2,5-Dioxopyrrolidin-1-yl adamantane-1-carboxyl-ate.

The title compound, C(15)H(19)NO(4), contains one crystallographically independent mol-ecule in the asymmetric unit. The N-O-C-O torsion angle is 1.97 (9)°. The two pairs of vicinal H atoms that lie above or below the plane defined by the five-membered pyrrolidine-2,5-dione ring are an average of 6.57 (5)° from being eclipsed. The average absolute C-C-C-C torsion angle in the adamantane skeleton, in which each fused cyclo-hexane ring is in a chair configuration, is 59.99 (5)°. The crystal packing is unremarkable.

Related literature

For the biological activity of adamantane-1-carboxylic acid derivatives, see: De Felice et al. (2007 ▶); Jia et al. (2005 ▶); Stouffer et al. (2008 ▶). For related structures, see: Molčanov et al. (2006 ▶); Thackeray & White (1977 ▶); Homan et al. (1997 ▶). For related structures produced via biocatalysis, see: Bailey et al. (1996 ▶); Ridyard et al. (1996 ▶). For the structure of a derivative of the title compound, see the following paper: Liu et al. (2009 ▶).

Experimental

Crystal data

C15H19NO4

M = 277.31

Monoclinic,

a = 6.6711 (3) Å

b = 29.4502 (14) Å

c = 7.0291 (3) Å

β = 104.447 (2)°

V = 1337.26 (10) Å3

Z = 4

Mo Kα radiation

μ = 0.10 mm−1

T = 150 K

0.30 × 0.28 × 0.10 mm

Data collection

Bruker APEXII–FR591 diffractometer

Absorption correction: multi-scan (SADABS; Sheldrick, 2007 ▶) T min = 0.888, T max = 0.990

51912 measured reflections

6819 independent reflections

6104 reflections with I > 2σ(I)

R int = 0.032

Refinement

R[F 2 > 2σ(F 2)] = 0.042

wR(F 2) = 0.120

S = 1.08

6819 reflections

181 parameters

H-atom parameters constrained

Δρmax = 0.44 e Å−3

Δρmin = −0.29 e Å−3

Data collection: APEX2 (Bruker, 2003 ▶); cell refinement: SAINT (Bruker, 2003 ▶); data reduction: SAINT and XPREP (Bruker, 2003 ▶); program(s) used to solve structure: SIR97 (Altomare et al., 1999 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: ORTEP-3 (Farrugia, 1997 ▶), WinGX32 (Farrugia, 1999 ▶) and POV-RAY (Cason, 2002 ▶); software used to prepare material for publication: enCIFer (Allen et al., 2004 ▶).

Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536809024209/bg2265sup1.cif

Structure factors: contains datablocks I. DOI: 10.1107/S1600536809024209/bg2265Isup2.hkl

Additional supplementary materials: crystallographic information; 3D view; checkCIF report

C15H19NO4	F(000) = 592
Mr = 277.31	Dx = 1.377 Mg m−3
Monoclinic, P21/n	Mo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2yn	Cell parameters from 9946 reflections
a = 6.6711 (3) Å	θ = 2.8–37.1°
b = 29.4502 (14) Å	µ = 0.10 mm−1
c = 7.0291 (3) Å	T = 150 K
β = 104.447 (2)°	Plate, colourless
V = 1337.26 (10) Å3	0.30 × 0.28 × 0.10 mm
Z = 4

Bruker APEXII–FR591 diffractometer	6819 independent reflections
Radiation source: rotating anode	6104 reflections with I > 2σ(I)
graphite	Rint = 0.032
ω+φ scans	θmax = 37.2°, θmin = 2.8°
Absorption correction: multi-scan (SADABS; Sheldrick, 2007)	h = −11→11
Tmin = 0.888, Tmax = 0.990	k = −49→50
51912 measured reflections	l = −11→11

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)] = 0.042	Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.120	H-atom parameters constrained
S = 1.08	w = 1/[σ2(Fo2) + (0.057P)2 + 0.2898P] where P = (Fo2 + 2Fc2)/3
6819 reflections	(Δ/σ)max < 0.001
181 parameters	Δρmax = 0.44 e Å−3
0 restraints	Δρmin = −0.29 e Å−3

Experimental. The crystal was coated in Exxon Paratone N hydrocarbon oil and mounted on a thin mohair fibre attached to a copper pin. Upon mounting on the diffractometer, the crystal was quenched to 150(K) under a cold nitrogen gas stream supplied by an Oxford Cryosystems Cryostream and data were collected at this temperature.

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.

	x	y	z	Uiso*/Ueq
C1	1.22052 (11)	0.15040 (3)	0.40895 (12)	0.02581 (14)
H1A	1.2692	0.1204	0.3753	0.031*
H1B	1.3395	0.1666	0.4946	0.031*
C2	1.04957 (11)	0.14401 (2)	0.51785 (10)	0.02258 (13)
H2	1.1055	0.1262	0.6407	0.027*
C3	0.86612 (11)	0.11819 (2)	0.38550 (10)	0.02168 (12)
H3A	0.7567	0.1135	0.4562	0.026*
H3B	0.9127	0.0881	0.3509	0.026*
C4	0.77940 (9)	0.146072 (19)	0.19724 (8)	0.01413 (9)
C5	0.95139 (10)	0.15250 (3)	0.08694 (9)	0.02086 (11)
H5A	0.9979	0.1225	0.0507	0.025*
H5B	0.8966	0.1700	−0.0352	0.025*
C6	1.13503 (10)	0.17802 (3)	0.22017 (11)	0.02310 (12)
H6	1.2464	0.1821	0.1491	0.028*
C7	1.06322 (11)	0.22477 (2)	0.27366 (11)	0.02349 (13)
H7A	1.1817	0.2414	0.3574	0.028*
H7B	1.0089	0.2427	0.1527	0.028*
C8	0.89390 (11)	0.21863 (2)	0.38360 (10)	0.01981 (11)
H8	0.8472	0.2491	0.4188	0.024*
C9	0.97680 (12)	0.19081 (3)	0.57139 (10)	0.02357 (13)
H9A	0.8665	0.1869	0.6417	0.028*
H9B	1.0939	0.2071	0.6593	0.028*
C10	0.70934 (10)	0.19322 (2)	0.25152 (10)	0.01816 (10)
H10A	0.6530	0.2110	0.1304	0.022*
H10B	0.5985	0.1897	0.3214	0.022*
C11	0.59920 (9)	0.12338 (2)	0.05527 (9)	0.01710 (10)
C12	0.27538 (10)	0.04257 (2)	−0.03135 (10)	0.01826 (10)
C13	0.14462 (10)	0.02270 (2)	−0.22012 (10)	0.02094 (11)
H13A	0.0197	0.0415	−0.2712	0.025*
H13B	0.1006	−0.0086	−0.1981	0.025*
C14	0.28296 (11)	0.02249 (2)	−0.36545 (10)	0.02184 (12)
H14A	0.3150	−0.0090	−0.3971	0.026*
H14B	0.2134	0.0382	−0.4888	0.026*
C15	0.47840 (10)	0.04733 (2)	−0.26279 (10)	0.01859 (11)
N1	0.46311 (9)	0.054259 (19)	−0.07064 (8)	0.01894 (10)
O1	0.45874 (9)	0.14099 (2)	−0.06059 (9)	0.02874 (13)
O2	0.61824 (8)	0.075815 (16)	0.06775 (8)	0.02138 (10)
O3	0.62486 (10)	0.05906 (2)	−0.32307 (10)	0.02936 (12)
O4	0.23579 (11)	0.04800 (2)	0.12597 (9)	0.02915 (12)

	U11	U22	U33	U12	U13	U23
C1	0.0157 (3)	0.0261 (3)	0.0305 (3)	0.0019 (2)	−0.0038 (2)	−0.0024 (2)
C2	0.0245 (3)	0.0195 (2)	0.0178 (2)	−0.0049 (2)	−0.0058 (2)	0.00400 (19)
C3	0.0244 (3)	0.0172 (2)	0.0185 (2)	−0.0061 (2)	−0.0039 (2)	0.00501 (18)
C4	0.0131 (2)	0.01371 (19)	0.01396 (19)	−0.00133 (16)	0.00043 (16)	0.00029 (15)
C5	0.0171 (2)	0.0291 (3)	0.0169 (2)	−0.0011 (2)	0.00514 (19)	−0.0038 (2)
C6	0.0144 (2)	0.0322 (3)	0.0230 (3)	−0.0042 (2)	0.0052 (2)	−0.0018 (2)
C7	0.0217 (3)	0.0217 (3)	0.0246 (3)	−0.0085 (2)	0.0012 (2)	0.0042 (2)
C8	0.0196 (3)	0.0159 (2)	0.0218 (3)	−0.00142 (18)	0.0012 (2)	−0.00345 (18)
C9	0.0275 (3)	0.0261 (3)	0.0153 (2)	−0.0063 (2)	0.0020 (2)	−0.0037 (2)
C10	0.0148 (2)	0.0168 (2)	0.0216 (2)	0.00051 (17)	0.00218 (19)	−0.00262 (18)
C11	0.0156 (2)	0.0163 (2)	0.0173 (2)	−0.00132 (17)	0.00011 (18)	−0.00125 (17)
C12	0.0194 (2)	0.0146 (2)	0.0210 (2)	−0.00237 (18)	0.0057 (2)	−0.00127 (18)
C13	0.0168 (2)	0.0197 (2)	0.0248 (3)	−0.00409 (19)	0.0022 (2)	−0.0032 (2)
C14	0.0234 (3)	0.0216 (3)	0.0189 (2)	−0.0042 (2)	0.0023 (2)	−0.0043 (2)
C15	0.0193 (2)	0.0166 (2)	0.0199 (2)	−0.00113 (18)	0.0051 (2)	−0.00084 (18)
N1	0.0178 (2)	0.0196 (2)	0.0182 (2)	−0.00664 (17)	0.00223 (17)	−0.00448 (16)
O1	0.0241 (3)	0.0233 (2)	0.0296 (3)	0.00305 (18)	−0.0106 (2)	−0.00286 (19)
O2	0.0205 (2)	0.01610 (18)	0.0224 (2)	−0.00444 (15)	−0.00436 (17)	−0.00179 (15)
O3	0.0271 (3)	0.0312 (3)	0.0341 (3)	−0.0051 (2)	0.0157 (2)	−0.0009 (2)
O4	0.0369 (3)	0.0291 (3)	0.0254 (2)	−0.0057 (2)	0.0152 (2)	−0.0041 (2)

C1—C2	1.5354 (12)	C8—C9	1.5348 (10)
C1—C6	1.5395 (11)	C8—C10	1.5386 (9)
C1—H1A	0.9900	C8—H8	1.0000
C1—H1B	0.9900	C9—H9A	0.9900
C2—C9	1.5387 (11)	C9—H9B	0.9900
C2—C3	1.5406 (9)	C10—H10A	0.9900
C2—H2	1.0000	C10—H10B	0.9900
C3—C4	1.5421 (8)	C11—O1	1.1956 (8)
C3—H3A	0.9900	C11—O2	1.4072 (8)
C3—H3B	0.9900	C12—O4	1.2099 (9)
C4—C11	1.5130 (8)	C12—N1	1.3913 (9)
C4—C10	1.5431 (8)	C12—C13	1.5121 (9)
C4—C5	1.5483 (9)	C13—C14	1.5381 (10)
C5—C6	1.5394 (10)	C13—H13A	0.9900
C5—H5A	0.9900	C13—H13B	0.9900
C5—H5B	0.9900	C14—C15	1.5120 (9)
C6—C7	1.5351 (11)	C14—H14A	0.9900
C6—H6	1.0000	C14—H14B	0.9900
C7—C8	1.5301 (11)	C15—O3	1.2083 (9)
C7—H7A	0.9900	C15—N1	1.3946 (9)
C7—H7B	0.9900	N1—O2	1.3849 (7)
C2—C1—C6	109.45 (5)	C7—C8—C10	109.46 (5)
C2—C1—H1A	109.8	C9—C8—C10	108.77 (5)
C6—C1—H1A	109.8	C7—C8—H8	109.5
C2—C1—H1B	109.8	C9—C8—H8	109.5
C6—C1—H1B	109.8	C10—C8—H8	109.5
H1A—C1—H1B	108.2	C8—C9—C2	109.62 (5)
C1—C2—C9	109.33 (6)	C8—C9—H9A	109.7
C1—C2—C3	109.66 (6)	C2—C9—H9A	109.7
C9—C2—C3	109.77 (6)	C8—C9—H9B	109.7
C1—C2—H2	109.4	C2—C9—H9B	109.7
C9—C2—H2	109.4	H9A—C9—H9B	108.2
C3—C2—H2	109.4	C8—C10—C4	109.92 (5)
C2—C3—C4	109.07 (5)	C8—C10—H10A	109.7
C2—C3—H3A	109.9	C4—C10—H10A	109.7
C4—C3—H3A	109.9	C8—C10—H10B	109.7
C2—C3—H3B	109.9	C4—C10—H10B	109.7
C4—C3—H3B	109.9	H10A—C10—H10B	108.2
H3A—C3—H3B	108.3	O1—C11—O2	121.17 (6)
C11—C4—C3	113.39 (5)	O1—C11—C4	128.04 (6)
C11—C4—C10	108.71 (5)	O2—C11—C4	110.74 (5)
C3—C4—C10	109.81 (5)	O4—C12—N1	124.15 (6)
C11—C4—C5	106.85 (5)	O4—C12—C13	130.05 (7)
C3—C4—C5	109.19 (5)	N1—C12—C13	105.80 (5)
C10—C4—C5	108.77 (5)	C12—C13—C14	105.90 (5)
C6—C5—C4	109.37 (5)	C12—C13—H13A	110.6
C6—C5—H5A	109.8	C14—C13—H13A	110.6
C4—C5—H5A	109.8	C12—C13—H13B	110.6
C6—C5—H5B	109.8	C14—C13—H13B	110.6
C4—C5—H5B	109.8	H13A—C13—H13B	108.7
H5A—C5—H5B	108.2	C15—C14—C13	105.66 (5)
C7—C6—C5	109.70 (6)	C15—C14—H14A	110.6
C7—C6—C1	109.50 (6)	C13—C14—H14A	110.6
C5—C6—C1	109.51 (6)	C15—C14—H14B	110.6
C7—C6—H6	109.4	C13—C14—H14B	110.6
C5—C6—H6	109.4	H14A—C14—H14B	108.7
C1—C6—H6	109.4	O3—C15—N1	123.96 (6)
C8—C7—C6	109.43 (5)	O3—C15—C14	130.34 (7)
C8—C7—H7A	109.8	N1—C15—C14	105.68 (5)
C6—C7—H7A	109.8	O2—N1—C12	121.72 (5)
C8—C7—H7B	109.8	O2—N1—C15	121.67 (6)
C6—C7—H7B	109.8	C12—N1—C15	116.30 (5)
H7A—C7—H7B	108.2	N1—O2—C11	111.87 (5)
C7—C8—C9	110.14 (6)
C6—C1—C2—C9	−60.05 (7)	C3—C4—C10—C8	59.67 (7)
C6—C1—C2—C3	60.35 (7)	C5—C4—C10—C8	−59.76 (6)
C1—C2—C3—C4	−60.62 (7)	C3—C4—C11—O1	151.19 (8)
C9—C2—C3—C4	59.51 (8)	C10—C4—C11—O1	28.75 (9)
C2—C3—C4—C11	179.35 (6)	C5—C4—C11—O1	−88.47 (9)
C2—C3—C4—C10	−58.83 (7)	C3—C4—C11—O2	−31.38 (8)
C2—C3—C4—C5	60.35 (7)	C10—C4—C11—O2	−153.82 (5)
C11—C4—C5—C6	176.77 (5)	C5—C4—C11—O2	88.96 (6)
C3—C4—C5—C6	−60.23 (7)	O4—C12—C13—C14	−177.07 (7)
C10—C4—C5—C6	59.58 (7)	N1—C12—C13—C14	2.61 (7)
C4—C5—C6—C7	−60.28 (7)	C12—C13—C14—C15	−6.58 (7)
C4—C5—C6—C1	59.93 (7)	C13—C14—C15—O3	−173.15 (7)
C2—C1—C6—C7	60.38 (7)	C13—C14—C15—N1	8.13 (7)
C2—C1—C6—C5	−59.95 (8)	O4—C12—N1—O2	−3.72 (10)
C5—C6—C7—C8	60.42 (7)	C13—C12—N1—O2	176.58 (5)
C1—C6—C7—C8	−59.79 (7)	O4—C12—N1—C15	−177.39 (7)
C6—C7—C8—C9	59.43 (7)	C13—C12—N1—C15	2.91 (8)
C6—C7—C8—C10	−60.11 (7)	O3—C15—N1—O2	0.32 (10)
C7—C8—C9—C2	−59.33 (7)	C14—C15—N1—O2	179.14 (6)
C10—C8—C9—C2	60.63 (7)	O3—C15—N1—C12	173.99 (7)
C1—C2—C9—C8	59.41 (7)	C14—C15—N1—C12	−7.19 (8)
C3—C2—C9—C8	−60.91 (8)	C12—N1—O2—C11	−89.36 (7)
C7—C8—C10—C4	60.29 (7)	C15—N1—O2—C11	83.97 (7)
C9—C8—C10—C4	−60.09 (7)	O1—C11—O2—N1	1.97 (9)
C11—C4—C10—C8	−175.76 (5)	C4—C11—O2—N1	−175.66 (5)