Download citation
Download citation
link to html
In the title compound, C21H28N2, the two benzene rings are oriented nearly perpendicular to each other, and the piperazine ring adopts a chair conformation.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536807004485/at2216sup1.cif
Contains datablocks global, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536807004485/at2216Isup2.hkl
Contains datablock I

CCDC reference: 640239

Key indicators

  • Single-crystal X-ray study
  • T = 291 K
  • Mean [sigma](C-C)= 0.004 Å
  • R factor = 0.057
  • wR factor = 0.163
  • Data-to-parameter ratio = 17.1

checkCIF/PLATON results

No syntax errors found


No errors found in this datablock

Computing details top

Data collection: SMART (Bruker, 2000); cell refinement: SAINT-Plus (Bruker, 2000); data reduction: SAINT-Plus; program(s) used to solve structure: SHELXTL (Bruker, 2000); program(s) used to refine structure: SHELXTL; molecular graphics: SHELXTL; software used to prepare material for publication: SHELXTL.

1-Benzyl-4-(4-tert-butylphenyl)piperazine top
Crystal data top
C21H28N2F(000) = 672
Mr = 308.45Dx = 1.123 Mg m3
Monoclinic, P21/cMelting point: 348 K
Hall symbol: -P 2ybcMo Kα radiation, λ = 0.71073 Å
a = 6.2461 (11) ÅCell parameters from 1891 reflections
b = 15.660 (3) Åθ = 2.0–22.7°
c = 18.678 (3) ŵ = 0.07 mm1
β = 92.626 (3)°T = 291 K
V = 1825.1 (6) Å3Block, colourless
Z = 40.30 × 0.26 × 0.24 mm
Data collection top
Bruker SMART APEX CCD
diffractometer
3582 independent reflections
Radiation source: sealed tube1936 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.076
φ and ω scansθmax = 26.0°, θmin = 1.7°
Absorption correction: multi-scan
(SADABS; Bruker, 2000)
h = 76
Tmin = 0.98, Tmax = 0.98k = 1719
9859 measured reflectionsl = 2322
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)] = 0.057H-atom parameters constrained
wR(F2) = 0.163 w = 1/[σ2(Fo2) + (0.0627P)2 + 0.22P]
where P = (Fo2 + 2Fc2)/3
S = 1.02(Δ/σ)max < 0.001
3582 reflectionsΔρmax = 0.41 e Å3
209 parametersΔρmin = 0.44 e Å3
0 restraintsExtinction correction: SHELXL97, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.014 (2)
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
C10.2032 (3)1.00147 (14)0.40692 (10)0.0443 (5)
C20.3784 (3)1.05636 (14)0.41193 (11)0.0502 (6)
H2A0.50751.03680.43270.060*
C30.3649 (3)1.13866 (15)0.38690 (11)0.0520 (6)
H3A0.48651.17290.39080.062*
C40.1770 (3)1.17320 (14)0.35592 (11)0.0484 (5)
C50.0018 (3)1.11941 (15)0.35419 (12)0.0567 (6)
H5A0.12911.14010.33590.068*
C60.0129 (3)1.03582 (15)0.37851 (12)0.0551 (6)
H6A0.10971.00210.37570.066*
C70.1724 (4)1.26349 (16)0.32499 (14)0.0665 (7)
C80.2652 (5)1.32704 (16)0.37979 (14)0.0779 (8)
H8A0.18171.32610.42170.117*
H8B0.26161.38340.35950.117*
H8C0.41071.31170.39280.117*
C90.3050 (4)1.26483 (17)0.25829 (14)0.0740 (8)
H9A0.24631.22480.22380.111*
H9B0.45051.24950.27120.111*
H9C0.30171.32110.23790.111*
C100.0545 (4)1.29243 (18)0.30268 (18)0.0917 (10)
H10A0.14191.29160.34360.138*
H10B0.11421.25450.26670.138*
H10C0.04991.34940.28370.138*
C110.0280 (3)0.86599 (14)0.43128 (13)0.0566 (6)
H11A0.03280.86060.38280.068*
H11B0.07530.89540.45970.068*
C120.0705 (4)0.77838 (14)0.46212 (13)0.0626 (7)
H12A0.12510.78360.51140.075*
H12B0.06250.74640.46200.075*
C130.4252 (3)0.78128 (14)0.42316 (13)0.0564 (6)
H13A0.53110.75170.39600.068*
H13B0.48020.78560.47240.068*
C140.3895 (3)0.86910 (14)0.39285 (13)0.0557 (6)
H14A0.52320.90070.39640.067*
H14B0.34540.86460.34250.067*
C150.2581 (4)0.64518 (15)0.44677 (13)0.0666 (7)
H15A0.12010.61730.45000.080*
H15B0.32620.64680.49450.080*
C160.3948 (4)0.59459 (14)0.39815 (13)0.0587 (6)
C170.3258 (5)0.58144 (16)0.32781 (14)0.0713 (7)
H17A0.19230.60200.31180.086*
C180.4506 (6)0.53853 (17)0.28085 (16)0.0853 (9)
H18A0.40120.53020.23360.102*
C190.6471 (6)0.50819 (18)0.30353 (19)0.0886 (9)
H19A0.73320.48050.27150.106*
C200.7175 (5)0.51851 (18)0.3737 (2)0.0915 (9)
H20A0.84950.49640.38950.110*
C210.5909 (5)0.56214 (17)0.42110 (16)0.0767 (8)
H21A0.63920.56940.46860.092*
N10.2256 (3)0.91600 (11)0.43064 (9)0.0465 (5)
N20.2257 (3)0.73258 (11)0.42046 (10)0.0537 (5)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.0382 (12)0.0529 (13)0.0420 (12)0.0010 (10)0.0038 (9)0.0059 (10)
C20.0406 (12)0.0578 (14)0.0517 (13)0.0029 (11)0.0034 (10)0.0002 (11)
C30.0437 (13)0.0569 (14)0.0554 (14)0.0045 (11)0.0029 (10)0.0019 (11)
C40.0454 (13)0.0547 (14)0.0454 (12)0.0056 (11)0.0039 (10)0.0041 (10)
C50.0423 (13)0.0612 (15)0.0661 (15)0.0099 (11)0.0033 (11)0.0035 (12)
C60.0376 (12)0.0570 (15)0.0703 (16)0.0013 (10)0.0004 (11)0.0063 (12)
C70.0689 (17)0.0673 (17)0.0637 (16)0.0067 (13)0.0061 (13)0.0045 (13)
C80.0897 (19)0.0587 (16)0.085 (2)0.0157 (15)0.0032 (16)0.0044 (14)
C90.0711 (17)0.0752 (18)0.0761 (18)0.0067 (14)0.0061 (14)0.0045 (14)
C100.078 (2)0.0697 (18)0.127 (3)0.0238 (15)0.0008 (18)0.0175 (17)
C110.0456 (13)0.0612 (15)0.0637 (15)0.0014 (11)0.0114 (11)0.0059 (12)
C120.0605 (15)0.0610 (15)0.0680 (16)0.0056 (12)0.0191 (12)0.0020 (12)
C130.0522 (14)0.0550 (14)0.0626 (15)0.0048 (11)0.0081 (11)0.0022 (11)
C140.0475 (13)0.0551 (14)0.0654 (15)0.0009 (11)0.0122 (11)0.0011 (11)
C150.0813 (18)0.0550 (15)0.0645 (16)0.0032 (13)0.0150 (14)0.0039 (12)
C160.0743 (17)0.0439 (13)0.0586 (16)0.0006 (12)0.0085 (13)0.0044 (11)
C170.0905 (19)0.0597 (16)0.0637 (17)0.0102 (14)0.0056 (15)0.0045 (13)
C180.123 (3)0.0652 (18)0.0680 (18)0.0162 (18)0.0103 (18)0.0012 (14)
C190.106 (3)0.0671 (19)0.095 (2)0.0096 (18)0.030 (2)0.0068 (17)
C200.078 (2)0.0691 (19)0.127 (3)0.0131 (15)0.002 (2)0.0091 (19)
C210.084 (2)0.0637 (17)0.0812 (19)0.0018 (15)0.0044 (16)0.0062 (14)
N10.0395 (10)0.0503 (11)0.0500 (11)0.0003 (8)0.0061 (8)0.0034 (8)
N20.0557 (12)0.0506 (11)0.0558 (11)0.0026 (9)0.0121 (9)0.0025 (9)
Geometric parameters (Å, º) top
C1—C61.388 (3)C11—H11B0.9700
C1—C21.392 (3)C12—N21.459 (3)
C1—N11.415 (3)C12—H12A0.9700
C2—C31.372 (3)C12—H12B0.9700
C2—H2A0.9300C13—N21.460 (3)
C3—C41.393 (3)C13—C141.500 (3)
C3—H3A0.9300C13—H13A0.9700
C4—C51.380 (3)C13—H13B0.9700
C4—C71.527 (3)C14—N11.467 (2)
C5—C61.386 (3)C14—H14A0.9700
C5—H5A0.9300C14—H14B0.9700
C6—H6A0.9300C15—N21.465 (3)
C7—C81.523 (3)C15—C161.501 (3)
C7—C101.527 (3)C15—H15A0.9700
C7—C91.528 (3)C15—H15B0.9700
C8—H8A0.9600C16—C211.376 (3)
C8—H8B0.9600C16—C171.379 (3)
C8—H8C0.9600C17—C181.375 (4)
C9—H9A0.9600C17—H17A0.9300
C9—H9B0.9600C18—C191.365 (4)
C9—H9C0.9600C18—H18A0.9300
C10—H10A0.9600C19—C201.372 (4)
C10—H10B0.9600C19—H19A0.9300
C10—H10C0.9600C20—C211.393 (4)
C11—N11.462 (3)C20—H20A0.9300
C11—C121.507 (3)C21—H21A0.9300
C11—H11A0.9700
C6—C1—C2116.3 (2)N2—C12—C11110.70 (18)
C6—C1—N1123.87 (19)N2—C12—H12A109.5
C2—C1—N1119.79 (18)C11—C12—H12A109.5
C3—C2—C1121.4 (2)N2—C12—H12B109.5
C3—C2—H2A119.3C11—C12—H12B109.5
C1—C2—H2A119.3H12A—C12—H12B108.1
C2—C3—C4122.9 (2)N2—C13—C14110.72 (18)
C2—C3—H3A118.5N2—C13—H13A109.5
C4—C3—H3A118.5C14—C13—H13A109.5
C5—C4—C3115.1 (2)N2—C13—H13B109.5
C5—C4—C7123.7 (2)C14—C13—H13B109.5
C3—C4—C7121.2 (2)H13A—C13—H13B108.1
C4—C5—C6122.8 (2)N1—C14—C13111.87 (18)
C4—C5—H5A118.6N1—C14—H14A109.2
C6—C5—H5A118.6C13—C14—H14A109.2
C5—C6—C1121.4 (2)N1—C14—H14B109.2
C5—C6—H6A119.3C13—C14—H14B109.2
C1—C6—H6A119.3H14A—C14—H14B107.9
C8—C7—C4110.5 (2)N2—C15—C16111.34 (19)
C8—C7—C10108.0 (2)N2—C15—H15A109.4
C4—C7—C10112.3 (2)C16—C15—H15A109.4
C8—C7—C9109.6 (2)N2—C15—H15B109.4
C4—C7—C9108.6 (2)C16—C15—H15B109.4
C10—C7—C9107.7 (2)H15A—C15—H15B108.0
C7—C8—H8A109.5C21—C16—C17118.5 (2)
C7—C8—H8B109.5C21—C16—C15122.0 (2)
H8A—C8—H8B109.5C17—C16—C15119.6 (2)
C7—C8—H8C109.5C18—C17—C16121.2 (3)
H8A—C8—H8C109.5C18—C17—H17A119.4
H8B—C8—H8C109.5C16—C17—H17A119.4
C7—C9—H9A109.5C19—C18—C17120.0 (3)
C7—C9—H9B109.5C19—C18—H18A120.0
H9A—C9—H9B109.5C17—C18—H18A120.0
C7—C9—H9C109.5C18—C19—C20120.0 (3)
H9A—C9—H9C109.5C18—C19—H19A120.0
H9B—C9—H9C109.5C20—C19—H19A120.0
C7—C10—H10A109.5C19—C20—C21119.9 (3)
C7—C10—H10B109.5C19—C20—H20A120.1
H10A—C10—H10B109.5C21—C20—H20A120.1
C7—C10—H10C109.5C16—C21—C20120.4 (3)
H10A—C10—H10C109.5C16—C21—H21A119.8
H10B—C10—H10C109.5C20—C21—H21A119.8
N1—C11—C12110.90 (19)C1—N1—C11115.95 (17)
N1—C11—H11A109.5C1—N1—C14112.61 (15)
C12—C11—H11A109.5C11—N1—C14110.10 (16)
N1—C11—H11B109.5C12—N2—C13108.17 (17)
C12—C11—H11B109.5C12—N2—C15111.43 (17)
H11A—C11—H11B108.0C13—N2—C15111.82 (19)
 

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