Buy article online - an online subscription or single-article purchase is required to access this article.
Download citation
Download citation
link to html
The title compound, C17H32N4, contains two piperazine heterocycles, which are methyl­ene bridged. The rings have chair conformations, with all substituents equatorial.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536806008622/bt2024sup1.cif
Contains datablocks I, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536806008622/bt2024Isup2.hkl
Contains datablock I

CCDC reference: 605233

Key indicators

  • Single-crystal X-ray study
  • T = 291 K
  • Mean [sigma](C-C) = 0.003 Å
  • R factor = 0.038
  • wR factor = 0.083
  • Data-to-parameter ratio = 17.4

checkCIF/PLATON results

No syntax errors found



Alert level B PLAT026_ALERT_3_B Ratio Observed / Unique Reflections too Low .... 34 Perc. PLAT230_ALERT_2_B Hirshfeld Test Diff for N12 - C16 .. 7.17 su
Alert level C PLAT029_ALERT_3_C _diffrn_measured_fraction_theta_full Low ....... 0.97 PLAT230_ALERT_2_C Hirshfeld Test Diff for N2 - C6 .. 5.72 su PLAT230_ALERT_2_C Hirshfeld Test Diff for N2 - C9 .. 6.17 su PLAT230_ALERT_2_C Hirshfeld Test Diff for C1 - C3 .. 5.83 su PLAT241_ALERT_2_C Check High Ueq as Compared to Neighbors for C4 PLAT242_ALERT_2_C Check Low Ueq as Compared to Neighbors for C3 PLAT242_ALERT_2_C Check Low Ueq as Compared to Neighbors for C13
0 ALERT level A = In general: serious problem 2 ALERT level B = Potentially serious problem 7 ALERT level C = Check and explain 0 ALERT level G = General alerts; check 0 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 2 ALERT type 3 Indicator that the structure quality may be low 0 ALERT type 4 Improvement, methodology, query or suggestion

Computing details top

Data collection: COLLECT (Nonius, 1998); cell refinement: DENZO and SCALEPACK (Otwinowski & Minor, 1997); data reduction: DENZO and SCALEPACK; program(s) used to solve structure: SHELXS97 (Sheldrick, 1990); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: SHELXTL-Plus (Sheldrick, 1991); software used to prepare material for publication: SHELXL97, PARST95 (Nardelli, 1995) and PLATON (Spek, 2003).

Bis[4-(2-methyl-2-propenyl)piperazin-1-yl]methane top
Crystal data top
C17H32N4Z = 2
Mr = 292.47F(000) = 324
Triclinic, P1Dx = 1.027 Mg m3
Hall symbol: -P 1Mo Kα radiation, λ = 0.71073 Å
a = 6.257 (2) ÅCell parameters from 6881 reflections
b = 11.719 (3) Åθ = 3.1–25.2°
c = 13.392 (5) ŵ = 0.06 mm1
α = 90.450 (13)°T = 291 K
β = 101.719 (8)°Block, colourless
γ = 100.067 (15)°0.20 × 0.15 × 0.15 mm
V = 945.7 (5) Å3
Data collection top
Nonius KappaCCD
diffractometer
1123 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tubeRint = 0.033
Graphite monochromatorθmax = 25.2°, θmin = 3.1°
Detector resolution: 19 vertical, 18 horizontal pixels mm-1h = 77
498 frames via ω–rotation (Δω=1°) and two times 60 s per frame (four sets at different κ–angles) scansk = 1314
6681 measured reflectionsl = 1515
3297 independent reflections
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)] = 0.038Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.083H-atom parameters constrained
S = 1.01 w = [exp{4.20(sinθ/λ)2}]/[σ2(Fo2)]
3297 reflections(Δ/σ)max = 0.001
190 parametersΔρmax = 0.09 e Å3
0 restraintsΔρmin = 0.11 e Å3
Special details top

Experimental. 1H NMR (500 MHz, CDCl3): δ 1.43 (s, 9H), 1.72 (s, 3H), 2.29 (4H), 2.83 (s, 2H). 3.39 (t, 4H, J = 4.7 Hz), 4.83 (s, 2H), 4.84 (s, 2H); 13C NMR (125 MHz, CDCl3): δ 20.8 (CH3), 28.4 (CH3), 50.7 (CH2), 52.9 (CH2), 65.3 (CH2), 79.4 (Cq), 113.1 (CH2), 142.4 (Cq), 154.8 (Cq); IR (KBr plate), ν (cm-1): 897 (m), 1009 (m), 1122 (s), 1168 (s), 1244 (s), 1362 (m), 1419 (s), 1696 (vs), 2801 (m), 2940 (s), 2980 (m); MS (FAB+ LR), m/z (%): (M)+, 240.0?(65); exact mass (FAB + HR): (M)+, 240.1852 ?(85) (calculated for C13H24N2O2: 240.1838).

1H NMR (500 MHz, CDCl3): δ 1.48 (s, 1H), 1.64 (s, 3H), 2.0–2.5 (4H), 2.74 (s, 2H), 2.77 (4H), 4.74 (s, 2H), 4.77 (s, 2H); 13C NMR (125 MHz, CDCl3): δ 20.7 (CH3), 46.0 (CH2), 54.5 (CH2), 65.8 (CH2), 112.6 (CH2), 142.5 (Cq); IR (KBr plate), ν (cm-1): 805 (m), 896 (s), 1014 (m), 1142 (s), 1370 (m), 1455 (s), 1651 (m), 2805 (s), 2940 (s), 2968 (s), 3073 (m) 3283 (w); MS (FAB+ LR), m/z (%): 141.1 (M + H+), (25); exact mass (FAB + HR): 141.1416 (M + H+), (100) (calculated for C8H17N2: 141.1392).

1H NMR (500 MHz, CDCl3): δ 1.71 (s, 3H), 2.28–2.60 (16H), 2.84 (s, 4H), 2.9 (s, 2H), 4.81 (s, 2H), 4.84 (s, 2H); 13C NMR (125 MHz, CDCl3): δ 20.9 (CH3), 51.6 (CH2), 53.2 (CH2), 65.4 (CH2), 81.1 (CH2), 112.7 (CH2), 142.8 (Cq); IR (KBr plate), ν (cm-1): 831 (m), 899 (vs), 1012 (s), 1049 (m), 1119 (m), 1147 (vs), 1166 (s), 1282 (s), 1342 (m), 1371 (m), 1456 (s), 1647 (m), 2758 (m), 2802 (s), 2939 (s), 2964 (s), 3074 (w); MS (FAB + LR), m/z (%): 291.4 (M + H+), (15); exact mass (FAB + HR): 291.2563 (M - H+), (100) (calculated for C17H31N4: 291.2548).

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
N10.3971 (3)1.20091 (14)0.61737 (13)0.0596 (5)
N20.3116 (2)1.01685 (13)0.75165 (13)0.0527 (5)
N110.1595 (2)0.68818 (13)0.90323 (13)0.0544 (5)
N120.1055 (2)0.90230 (12)0.86038 (12)0.0502 (5)
C10.7059 (4)1.2833 (2)0.4303 (2)0.1042 (9)
H1A0.84481.32250.42380.125*
H1B0.63011.22340.38370.125*
C20.7310 (4)1.40858 (19)0.5829 (2)0.1124 (10)
H2A0.87351.44070.56910.169*
H2B0.74991.37830.64990.169*
H2C0.64231.46810.57940.169*
C30.6170 (4)1.3126 (2)0.5051 (2)0.0730 (7)
C40.3933 (3)1.24962 (19)0.51690 (17)0.0826 (8)
H4A0.28921.30290.50610.099*
H4B0.34101.18740.46480.099*
C50.1726 (3)1.15719 (18)0.63186 (17)0.0749 (7)
H5A0.09971.09630.58050.090*
H5B0.08731.21930.62410.090*
C60.1820 (3)1.11001 (17)0.73703 (17)0.0686 (7)
H6A0.24841.17210.78820.082*
H6B0.03251.08070.74600.082*
C70.5355 (3)1.06116 (16)0.73701 (16)0.0643 (6)
H7A0.62200.99950.74520.077*
H7B0.60771.12260.78790.077*
C80.5246 (3)1.10713 (17)0.63196 (16)0.0675 (7)
H8A0.67381.13540.62220.081*
H8B0.45611.04480.58130.081*
C90.3204 (3)0.96918 (16)0.85167 (16)0.0608 (6)
H9A0.36461.03190.90350.073*
H9B0.43110.91950.86360.073*
C110.6125 (4)0.47358 (19)0.7867 (2)0.0988 (9)
H11A0.64390.40260.75040.119*
H11B0.71380.52390.77570.119*
C120.2518 (4)0.42637 (17)0.87620 (18)0.0926 (8)
H12A0.29980.35760.83230.139*
H12B0.23310.40530.94620.139*
H12C0.11310.46710.86400.139*
C130.4226 (4)0.50311 (19)0.85455 (18)0.0674 (7)
C140.3672 (3)0.61601 (16)0.91652 (16)0.0663 (6)
H14A0.48730.65890.89690.080*
H14B0.35560.59970.98810.080*
C150.1805 (3)0.72908 (16)0.79939 (15)0.0597 (6)
H15A0.29680.77520.78580.072*
H15B0.22070.66320.75080.072*
C160.0372 (3)0.80158 (16)0.78711 (15)0.0585 (6)
H16A0.15140.75400.79750.070*
H16B0.02170.82850.71810.070*
C170.1222 (3)0.86266 (15)0.96475 (15)0.0571 (6)
H17A0.15840.92921.01260.069*
H17B0.24010.81770.98040.069*
C180.0957 (3)0.78876 (16)0.97590 (15)0.0601 (6)
H18A0.08160.76211.04490.072*
H18B0.21130.83550.96450.072*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
N10.0492 (11)0.0679 (12)0.0641 (14)0.0111 (9)0.0162 (10)0.0240 (10)
N20.0458 (11)0.0518 (11)0.0606 (14)0.0063 (8)0.0127 (9)0.0157 (9)
N110.0650 (12)0.0469 (11)0.0523 (13)0.0031 (9)0.0205 (10)0.0065 (10)
N120.0546 (11)0.0454 (10)0.0466 (12)0.0004 (8)0.0087 (9)0.0033 (9)
C10.095 (2)0.141 (2)0.075 (2)0.0075 (17)0.0272 (17)0.0267 (19)
C20.127 (2)0.089 (2)0.120 (3)0.0124 (16)0.051 (2)0.0069 (19)
C30.0695 (17)0.0866 (19)0.0661 (19)0.0138 (14)0.0203 (15)0.0315 (15)
C40.0743 (18)0.1015 (19)0.072 (2)0.0124 (13)0.0161 (14)0.0354 (15)
C50.0529 (15)0.0886 (17)0.086 (2)0.0164 (12)0.0175 (14)0.0319 (14)
C60.0534 (14)0.0748 (16)0.0833 (19)0.0140 (12)0.0244 (13)0.0262 (14)
C70.0540 (14)0.0650 (15)0.0788 (19)0.0149 (11)0.0209 (13)0.0221 (13)
C80.0623 (15)0.0684 (15)0.0781 (19)0.0114 (12)0.0290 (14)0.0152 (13)
C90.0549 (14)0.0538 (13)0.0694 (18)0.0034 (10)0.0083 (12)0.0117 (12)
C110.092 (2)0.0824 (18)0.108 (2)0.0106 (14)0.0114 (18)0.0112 (16)
C120.115 (2)0.0598 (16)0.104 (2)0.0133 (14)0.0266 (17)0.0098 (15)
C130.0734 (17)0.0551 (15)0.0726 (19)0.0044 (13)0.0256 (15)0.0144 (14)
C140.0707 (15)0.0571 (14)0.0740 (17)0.0012 (11)0.0306 (13)0.0122 (13)
C150.0670 (15)0.0541 (14)0.0558 (16)0.0019 (11)0.0154 (12)0.0049 (12)
C160.0667 (15)0.0579 (14)0.0499 (15)0.0035 (11)0.0165 (12)0.0079 (12)
C170.0657 (15)0.0539 (14)0.0497 (16)0.0080 (11)0.0099 (12)0.0043 (11)
C180.0718 (15)0.0597 (14)0.0522 (15)0.0117 (11)0.0204 (12)0.0077 (12)
Geometric parameters (Å, º) top
N1—C81.459 (2)C7—C81.503 (3)
N1—C51.461 (2)C7—H7A0.9700
N1—C41.463 (2)C7—H7B0.9700
N2—C91.450 (2)C8—H8A0.9700
N2—C71.459 (2)C8—H8B0.9700
N2—C61.462 (2)C9—H9A0.9700
N11—C151.463 (2)C9—H9B0.9700
N11—C141.465 (2)C11—C131.330 (3)
N11—C181.468 (2)C11—H11A0.9300
N12—C91.460 (2)C11—H11B0.9300
N12—C171.466 (2)C12—C131.500 (3)
N12—C161.474 (2)C12—H12A0.9600
C1—C31.311 (3)C12—H12B0.9600
C1—H1A0.9300C12—H12C0.9600
C1—H1B0.9300C13—C141.505 (3)
C2—C31.503 (3)C14—H14A0.9700
C2—H2A0.9600C14—H14B0.9700
C2—H2B0.9600C15—C161.514 (2)
C2—H2C0.9600C15—H15A0.9700
C3—C41.503 (3)C15—H15B0.9700
C4—H4A0.9700C16—H16A0.9700
C4—H4B0.9700C16—H16B0.9700
C5—C61.511 (3)C17—C181.518 (2)
C5—H5A0.9700C17—H17A0.9700
C5—H5B0.9700C17—H17B0.9700
C6—H6A0.9700C18—H18A0.9700
C6—H6B0.9700C18—H18B0.9700
C8—N1—C5108.91 (16)N1—C8—H8B109.4
C8—N1—C4111.63 (18)C7—C8—H8B109.4
C5—N1—C4111.16 (17)H8A—C8—H8B108.0
C9—N2—C7110.17 (15)N2—C9—N12111.33 (16)
C9—N2—C6112.05 (17)N2—C9—H9A109.4
C7—N2—C6109.13 (15)N12—C9—H9A109.4
C15—N11—C14110.91 (16)N2—C9—H9B109.4
C15—N11—C18109.00 (15)N12—C9—H9B109.4
C14—N11—C18110.93 (16)H9A—C9—H9B108.0
C9—N12—C17108.54 (16)C13—C11—H11A120.0
C9—N12—C16111.43 (16)C13—C11—H11B120.0
C17—N12—C16109.73 (15)H11A—C11—H11B120.0
C3—C1—H1A120.0C13—C12—H12A109.5
C3—C1—H1B120.0C13—C12—H12B109.5
H1A—C1—H1B120.0H12A—C12—H12B109.5
C3—C2—H2A109.5C13—C12—H12C109.5
C3—C2—H2B109.5H12A—C12—H12C109.5
H2A—C2—H2B109.5H12B—C12—H12C109.5
C3—C2—H2C109.5C11—C13—C12122.9 (2)
H2A—C2—H2C109.5C11—C13—C14121.7 (2)
H2B—C2—H2C109.5C12—C13—C14115.4 (2)
C1—C3—C2122.6 (2)N11—C14—C13112.95 (17)
C1—C3—C4120.6 (3)N11—C14—H14A109.0
C2—C3—C4116.8 (2)C13—C14—H14A109.0
N1—C4—C3112.84 (19)N11—C14—H14B109.0
N1—C4—H4A109.0C13—C14—H14B109.0
C3—C4—H4A109.0H14A—C14—H14B107.8
N1—C4—H4B109.0N11—C15—C16109.88 (17)
C3—C4—H4B109.0N11—C15—H15A109.7
H4A—C4—H4B107.8C16—C15—H15A109.7
N1—C5—C6109.86 (17)N11—C15—H15B109.7
N1—C5—H5A109.7C16—C15—H15B109.7
C6—C5—H5A109.7H15A—C15—H15B108.2
N1—C5—H5B109.7N12—C16—C15111.46 (17)
C6—C5—H5B109.7N12—C16—H16A109.3
H5A—C5—H5B108.2C15—C16—H16A109.3
N2—C6—C5111.09 (18)N12—C16—H16B109.3
N2—C6—H6A109.4C15—C16—H16B109.3
C5—C6—H6A109.4H16A—C16—H16B108.0
N2—C6—H6B109.4N12—C17—C18110.20 (17)
C5—C6—H6B109.4N12—C17—H17A109.6
H6A—C6—H6B108.0C18—C17—H17A109.6
N2—C7—C8109.67 (17)N12—C17—H17B109.6
N2—C7—H7A109.7C18—C17—H17B109.6
C8—C7—H7A109.7H17A—C17—H17B108.1
N2—C7—H7B109.7N11—C18—C17111.48 (16)
C8—C7—H7B109.7N11—C18—H18A109.3
H7A—C7—H7B108.2C17—C18—H18A109.3
N1—C8—C7111.17 (18)N11—C18—H18B109.3
N1—C8—H8A109.4C17—C18—H18B109.3
C7—C8—H8A109.4H18A—C18—H18B108.0
C8—N1—C4—C367.4 (2)C17—N12—C9—N2176.62 (15)
C5—N1—C4—C3170.77 (19)C16—N12—C9—N262.4 (2)
C1—C3—C4—N1124.0 (2)C15—N11—C14—C1367.0 (2)
C2—C3—C4—N155.6 (3)C18—N11—C14—C13171.69 (17)
C8—N1—C5—C657.9 (2)C11—C13—C14—N11122.4 (2)
C4—N1—C5—C6178.73 (18)C12—C13—C14—N1158.7 (2)
C9—N2—C6—C5179.23 (16)C14—N11—C15—C16179.00 (16)
C7—N2—C6—C558.5 (2)C18—N11—C15—C1658.6 (2)
N1—C5—C6—N258.7 (2)C9—N12—C16—C15177.38 (17)
C9—N2—C7—C8178.34 (17)C17—N12—C16—C1557.1 (2)
C6—N2—C7—C858.2 (2)N11—C15—C16—N1258.9 (2)
C5—N1—C8—C759.3 (2)C9—N12—C17—C18177.85 (15)
C4—N1—C8—C7177.59 (16)C16—N12—C17—C1855.9 (2)
N2—C7—C8—N159.9 (2)C15—N11—C18—C1759.0 (2)
C7—N2—C9—N12167.72 (16)C14—N11—C18—C17178.57 (17)
C6—N2—C9—N1270.6 (2)N12—C17—C18—N1158.1 (2)
 

Subscribe to Acta Crystallographica Section E: Crystallographic Communications

The full text of this article is available to subscribers to the journal.

If you have already registered and are using a computer listed in your registration details, please email support@iucr.org for assistance.

Buy online

You may purchase this article in PDF and/or HTML formats. For purchasers in the European Community who do not have a VAT number, VAT will be added at the local rate. Payments to the IUCr are handled by WorldPay, who will accept payment by credit card in several currencies. To purchase the article, please complete the form below (fields marked * are required), and then click on `Continue'.
E-mail address* 
Repeat e-mail address* 
(for error checking) 

Format*   PDF (US $40)
   HTML (US $40)
   PDF+HTML (US $50)
In order for VAT to be shown for your country javascript needs to be enabled.

VAT number 
(non-UK EC countries only) 
Country* 
 

Terms and conditions of use
Contact us

Follow Acta Cryst. E
Sign up for e-alerts
Follow Acta Cryst. on Twitter
Follow us on facebook
Sign up for RSS feeds