X-ray tube (dual wavelength), Rigaku (Mo) X-ray DW Source2267 reflections with I > 2σ(I)
Mirror monochromatorRint = 0.077
ω scansθmax = 29.3°, θmin = 2.2°
Absorption correction: analytical
CrysAlisPro 1.171.39.46e (Rigaku Oxford Diffraction, 2018) Analytical numeric absorption correction using a multifaceted crystal model based on expressions derived by R.C. Clark & J.S. Reid. (Clark, R. C. & Reid, J. S. (1995). Acta Cryst. A51, 887-897) Empirical absorption correction using spherical harmonics, implemented in SCALE3 ABSPACK scaling algorithm.
h = 2827
Tmin = 0.995, Tmax = 0.999k = 45
15782 measured reflectionsl = 4447
Refinement top
Refinement on F20 restraints
Least-squares matrix: fullHydrogen site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.061All H-atom parameters refined
wR(F2) = 0.161 w = 1/[σ2(Fo2) + (0.064P)2 + 4.3398P]
where P = (Fo2 + 2Fc2)/3
S = 1.04(Δ/σ)max < 0.001
3387 reflectionsΔρmax = 0.36 e Å3
265 parametersΔρmin = 0.31 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
C10.46649 (10)0.4336 (5)0.37519 (5)0.0157 (4)
C20.55623 (10)0.4524 (6)0.34435 (5)0.0161 (4)
C30.55512 (10)0.6574 (5)0.40463 (5)0.0158 (4)
C40.39873 (10)0.3470 (6)0.37539 (5)0.0166 (4)
C50.36736 (10)0.1794 (6)0.34434 (6)0.0178 (5)
H50.3907 (12)0.100 (7)0.3225 (7)0.026 (7)*
C60.30406 (11)0.1097 (6)0.34547 (6)0.0198 (5)
H60.2813 (12)0.002 (7)0.3241 (7)0.023 (6)*
C70.30057 (11)0.3514 (6)0.40471 (6)0.0198 (5)
H70.2755 (11)0.415 (7)0.4245 (7)0.023 (6)*
C80.36359 (10)0.4354 (6)0.40641 (6)0.0180 (5)
H80.3822 (11)0.565 (7)0.4282 (7)0.019 (6)*
C90.59187 (10)0.3819 (5)0.30983 (5)0.0165 (4)
C100.65489 (10)0.4706 (6)0.30943 (6)0.0176 (5)
H100.6778 (12)0.569 (7)0.3314 (8)0.029 (7)*
C110.68562 (11)0.4096 (6)0.27623 (6)0.0195 (5)
H110.7307 (11)0.465 (6)0.2762 (6)0.013 (5)*
C120.59733 (11)0.1828 (6)0.24561 (6)0.0196 (5)
H120.5774 (11)0.058 (7)0.2226 (7)0.023 (6)*
C130.56207 (10)0.2323 (6)0.27722 (6)0.0176 (5)
H130.5182 (12)0.168 (6)0.2761 (6)0.017 (6)*
C140.58985 (10)0.8110 (6)0.43863 (5)0.0166 (4)
C150.56255 (11)0.8173 (6)0.47367 (6)0.0179 (5)
H150.5189 (12)0.727 (7)0.4764 (7)0.019 (6)*
C160.59785 (11)0.9522 (6)0.50500 (6)0.0194 (5)
H160.5821 (12)0.959 (7)0.5310 (8)0.031 (7)*
C170.68175 (11)1.0684 (6)0.46954 (6)0.0204 (5)
H170.7239 (12)1.159 (6)0.4687 (6)0.015 (6)*
C180.65064 (10)0.9411 (6)0.43652 (6)0.0183 (5)
H180.6722 (13)0.937 (7)0.4143 (8)0.033 (7)*
N10.49564 (9)0.3601 (5)0.34331 (5)0.0177 (4)
N20.58829 (9)0.6047 (5)0.37388 (5)0.0178 (4)
N30.49416 (8)0.5796 (5)0.40674 (5)0.0177 (4)
N40.26973 (9)0.1931 (5)0.37504 (5)0.0213 (4)
N50.65767 (9)0.2697 (5)0.24436 (5)0.0201 (4)
N60.65636 (9)1.0758 (5)0.50378 (5)0.0203 (4)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.0245 (11)0.0154 (10)0.0072 (9)0.0005 (8)0.0009 (8)0.0023 (8)
C20.0244 (11)0.0163 (10)0.0076 (9)0.0011 (9)0.0008 (8)0.0003 (8)
C30.0247 (11)0.0164 (10)0.0064 (9)0.0016 (9)0.0010 (8)0.0013 (8)
C40.0238 (11)0.0175 (10)0.0086 (9)0.0013 (8)0.0009 (8)0.0026 (8)
C50.0264 (11)0.0198 (11)0.0072 (9)0.0007 (9)0.0010 (8)0.0006 (8)
C60.0258 (12)0.0222 (11)0.0110 (10)0.0001 (9)0.0017 (8)0.0000 (9)
C70.0242 (11)0.0235 (11)0.0120 (10)0.0007 (9)0.0043 (8)0.0014 (8)
C80.0256 (11)0.0204 (11)0.0078 (9)0.0007 (9)0.0009 (8)0.0011 (8)
C90.0249 (11)0.0174 (10)0.0074 (9)0.0017 (9)0.0018 (8)0.0005 (8)
C100.0237 (11)0.0222 (11)0.0068 (9)0.0001 (9)0.0006 (8)0.0011 (8)
C110.0242 (12)0.0236 (11)0.0108 (10)0.0023 (9)0.0026 (8)0.0004 (9)
C120.0288 (12)0.0220 (11)0.0079 (9)0.0017 (9)0.0001 (8)0.0011 (8)
C130.0219 (11)0.0205 (11)0.0104 (10)0.0009 (9)0.0007 (8)0.0004 (8)
C140.0226 (11)0.0179 (10)0.0090 (9)0.0025 (9)0.0019 (8)0.0003 (8)
C150.0226 (11)0.0201 (11)0.0111 (10)0.0009 (9)0.0011 (8)0.0003 (8)
C160.0271 (12)0.0225 (11)0.0086 (9)0.0024 (9)0.0004 (8)0.0003 (8)
C170.0232 (12)0.0247 (11)0.0130 (10)0.0015 (9)0.0019 (8)0.0012 (9)
C180.0259 (12)0.0194 (11)0.0097 (9)0.0014 (9)0.0023 (8)0.0001 (8)
N10.0247 (10)0.0200 (9)0.0085 (8)0.0002 (8)0.0014 (7)0.0002 (7)
N20.0242 (10)0.0221 (9)0.0072 (8)0.0001 (8)0.0008 (7)0.0009 (7)
N30.0228 (9)0.0216 (9)0.0084 (8)0.0011 (8)0.0001 (7)0.0002 (7)
N40.0238 (10)0.0256 (10)0.0145 (9)0.0016 (8)0.0017 (7)0.0004 (8)
N50.0270 (10)0.0235 (10)0.0101 (8)0.0019 (8)0.0025 (7)0.0011 (7)
N60.0283 (11)0.0237 (10)0.0085 (8)0.0017 (8)0.0013 (7)0.0016 (7)
Geometric parameters (Å, º) top
C1—C41.480 (3)C9—C131.395 (3)
C1—N11.342 (3)C10—H100.96 (3)
C1—N31.342 (3)C10—C111.391 (3)
C2—C91.493 (3)C11—H110.98 (2)
C2—N11.335 (3)C11—N51.344 (3)
C2—N21.336 (3)C12—H121.01 (3)
C3—C141.485 (3)C12—C131.390 (3)
C3—N21.341 (3)C12—N51.329 (3)
C3—N31.337 (3)C13—H130.96 (2)
C4—C51.395 (3)C14—C151.394 (3)
C4—C81.399 (3)C14—C181.389 (3)
C5—H50.98 (3)C15—H151.00 (3)
C5—C61.376 (3)C15—C161.392 (3)
C6—H60.96 (3)C16—H160.99 (3)
C6—N41.343 (3)C16—N61.332 (3)
C7—H70.93 (2)C17—H170.96 (3)
C7—C81.377 (3)C17—C181.387 (3)
C7—N41.338 (3)C17—N61.349 (3)
C8—H80.97 (3)C18—H180.93 (3)
C9—C101.384 (3)
N1—C1—C4117.30 (18)C10—C11—H11118.4 (13)
N3—C1—C4117.79 (17)N5—C11—C10123.8 (2)
N3—C1—N1124.9 (2)N5—C11—H11117.8 (13)
N1—C2—C9117.99 (18)C13—C12—H12118.9 (14)
N1—C2—N2125.51 (18)N5—C12—H12116.7 (14)
N2—C2—C9116.50 (19)N5—C12—C13124.3 (2)
N2—C3—C14116.45 (19)C9—C13—H13121.9 (14)
N3—C3—C14118.61 (17)C12—C13—C9118.0 (2)
N3—C3—N2124.93 (18)C12—C13—H13120.1 (14)
C5—C4—C1121.12 (18)C15—C14—C3120.35 (19)
C5—C4—C8117.6 (2)C18—C14—C3120.94 (18)
C8—C4—C1121.26 (19)C18—C14—C15118.68 (19)
C4—C5—H5120.3 (15)C14—C15—H15121.2 (14)
C6—C5—C4119.2 (2)C16—C15—C14118.2 (2)
C6—C5—H5120.4 (15)C16—C15—H15120.6 (14)
C5—C6—H6120.5 (15)C15—C16—H16122.8 (16)
N4—C6—C5123.9 (2)N6—C16—C15124.26 (19)
N4—C6—H6115.5 (15)N6—C16—H16112.9 (16)
C8—C7—H7120.6 (15)C18—C17—H17119.6 (14)
N4—C7—H7114.7 (15)N6—C17—H17116.5 (14)
N4—C7—C8124.6 (2)N6—C17—C18123.9 (2)
C4—C8—H8121.4 (14)C14—C18—H18123.1 (17)
C7—C8—C4118.52 (19)C17—C18—C14118.44 (19)
C7—C8—H8120.0 (14)C17—C18—H18118.3 (17)
C10—C9—C2120.41 (18)C2—N1—C1114.73 (17)
C10—C9—C13118.86 (19)C2—N2—C3114.83 (19)
C13—C9—C2120.7 (2)C3—N3—C1115.04 (17)
C9—C10—H10122.0 (15)C7—N4—C6116.23 (19)
C9—C10—C11118.30 (19)C12—N5—C11116.70 (18)
C11—C10—H10119.7 (15)C16—N6—C17116.52 (18)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C10—H10···N4i0.96 (3)2.57 (3)3.497 (3)161 (2)
C11—H11···N5ii0.98 (2)2.67 (2)3.522 (3)144.7 (18)
C17—H17···N6iii0.96 (3)2.69 (3)3.521 (3)144.6 (18)
C18—H18···N4i0.93 (3)2.61 (3)3.466 (3)154 (2)
Symmetry codes: (i) x+1/2, y+1, z; (ii) x+3/2, y+1/2, z+1/2; (iii) x+3/2, y, z+1.
 

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