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In the title compound, C19H34N6O2, both morpholine rings adopt chair conformations. In the crystal structure, N—H...N hydrogen bonds link the mol­ecules into chains along c.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536807043462/sj2350sup1.cif
Contains datablocks I, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536807043462/sj2350Isup2.hkl
Contains datablock I

CCDC reference: 664198

Key indicators

  • Single-crystal X-ray study
  • T = 113 K
  • Mean [sigma](C-C) = 0.002 Å
  • R factor = 0.039
  • wR factor = 0.103
  • Data-to-parameter ratio = 14.4

checkCIF/PLATON results

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Alert level G PLAT860_ALERT_3_G Note: Number of Least-Squares Restraints ....... 1
0 ALERT level A = In general: serious problem 0 ALERT level B = Potentially serious problem 0 ALERT level C = Check and explain 1 ALERT level G = General alerts; check 0 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 0 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 0 ALERT type 4 Improvement, methodology, query or suggestion 0 ALERT type 5 Informative message, check

Comment top

The title compound (I) is an important intermediate in the preparation of hindered light stabilizers(Borzatta & Carrozza, 1991). Compounds containing a triazine ring are widely used in polymers, dyes, drugs and hindered amine light stabilizers (Deng et al., 2006). We report here the crystal structure of the title compound (I) (Fig. 1). In (I) both morpholine rings adopt a chair conformation and the triazine ring is essentially planar with an r.m.s. deviation from the mean plane of 0.0105 Å. In the crystal N6—H6C···N1 hydrogen bonds link the molecules into chains along c, Table 1.

Related literature top

For the preparation and uses of the title compound and similar compounds, see: Borzatta & Carrozza (1991); Deng et al. (2006); Kaiser & Thurston (1951).

Experimental top

The title compound was prepared according to the method of Kaiser & Thurston (1951) in 71% yield. Crystals of (I) were obtained by slow evaporation of a solution in methanol (m.p. 431–433 K).

Refinement top

The amine H atom was located in a Fourier map and was refined freely with an isotropic displacement parameter. All other H atoms were positioned geometrically and refined using a riding model with d(C—H) = 0.97 Å, Uiso = 1.2Ueq (C) for CH2 and 0.96 Å, Uiso = 1.5Ueq (C) for CH3 atoms.

Structure description top

The title compound (I) is an important intermediate in the preparation of hindered light stabilizers(Borzatta & Carrozza, 1991). Compounds containing a triazine ring are widely used in polymers, dyes, drugs and hindered amine light stabilizers (Deng et al., 2006). We report here the crystal structure of the title compound (I) (Fig. 1). In (I) both morpholine rings adopt a chair conformation and the triazine ring is essentially planar with an r.m.s. deviation from the mean plane of 0.0105 Å. In the crystal N6—H6C···N1 hydrogen bonds link the molecules into chains along c, Table 1.

For the preparation and uses of the title compound and similar compounds, see: Borzatta & Carrozza (1991); Deng et al. (2006); Kaiser & Thurston (1951).

Computing details top

Data collection: CrystalClear (Rigaku/MSC, 2005); cell refinement: CrystalClear (Rigaku/MSC, 2005); data reduction: CrystalClear (Rigaku/MSC, 2005); program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: SHELXTL (Bruker, 1997); software used to prepare material for publication: SHELXTL (Bruker, 1997).

Figures top
[Figure 1] Fig. 1. A view of the molecular structure of (I). Displacement ellipsoids are drawn at the 30% probability level and H atoms are shown as small spheres of arbitrary radii.
4,6-Dimorpholino-N-(2,4,4-trimethylpentan-2-yl)-1,3,5-triazin-2-amine top
Crystal data top
C19H34N6O2F(000) = 824
Mr = 378.52Dx = 1.217 Mg m3
Monoclinic, P21/cMelting point: 431-433 K K
Hall symbol: -P 2ybcMo Kα radiation, λ = 0.71073 Å
a = 10.247 (2) ÅCell parameters from 5929 reflections
b = 16.718 (3) Åθ = 2.1–27.9°
c = 12.107 (2) ŵ = 0.08 mm1
β = 94.82 (3)°T = 113 K
V = 2066.6 (7) Å3Block, colorless
Z = 40.08 × 0.08 × 0.02 mm
Data collection top
Rigaku Saturn CCD
diffractometer
3641 independent reflections
Radiation source: rotating anode3159 reflections with I > 2σ(I)
Confocal monochromatorRint = 0.034
ω scansθmax = 25.0°, θmin = 2.1°
Absorption correction: multi-scan
(CrystalClear; Rigaku/MSC, 2005)
h = 1212
Tmin = 0.984, Tmax = 0.998k = 1819
20763 measured reflectionsl = 1414
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.039Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.103H atoms treated by a mixture of independent and constrained refinement
S = 1.09 w = 1/[σ2(Fo2) + (0.0648P)2 + 0.0832P]
where P = (Fo2 + 2Fc2)/3
3641 reflections(Δ/σ)max < 0.001
253 parametersΔρmax = 0.20 e Å3
1 restraintΔρmin = 0.27 e Å3
Crystal data top
C19H34N6O2V = 2066.6 (7) Å3
Mr = 378.52Z = 4
Monoclinic, P21/cMo Kα radiation
a = 10.247 (2) ŵ = 0.08 mm1
b = 16.718 (3) ÅT = 113 K
c = 12.107 (2) Å0.08 × 0.08 × 0.02 mm
β = 94.82 (3)°
Data collection top
Rigaku Saturn CCD
diffractometer
3641 independent reflections
Absorption correction: multi-scan
(CrystalClear; Rigaku/MSC, 2005)
3159 reflections with I > 2σ(I)
Tmin = 0.984, Tmax = 0.998Rint = 0.034
20763 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0391 restraint
wR(F2) = 0.103H atoms treated by a mixture of independent and constrained refinement
S = 1.09Δρmax = 0.20 e Å3
3641 reflectionsΔρmin = 0.27 e Å3
253 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
O10.82017 (9)0.02524 (5)0.97507 (7)0.0292 (2)
O20.14099 (9)0.33956 (6)0.65039 (9)0.0375 (3)
N10.55524 (10)0.20367 (6)0.72321 (8)0.0181 (2)
N20.70950 (10)0.14783 (6)0.60724 (8)0.0173 (2)
N30.54840 (9)0.24124 (6)0.53212 (8)0.0170 (2)
N40.70730 (10)0.11069 (6)0.79018 (8)0.0203 (2)
N50.40537 (10)0.29537 (6)0.64901 (8)0.0235 (3)
N60.69655 (10)0.18699 (6)0.42305 (8)0.0173 (2)
C10.65477 (11)0.15522 (7)0.70307 (9)0.0166 (3)
C20.65151 (11)0.19201 (7)0.52442 (9)0.0156 (3)
C30.50656 (11)0.24526 (7)0.63360 (9)0.0165 (3)
C40.63464 (13)0.09771 (7)0.88701 (10)0.0218 (3)
H4A0.58070.05020.87620.026*
H4B0.57750.14290.89680.026*
C50.72851 (14)0.08778 (8)0.98842 (10)0.0273 (3)
H5A0.77540.13751.00330.033*
H5B0.67960.07601.05170.033*
C60.89372 (13)0.04203 (8)0.88310 (11)0.0275 (3)
H6A0.95640.00070.87540.033*
H6B0.94230.09130.89710.033*
C70.80720 (12)0.05017 (7)0.77602 (10)0.0227 (3)
H7A0.85960.06570.71650.027*
H7B0.76590.00070.75680.027*
C80.34451 (13)0.30169 (8)0.75292 (11)0.0275 (3)
H8A0.35910.35470.78400.033*
H8B0.38320.26300.80560.033*
C90.19977 (14)0.28629 (9)0.73206 (13)0.0362 (4)
H9A0.18570.23150.70730.043*
H9B0.15840.29300.80060.043*
C100.19844 (13)0.32924 (9)0.54852 (12)0.0308 (3)
H10A0.15700.36540.49360.037*
H10B0.18280.27500.52220.037*
C110.34334 (12)0.34494 (8)0.56048 (10)0.0233 (3)
H11A0.38060.33280.49130.028*
H11B0.35940.40100.57750.028*
C120.81655 (11)0.14606 (7)0.39230 (10)0.0191 (3)
C130.82342 (13)0.16201 (8)0.26896 (10)0.0254 (3)
H13A0.74460.14320.22870.038*
H13B0.89740.13440.24350.038*
H13C0.83250.21840.25690.038*
C140.93531 (12)0.18489 (8)0.45587 (11)0.0267 (3)
H14A0.93500.24130.44110.040*
H14B1.01410.16160.43260.040*
H14C0.93140.17620.53390.040*
C150.81944 (12)0.05571 (7)0.42141 (10)0.0195 (3)
H15A0.90570.03640.40710.023*
H15B0.81420.05210.50090.023*
C160.71964 (12)0.00559 (7)0.36787 (10)0.0236 (3)
C170.71755 (15)0.07566 (8)0.44923 (12)0.0337 (3)
H17A0.66040.11670.41780.051*
H17B0.68640.05740.51740.051*
H17C0.80450.09680.46340.051*
C180.76316 (15)0.03851 (8)0.25880 (11)0.0345 (4)
H18A0.70000.07670.22840.052*
H18B0.84680.06410.27240.052*
H18C0.77000.00460.20720.052*
C190.58034 (13)0.02736 (8)0.34862 (12)0.0323 (3)
H19A0.57800.06860.29330.048*
H19B0.55390.04920.41660.048*
H19C0.52170.01500.32390.048*
H6C0.6524 (12)0.2176 (7)0.3734 (9)0.022 (3)*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O10.0367 (5)0.0304 (5)0.0197 (5)0.0065 (4)0.0024 (4)0.0063 (4)
O20.0223 (5)0.0435 (6)0.0477 (7)0.0075 (4)0.0092 (5)0.0084 (5)
N10.0206 (5)0.0188 (5)0.0151 (5)0.0024 (4)0.0018 (4)0.0003 (4)
N20.0190 (5)0.0187 (5)0.0142 (5)0.0010 (4)0.0009 (4)0.0005 (4)
N30.0170 (5)0.0180 (5)0.0161 (5)0.0004 (4)0.0014 (4)0.0006 (4)
N40.0236 (6)0.0220 (5)0.0152 (5)0.0047 (4)0.0016 (4)0.0023 (4)
N50.0224 (6)0.0300 (6)0.0186 (6)0.0097 (5)0.0054 (4)0.0041 (4)
N60.0194 (5)0.0192 (5)0.0134 (5)0.0038 (4)0.0022 (4)0.0024 (4)
C10.0186 (6)0.0163 (6)0.0148 (6)0.0019 (5)0.0004 (5)0.0009 (5)
C20.0160 (6)0.0149 (6)0.0157 (6)0.0029 (5)0.0004 (5)0.0005 (5)
C30.0161 (6)0.0170 (6)0.0165 (6)0.0018 (5)0.0013 (5)0.0008 (5)
C40.0286 (7)0.0219 (7)0.0152 (6)0.0022 (5)0.0041 (5)0.0010 (5)
C50.0391 (8)0.0251 (7)0.0171 (7)0.0033 (6)0.0005 (6)0.0001 (5)
C60.0266 (7)0.0298 (7)0.0253 (7)0.0025 (6)0.0018 (6)0.0052 (6)
C70.0244 (7)0.0234 (7)0.0203 (7)0.0051 (5)0.0010 (5)0.0010 (5)
C80.0304 (7)0.0301 (7)0.0235 (7)0.0097 (6)0.0103 (6)0.0011 (6)
C90.0323 (8)0.0360 (8)0.0425 (9)0.0045 (6)0.0165 (7)0.0083 (7)
C100.0254 (7)0.0312 (8)0.0348 (8)0.0023 (6)0.0029 (6)0.0010 (6)
C110.0239 (7)0.0227 (7)0.0234 (7)0.0063 (5)0.0021 (5)0.0031 (5)
C120.0177 (6)0.0215 (6)0.0185 (6)0.0022 (5)0.0042 (5)0.0006 (5)
C130.0288 (7)0.0270 (7)0.0216 (7)0.0064 (6)0.0092 (6)0.0039 (5)
C140.0219 (7)0.0275 (7)0.0310 (8)0.0024 (5)0.0045 (6)0.0004 (6)
C150.0191 (6)0.0221 (7)0.0174 (6)0.0055 (5)0.0019 (5)0.0013 (5)
C160.0254 (7)0.0208 (7)0.0244 (7)0.0017 (5)0.0007 (5)0.0013 (5)
C170.0368 (8)0.0246 (7)0.0401 (9)0.0019 (6)0.0057 (7)0.0036 (6)
C180.0476 (9)0.0275 (8)0.0275 (8)0.0046 (7)0.0013 (7)0.0063 (6)
C190.0253 (7)0.0275 (8)0.0428 (9)0.0029 (6)0.0048 (6)0.0058 (6)
Geometric parameters (Å, º) top
O1—C51.4237 (16)C9—H9A0.9700
O1—C61.4239 (16)C9—H9B0.9700
O2—C101.4211 (17)C10—C111.5027 (18)
O2—C91.4259 (17)C10—H10A0.9700
N1—C11.3407 (15)C10—H10B0.9700
N1—C31.3484 (15)C11—H11A0.9700
N2—C11.3360 (15)C11—H11B0.9700
N2—C21.3430 (15)C12—C131.5243 (17)
N3—C31.3366 (15)C12—C141.5287 (18)
N3—C21.3487 (15)C12—C151.5508 (17)
N4—C11.3641 (15)C13—H13A0.9600
N4—C41.4569 (15)C13—H13B0.9600
N4—C71.4596 (16)C13—H13C0.9600
N5—C31.3580 (16)C14—H14A0.9600
N5—C81.4541 (16)C14—H14B0.9600
N5—C111.4577 (16)C14—H14C0.9600
N6—C21.3496 (15)C15—C161.5507 (18)
N6—C121.4818 (15)C15—H15A0.9700
N6—H6C0.885 (8)C15—H15B0.9700
C4—C51.5039 (18)C16—C191.5295 (18)
C4—H4A0.9700C16—C181.5311 (18)
C4—H4B0.9700C16—C171.5318 (18)
C5—H5A0.9700C17—H17A0.9600
C5—H5B0.9700C17—H17B0.9600
C6—C71.5138 (18)C17—H17C0.9600
C6—H6A0.9700C18—H18A0.9600
C6—H6B0.9700C18—H18B0.9600
C7—H7A0.9700C18—H18C0.9600
C7—H7B0.9700C19—H19A0.9600
C8—C91.506 (2)C19—H19B0.9600
C8—H8A0.9700C19—H19C0.9600
C8—H8B0.9700
C5—O1—C6109.97 (9)O2—C10—H10A109.2
C10—O2—C9110.15 (10)C11—C10—H10A109.2
C1—N1—C3113.63 (10)O2—C10—H10B109.2
C1—N2—C2113.95 (10)C11—C10—H10B109.2
C3—N3—C2114.07 (10)H10A—C10—H10B107.9
C1—N4—C4120.55 (10)N5—C11—C10109.74 (11)
C1—N4—C7121.50 (10)N5—C11—H11A109.7
C4—N4—C7113.71 (10)C10—C11—H11A109.7
C3—N5—C8123.48 (10)N5—C11—H11B109.7
C3—N5—C11122.71 (10)C10—C11—H11B109.7
C8—N5—C11113.74 (10)H11A—C11—H11B108.2
C2—N6—C12127.71 (10)N6—C12—C13105.85 (10)
C2—N6—H6C112.8 (8)N6—C12—C14108.64 (10)
C12—N6—H6C119.0 (8)C13—C12—C14108.58 (10)
N2—C1—N1126.51 (11)N6—C12—C15113.14 (9)
N2—C1—N4116.99 (10)C13—C12—C15113.04 (10)
N1—C1—N4116.47 (10)C14—C12—C15107.45 (10)
N2—C2—N3125.73 (10)C12—C13—H13A109.5
N2—C2—N6118.76 (10)C12—C13—H13B109.5
N3—C2—N6115.50 (10)H13A—C13—H13B109.5
N3—C3—N1126.02 (11)C12—C13—H13C109.5
N3—C3—N5117.71 (11)H13A—C13—H13C109.5
N1—C3—N5116.27 (10)H13B—C13—H13C109.5
N4—C4—C5109.77 (11)C12—C14—H14A109.5
N4—C4—H4A109.7C12—C14—H14B109.5
C5—C4—H4A109.7H14A—C14—H14B109.5
N4—C4—H4B109.7C12—C14—H14C109.5
C5—C4—H4B109.7H14A—C14—H14C109.5
H4A—C4—H4B108.2H14B—C14—H14C109.5
O1—C5—C4111.79 (10)C16—C15—C12123.32 (10)
O1—C5—H5A109.3C16—C15—H15A106.5
C4—C5—H5A109.3C12—C15—H15A106.5
O1—C5—H5B109.3C16—C15—H15B106.5
C4—C5—H5B109.3C12—C15—H15B106.5
H5A—C5—H5B107.9H15A—C15—H15B106.5
O1—C6—C7112.15 (11)C19—C16—C18109.50 (11)
O1—C6—H6A109.2C19—C16—C17108.06 (11)
C7—C6—H6A109.2C18—C16—C17107.49 (11)
O1—C6—H6B109.2C19—C16—C15113.57 (10)
C7—C6—H6B109.2C18—C16—C15111.62 (11)
H6A—C6—H6B107.9C17—C16—C15106.32 (11)
N4—C7—C6109.13 (10)C16—C17—H17A109.5
N4—C7—H7A109.9C16—C17—H17B109.5
C6—C7—H7A109.9H17A—C17—H17B109.5
N4—C7—H7B109.9C16—C17—H17C109.5
C6—C7—H7B109.9H17A—C17—H17C109.5
H7A—C7—H7B108.3H17B—C17—H17C109.5
N5—C8—C9109.31 (12)C16—C18—H18A109.5
N5—C8—H8A109.8C16—C18—H18B109.5
C9—C8—H8A109.8H18A—C18—H18B109.5
N5—C8—H8B109.8C16—C18—H18C109.5
C9—C8—H8B109.8H18A—C18—H18C109.5
H8A—C8—H8B108.3H18B—C18—H18C109.5
O2—C9—C8111.24 (11)C16—C19—H19A109.5
O2—C9—H9A109.4C16—C19—H19B109.5
C8—C9—H9A109.4H19A—C19—H19B109.5
O2—C9—H9B109.4C16—C19—H19C109.5
C8—C9—H9B109.4H19A—C19—H19C109.5
H9A—C9—H9B108.0H19B—C19—H19C109.5
O2—C10—C11111.91 (11)
C2—N2—C1—N13.13 (17)C6—O1—C5—C459.52 (14)
C2—N2—C1—N4178.72 (10)N4—C4—C5—O155.56 (14)
C3—N1—C1—N22.64 (16)C5—O1—C6—C759.49 (14)
C3—N1—C1—N4179.21 (10)C1—N4—C7—C6150.99 (11)
C4—N4—C1—N2163.16 (10)C4—N4—C7—C652.03 (14)
C7—N4—C1—N27.73 (16)O1—C6—C7—N455.05 (14)
C4—N4—C1—N118.50 (16)C3—N5—C8—C9124.15 (13)
C7—N4—C1—N1173.93 (10)C11—N5—C8—C952.85 (15)
C1—N2—C2—N30.82 (16)C10—O2—C9—C860.37 (15)
C1—N2—C2—N6177.92 (10)N5—C8—C9—O256.35 (15)
C3—N3—C2—N21.58 (16)C9—O2—C10—C1159.46 (15)
C3—N3—C2—N6179.64 (10)C3—N5—C11—C10125.17 (13)
C12—N6—C2—N29.04 (17)C8—N5—C11—C1051.86 (15)
C12—N6—C2—N3172.09 (10)O2—C10—C11—N554.40 (14)
C2—N3—C3—N12.16 (16)C2—N6—C12—C13177.64 (11)
C2—N3—C3—N5178.14 (10)C2—N6—C12—C1461.20 (15)
C1—N1—C3—N30.26 (16)C2—N6—C12—C1558.04 (15)
C1—N1—C3—N5179.96 (10)N6—C12—C15—C1663.93 (15)
C8—N5—C3—N3175.78 (11)C13—C12—C15—C1656.37 (15)
C11—N5—C3—N30.96 (17)C14—C12—C15—C16176.15 (11)
C8—N5—C3—N13.95 (17)C12—C15—C16—C1937.84 (16)
C11—N5—C3—N1179.31 (11)C12—C15—C16—C1886.53 (14)
C1—N4—C4—C5150.20 (11)C12—C15—C16—C17156.54 (11)
C7—N4—C4—C552.59 (13)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N6—H6C···N1i0.89 (1)2.39 (1)3.2715 (15)172 (1)
Symmetry code: (i) x, y+1/2, z1/2.

Experimental details

Crystal data
Chemical formulaC19H34N6O2
Mr378.52
Crystal system, space groupMonoclinic, P21/c
Temperature (K)113
a, b, c (Å)10.247 (2), 16.718 (3), 12.107 (2)
β (°) 94.82 (3)
V3)2066.6 (7)
Z4
Radiation typeMo Kα
µ (mm1)0.08
Crystal size (mm)0.08 × 0.08 × 0.02
Data collection
DiffractometerRigaku Saturn CCD
Absorption correctionMulti-scan
(CrystalClear; Rigaku/MSC, 2005)
Tmin, Tmax0.984, 0.998
No. of measured, independent and
observed [I > 2σ(I)] reflections
20763, 3641, 3159
Rint0.034
(sin θ/λ)max1)0.595
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.039, 0.103, 1.09
No. of reflections3641
No. of parameters253
No. of restraints1
H-atom treatmentH atoms treated by a mixture of independent and constrained refinement
Δρmax, Δρmin (e Å3)0.20, 0.27

Computer programs: CrystalClear (Rigaku/MSC, 2005), SHELXS97 (Sheldrick, 1997), SHELXL97 (Sheldrick, 1997), SHELXTL (Bruker, 1997).

Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N6—H6C···N1i0.885 (8)2.392 (9)3.2715 (15)172.4 (11)
Symmetry code: (i) x, y+1/2, z1/2.
 

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