• No results found

Quinolinium fumarate

N/A
N/A
Protected

Academic year: 2020

Share "Quinolinium fumarate"

Copied!
7
0
0

Loading.... (view fulltext now)

Full text

(1)

Acta Cryst.(2003). E59, o397±o398 DOI: 10.1107/S1600536803004446 Ning Shanet al. C9H8N+C4H3O4ÿ

o397

organic papers

Acta Crystallographica Section E

Structure Reports Online

ISSN 1600-5368

Quinolinium fumarate

Ning Shan,* Elaine Batchelor and William Jones

Department of Chemistry, University of Cambridge, Lensfield Road, Cambridge CB2 1EW, England

Correspondence e-mail: [email protected]

Key indicators

Single-crystal X-ray study

T= 140 K

Mean(C±C) = 0.002 AÊ

Rfactor = 0.034

wRfactor = 0.085

Data-to-parameter ratio = 14.3

For details of how these key indicators were automatically derived from the article, see http://journals.iucr.org/e.

#2003 International Union of Crystallography Printed in Great Britain ± all rights reserved

In the title complex, C9H8N+C4H3O4ÿ, fumarate anions are

linked by OÐH O hydrogen bonds, forming in®nite supramolecular chains along thec axis. Quinolinium cations are attached to the anionic chains via NÐH O and CÐ H O interactions. The crystal structure determination con®rms the protonation of the quinoline N atom and deprotonation of one of the carboxylic acid groups of fumaric acid.

Comment

Fumaric acid is an organic dicarboxylic acid which crystallizes in two polymorphic forms: one in the monoclinic space group P21/c(Brown, 1966) and the other in the triclinic space group

P1 (Bednowitz & Post, 1966). In both crystal structures, acid molecules are linked by carboxylic acidR2

2(8) hydrogen-bond

pairs, forming one-dimensional supramolecular tapes. Fumaric acid is of interest since it is known to form supramolecular assemblies with N-aromatic complexes (Batcheloret al., 2000). As part of our analysis of supramolecular architectures, the structure of the title complex, (I), was determined at 140 K.

(I) consists of a 1:1 complex of fumarate anions and quinolinium cations. The asymmetric unit and atomic numbering scheme are shown in Fig. 1. Zigzag supramolecular acid chains are formed along the c axis via O1ÐH01 O3 hydrogen bonds (Table 2). In addition, quinolinium cations are linked to the acid chains (Fig. 2) by N1ÐH02 O4 hydrogen bonds and C9ÐH9 O3 interactions. Proton transfer is observed between the carboxylic acid group and the quinoline N atom (Table 1). Quinolinium cations form in®nite stacks along the b axis, the distance between adjacent mol-ecules within a stack beingca3.5 AÊ.

Experimental

Fumaric acid and quinoline were obtained from Aldrich without further puri®cation. 46 mg of the acid and 52 mg of the base were mixed and dissolved in a mixture of 9 ml of ethyl acetate and 10 drops of methanol. Crystals of (I) were obtained by slow evaporation at room temperature.

(2)

Crystal data

C9H8N+C4H3O4ÿ

Mr= 245.23

Orthorhombic,Pca21

a= 22.5838 (5) AÊ

b= 3.7273 (1) AÊ

c= 13.2912 (5) AÊ

V= 1118.81 (6) AÊ3

Z= 4

Dx= 1.456 Mg mÿ3

MoKradiation Cell parameters from 9880

re¯ections

= 1.8±27.5

= 0.11 mmÿ1

T= 140 (2) K Block, colourless 0.230.230.16 mm

Data collection

Nonius KappaCCD diffractometer Thin-slice!and'scans Absorption correction: multi-scan

(SORTAV; Blessing, 1995)

Tmin= 0.877,Tmax= 0.985

9868 measured re¯ections 2329 independent re¯ections

2118 re¯ections withI> 2(I)

Rint= 0.050 max= 27.5

h=ÿ23!29

k=ÿ4!3

l=ÿ17!14

Re®nement

Re®nement onF2

R[F2> 2(F2)] = 0.034

wR(F2) = 0.085

S= 1.08 2325 re¯ections 163 parameters

H-atom parameters constrained

w= 1/[2(F

o2) + (0.0494P)2

+ 0.0496P]

whereP= (Fo2+ 2Fc2)/3

(/)max= 0.001 max= 0.20 e AÊÿ3 min=ÿ0.23 e AÊÿ3

Table 1

Selected geometric parameters (AÊ).

O2ÐC10 1.207 (2)

O4ÐC13 1.282 (2) O3ÐC13O1ÐC10 1.233 (2)1.330 (2)

Table 2

Hydrogen-bonding geometry (AÊ,).

DÐH A DÐH H A D A DÐH A

N1ÐH02 O4i 0.88 1.67 2.553 (2) 179

C9ÐH9 O3i 0.95 2.79 3.348 (2) 119

O1ÐH01 O3ii 0.84 1.83 2.667 (2) 177

C3ÐH3 O2 0.95 2.35 3.284 (2) 168

Symmetry codes: (i)xÿ1

2;2ÿy;z; (ii) 2ÿx;2ÿy;zÿ12.

All H atoms bonded to C atoms were placed geometrically and re®ned using a riding model, with Uiso for each H atom taken as

1.2Ueqof the carrier atom. Atoms H01 and H02 were located from a

difference Fourier map and re®ned using a riding model. The abso-lute structure was not determined. Friedel opposites were merged prior to merging of data inPca21.

Data collection:COLLECT(Nonius, 1998); cell re®nement:HKL SCALEPACK(Otwinowski & Minor, 1997); data reduction: HKL DENZO (Otwinowski & Minor, 1997) and SCALEPACK; program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to re®ne structure:SHELXL97 (Sheldrick, 1997); molecular graphics:XP(Sheldrick, 1993); software used to prepare material for publication:SHELXL97.

We are grateful for a DWEF Cambridge Scholarship and ORS Award (NS), as well as ®nancial assistance from the EPSRC for the purchase of the CCD diffractometer. We also thank Dr J. E. Davies for data collection.

References

Batchelor, E., Klinowski, J. & Jones, W. (2000).J. Mater. Chem.10, 839±848. Bednowitz, A. L. & Post, B. (1966).Acta Cryst.21, 566±571.

Blessing, R. H. (1995).Acta Cryst.A51, 33±38. Brown, C. J. (1966).Acta Cryst.21, 1±5. Flack, H. D. (1983).Acta Cryst.A39, 876±881.

Nonius (1998).COLLECT. Nonius BV, Delft, The Netherlands.

Otwinowski, Z. & Minor, W. (1997). Methods in Enzymology, Vol. 276,

Macromolecular Crystallography, Part A, edited by C. W. Carter Jr and R. M. Sweet, pp. 307±326. New York: Academic Press.

Sheldrick, G. M. (1993).XP. University of GoÈttingen, Germany.

Sheldrick, G. M. (1997). SHELXL97 and SHELXS97. University of GoÈttingen, Germany.

Watkin, D. J., Prout, C. K. & Pearce, L. J. (1996).CAMERON. Chemical Crystallography Laboratory, University of Oxford, England.

Figure 2

Projection on to (010), showing the zigzag supramolecular tapes formed by OÐH O hydrogen bonds and proton transfer between the carboxylic acid and the aromatic N atom (CAMERON; Watkinet al., 1996).

Figure 1

(3)

supporting information

sup-1

Acta Cryst. (2003). E59, o397–o398

supporting information

Acta Cryst. (2003). E59, o397–o398 [doi:10.1107/S1600536803004446]

Quinolinium fumarate

Ning Shan, Elaine Batchelor and William Jones

S1. Comment

Fumaric acid is an organic dicarboxylic acid which crystallizes in two polymorphic forms: one in the monoclinic space

group P21/c (Brown, 1966) and the other in the triclinic space group P1 (Bednowitz & Post, 1966). In both crystal

structures, acid molecules are linked by carboxylic acid R22(8) hydrogen-bond pairs, forming one-dimensional

supramolecular tapes. Fumaric acid is of interest since it is known to form supramolecular assemblies with N-aromatic

complexes (Batchelor et al., 2000). As part of our analysis of supramolecular architectures, the structure of the title

complex, (I), was determined at 140 K.

(I) consists of a 1:1 complex of fumarate anions and quinolinium cations. The asymmetric unit and atomic numbering

scheme are shown in Fig. 1. Zigzag supramolecular acid chains are formed along the c axis via O1—H01···O3 hydrogen

bonds (Table 2). In addition, quinolinium cations are linked to the acid chains (Fig. 2) by N1—H02···O4 hydrogen bonds

and C9—H9···O3 interactions. Proton transfer is observed between the carboxylic acid group and the quinoline N atom

(Table 1). Quinolinium cations form infinite stacks along the b axis with the distance between adjacent molecules within

a stack being ca 3.5 Å.

S2. Experimental

Fumaric acid and quinoline were obtained from Aldrich without further purification. 46 mg of the acid and 52 mg of the

base were mixed and dissolved in 9 ml of ethyl acetate and 10 drops of methanol mixture. Crystals of (I) were obtained

by slow evaporation at room temperature.

S3. Refinement

All H atoms bonded to C atoms were placed geometrically and refined using a riding model, with the Uiso values for each

H atom taken as 1.2 Ueq of the carrier atom. Atoms H01 and H02 were located from difference Fourier maps and refined

(4)
[image:4.610.127.484.75.246.2]

Figure 1

The molecular unit of (I), showing displacement ellipsoids at the 50% probability level (XP; Sheldrick, 1993).

Figure 2

Projection onto (010), showing the zigzag supramolecular tapes formed by O—H···O hydrogen bonds and proton transfer

between the carboxylic acid and the aromatic N atom (CAMERON; Watkin et al., 1996).

Quinolinium Fumarate

Crystal data

C9H8N+·C4H3O4Mr = 245.23

Orthorhombic, Pca21 a = 22.5838 (5) Å

c = 13.2912 (5) Å V = 1118.81 (6) Å3 Z = 4

[image:4.610.128.485.285.564.2]
(5)

supporting information

sup-3

Acta Cryst. (2003). E59, o397–o398 Dx = 1.456 Mg m−3

Dm = no Mg m−3

Dm measured by not measured Melting point: not measured K Mo radiation, λ = 0.71073 Å Cell parameters from 9880 reflections

θ = 1.8–27.5° µ = 0.11 mm−1 T = 140 K Block, colourless 0.23 × 0.23 × 0.16 mm

Data collection

Nonius KappaCCD diffractometer

Radiation source: fine-focus sealed tube Graphite monochromator

thin–slice ω and φ scans

Absorption correction: multi-scan (SORTAV; Blessing, 1995) Tmin = 0.877, Tmax = 0.985

9868 measured reflections 2329 independent reflections 2118 reflections with I > 2σ(I) Rint = 0.050

θmax = 27.5°, θmin = 1.8° h = −23→29

k = −4→3 l = −17→14

Refinement

Refinement on F2 Least-squares matrix: full R[F2 > 2σ(F2)] = 0.034 wR(F2) = 0.085 S = 1.08 2325 reflections 163 parameters 1 restraint

Primary atom site location: structure-invariant direct methods

Secondary atom site location: difference Fourier map

Hydrogen site location: inferred from neighbouring sites

H-atom parameters constrained w = 1/[σ2(F

o2) + (0.0494P)2 + 0.0496P] where P = (Fo2 + 2Fc2)/3

(Δ/σ)max = 0.001 Δρmax = 0.20 e Å−3 Δρmin = −0.23 e Å−3

Special details

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)

x y z Uiso*/Ueq

N1 0.70065 (6) 0.3852 (3) 0.91328 (10) 0.0229 (3)

H02 0.6801 0.4547 0.8605 0.028*

O2 0.92188 (5) 0.7454 (3) 0.61425 (10) 0.0331 (3)

O4 1.14159 (4) 1.4168 (3) 0.75918 (9) 0.0311 (3)

O3 1.06865 (5) 1.2868 (3) 0.86560 (10) 0.0378 (3)

O1 0.99508 (5) 0.9657 (3) 0.51896 (9) 0.0319 (3)

H01 0.9738 0.8899 0.4717 0.038*

C7 0.76386 (7) 0.1615 (4) 1.08004 (12) 0.0259 (4)

H7 0.7852 0.0819 1.1375 0.031*

(6)

C2 0.78992 (7) 0.5428 (4) 0.82504 (12) 0.0252 (3)

H2 0.7674 0.6179 0.7684 0.030*

C9 0.67253 (6) 0.2611 (4) 0.99297 (14) 0.0266 (3)

H9 0.6305 0.2499 0.9923 0.032*

C13 1.08959 (7) 1.3009 (4) 0.78005 (12) 0.0242 (3)

C1 0.76118 (6) 0.4082 (4) 0.91110 (11) 0.0214 (3)

C3 0.85029 (7) 0.5651 (4) 0.82326 (14) 0.0302 (4)

H3 0.8697 0.6538 0.7649 0.036*

C5 0.85695 (6) 0.3265 (4) 0.99134 (14) 0.0279 (3)

H5 0.8802 0.2543 1.0474 0.034*

C8 0.70331 (7) 0.1452 (4) 1.07873 (12) 0.0282 (4)

H8 0.6823 0.0561 1.1354 0.034*

C12 1.05486 (7) 1.1844 (4) 0.68978 (13) 0.0240 (3)

H12 1.0709 1.2313 0.6250 0.029*

C10 0.96883 (6) 0.8973 (4) 0.60642 (12) 0.0247 (3)

C11 1.00317 (7) 1.0202 (4) 0.69517 (13) 0.0255 (3)

H11 0.9869 0.9780 0.7600 0.031*

C4 0.88398 (7) 0.4575 (4) 0.90732 (14) 0.0312 (4)

H4 0.9259 0.4764 0.9054 0.037*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23

N1 0.0249 (7) 0.0232 (6) 0.0207 (7) 0.0025 (5) −0.0042 (5) 0.0000 (5)

O2 0.0252 (6) 0.0458 (7) 0.0283 (7) −0.0099 (5) 0.0005 (5) 0.0003 (5)

O4 0.0261 (6) 0.0434 (7) 0.0239 (6) −0.0082 (5) −0.0008 (5) −0.0017 (5)

O3 0.0381 (7) 0.0523 (8) 0.0230 (7) −0.0140 (5) 0.0026 (6) −0.0002 (5)

O1 0.0277 (6) 0.0455 (7) 0.0225 (6) −0.0095 (5) −0.0003 (5) −0.0034 (5)

C7 0.0347 (9) 0.0218 (7) 0.0211 (9) −0.0003 (6) −0.0040 (6) 0.0013 (6)

C6 0.0289 (8) 0.0176 (6) 0.0218 (8) 0.0013 (5) −0.0037 (7) −0.0017 (6)

C2 0.0323 (8) 0.0240 (7) 0.0193 (8) 0.0006 (6) −0.0020 (7) 0.0010 (6)

C9 0.0268 (7) 0.0266 (7) 0.0265 (8) −0.0005 (6) 0.0019 (8) −0.0012 (6)

C13 0.0273 (7) 0.0242 (7) 0.0212 (9) −0.0019 (6) −0.0012 (7) 0.0002 (6)

C1 0.0264 (8) 0.0167 (6) 0.0212 (8) 0.0008 (5) −0.0005 (6) −0.0033 (5)

C3 0.0335 (8) 0.0290 (8) 0.0281 (9) −0.0019 (6) 0.0058 (7) 0.0022 (7)

C5 0.0277 (8) 0.0250 (7) 0.0311 (9) −0.0008 (6) −0.0089 (7) 0.0005 (7)

C8 0.0364 (9) 0.0271 (8) 0.0211 (9) −0.0022 (6) 0.0035 (7) 0.0008 (6)

C12 0.0278 (8) 0.0238 (6) 0.0202 (8) 0.0007 (6) 0.0021 (6) 0.0007 (6)

C10 0.0232 (8) 0.0264 (7) 0.0245 (9) 0.0005 (6) −0.0023 (7) −0.0002 (6)

C11 0.0263 (8) 0.0303 (8) 0.0198 (8) −0.0017 (6) 0.0023 (6) 0.0003 (7)

C4 0.0254 (8) 0.0296 (8) 0.0385 (10) −0.0001 (6) −0.0001 (7) −0.0001 (7)

Geometric parameters (Å, º)

N1—C9 1.319 (2) C2—H2 0.9500

N1—C1 1.3702 (19) C9—C8 1.403 (2)

N1—H02 0.8800 C9—H9 0.9500

(7)

supporting information

sup-5

Acta Cryst. (2003). E59, o397–o398

O4—C13 1.282 (2) C3—C4 1.410 (3)

O3—C13 1.233 (2) C3—H3 0.9500

O1—C10 1.330 (2) C5—C4 1.363 (3)

O1—H01 0.8400 C5—H5 0.9500

C7—C8 1.369 (2) C8—H8 0.9500

C7—C6 1.414 (2) C12—C11 1.320 (2)

C7—H7 0.9500 C12—H12 0.9500

C6—C1 1.414 (2) C10—C11 1.484 (2)

C6—C5 1.414 (2) C11—H11 0.9500

C2—C3 1.366 (2) C4—H4 0.9500

C2—C1 1.408 (2)

C9—N1—C1 121.29 (14) C2—C3—C4 120.50 (15)

C9—N1—H02 119.4 C2—C3—H3 119.7

C1—N1—H02 119.4 C4—C3—H3 119.7

C10—O1—H01 109.5 C4—C5—C6 120.40 (16)

C8—C7—C6 119.72 (14) C4—C5—H5 119.8

C8—C7—H7 120.1 C6—C5—H5 119.8

C6—C7—H7 120.1 C7—C8—C9 119.44 (14)

C7—C6—C1 118.29 (13) C7—C8—H8 120.3

C7—C6—C5 123.20 (15) C9—C8—H8 120.3

C1—C6—C5 118.51 (15) C11—C12—C13 123.63 (15)

C3—C2—C1 119.72 (14) C11—C12—H12 118.2

C3—C2—H2 120.1 C13—C12—H12 118.2

C1—C2—H2 120.1 O2—C10—O1 123.86 (15)

N1—C9—C8 121.46 (13) O2—C10—C11 122.37 (15)

N1—C9—H9 119.3 O1—C10—C11 113.76 (12)

C8—C9—H9 119.3 C12—C11—C10 124.19 (16)

O3—C13—O4 124.44 (15) C12—C11—H11 117.9

O3—C13—C12 121.72 (14) C10—C11—H11 117.9

O4—C13—C12 113.84 (14) C5—C4—C3 120.62 (15)

N1—C1—C2 119.96 (14) C5—C4—H4 119.7

N1—C1—C6 119.80 (13) C3—C4—H4 119.7

C2—C1—C6 120.24 (13)

Hydrogen-bond geometry (Å, º)

D—H···A D—H H···A D···A D—H···A

N1—H02···O4i 0.88 1.67 2.553 (2) 179

C9—H9···O3i 0.95 2.79 3.348 (2) 119

O1—H01···O3ii 0.84 1.83 2.667 (2) 177

C3—H3···O2 0.95 2.35 3.284 (2) 168

Figure

Figure 1

References

Related documents

This signi � cantly higher level of negotiation in the touch table condition as compared with the laptop demonstrates a higher quantity of collaborative behaviour, as negotiation is

Representative images of the GL261-eGFP- gliomas and CD31 + tumor vasculature in wild-type (wt) mice (top), Nrp1 MgKO mice (middle), and wt mice administered the Nrp1

Thus, also bearing in mind the complex heterogeneity (sometimes species-specific) of these non parenchymal cells, our aim was to investigate the structural aspects of the liver,

The use of umbilical cord blood as an alternative to bone marrow as a source of haematopoietic stem cells for the treatment of certain diseases has been on an increase since the

In the region-of-interest analy- sis, FA values were significantly lower ( P ⬍ .001) in patients with iNPH than in control subjects in the posterior third of the body (c) and

In addition to the human capital variables that are the determinants of the wage level (Blau & Kahn, 2003), we also control for other variables in the analysis to overcome

Despite the fact that the commuting rate of 21.8% is only slightly above the country average, a careful observation of the commuting categories in each county (Table 2) for