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The structure determination of the tetraaza macrocyclic title compound, C24H46N6, shows that its molecule represents a meso-isomer; it occupies a special position about the crystallographic inversion centre. The pendent ethylcyano arms are oriented above and below the N4 plane and are directed away from the central cavity.
Supporting information
CCDC reference: 170303
Key indicators
- Single-crystal X-ray study
- T = 173 K
- Mean (C-C) = 0.002 Å
- R factor = 0.045
- wR factor = 0.143
- Data-to-parameter ratio = 26.7
checkCIF results
No syntax errors found
ADDSYM reports no extra symmetry
Alert Level C:
ABSMU_01 Alert C The ratio of given/expected absorption coefficient lies
outside the range 0.99 <> 1.01
Calculated value of mu = 0.067
Value of mu given = 0.070
0 Alert Level A = Potentially serious problem
0 Alert Level B = Potential problem
1 Alert Level C = Please check
Data collection: MSC/AFC Diffractometer Control Software (Molecular Structure
Corporation, 1996); cell refinement: MSC/AFC Diffractometer Control Software; data reduction: TEXSAN for Windows (Molecular Structure Corporation, 1997); program(s) used to solve structure: SIR97 (Altomare et al., 1994); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); software used to prepare material for publication: SHELXL97.
Crystal data top
C24H46N6 | F(000) = 464 |
Mr = 418.67 | Dx = 1.107 Mg m−3 |
Monoclinic, P21/c | Mo Kα radiation, λ = 0.71069 Å |
Hall symbol: P 2ybc | Cell parameters from 23 reflections |
a = 7.974 (3) Å | θ = 7.4–10.4° |
b = 17.685 (4) Å | µ = 0.07 mm−1 |
c = 9.007 (6) Å | T = 173 K |
β = 98.74 (4)° | Block, colourless |
V = 1255.4 (10) Å3 | 0.48 × 0.44 × 0.40 mm |
Z = 2 | |
Data collection top
Rigaku AFC-7R diffractometer | Rint = 0.013 |
Radiation source: Rotating anode | θmax = 30.0°, θmin = 3.2° |
Graphite monochromator | h = 0→11 |
ω–2θ scans | k = 0→24 |
4008 measured reflections | l = −12→12 |
3652 independent reflections | 3 standard reflections every 400 reflections |
2496 reflections with I > 2σ(I) | intensity decay: 1.6% |
Refinement top
Refinement on F2 | Primary atom site location: structure-invariant direct methods |
Least-squares matrix: full | Secondary atom site location: difference Fourier map |
R[F2 > 2σ(F2)] = 0.045 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.143 | H-atom parameters constrained |
S = 1.04 | w = 1/[σ2(Fo2) + (0.0749P)2 + 0.2245P] where P = (Fo2 + 2Fc2)/3 |
3652 reflections | (Δ/σ)max < 0.001 |
137 parameters | Δρmax = 0.28 e Å−3 |
0 restraints | Δρmin = −0.22 e Å−3 |
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 | x | y | z | Uiso*/Ueq | |
N1 | 0.36036 (11) | 0.41055 (5) | 0.14026 (11) | 0.0220 (2) | |
N4 | 0.59827 (11) | 0.53730 (5) | 0.16281 (10) | 0.0219 (2) | |
H4N | 0.5543 | 0.5522 | 0.0658 | 0.025* | |
N12 | 0.8169 (2) | 0.28424 (10) | 0.45658 (17) | 0.0601 (4) | |
C2 | 0.31546 (14) | 0.48660 (7) | 0.18771 (13) | 0.0244 (2) | |
H2A | 0.2364 | 0.4811 | 0.2618 | 0.0438 (10)* | |
H2B | 0.2535 | 0.5131 | 0.0992 | 0.0438 (10)* | |
C3 | 0.46374 (14) | 0.53685 (7) | 0.25718 (13) | 0.0265 (2) | |
H3 | 0.5117 | 0.5152 | 0.3572 | 0.0350 (8)* | |
C3' | 0.38959 (19) | 0.61482 (9) | 0.2834 (2) | 0.0461 (4) | |
H3A | 0.4808 | 0.6487 | 0.3278 | 0.0526 (11)* | |
H3B | 0.3056 | 0.6099 | 0.3517 | 0.0526 (11)* | |
H3C | 0.3349 | 0.6357 | 0.1873 | 0.0526 (11)* | |
C5 | 0.74362 (15) | 0.58700 (7) | 0.21402 (13) | 0.0266 (2) | |
H5 | 0.7006 | 0.6387 | 0.2326 | 0.0350 (8)* | |
C5' | 0.84607 (18) | 0.55706 (10) | 0.35956 (15) | 0.0426 (4) | |
H5A | 0.7727 | 0.5539 | 0.4373 | 0.0526 (11)* | |
H5B | 0.9408 | 0.5914 | 0.3928 | 0.0526 (11)* | |
H5C | 0.8903 | 0.5067 | 0.3418 | 0.0526 (11)* | |
C6 | 0.85799 (14) | 0.59193 (7) | 0.09233 (13) | 0.0255 (2) | |
H6A | 0.8898 | 0.5398 | 0.0681 | 0.0438 (10)* | |
H6B | 0.9636 | 0.6182 | 0.1361 | 0.0438 (10)* | |
C7 | 0.78791 (14) | 0.63197 (6) | −0.05734 (14) | 0.0251 (2) | |
C7' | 0.93405 (16) | 0.63931 (8) | −0.15048 (16) | 0.0338 (3) | |
H7A | 0.9718 | 0.5888 | −0.1757 | 0.0526 (11)* | |
H7B | 1.0289 | 0.6665 | −0.0919 | 0.0526 (11)* | |
H7C | 0.8944 | 0.6673 | −0.2431 | 0.0526 (11)* | |
C7'' | 0.73113 (18) | 0.71188 (7) | −0.01892 (18) | 0.0363 (3) | |
H7D | 0.6383 | 0.7081 | 0.0406 | 0.0526 (11)* | |
H7E | 0.6921 | 0.7396 | −0.1120 | 0.0526 (11)* | |
H7F | 0.8268 | 0.7388 | 0.0391 | 0.0526 (11)* | |
C10 | 0.45731 (14) | 0.36813 (7) | 0.26500 (13) | 0.0287 (3) | |
H10A | 0.3976 | 0.3204 | 0.2808 | 0.0438 (10)* | |
H10B | 0.4663 | 0.3983 | 0.3585 | 0.0438 (10)* | |
C11 | 0.63533 (15) | 0.35045 (8) | 0.22959 (15) | 0.0308 (3) | |
H11A | 0.6257 | 0.3175 | 0.1399 | 0.0438 (10)* | |
H11B | 0.6910 | 0.3981 | 0.2061 | 0.0438 (10)* | |
C12 | 0.73976 (17) | 0.31303 (8) | 0.35538 (16) | 0.0357 (3) | |
Atomic displacement parameters (Å2) top | U11 | U22 | U33 | U12 | U13 | U23 |
N1 | 0.0184 (4) | 0.0228 (4) | 0.0248 (4) | 0.0001 (3) | 0.0034 (3) | 0.0033 (3) |
N4 | 0.0208 (4) | 0.0248 (4) | 0.0197 (4) | −0.0030 (3) | 0.0019 (3) | −0.0014 (3) |
N12 | 0.0558 (9) | 0.0729 (11) | 0.0495 (8) | 0.0318 (8) | 0.0010 (7) | 0.0124 (7) |
C2 | 0.0216 (5) | 0.0264 (5) | 0.0256 (5) | −0.0004 (4) | 0.0052 (4) | −0.0016 (4) |
C3 | 0.0257 (5) | 0.0332 (6) | 0.0211 (5) | −0.0038 (4) | 0.0053 (4) | −0.0049 (4) |
C3' | 0.0362 (7) | 0.0441 (8) | 0.0614 (10) | −0.0064 (6) | 0.0187 (7) | −0.0289 (7) |
C5 | 0.0233 (5) | 0.0288 (6) | 0.0268 (5) | −0.0042 (4) | 0.0004 (4) | −0.0059 (4) |
C5' | 0.0337 (7) | 0.0640 (10) | 0.0268 (6) | −0.0077 (6) | −0.0057 (5) | −0.0013 (6) |
C6 | 0.0188 (5) | 0.0268 (6) | 0.0300 (6) | −0.0025 (4) | 0.0010 (4) | −0.0037 (4) |
C7 | 0.0202 (5) | 0.0222 (5) | 0.0336 (6) | −0.0024 (4) | 0.0060 (4) | 0.0002 (4) |
C7' | 0.0260 (6) | 0.0337 (6) | 0.0441 (7) | −0.0068 (5) | 0.0128 (5) | 0.0012 (5) |
C7'' | 0.0366 (7) | 0.0212 (6) | 0.0515 (8) | −0.0002 (5) | 0.0075 (6) | −0.0017 (5) |
C10 | 0.0241 (5) | 0.0344 (6) | 0.0286 (6) | 0.0052 (4) | 0.0069 (4) | 0.0097 (5) |
C11 | 0.0240 (5) | 0.0345 (6) | 0.0345 (6) | 0.0065 (5) | 0.0064 (5) | 0.0078 (5) |
C12 | 0.0308 (6) | 0.0362 (7) | 0.0401 (7) | 0.0093 (5) | 0.0054 (5) | 0.0030 (6) |
Geometric parameters (Å, º) top
N1—C2 | 1.4719 (15) | C5—C6 | 1.5311 (18) |
N1—C7i | 1.5010 (15) | C5—C5' | 1.5299 (19) |
N1—C10 | 1.4693 (16) | C6—C7 | 1.5498 (18) |
N4—C3 | 1.4665 (16) | C7—N1i | 1.5010 (15) |
N4—C5 | 1.4718 (15) | C7—C7'' | 1.5393 (17) |
N12—C12 | 1.139 (2) | C7—C7' | 1.5414 (17) |
C2—C3 | 1.5344 (17) | C10—C11 | 1.5337 (17) |
C3—C3' | 1.5326 (19) | C11—C12 | 1.4589 (19) |
| | | |
C10—N1—C2 | 111.56 (10) | C5—C6—C7 | 118.26 (10) |
C10—N1—C7i | 114.06 (9) | N1i—C7—C7'' | 109.60 (10) |
C2—N1—C7i | 113.22 (9) | N1i—C7—C7' | 112.02 (10) |
C3—N4—C5 | 115.61 (9) | C7''—C7—C7' | 108.52 (10) |
N1—C2—C3 | 116.18 (10) | N1i—C7—C6 | 110.88 (9) |
N4—C3—C3' | 114.69 (11) | C7''—C7—C6 | 107.66 (11) |
N4—C3—C2 | 110.67 (9) | C7'—C7—C6 | 108.02 (10) |
C3'—C3—C2 | 107.00 (10) | N1—C10—C11 | 109.95 (10) |
N4—C5—C6 | 109.64 (9) | C12—C11—C10 | 111.60 (11) |
N4—C5—C5' | 110.76 (11) | N12—C12—C11 | 177.59 (15) |
C6—C5—C5' | 109.54 (11) | | |
Symmetry code: (i) −x+1, −y+1, −z. |
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