supplementary materials


jh2206 scheme

Acta Cryst. (2010). E66, o2631    [ doi:10.1107/S1600536810037335 ]

2-(1,3-Dioxoisoindolin-2-yl)acetonitrile

Y. Aouine, A. Alami, A. El Hallaoui, A. Elachqar and H. Zouihri

Abstract top

The asymmetric unit of the title compound, C10H6N2O2, contains two independent molecules. The dihedral angles between the acetonitrile and the 1H-isoindole-1,3(2H)-dione units are 69.0 (7)° and 77.0 (5)° in the two molecules. One of the two terminal N atoms is disordered over two positions in a 0.66 (8):0,34 (8) ratio. In the crystal structure, the molecules are linked by intermolecular C-H...O hydrogen bonds.

Comment top

With the aim of developing new tetrazolic derived, an analog isosteric of the glycine, we have prepared 2-(1,3-dioxoisoindolin-2-yl)acetonitrile,a key intermediate, starting from 2-(bromomethyl)isoindoline-1,3-dione.

The asymmetric unit of the new synthetized 2-(1,3-dioxoisoindolin-2-yl)acetonitrile, C10H6N2O2, contains two independent molecules. The dihedral angles between the acetonitrile and the 1H-isoindole-1,3(2H)-dione are 69.0 (7)° and 77.0 (5)°, respictively.

One of the two terminal N is disordered over two positions with occupancy of 0.66 (8) for the major site. In the crystal structure, the molecules are linked by intermolecular C—H···O hydrogen bonds.

Related literature top

For the use of tetrazoles as pesticides, see: Schocken et al. (1989); Yanagi et al. (2001); Lim et al. (2007) and as antihypertensive, antialergic, antibiotic and anticonvulsant agents, see: Hashimoto et al. (1998); Berghmans et al. (2007). For their use in cancer, AIDS and obesity treatments, see: Tamura et al. (1998); Shih et al. (1999); Muraglia et al. (2006). A major advantage of tetrazoles over carboxylic acids is that they are resistant to many biological metabolic degradation pathways, see: Singh et al. (1980).

Experimental top

A mixture containing 4.8 g (0.02 mol) of 2-(bromomethyl)isoindoline-1,3-dione, 6.5 g KCN (0.1 mol), and 60 ml of anhydrous acetonitrile is heated overnight at 60°C, and then filtered. The residue is washed twice with acetonitrile, and the filtrate was concentrated under vacuum. The solid obtained is purified by chromatography on silica gel column (eluent: ether / hexane: 2 / 3).

Yield= 80% (white solid); F= 122–124°C; Rf = 0.31(ether/hexane3:1).

IR (KBr) ν cm-1: 3070(CHarom),2947/2983 (CH), 1692/1709 (2 C=O), 1557/1613 (C=C). δH (CDCl3): 4.57 (2HCH2,s); 7.60–8.10 (4Harom, m). δC (CDCl3): 28.1(CH2);115.01(CN); 127.5; 132.1; 133.3(Carom); 168.28(2 C=O).

MS—EI: [M]+=186.

Elemental analysis for C10H6N2O2 Calcd(Found):C 64.51(64.62), H 3.22(3.31), N 15.02(14.94).

Refinement top

All H atoms were fixed geometrically and treated as riding with C—H = 0.97 Å (methyne) and 0.93Å (aromatic) with Uiso(H) = 1.2Ueq(C).

One of the terminals N was found disordered over. Two sets of positions were defined for the disordered N and the site occupation factors were refined while restraining their sum to unity. The site occupation factor of the major component was refined to 0.66 (8).

Computing details top

Data collection: APEX2 (Bruker, 2005); cell refinement: SAINT (Bruker, 2005); data reduction: SAINT (Bruker, 2005); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: PLATON (Spek, 2009); software used to prepare material for publication: publCIF (Westrip, 2010).

Figures top
[Figure 1] Fig. 1. Two independent molecules of the title compound showing the atom-labelling scheme and 30% probability displacement ellipsoids. Only major parts of disordered N are shown.
[Figure 2] Fig. 2. Partial packing view showing the formation of a chain through C—H···O hydrogen bonds shown as dashed lines.
[Figure 3] Fig. 3. View of the title compound showing displacement ellipsoids at the 50% probability level.
2-(1,3-Dioxoisoindolin-2-yl)acetonitrile top
Crystal data top
C10H6N2O2Z = 4
Mr = 186.17F(000) = 384
Triclinic, P1Dx = 1.385 Mg m3
Hall symbol: -P 1Melting point: 395 K
a = 8.0960 (2) ÅMo Kα radiation, λ = 0.71073 Å
b = 8.4371 (2) ÅCell parameters from 2714 reflections
c = 14.3118 (3) Åθ = 2.7–25.3°
α = 85.072 (1)°µ = 0.10 mm1
β = 79.272 (1)°T = 296 K
γ = 68.421 (1)°Block, colourless
V = 893.02 (4) Å30.25 × 0.24 × 0.16 mm
Data collection top
Bruker APEXII CCD detector
diffractometer
2885 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tubeRint = 0.034
graphiteθmax = 27.0°, θmin = 1.5°
ω and φ scansh = 1010
18332 measured reflectionsk = 1010
3906 independent reflectionsl = 1718
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)] = 0.043Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.128H-atom parameters constrained
S = 1.05 w = 1/[σ2(Fo2) + (0.0697P)2 + 0.070P]
where P = (Fo2 + 2Fc2)/3
3906 reflections(Δ/σ)max = 0.005
267 parametersΔρmax = 0.19 e Å3
6 restraintsΔρmin = 0.19 e Å3
Crystal data top
C10H6N2O2γ = 68.421 (1)°
Mr = 186.17V = 893.02 (4) Å3
Triclinic, P1Z = 4
a = 8.0960 (2) ÅMo Kα radiation
b = 8.4371 (2) ŵ = 0.10 mm1
c = 14.3118 (3) ÅT = 296 K
α = 85.072 (1)°0.25 × 0.24 × 0.16 mm
β = 79.272 (1)°
Data collection top
Bruker APEXII CCD detector
diffractometer
2885 reflections with I > 2σ(I)
18332 measured reflectionsRint = 0.034
3906 independent reflectionsθmax = 27.0°
Refinement top
R[F2 > 2σ(F2)] = 0.043H-atom parameters constrained
wR(F2) = 0.128Δρmax = 0.19 e Å3
S = 1.05Δρmin = 0.19 e Å3
3906 reflectionsAbsolute structure: ?
267 parametersFlack parameter: ?
6 restraintsRogers parameter: ?
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)
C110.73565 (18)0.39842 (17)0.04371 (10)0.0471 (3)
C160.75085 (18)0.49910 (17)0.03635 (10)0.0461 (3)
C100.7395 (2)0.48752 (18)0.12747 (11)0.0497 (3)
C170.7711 (2)0.65409 (18)0.00671 (11)0.0527 (4)
C180.7772 (2)0.76260 (19)0.15037 (12)0.0582 (4)
H18A0.83600.83270.11120.070*
H18B0.85030.70490.19840.070*
C150.7474 (2)0.4505 (2)0.12523 (12)0.0612 (4)
H150.75590.51950.17880.073*
C140.7309 (2)0.2948 (2)0.13128 (13)0.0685 (5)
H140.72910.25770.19030.082*
C190.5995 (3)0.8711 (2)0.19668 (15)0.0745 (5)
C120.7182 (3)0.2438 (2)0.03696 (14)0.0670 (5)
H120.70750.17540.09060.080*
C130.7170 (3)0.1937 (2)0.05234 (15)0.0750 (5)
H130.70650.08930.05890.090*
C200.91639 (18)0.46404 (18)0.38170 (10)0.0462 (3)
C260.72827 (18)0.4498 (2)0.52338 (10)0.0495 (3)
C210.78905 (18)0.56105 (19)0.46334 (10)0.0472 (3)
C270.81143 (19)0.2782 (2)0.48113 (11)0.0512 (4)
C281.0390 (2)0.1584 (2)0.33559 (12)0.0598 (4)
H28A1.12020.07410.37270.072*
H28B1.11140.20150.28570.072*
C220.7336 (2)0.7317 (2)0.48390 (12)0.0600 (4)
H220.77400.80680.44330.072*
C290.9423 (2)0.0764 (2)0.29222 (14)0.0661 (5)
C230.6146 (2)0.7856 (2)0.56814 (14)0.0715 (5)
H230.57440.89960.58430.086*
C250.6098 (2)0.5045 (3)0.60702 (12)0.0640 (4)
H250.56860.42970.64750.077*
C240.5549 (2)0.6749 (3)0.62815 (13)0.0725 (5)
H240.47580.71540.68420.087*
O110.72249 (19)0.44907 (16)0.21083 (8)0.0739 (4)
O120.7926 (2)0.77161 (16)0.05386 (10)0.0863 (4)
O201.00395 (15)0.51155 (14)0.31593 (8)0.0613 (3)
O210.79522 (16)0.14499 (15)0.50949 (9)0.0727 (4)
N110.76467 (16)0.63694 (14)0.09160 (9)0.0497 (3)
N210.92041 (16)0.29721 (15)0.39635 (8)0.0494 (3)
N220.8731 (3)0.0080 (2)0.25846 (16)0.1020 (7)
N12A0.4599 (15)0.972 (4)0.222 (2)0.100 (4)0.66 (8)
N12B0.466 (4)0.916 (6)0.252 (3)0.085 (6)0.34 (8)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C110.0471 (8)0.0391 (7)0.0555 (8)0.0166 (6)0.0054 (6)0.0037 (6)
C160.0411 (7)0.0434 (7)0.0506 (8)0.0148 (6)0.0017 (6)0.0064 (6)
C100.0539 (8)0.0439 (8)0.0529 (9)0.0215 (6)0.0049 (6)0.0009 (6)
C170.0550 (8)0.0447 (8)0.0597 (9)0.0227 (7)0.0037 (7)0.0018 (7)
C180.0611 (9)0.0469 (8)0.0728 (10)0.0233 (7)0.0141 (8)0.0108 (7)
C150.0567 (9)0.0693 (10)0.0519 (9)0.0200 (8)0.0035 (7)0.0102 (8)
C140.0631 (10)0.0669 (11)0.0705 (11)0.0135 (8)0.0062 (8)0.0307 (9)
C190.0700 (12)0.0728 (12)0.0872 (14)0.0258 (10)0.0134 (10)0.0353 (10)
C120.0875 (12)0.0422 (8)0.0784 (12)0.0294 (8)0.0189 (9)0.0008 (8)
C130.0835 (12)0.0453 (9)0.1006 (15)0.0209 (9)0.0214 (11)0.0213 (9)
C200.0446 (7)0.0517 (8)0.0462 (8)0.0201 (6)0.0124 (6)0.0007 (6)
C260.0418 (7)0.0632 (9)0.0449 (8)0.0185 (7)0.0123 (6)0.0011 (7)
C210.0432 (7)0.0540 (8)0.0462 (8)0.0167 (6)0.0127 (6)0.0035 (6)
C270.0455 (8)0.0578 (9)0.0532 (8)0.0209 (7)0.0143 (6)0.0073 (7)
C280.0518 (9)0.0554 (9)0.0701 (10)0.0151 (7)0.0088 (8)0.0125 (8)
C220.0573 (9)0.0558 (9)0.0674 (10)0.0164 (7)0.0166 (8)0.0072 (8)
C290.0628 (10)0.0485 (9)0.0830 (12)0.0116 (8)0.0123 (9)0.0185 (8)
C230.0590 (10)0.0699 (11)0.0766 (12)0.0041 (8)0.0181 (9)0.0257 (10)
C250.0492 (9)0.0898 (13)0.0496 (9)0.0219 (8)0.0069 (7)0.0001 (8)
C240.0517 (9)0.0973 (15)0.0572 (10)0.0114 (9)0.0049 (8)0.0202 (10)
O110.1064 (10)0.0764 (8)0.0524 (7)0.0494 (8)0.0150 (6)0.0068 (6)
O120.1289 (12)0.0668 (8)0.0810 (9)0.0601 (8)0.0181 (8)0.0195 (7)
O200.0651 (7)0.0686 (7)0.0530 (6)0.0320 (6)0.0011 (5)0.0014 (5)
O210.0695 (7)0.0627 (7)0.0869 (9)0.0291 (6)0.0133 (6)0.0184 (6)
N110.0584 (7)0.0396 (6)0.0556 (7)0.0229 (5)0.0072 (6)0.0052 (5)
N210.0499 (7)0.0496 (7)0.0498 (7)0.0186 (5)0.0072 (5)0.0065 (5)
N220.0928 (13)0.0766 (11)0.1438 (18)0.0253 (10)0.0265 (12)0.0498 (12)
N12A0.078 (2)0.098 (7)0.114 (8)0.013 (4)0.013 (4)0.048 (7)
N12B0.079 (5)0.081 (10)0.088 (10)0.020 (6)0.005 (5)0.040 (7)
Geometric parameters (Å, °) top
C11—C121.376 (2)C20—N211.3944 (18)
C11—C161.381 (2)C20—C211.481 (2)
C11—C101.480 (2)C26—C211.380 (2)
C16—C151.378 (2)C26—C251.381 (2)
C16—C171.482 (2)C26—C271.482 (2)
C10—O111.2052 (18)C21—C221.382 (2)
C10—N111.3903 (18)C27—O211.2066 (17)
C17—O121.1989 (18)C27—N211.3958 (19)
C17—N111.395 (2)C28—N211.4445 (19)
C18—N111.4511 (18)C28—C291.460 (2)
C18—C191.458 (2)C28—H28A0.9700
C18—H18A0.9700C28—H28B0.9700
C18—H18B0.9700C22—C231.388 (2)
C15—C141.380 (2)C22—H220.9300
C15—H150.9300C29—N221.125 (2)
C14—C131.369 (3)C23—C241.372 (3)
C14—H140.9300C23—H230.9300
C12—C131.383 (3)C25—C241.383 (3)
C12—H120.9300C25—H250.9300
C13—H130.9300C24—H240.9300
C20—O201.2021 (17)
C12—C11—C16120.65 (14)C21—C26—C27108.31 (13)
C12—C11—C10130.71 (15)C25—C26—C27130.42 (15)
C16—C11—C10108.64 (12)C26—C21—C22121.60 (14)
C15—C16—C11121.80 (13)C26—C21—C20108.40 (13)
C15—C16—C17130.20 (14)C22—C21—C20129.99 (14)
C11—C16—C17108.00 (13)O21—C27—N21124.00 (15)
O11—C10—N11123.96 (14)O21—C27—C26130.39 (15)
O11—C10—C11130.57 (14)N21—C27—C26105.61 (12)
N11—C10—C11105.46 (12)N21—C28—C29112.91 (13)
O12—C17—N11124.60 (15)N21—C28—H28A109.0
O12—C17—C16129.75 (15)C29—C28—H28A109.0
N11—C17—C16105.63 (12)N21—C28—H28B109.0
N11—C18—C19111.30 (13)C29—C28—H28B109.0
N11—C18—H18A109.4H28A—C28—H28B107.8
C19—C18—H18A109.4C21—C22—C23116.75 (17)
N11—C18—H18B109.4C21—C22—H22121.6
C19—C18—H18B109.4C23—C22—H22121.6
H18A—C18—H18B108.0N22—C29—C28177.51 (18)
C16—C15—C14117.07 (16)C24—C23—C22121.71 (17)
C16—C15—H15121.5C24—C23—H23119.1
C14—C15—H15121.5C22—C23—H23119.1
C13—C14—C15121.47 (16)C26—C25—C24117.30 (17)
C13—C14—H14119.3C26—C25—H25121.4
C15—C14—H14119.3C24—C25—H25121.4
C11—C12—C13117.66 (16)C23—C24—C25121.36 (16)
C11—C12—H12121.2C23—C24—H24119.3
C13—C12—H12121.2C25—C24—H24119.3
C14—C13—C12121.34 (16)C10—N11—C17112.21 (12)
C14—C13—H13119.3C10—N11—C18123.66 (13)
C12—C13—H13119.3C17—N11—C18124.11 (12)
O20—C20—N21124.84 (14)C20—N21—C27112.00 (12)
O20—C20—C21129.50 (14)C20—N21—C28123.18 (12)
N21—C20—C21105.65 (12)C27—N21—C28124.49 (13)
C21—C26—C25121.28 (15)
Hydrogen-bond geometry (Å, °) top
D—H···AD—HH···AD···AD—H···A
C13—H13···O12i0.932.513.386 (2)158
C15—H15···O20ii0.932.453.144 (2)132
C18—H18B···O200.972.423.372 (2)167
C28—H28A···O21iii0.972.393.298 (2)156
Symmetry codes: (i) x, y−1, z; (ii) −x+2, −y+1, −z; (iii) −x+2, −y, −z+1.
Table 1
Hydrogen-bond geometry (Å, °)
top
D—H···AD—HH···AD···AD—H···A
C13—H13···O12i0.932.513.386 (2)158
C15—H15···O20ii0.932.453.144 (2)132
C18—H18B···O200.972.423.372 (2)167
C28—H28A···O21iii0.972.393.298 (2)156
Symmetry codes: (i) x, y−1, z; (ii) −x+2, −y+1, −z; (iii) −x+2, −y, −z+1.
Acknowledgements top

The authors thank the CNRST, Morocco, for making this work possible.

references
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