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In the title compound, C14H26ClN5, the triazine ring is almost planar and both pendant alkyl chains are disordered; the site occupancy ratios are 0.5:0.5 for the tert-butyl chain and approximately 0.6:0.4 for the n-propyl chain. The crystal packing is consolidated by N—H...N hydrogen bonds, resulting in infinite chains propagating along [001].

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536807025950/hb2437sup1.cif
Contains datablocks I, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536807025950/hb2437Isup2.hkl
Contains datablock I

CCDC reference: 655594

Key indicators

  • Single-crystal X-ray study
  • T = 294 K
  • Mean [sigma](C-C) = 0.005 Å
  • Disorder in main residue
  • R factor = 0.061
  • wR factor = 0.199
  • Data-to-parameter ratio = 13.5

checkCIF/PLATON results

No syntax errors found



Alert level B PLAT220_ALERT_2_B Large Non-Solvent C Ueq(max)/Ueq(min) ... 3.63 Ratio PLAT241_ALERT_2_B Check High Ueq as Compared to Neighbors for C10'
Alert level C PLAT066_ALERT_1_C Predicted and Reported Transmissions Identical . ? PLAT094_ALERT_2_C Ratio of Maximum / Minimum Residual Density .... 2.76 PLAT222_ALERT_3_C Large Non-Solvent H Ueq(max)/Ueq(min) ... 3.77 Ratio PLAT241_ALERT_2_C Check High Ueq as Compared to Neighbors for C9' PLAT241_ALERT_2_C Check High Ueq as Compared to Neighbors for C11 PLAT241_ALERT_2_C Check High Ueq as Compared to Neighbors for C13' PLAT242_ALERT_2_C Check Low Ueq as Compared to Neighbors for C8 PLAT301_ALERT_3_C Main Residue Disorder ......................... 23.00 Perc. PLAT340_ALERT_3_C Low Bond Precision on C-C Bonds (x 1000) Ang ... 5 PLAT412_ALERT_2_C Short Intra XH3 .. XHn H6A .. H11E .. 1.84 Ang. PLAT720_ALERT_4_C Number of Unusual/Non-Standard Label(s) ........ 3 PLAT779_ALERT_2_C Suspect or Irrelevant (Bond) Angle in CIF ...... 26.00 Deg. C11 -C8 -C11' 1.555 1.555 1.555 PLAT779_ALERT_2_C Suspect or Irrelevant (Bond) Angle in CIF ...... 22.30 Deg. C10' -C8 -C10 1.555 1.555 1.555 PLAT779_ALERT_2_C Suspect or Irrelevant (Bond) Angle in CIF ...... 29.60 Deg. C9 -C8 -C9' 1.555 1.555 1.555
Alert level G PLAT860_ALERT_3_G Note: Number of Least-Squares Restraints ....... 124
0 ALERT level A = In general: serious problem 2 ALERT level B = Potentially serious problem 14 ALERT level C = Check and explain 1 ALERT level G = General alerts; check 1 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 11 ALERT type 2 Indicator that the structure model may be wrong or deficient 4 ALERT type 3 Indicator that the structure quality may be low 1 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 of hindered light stabilizers (Borzatta & Carrozza, 1991). The triazine ring in (I) is essentially planar with an r.m.s. deviation from the mean plane of 0.0173 Å. Both alkyl side chains are disordered. The crystal packing is consolidated by N—H···N hydrogen bonds (Table 1).

Related literature top

For a related structure, see: Deng et al. (2006). For background, see: Kaiser & Thurston (1951); Borzatta & Carrozza, (1991).

Experimental top

The title compound was prepared according to the method of Kaiser & Thurston (1951). 2,4,6-Trichloro-1,3,5-triazine (40.0 g, 0.217 mol) was dissolved in toluene (120 ml) and then cooled to 278 K. With stirring, a solution of 2,4,4-trimethylpentan-2-amine (27.5 g, 0.213 mol) in toluene (50 ml) was then added dropwise to the mixture over a period of 0.5 h. Then a solution of Na2CO3 (23.02 g, 0.217 mol) in water (50 ml) was then added dropwise for 0.5 h. The mixture was stirred at 273–278 K for a further 3 h. Propan-1-amine (12.80 g, 0.217 mol) and solid Na2CO3 (23.02 g, 0.217 mol) were added to the mixture, maintaining the temperature at 338 k for 5 h. The title compound (52.18 g) was obtained in powder form in a yield of 80.2%. Crystals of (I) were obtained by slow evaporation of a solution of methanol.

Refinement top

Both alkyl side chains are disordered over two positions, in a 0.5:0.5 ratio for the tert-butyl containing side chain, and a 0.592 (8):0.408 (8) ratio for the n-propyl chain (occupancy sum for the latter constrained to unity).

The H atoms were positioned geometrically (N—H = 0.86 Å, C—H = 0.96–0.97 Å), and refined as riding with Uiso(H) = 1.2Ueq(carrier) or 1.5eq(methyl C).

Structure description top

The title compound, (I), is an important intermediate of hindered light stabilizers (Borzatta & Carrozza, 1991). The triazine ring in (I) is essentially planar with an r.m.s. deviation from the mean plane of 0.0173 Å. Both alkyl side chains are disordered. The crystal packing is consolidated by N—H···N hydrogen bonds (Table 1).

For a related structure, see: Deng et al. (2006). For background, see: Kaiser & Thurston (1951); Borzatta & Carrozza, (1991).

Computing details top

Data collection: SMART (Bruker, 1997); cell refinement: SAINT (Bruker, 1997); data reduction: SAINT; 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.

Figures top
[Figure 1] Fig. 1. A view of (I) with displacement ellopsoids drawn at the 30% probability level and H atoms are shown as spheres of arbitrary radius.
6-Chloro-N2-propyl-N4-(2,4,4-trimethylpentan-2-yl)-1,3,5-triazine- 2,4-diamine top
Crystal data top
C14H26ClN5F(000) = 1296
Mr = 299.85Dx = 1.147 Mg m3
Monoclinic, C2/cMelting point = 427–429 K
Hall symbol: -C 2ycMo Kα radiation, λ = 0.71073 Å
a = 19.354 (4) ÅCell parameters from 2001 reflections
b = 8.1265 (16) Åθ = 2.7–21.9°
c = 22.312 (4) ŵ = 0.22 mm1
β = 98.211 (4)°T = 294 K
V = 3473.3 (11) Å3Prism, colorless
Z = 80.24 × 0.20 × 0.14 mm
Data collection top
Bruker SMART 1000 CCD
diffractometer
3070 independent reflections
Radiation source: fine-focus sealed tube1927 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.043
ω scansθmax = 25.0°, θmin = 1.8°
Absorption correction: multi-scan
(SADABS; Bruker, 1997)
h = 2222
Tmin = 0.949, Tmax = 0.970k = 99
8715 measured reflectionsl = 2621
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)] = 0.061Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.200H-atom parameters constrained
S = 1.04 w = 1/[σ2(Fo2) + (0.1008P)2 + 4.0532P]
where P = (Fo2 + 2Fc2)/3
3070 reflections(Δ/σ)max = 0.001
227 parametersΔρmax = 0.82 e Å3
124 restraintsΔρmin = 0.30 e Å3
Crystal data top
C14H26ClN5V = 3473.3 (11) Å3
Mr = 299.85Z = 8
Monoclinic, C2/cMo Kα radiation
a = 19.354 (4) ŵ = 0.22 mm1
b = 8.1265 (16) ÅT = 294 K
c = 22.312 (4) Å0.24 × 0.20 × 0.14 mm
β = 98.211 (4)°
Data collection top
Bruker SMART 1000 CCD
diffractometer
3070 independent reflections
Absorption correction: multi-scan
(SADABS; Bruker, 1997)
1927 reflections with I > 2σ(I)
Tmin = 0.949, Tmax = 0.970Rint = 0.043
8715 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.061124 restraints
wR(F2) = 0.200H-atom parameters constrained
S = 1.04Δρmax = 0.82 e Å3
3070 reflectionsΔρmin = 0.30 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.

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*/UeqOcc. (<1)
Cl11.12154 (5)0.54065 (15)0.15428 (4)0.0679 (4)
N11.01263 (14)0.5960 (3)0.07597 (11)0.0428 (7)
N21.01295 (13)0.7029 (3)0.17513 (11)0.0410 (7)
N30.91505 (13)0.7532 (3)0.09899 (11)0.0409 (7)
N40.91928 (15)0.6518 (4)0.00350 (12)0.0561 (9)
H40.94100.59490.02040.067*
N50.91712 (13)0.8346 (4)0.19857 (12)0.0438 (7)
H50.94190.84060.23370.053*
C11.03866 (16)0.6232 (4)0.13245 (15)0.0409 (8)
C20.94741 (16)0.7621 (4)0.15558 (14)0.0366 (8)
C30.94923 (17)0.6693 (4)0.06058 (14)0.0407 (8)
C40.84639 (17)0.9060 (4)0.19365 (16)0.0441 (8)
C50.79276 (19)0.7711 (5)0.1755 (2)0.0646 (11)
H5A0.79650.73410.13530.097*
H5B0.74670.81360.17670.097*
H5C0.80130.68050.20320.097*
C60.8389 (2)0.9614 (6)0.25784 (18)0.0707 (12)
H6A0.87201.04700.27020.106*
H6B0.84740.86970.28500.106*
H6C0.79251.00210.25860.106*
C70.83308 (19)1.0435 (4)0.14660 (17)0.0529 (9)
H7A0.78481.07660.14610.063*
H7B0.83570.99260.10770.063*
C80.8755 (2)1.2031 (5)0.1477 (2)0.0786 (14)
C90.9459 (5)1.1708 (16)0.1267 (5)0.081 (3)0.50
H9A0.97201.27150.12800.122*0.50
H9B0.93861.12920.08610.122*0.50
H9C0.97141.09130.15300.122*0.50
C100.8316 (8)1.301 (2)0.0956 (7)0.111 (5)0.50
H10A0.85261.40680.09160.166*0.50
H10B0.78501.31540.10470.166*0.50
H10C0.83021.24130.05830.166*0.50
C110.8522 (8)1.3241 (19)0.1929 (6)0.110 (5)0.50
H11A0.87941.42300.19330.165*0.50
H11B0.85871.27570.23250.165*0.50
H11C0.80371.35000.18120.165*0.50
C9'0.9560 (5)1.1719 (18)0.1623 (6)0.100 (4)0.50
H9'A0.98041.27490.16290.150*0.50
H9'B0.97061.10200.13170.150*0.50
H9'C0.96641.11960.20110.150*0.50
C10'0.8601 (9)1.299 (3)0.0881 (7)0.133 (6)0.50
H10D0.88741.39780.09080.200*0.50
H10E0.81141.32640.08070.200*0.50
H10F0.87181.23210.05550.200*0.50
C11'0.8846 (7)1.3011 (17)0.2076 (5)0.090 (4)0.50
H11D0.91201.39780.20330.135*0.50
H11E0.90781.23370.23960.135*0.50
H11F0.83961.33280.21700.135*0.50
C120.8530 (2)0.7219 (6)0.02092 (18)0.0785 (15)0.592 (8)
H12A0.81960.68700.00510.094*0.592 (8)
H12B0.83890.67080.06010.094*0.592 (8)
C130.8442 (6)0.8996 (11)0.0295 (5)0.119 (3)0.592 (8)
H13A0.85810.95830.00810.143*0.592 (8)
H13B0.79610.92690.04480.143*0.592 (8)
C140.8909 (6)0.9395 (18)0.0745 (5)0.129 (3)0.592 (8)
H14A0.89291.05670.07940.193*0.592 (8)
H14B0.87320.88960.11260.193*0.592 (8)
H14C0.93680.89800.06070.193*0.592 (8)
C12'0.8530 (2)0.7219 (6)0.02092 (18)0.0785 (15)0.408 (8)
H12C0.83170.77180.01150.094*0.408 (8)
H12D0.82220.63560.03900.094*0.408 (8)
C13'0.8621 (9)0.8539 (16)0.0695 (6)0.122 (3)0.408 (8)
H13C0.88660.80720.10050.146*0.408 (8)
H13D0.81670.89190.08870.146*0.408 (8)
C14'0.9031 (9)0.995 (2)0.0388 (9)0.127 (4)0.408 (8)
H14D0.88211.09740.05340.190*0.408 (8)
H14E0.95020.99090.04750.190*0.408 (8)
H14F0.90320.98810.00420.190*0.408 (8)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Cl10.0464 (6)0.0923 (8)0.0621 (7)0.0296 (5)0.0018 (5)0.0159 (5)
N10.0408 (15)0.0505 (18)0.0374 (16)0.0101 (13)0.0058 (12)0.0052 (13)
N20.0356 (14)0.0494 (17)0.0384 (15)0.0072 (13)0.0063 (12)0.0056 (13)
N30.0414 (15)0.0463 (17)0.0348 (15)0.0116 (13)0.0042 (12)0.0024 (12)
N40.0573 (19)0.073 (2)0.0359 (16)0.0262 (17)0.0011 (14)0.0091 (15)
N50.0354 (14)0.0586 (19)0.0375 (15)0.0113 (13)0.0054 (12)0.0083 (13)
C10.0343 (17)0.043 (2)0.045 (2)0.0076 (15)0.0056 (15)0.0022 (15)
C20.0341 (16)0.0370 (19)0.0390 (18)0.0026 (14)0.0061 (14)0.0030 (14)
C30.0436 (18)0.042 (2)0.0363 (18)0.0059 (15)0.0046 (15)0.0012 (14)
C40.0374 (18)0.043 (2)0.054 (2)0.0100 (15)0.0130 (16)0.0000 (16)
C50.045 (2)0.055 (3)0.098 (3)0.0007 (18)0.020 (2)0.007 (2)
C60.072 (3)0.083 (3)0.063 (3)0.029 (2)0.030 (2)0.001 (2)
C70.051 (2)0.044 (2)0.065 (2)0.0107 (18)0.0143 (18)0.0011 (18)
C80.091 (3)0.045 (3)0.106 (4)0.000 (2)0.039 (3)0.001 (2)
C90.085 (6)0.064 (5)0.102 (7)0.015 (5)0.042 (5)0.004 (6)
C100.122 (9)0.081 (6)0.135 (8)0.001 (7)0.039 (7)0.051 (6)
C110.126 (9)0.071 (7)0.131 (8)0.006 (7)0.014 (7)0.027 (6)
C9'0.102 (7)0.079 (6)0.125 (8)0.026 (5)0.035 (6)0.001 (7)
C10'0.150 (10)0.111 (8)0.146 (9)0.011 (8)0.047 (7)0.046 (7)
C11'0.097 (8)0.060 (6)0.113 (7)0.012 (6)0.016 (6)0.018 (5)
C120.075 (3)0.107 (4)0.048 (2)0.038 (3)0.012 (2)0.015 (2)
C130.121 (4)0.122 (4)0.112 (4)0.010 (3)0.013 (3)0.005 (3)
C140.131 (5)0.129 (5)0.126 (5)0.002 (4)0.016 (4)0.002 (4)
C12'0.075 (3)0.107 (4)0.048 (2)0.038 (3)0.012 (2)0.015 (2)
C13'0.121 (4)0.122 (4)0.121 (4)0.007 (4)0.014 (4)0.001 (4)
C14'0.129 (5)0.128 (5)0.122 (5)0.003 (4)0.016 (4)0.003 (4)
Geometric parameters (Å, º) top
Cl1—C11.743 (3)C9—H9B0.9600
N1—C11.307 (4)C9—H9C0.9600
N1—C31.363 (4)C10—H10A0.9600
N2—C11.307 (4)C10—H10B0.9600
N2—C21.369 (4)C10—H10C0.9600
N3—C21.329 (4)C11—H11A0.9600
N3—C31.342 (4)C11—H11B0.9600
N4—C31.329 (4)C11—H11C0.9600
N4—C121.438 (5)C9'—H9'A0.9600
N4—H40.8600C9'—H9'B0.9600
N5—C21.331 (4)C9'—H9'C0.9600
N5—C41.476 (4)C10'—H10D0.9600
N5—H50.8600C10'—H10E0.9600
C4—C51.524 (5)C10'—H10F0.9600
C4—C61.528 (5)C11'—H11D0.9600
C4—C71.529 (5)C11'—H11E0.9600
C5—H5A0.9600C11'—H11F0.9600
C5—H5B0.9600C12—C131.464 (8)
C5—H5C0.9600C12—H12A0.9700
C6—H6A0.9600C12—H12B0.9700
C6—H6B0.9600C13—C141.478 (9)
C6—H6C0.9600C13—H13A0.9700
C7—C81.534 (6)C13—H13B0.9700
C7—H7A0.9700C14—H14A0.9600
C7—H7B0.9700C14—H14B0.9600
C8—C111.522 (9)C14—H14C0.9600
C8—C91.524 (8)C13'—C14'1.506 (10)
C8—C10'1.533 (9)C13'—H13C0.9700
C8—C11'1.543 (8)C13'—H13D0.9700
C8—C101.557 (9)C14'—H14D0.9600
C8—C9'1.566 (9)C14'—H14E0.9600
C9—H9A0.9600C14'—H14F0.9600
C1—N1—C3112.2 (3)C8—C9—H9A109.5
C1—N2—C2112.0 (3)C8—C9—H9B109.5
C2—N3—C3115.2 (3)H9A—C9—H9B109.5
C3—N4—C12124.4 (3)C8—C9—H9C109.5
C3—N4—H4117.8H9A—C9—H9C109.5
C12—N4—H4117.8H9B—C9—H9C109.5
C2—N5—C4128.3 (3)C8—C10—H10A109.5
C2—N5—H5115.9C8—C10—H10B109.5
C4—N5—H5115.9H10A—C10—H10B109.5
N2—C1—N1130.6 (3)C8—C10—H10C109.5
N2—C1—Cl1114.7 (2)H10A—C10—H10C109.5
N1—C1—Cl1114.6 (2)H10B—C10—H10C109.5
N3—C2—N5120.8 (3)C8—C11—H11A109.5
N3—C2—N2125.0 (3)C8—C11—H11B109.5
N5—C2—N2114.2 (3)H11A—C11—H11B109.5
N4—C3—N3118.6 (3)C8—C11—H11C109.5
N4—C3—N1116.6 (3)H11A—C11—H11C109.5
N3—C3—N1124.7 (3)H11B—C11—H11C109.5
N5—C4—C5109.0 (3)C8—C9'—H9'A109.5
N5—C4—C6104.9 (3)C8—C9'—H9'B109.5
C5—C4—C6107.9 (3)H9'A—C9'—H9'B109.5
N5—C4—C7113.7 (3)C8—C9'—H9'C109.5
C5—C4—C7107.6 (3)H9'A—C9'—H9'C109.5
C6—C4—C7113.5 (3)H9'B—C9'—H9'C109.5
C4—C5—H5A109.5C8—C10'—H10D109.5
C4—C5—H5B109.5C8—C10'—H10E109.5
H5A—C5—H5B109.5H10D—C10'—H10E109.5
C4—C5—H5C109.5C8—C10'—H10F109.5
H5A—C5—H5C109.5H10D—C10'—H10F109.5
H5B—C5—H5C109.5H10E—C10'—H10F109.5
C4—C6—H6A109.5C8—C11'—H11D109.5
C4—C6—H6B109.5C8—C11'—H11E109.5
H6A—C6—H6B109.5H11D—C11'—H11E109.5
C4—C6—H6C109.5C8—C11'—H11F109.5
H6A—C6—H6C109.5H11D—C11'—H11F109.5
H6B—C6—H6C109.5H11E—C11'—H11F109.5
C4—C7—C8124.7 (3)N4—C12—C13121.4 (6)
C4—C7—H7A106.1N4—C12—H12A107.0
C8—C7—H7A106.1C13—C12—H12A107.0
C4—C7—H7B106.1N4—C12—H12B107.0
C8—C7—H7B106.1C13—C12—H12B107.0
H7A—C7—H7B106.3H12A—C12—H12B106.7
C11—C8—C9132.6 (9)C12—C13—C14103.6 (9)
C11—C8—C10'102.0 (12)C12—C13—H13A111.0
C9—C8—C10'83.9 (8)C14—C13—H13A111.0
C11—C8—C7110.4 (8)C12—C13—H13B111.0
C9—C8—C7110.4 (6)C14—C13—H13B111.0
C10'—C8—C7112.2 (10)H13A—C13—H13B109.0
C11—C8—C11'26.0 (7)C13—C14—H14A109.5
C9—C8—C11'111.0 (8)C13—C14—H14B109.5
C10'—C8—C11'118.2 (12)H14A—C14—H14B109.5
C7—C8—C11'116.4 (6)C13—C14—H14C109.5
C11—C8—C1089.0 (10)H14A—C14—H14C109.5
C9—C8—C10106.0 (8)H14B—C14—H14C109.5
C10'—C8—C1022.3 (10)C14'—C13'—H13C110.0
C7—C8—C10100.7 (8)C14'—C13'—H13D110.0
C11'—C8—C10111.4 (10)H13C—C13'—H13D108.4
C11—C8—C9'110.3 (9)C13'—C14'—H14D109.5
C9—C8—C9'29.6 (6)C13'—C14'—H14E109.5
C10'—C8—C9'109.1 (8)H14D—C14'—H14E109.5
C7—C8—C9'112.4 (6)C13'—C14'—H14F109.5
C11'—C8—C9'85.3 (8)H14D—C14'—H14F109.5
C10—C8—C9'131.2 (8)H14E—C14'—H14F109.5
C2—N2—C1—N11.6 (5)C1—N1—C3—N33.1 (5)
C2—N2—C1—Cl1178.9 (2)C2—N5—C4—C561.2 (4)
C3—N1—C1—N22.2 (6)C2—N5—C4—C6176.6 (3)
C3—N1—C1—Cl1177.3 (2)C2—N5—C4—C758.9 (5)
C3—N3—C2—N5176.4 (3)N5—C4—C7—C859.1 (4)
C3—N3—C2—N24.6 (5)C5—C4—C7—C8179.9 (3)
C4—N5—C2—N33.2 (5)C6—C4—C7—C860.7 (4)
C4—N5—C2—N2177.7 (3)C4—C7—C8—C1179.3 (8)
C1—N2—C2—N35.3 (5)C4—C7—C8—C976.1 (7)
C1—N2—C2—N5175.7 (3)C4—C7—C8—C10'167.8 (9)
C12—N4—C3—N32.1 (6)C4—C7—C8—C11'51.6 (8)
C12—N4—C3—N1179.3 (4)C4—C7—C8—C10172.2 (8)
C2—N3—C3—N4178.4 (3)C4—C7—C8—C9'44.4 (7)
C2—N3—C3—N10.1 (5)C3—N4—C12—C1369.5 (7)
C1—N1—C3—N4178.5 (3)N4—C12—C13—C1463.0 (10)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N4—H4···N1i0.862.253.099 (4)169
N5—H5···N2ii0.862.383.135 (4)147
Symmetry codes: (i) x+2, y+1, z; (ii) x+2, y, z+1/2.

Experimental details

Crystal data
Chemical formulaC14H26ClN5
Mr299.85
Crystal system, space groupMonoclinic, C2/c
Temperature (K)294
a, b, c (Å)19.354 (4), 8.1265 (16), 22.312 (4)
β (°) 98.211 (4)
V3)3473.3 (11)
Z8
Radiation typeMo Kα
µ (mm1)0.22
Crystal size (mm)0.24 × 0.20 × 0.14
Data collection
DiffractometerBruker SMART 1000 CCD
Absorption correctionMulti-scan
(SADABS; Bruker, 1997)
Tmin, Tmax0.949, 0.970
No. of measured, independent and
observed [I > 2σ(I)] reflections
8715, 3070, 1927
Rint0.043
(sin θ/λ)max1)0.595
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.061, 0.200, 1.04
No. of reflections3070
No. of parameters227
No. of restraints124
H-atom treatmentH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.82, 0.30

Computer programs: SMART (Bruker, 1997), SAINT (Bruker, 1997), SAINT, SHELXS97 (Sheldrick, 1997), SHELXL97 (Sheldrick, 1997), SHELXTL (Bruker, 1997), SHELXTL.

Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N4—H4···N1i0.862.253.099 (4)169
N5—H5···N2ii0.862.383.135 (4)147
Symmetry codes: (i) x+2, y+1, z; (ii) x+2, y, z+1/2.
 

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