Jiaxin Hua, Leonard J. Barbourb and George W. Gokel*a
aDepartments of Molecular Biology & Pharmacology and Chemistry, Division of Bioorganic Chemistry, Washington University School of Medicine, Campus Box 8103, 660 S. Euclid Ave., St. Louis, MO 63110, USA. E-mail: ggokel@molecool.wustl.edu; Fax: +1 314/362-9298; Tel: +1 314/362-9297
bDepartment of Chemistry, University of Stellenbosch, 7602, Matieland, South Africa
First published on 16th June 2004
The potential importance in biology of ammonium–arene cation–π interactions has fostered the development of a model system that uses ferrocene as a scaffold that can rotate groups with respect to each other while maintaining them at a fixed distance. The preparation of 1-benzyl-1′-N,N-dimethylaminomethylferrocene methiodide is reported along with the solid state structure of it and its precursor. Clear evidence is presented for an intermolecular ammonium–arene interaction. The results are analyzed in the context of existing arene–ammonium ion contacts.
We have long been interested in the problem of defining the cation–π interaction specifically for the alkali metal cations Na+ and K+ because these are the most abundant metal cations in vivo. Solution and solid state work that we conducted in the 1980s failed to provide definitive evidence for interactions of these ions with either Na+ or K+ when the π-donors were benzene, alkene, or alkyne.19,20 The latter studies were conducted with lariat ether receptor molecules. Remarkably, minor alterations to the sidechains of these earlier systems21,22 led to a large number of solid state structures that clearly show cation–π interactions. These involve sodium and potassium cations with alkenes,23 alkynes,24 benzene, phenol,25 and indole.26,27 Aromatic residues such as imidazole (the histidine sidechain arene)28 and pentafluorophenyl,29 which were expected not to form π-complexes, did not show cation–π interactions under similar circumstances. We have recently reviewed these results.30,31
Ammonium ion–π complexes are also of great potential interest in biology. The π-donor sidechains of the amino acids are as above. The potential cation–π interaction would involve the sidechain residues of either lysine (Lys, K) or arginine (Arg, R), i.e. amino or guanidine. Note that lysine and arginine occur to the extent of about 1 in 9 amino acids in all known protein sequences. Both the lysine amino group (pKa 10.5) and arginine's guanidine (pKa 12.8) are fully protonated at physiological pH (∼7.4). Thus, cation–π interactions could occur involving the sidechain residues of Lys or Arg with the π-donors Phe, Tyr, or Trp by either interchain or intrachain proximity. The possibility of such interactions was recognized two decades ago by Burley and Petsko, who searched the Protein Data Bank for indications of proximity between sidechain amino groups and arenes.32 Ammonium ion interactions with arenes were also studied using this technique.33 We report here the development of a chemical model system designed to probe such ammonium ion–arene interactions.
Our experience using ferrocene as a scaffold that can undergo rotation on its “molecular ball bearing”37,38 suggested its use in this application. Ferrocene (1) has several useful and unusual properties in the context of supramolecular chemistry. The two aromatic rings of ferrocene are parallel and separated by 3.25 Å. They rotate with respect to each other on an iron atom—a low energy “ball bearing.” Synthetic access is gained readily by acylation of ferrocene's electron rich arenes. Although its use in the present work was not anticipated, the potential for redox switching37 and metal ion donation39 by ferrocene enhanced our interest in this scaffold. After our own effort in this area began, a report appeared in which ferrocene was used as a β-turn mimetic.40 The latter studies were not directed to cation–π interactions, but the use of ferrocene to enforce sidechain proximity is similar in concept to our own approach. An earlier paper reported that ferrocene, when 1,1′-disubstituted by two valine esters, formed intramolecular hydrogen bonds that stabilized a syn sidearm conformation.41
Corey–Pauling–Koltun (CPK) molecular models suggested that when a π-donor and an ammonium cation were present on the 1- and 1′-rings of ferrocene, they could rotate into proximity if such an interaction was favorable. This is illustrated in Scheme 1 for 1-benzyl-1′-trimethylammoniomethylferrocene, 2. Compound 2 was designed to exploit ferrocene's rotational dynamics in the hope that evidence for an ammonium–π interaction would be obtained. The syn and anti conformations of 2 represent the two structural extremes for this compound. When anti, there should be no intramolecular ammonium–π interaction. In the syn conformation, such an interaction might be detectable either in solution or by X-ray methods.
![]() | ||
| Scheme 1 | ||
In designing 2, we searched the Cambridge Structural Database (CSD) to guide our choice of molecules. Two solid state structures of interest are 1,1′-dibenzylferrocene (CSD: NUYQAZ)42 and 1,1′-bis(2-pyridinomethylaminocarbonyl)ferrocene (JATPUP)43 (Fig. 1). Dibenzylferrocene (3) is in an extended conformation in which the two cyclopentadiene rings are anti and the sidechains are pointed in opposite directions. The structure of 3 has been rendered using the program X-Seed44–46 such that ferrocene is in the space-filling (CPK) metaphor and the chains are represented as sticks. This was done to show the extent to which the cyclopentadienyl rings envelop Fe(II).
![]() | ||
| Fig. 1 1,1′-Disubstituted ferrocenes 3 and 4 are in conformations in which the sidearms are, respectively, anti and syn. | ||
The structure of picolinamine derivative 4 has two arms, as does 3, but they are positioned on the same side of ferrocene. The organometallic residue is in the syn arrangement and the sidechains exhibit N–H⋯N hydrogen bonding. The latter example supports the notion that when a weak force interaction occurs in the sidechain, the conformation of ferrocene will be appropriate to sustain it. The structures are shown in Fig. 1.
The successful approach to 2 is shown in Scheme 2. Ferrocene was treated with N,N-dimethylcarbamoyl chloride [(CH3)2NCOCl] and AlCl3 at ambient temperature for 20 h. N,N-Dimethylferrocenecarboxamide 5
(obtained as yellow needles, 42%) was acylated with PhCOCl (2 equiv) and AlCl3
(3 equiv). 1-Benzoyl-1′-N,N-dimethylferrocenecarboxamide (6, C6H5–CO–C5H4FeC5H4–CONMe2) was obtained in 62% yield as a red oil. The latter proved to be unstable and partially decomposed during flash column chromatography. In subsequent preparations, it was reduced immediately with LiAlH4–AlCl3 to afford 7, 1-benzyl-1′-N,N-dimethylaminomethylferrocene (88%), as a red oil that solidified after lengthy drying under high vacuum. Evaporation of a hexane solution containing 7 at 0
°C for 3 weeks afforded yellow parallelepipeds, mp 48–49
°C. These crystals proved to be useful for X-ray analysis. Finally, compound 7 was treated with excess CH3I overnight to afford the ammonium salt 2 as a yellow solid in 90% yield. Crystallization from acetone gave 2 as light yellow rhombohedroids, mp
=
172–174
°C.
![]() | ||
| Scheme 2 | ||
) 2.85 Å in length and the O–H⋯N bond angle is nearly linear, i.e. 170°. The distance between nitrogens in adjacent molecules is 5.9 Å and the centroid-to-centroid distance between adjacent benzene rings is essentially the same. The interplane distance of the cyclopentadienes in ferrocene is 3.33 Å and the Cp rings are parallel. No interaction between the sidearms is apparent.![]() | ||
| Fig. 2 Solid state structure showing two molecules of 7 linked by a water molecule. | ||
Although the structure of precursor 7 exhibits some interesting features, the goal was to detect ammonium ion cation–π interactions in 2. We surmised that the most favorable cation–π interaction would be intramolecular. The structure of compound 2 is shown in Fig. 3. The asymmetric unit consists of two separate molecules in different conformations. In one molecule, the benzene ring turns upward from the ferrocene ring plane at an angle of 107°, as in the structure of 7. The other monomer is disordered. The benzyl sidearm in the latter has two possible directions while the lower part of the ferrocene is fixed. The two arrangements are shown in the left hand structure of Fig. 3. In neither position is there proximity to the benzyl group, and the intramolecular trimethylammonium cation is essentially vertical to the ferrocene unit. The trimethylammonium sidearms adopt similar positions in the two molecules—they turn downward from the ferrocene ring plane at an angle of 111°. The iodide anions are 4.47 Å and 4.66 Å distant from the nearer nitrogen. The sidearms in neither structure are in the anti arrangement. Instead, the sidearms are roughly on the same side of the ferrocene in each case but the dihedral angles are 105°, 69°, and −63°. There does not appear to be any intramolecular cation–π interaction.
![]() | ||
| Fig. 3 Structure of 1′-benzylferrocenylmethyltrimethylammonium iodide, 2, showing two molecules present in the unit cell. The left hand structure is disordered. | ||
Fig. 4 shows the intermolecular cation–π interaction of three molecules of 2—contributed by two unit cells. The dotted lines indicate contacts between benzene and ammonium ions. The trimethylammonium cation of the central ferrocene is almost vertical at the top of the nearby benzene ring. The nearest methyl carbon is 4 Å away from the benzene centroid. The ammonium cation (N+) is 4.66 Å from the centroid. A second, similar contact occurs in an adjacent pair. A line dropped from nitrogen to the arene's centroid makes an angle of about 12° from vertical. The distance between the cationic nitrogen atom and the arene's centroid is 4.7 Å.
![]() | ||
| Fig. 4 Three molecules of 2 showing ammonium ion to arene contact. Note the disorder in the right and left monomers. | ||
![]() | ||
| Fig. 5 Systems having close quaternary ammonium to arene contacts, labeled by their CSD descriptors: GOFGOX, GOVSOZ, HIBMEK, and WOLWAV. | ||
The intermolecular contacts in GOFGOX, GOVSOZ, and HIBMEK are likewise short, all being approximately 4.4 Å. In GOVSOZ, however, the closest benzene ring is angled significantly and the closest carbon is ∼4.23 Å from the nitrogen atom, but the centroid is ∼4.8 Å away. The nitrogen atom of tetra-n-butylammonium ion in HIBMEK is ∼4.2 Å from the nearest phenoxy ring in the bismuth complex shown. The interaction is along a line only 17° from perpendicular. A special situation arises for GOFGOX, in which benzene rings are both inter- and intramolecular with respect to the ammonium nitrogen atom. The ammonium salt's arene is folded back so that there is contact between it and its intramolecular ammonium ion. In addition, the ammonium nitrogen is proximate to the benzene rings present in the resorcinarene. All distances are in the range 4.5–4.7 Å.
![]() | ||
| Fig. 6 Solid state structure of 8 as reported in the literature.51 | ||
The contact between an arene and trimethylammonium is necessarily limited in distance by the methyl group hydrogens. This is shown in Fig. 7. Tetramethylammonium cation is shown in panels A and B in the ball and stick and space filling metaphors, respectively. The solvent accessible surface, which reflects the closest approach of a π-donor, is shown in panel C. In principle, the best contact is the one that has both the shortest distance and the most favorable orientation. The ideal interaction between benzene and a point charge would be along a line perpendicular to the aromatic ring. In their study of protein structures, Burley and Petsko found that “[t]he normalized frequency distribution of 1556 amino–aromatic contact distances… reaches a maximum at about 4.75 Å.”32
![]() | ||
| Fig. 7 Molecular models of tetra-n-butylammonium cation in (A) the ball and stick and (B) space-filling metaphors. Model C shows the calculated solvent exposed surface. | ||
The findings of Burley and Petsko with respect to bond angle were less clear. The intermolecular interaction between two molecules of 2 can be determined from the crystal structure data. A line drawn from the centroid of one molecule of 2 to the nitrogen of a second molecule is 4.70 Å. The line diverges from perpendicular by ∼19°. It is currently unclear how packing forces influence the angle but the intermolecular π–N+ distance is clearly appropriate for a cation–π contact.
Ferrocene, 1, was obtained commercially and crystallized from heptane prior to use.
°C. 1H-NMR (CDCI3): 3.21 (s, 9H, –CH3
×
3), 3.72 (s, 2H, –CH2Ph), 4.21–4.28 (m, 6H, ferrocene), 4.48 (m, 2H, ferrocene), 4.64 (s, 2H, –CH2NME3), 7.18–7.28 (m, 5H, phenyl). 13C-NMR: 35.40, 52.47, 66.93, 69.14, 69.94, 71.29, 72.08, 72.68, 89.67, 126.04, 128.33, 128.69, 141.29. Anal. Calcd for C21H26NIFe: C, 53.10; H, 5.47; N, 2.95%. Found: C, 53.39; H, 5.49; N, 3.05%.
=
475.18, 0.35
×
0.30
×
0.20 mm3, triclinic, space group P
(No. 2), a
=
9.7909(15), b
=
13.640(2), c
=
15.018(2)
Å, α
=
94.261(3), β
=
92.364(3), γ
=
97.445(3)°, V
=
1980.5(5)
Å3, Z
=
4, Dc
=
1.594 g cm−3, F000
=
952, MoKα radiation, λ
=
0.71073 Å, T
=
173(2)K, 2θmax
=
54.2°, 12
560 reflections collected, 8549 unique (Rint
=
0.0401). Final GooF
=
1.279, R1
=
0.1182, wR2
=
0.2179, R indices based on 5885 reflections with I
>
2σ(I)
(refinement on F2), 370 parameters, 243 restraints. Lp and absorption corrections applied, μ
=
2.322 mm−1.
°C. The reaction mixture was stirred at room temperature for 20 h, poured into ice–water, and extracted with CH2Cl2
(3
×
20 mL). The organic layers were combined, washed with saturated Na2CO3
(30 mL) and water (30 mL) and then dried over MgSO4. Flash column chromatography (silica gel, eluted with 1 ∶ 4 Me2CO–hexanes) afforded 5 as yellow needles, (2.15 g, 42%) which was recrystallized from hexanes, mp
=
114–115
°C (lit.52 mp
=
119–121
°C).
°C. N,N-dimethylferrocenecarboxamide (0.70 g, 2.7 mmol) in 20 mL CH2Cl2 was then added dropwise during 10 min. The reaction mixture was stirred at −30
°C for 1 h, and at 0
°C for 5 h, poured into ice–water, extracted with CH2Cl2
(3
×
20 mL), the organic layers were combined and washed with saturated Na2CO3
(30 mL), and water (30 mL). After drying (MgSO4), flash column chromatography (silica gel, eluted with 1 ∶ 4 Me2CO–hexanes) afforded 3 as a dark red oil (0.6 g, 62%). IR: 3088, 2927, 1636, 1619, 1499, 1449, 1395, 1376, 1286 cm−1. 1H-NMR (CDCl3): 3.01 (s, 6H, –CH3), 4.33–5.30 (m, 8H, ferrocene), 7.48–7.89 (m, 5H, PhH). 13C-NMR: 36.20, 38.84, 71.42, 72.23, 72.96, 74.74, 78.85, 80.42, 128.06, 128.18, 131.65, 139.33, 169.11, 198.50.
=
48–49
°C. IR: 3084, 3028, 2936, 2812, 2765, 1603, 1495, 1454, 1039, 1021 cm−1. 1H-NMR (CDCl3): 2.15 (s, 6H, –CH3), 3.22 (s, 2H, –CH2NMe2), 3.66 (s, 2H, –CH2Ph), 4.02–4.10 (m, 8H, ferrocene), 7.15–7.25 (m, 5H, phenyl). 13C-NMR: 35.75, 44.67, 58.91, 68.05, 68.70, 69.06, 70.67, 83.25, 87.91, 125.83, 128.15, 128.25, 141.43. Anal. Calcd for C20H23NFe: C, 72.12; H, 6.91; N, 4.21%. Found: C, 72.24; H, 6.82; N, 4.13%.
=
684.50, 0.25
×
0.25
×
0.10 mm3, monoclinic, space group C2/c
(No. 15), a
=
31.690(5), b
=
5.9141(9), c
=
19.117(3)
Å, β
=
110.715(3)°, V
=
3351.2(9)
Å3, Z
=
4, Dc
=
1.357 g cm−3, F000
=
1448, MoKα radiation, λ
=
0.71073 Å, T
=
173(2)K, 2θmax
=
54.2°, 9145 reflections collected, 3688 unique (Rint
=
0.0488). Final GooF
=
0.997, R1
=
0.0433, wR2
=
0.0861, R indices based on 2640 reflections with I
>
2σ(I)
(refinement on F2), 208 parameters, 0 restraints. Lp and absorption corrections applied, μ
=
0.900 mm−1. CCDC reference numbers 222951–222952. See http://www.rsc.org/suppdata/nj/b3/b313422a/ for crystallographic data in .cif or other electronic format.
507–13 CrossRef CAS.
088–12
093 CrossRef CAS.
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