supplementary materials


lh2624 scheme

Acta Cryst. (2008). E64, o1058    [ doi:10.1107/S1600536808013548 ]

N-(2-Methoxyethyl)phthalimide

Y. L. Sim, A. Ariffin and S. W. Ng

Abstract top

The title molecule, C11H11NO3, lies on a crystallographic mirror plane which bisects the plane of the phthalimide unit and contains the C and O atoms of the 2-methoxyethyl group.

Comment top

The title compound was previously reported in a kinetic study (Khan, 1994). We intend to carry out studies on the medicinal properties of the compound; some such properties have been reported (Chapman et al., 1989; Hall et al., 1994). The molecule of N-(2-methoxyethyl)phthalimide lies on a mirror plane that relates one half of the phthalamido portion of the molecule to the other; the 2-methoxyethyl substituent lies on the mirror plane itself (Fig. 1).

Related literature top

For medicinal properties of the title compound, see: Chapman et al. (1989); Hall et al. (1994). For a kinetic study of the reaction that yields the compound, see: Khan (1994).

Experimental top

Phthalic anhydride (2.59 g, 17.5 mmol) and 2-methoxyethylamine (1.50 ml, 17.5 mmol) were dissolved in acetic acid (25 ml). The mixture was heated at 393–413 K for 4 h; the reaction was monitored by TLC. Water was added to precipitate the product, which was collected (80% yield.) Crystals were obtained upon recrystallization from water.

Refinement top

Carbon-bound H-atoms were placed in calculated positions (C—H 0.95 to 0.99 Å) and were included in the refinement in the riding model approximation, with U(H) set to 1.2–1.5 U(C).

Computing details top

Data collection: APEX2 (Bruker, 2007); cell refinement: SAINT (Bruker, 2007); data reduction: SAINT (Bruker, 2007); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: X-SEED (Barbour, 2001); software used to prepare material for publication: publCIF (Westrip, 2008).

Figures top
[Figure 1] Fig. 1. Thermal ellipsoid plot (Barbour, 2001) of C11H11NO3 at the 70% probability level. Hydrogen atoms are drawn as spheres of arbitrary radiius. Symmetry transformation (i): x, 1/2 – y, z.
N-(2-Methoxyethyl)phthalimide top
Crystal data top
C11H11NO3F000 = 432
Mr = 205.21Dx = 1.410 Mg m3
Orthorhombic, PnmaMo Kα radiation
λ = 0.71073 Å
Hall symbol: -P 2ac 2nCell parameters from 2463 reflections
a = 7.0514 (2) Åθ = 2.6–28.3º
b = 9.3852 (2) ŵ = 0.10 mm1
c = 14.6024 (4) ÅT = 100 (2) K
V = 966.37 (4) Å3Prism, colorless
Z = 40.30 × 0.20 × 0.10 mm
Data collection top
Bruker SMART APEX
diffractometer
986 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tubeRint = 0.039
Monochromator: graphiteθmax = 27.5º
T = 100(2) Kθmin = 2.6º
ω scansh = 8→9
Absorption correction: Nonek = 12→12
7349 measured reflectionsl = 12→18
1164 independent reflections
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)] = 0.059H-atom parameters constrained
wR(F2) = 0.206  w = 1/[σ2(Fo2) + (0.1433P)2 + 0.309P]
where P = (Fo2 + 2Fc2)/3
S = 1.11(Δ/σ)max = 0.001
1164 reflectionsΔρmax = 0.50 e Å3
77 parametersΔρmin = 0.50 e Å3
Primary atom site location: structure-invariant direct methods
Crystal data top
C11H11NO3V = 966.37 (4) Å3
Mr = 205.21Z = 4
Orthorhombic, PnmaMo Kα
a = 7.0514 (2) ŵ = 0.10 mm1
b = 9.3852 (2) ÅT = 100 (2) K
c = 14.6024 (4) Å0.30 × 0.20 × 0.10 mm
Data collection top
Bruker SMART APEX
diffractometer
1164 independent reflections
Absorption correction: None986 reflections with I > 2σ(I)
7349 measured reflectionsRint = 0.039
Refinement top
R[F2 > 2σ(F2)] = 0.05977 parameters
wR(F2) = 0.206H-atom parameters constrained
S = 1.11Δρmax = 0.50 e Å3
1164 reflectionsΔρmin = 0.50 e Å3
Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/UeqOcc. (<1)
O10.2012 (2)0.00647 (14)0.60172 (9)0.0229 (5)
O20.3277 (3)0.25000.33669 (12)0.0161 (5)
N10.2007 (4)0.25000.57847 (14)0.0167 (6)
C10.2372 (3)0.17575 (18)0.89087 (12)0.0176 (5)
H10.24340.12600.94750.021*
C20.2281 (3)0.09866 (19)0.80904 (12)0.0168 (5)
H20.22800.00260.80880.020*
C30.2194 (3)0.17598 (18)0.72848 (11)0.0144 (5)
C40.2072 (3)0.12658 (18)0.63197 (13)0.0171 (5)
C50.1763 (4)0.25000.47961 (16)0.0176 (6)
H5A0.10340.33540.46100.021*0.50
H5B0.10340.16460.46100.021*0.50
C60.3665 (4)0.25000.43155 (16)0.0175 (6)
H6A0.44040.33570.44860.021*0.50
H6B0.44040.16430.44860.021*0.50
C70.4974 (4)0.25000.28287 (17)0.0210 (7)
H7A0.46420.25000.21770.031*
H7B0.57210.16470.29700.031*0.50
H7C0.57210.33530.29700.031*0.50
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O10.0377 (10)0.0142 (8)0.0166 (8)0.0009 (6)0.0011 (6)0.0037 (5)
O20.0210 (11)0.0178 (9)0.0093 (9)0.0000.0003 (7)0.000
N10.0282 (14)0.0143 (11)0.0075 (10)0.0000.0000 (8)0.000
C10.0240 (10)0.0185 (10)0.0102 (9)0.0008 (7)0.0016 (6)0.0018 (6)
C20.0237 (11)0.0134 (8)0.0133 (9)0.0006 (7)0.0001 (7)0.0017 (6)
C30.0189 (10)0.0142 (9)0.0101 (9)0.0001 (7)0.0003 (6)0.0012 (6)
C40.0258 (11)0.0133 (9)0.0121 (9)0.0011 (7)0.0006 (7)0.0004 (6)
C50.0220 (14)0.0216 (12)0.0091 (12)0.0000.0024 (9)0.000
C60.0239 (15)0.0197 (11)0.0088 (12)0.0000.0011 (9)0.000
C70.0284 (17)0.0196 (12)0.0149 (12)0.0000.0043 (11)0.000
Geometric parameters (Å, °) top
O1—C41.211 (2)C3—C3i1.389 (3)
O2—C61.412 (3)C3—C41.486 (2)
O2—C71.432 (3)C5—C61.514 (4)
N1—C41.398 (2)C5—H5A0.9900
N1—C4i1.398 (2)C5—H5B0.9900
N1—C51.454 (3)C6—H6A0.9900
C1—C1i1.394 (3)C6—H6B0.9900
C1—C21.398 (2)C7—H7A0.9800
C1—H10.9500C7—H7B0.9800
C2—C31.384 (2)C7—H7C0.9800
C2—H20.9500
C6—O2—C7112.1 (2)N1—C5—H5A109.5
C4—N1—C4i111.9 (2)C6—C5—H5A109.5
C4—N1—C5123.97 (11)N1—C5—H5B109.5
C4i—N1—C5123.97 (11)C6—C5—H5B109.5
C1i—C1—C2121.16 (10)H5A—C5—H5B108.1
C1i—C1—H1119.4O2—C6—C5106.5 (2)
C2—C1—H1119.4O2—C6—H6A110.4
C3—C2—C1117.21 (17)C5—C6—H6A110.4
C3—C2—H2121.4O2—C6—H6B110.4
C1—C2—H2121.4C5—C6—H6B110.4
C2—C3—C3i121.63 (11)H6A—C6—H6B108.6
C2—C3—C4130.19 (16)O2—C7—H7A109.5
C3i—C3—C4108.18 (9)O2—C7—H7B109.5
O1—C4—N1124.48 (17)H7A—C7—H7B109.5
O1—C4—C3129.64 (16)O2—C7—H7C109.5
N1—C4—C3105.87 (15)H7A—C7—H7C109.5
N1—C5—C6110.8 (2)H7B—C7—H7C109.5
C1i—C1—C2—C30.1 (2)C3i—C3—C4—O1179.02 (19)
C1—C2—C3—C3i0.1 (2)C2—C3—C4—N1179.5 (2)
C1—C2—C3—C4179.47 (19)C3i—C3—C4—N10.07 (17)
C4i—N1—C4—O1179.03 (13)C4—N1—C5—C692.3 (2)
C5—N1—C4—O13.2 (4)C4i—N1—C5—C692.3 (2)
C4i—N1—C4—C30.1 (3)C7—O2—C6—C5180.0
C5—N1—C4—C3176.0 (2)N1—C5—C6—O2180.0
C2—C3—C4—O10.5 (4)
Symmetry codes: (i) x, −y+1/2, z.
Acknowledgements top

We thank the SAGA grant (06–02-03–0147) for supporting this study, and the University of Malaya for the purchase of the diffractometer.

references
References top

Barbour, L. J. (2001). J. Supramol. Chem. 1, 189–191.

Bruker (2007). APEX2 and SAINT. Bruker AXS Inc., Madison, Wisconsin, USA.

Chapman, J. M., Sowell, J. W., Abdalla, G., Hall, I. H. & Wong, O. T. (1989). J. Pharm. Sci. 78, 903–909.

Hall, I. H., Chapman, J. M. & Wong, O. T. (1994). Anti-Cancer Drugs, 5, 75–82.

Khan, M. N. (1994). Ind. J. Chem. B33, 646–650.

Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122.

Westrip, S. P. (2008). publCIF. In preparation.