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Inorganica Chimica Acta 358 (2005) 2618–2628
Co (II), Ni(II) and Cu(II) complexes with a new pendantarmed macrocyclic ligand showing several p,p-interactions
Laura Valencia *, Rufina Bastida *, Ma del Carmen Fernandez-Fernandez,Alejandro Macıas, Manuel Vicente
University of Santiago de Compostela, Departamento de Quımica Inorganica, Avenida de las Ciencias s/n, 15782 Santiago de Compostela, Spain
Received 8 September 2004; accepted 1 March 2005
Available online 6 April 2005
Abstract
A new ligand, L, bearing four cyanoethyl pendant groups has been synthesized by reaction of the precursor ligand L1 with acry-
lonitrile. The X-ray crystal structure of ligand L reveals the presence of a nanotubular structure in the solid state connected by inter-
molecular p,p-stacking interactions between adjacent pyridine rings. The coordination capability towards transition metal ions
[Co(II), Ni(II) and Cu(II)] has been investigated starting from the hydrated nitrate and perchlorate salts of the metals. The new
ligand L and the metal complexes obtained were characterized by elemental analysis, FAB MS, conductivity measurements,
magnetic studies, IR and UV–vis spectroscopy. Furthermore, the crystal structure of ligand L and of the complexes [CoL][Co
(NO3)4] Æ CH3CN (1), [NiL](NO3)2 (3), [NiL](ClO4)2 Æ CH3CN Æ 3H2O (4), [CuL][Cu(NO3)3(H2O)2](NO3) Æ H2O (5) and [CuL]
(ClO4)2 Æ 2CH3CN (6) were determined. The nitrate ions in the complexes are located near the pyridine rings and p,p-stacking inter-
actions between pyridine rings, nitrate ions and nitrile groups have been found.
� 2005 Elsevier B.V. All rights reserved.
Keywords: Macrocycle; Transition metal ions; p,p-stacking; Metal complexes; Crystal structures
1. Introduction
In recent decades, azamacrocyclic ligands have been
the subject of many investigations as they tend to exhibit
high thermodynamic and kinetic stabilities and also
show interesting coordination properties – they are
capable of forming mononuclear and dinuclear com-
plexes [1–3]. Oxaaza- and azamacrocycles containing
pyridine rings have been the subject of numerous inves-tigations by our research group [4–7]. It has been shown
that p,p-interactions between aromatic rings play an
important role in how the complexes or coordination
polymers are packed in the crystal lattice, and a wide
0020-1693/$ - see front matter � 2005 Elsevier B.V. All rights reserved.
doi:10.1016/j.ica.2005.03.010
* Corresponding author. Tel.: +34 981 528 073; fax: +34 981 597 525.
E-mail addresses: [email protected] (L. Valencia), [email protected]
(R. Bastida).
variety of p,p-interactions have been reported betweenaromatic groups. In previous papers, we reported the
coordination capability of different azamacrocycles
bearing pendant arm groups derived from the ligand
L1 (see Scheme 1) [8,9]. The cavity of this 18-membered
precursor does not seem appropriate for encapsulating
two metal ions; nevertheless, the presence of additional
donor atoms on the pendant groups usually led to differ-
ent and unexpected stoichiometries and coordinationgeometries in the complexes [10]. The linear nature of
the nitrile groups does not allow them to participate in
intramolecular coordination but they can interact with
additional metal ions. As part of our ongoing program,
a new macrocyclic ligand L, which contains two pyridine
rings in the ligand skeleton and bears four cyanoethyl
pendant groups, has been synthesized. In the solid state,
L presents a nanotubular structure arranged by p,p-stacking interactions between the pyridine groups. This
Scheme 1.
L. Valencia et al. / Inorganica Chimica Acta 358 (2005) 2618–2628 2619
situation is similar to that previously described for L2.
The complexation capacity of the ligand L toward a
range of first row transition metals has been studied.
The crystal structures of [CoL][Co(NO3)4] Æ CH3CN(1), [NiL](NO3)2 (3), [NiL](ClO4)2 Æ CH3CN Æ 3H2O (4),
[CuL][Cu(NO3)3(H2O)2](NO3) Æ H2O (5) and [CuL]
(ClO4)2 Æ 2CH3CN (6) were determined. The X-ray
structure of the nitrate complexes reveals p,p-stackinginteractions between pyridine rings, nitrate ions and ni-
trile groups.
2. Experimental
2.1. Measurements
Elemental analyses were performed on a Carlo-Erba
EA microanalyser. Infra-red spectra were recorded as
KBr discs on a Bruker IFS-66V spectrometer. L-SIMS
mass spectra were recorded using a Micromass Autospec
spectrometer with 3-nitrobenzyl alcohol as the matrix.
Conductivity measurements were carried out in
10�3 mol dm�3 DMF solutions at 20 �C using a WTW
LF3 conductivimeter. The 1H NMR spectrum of L
was recorded on a Bruker 500 MHz spectrometer and
CD3CN was used as the solvent. Solid state electronic
spectra were recorded on a Hitachi 4-3200 spectropho-
tometer using MgCO3 as a reference. Magnetic studieswere performed at r.t. on a vibration sample magnetom-
eter (VSM) Digital Measurement System 1660 with a
magnetic field of 5000 G.
2.2. Chemicals and starting materials
2,6-Pyridinedimethanol, ethylenediamine, acryloni-
trile and hydrated nitrate and perchlorate salts werecommercial products (from Alfa and Aldrich) and were
used without further purification. Solvents were of re-
agent grade and were purified by the usual methods.
Caution: Although problems were not encountered dur-
ing the course of this work, attention is drawn to the
potentially explosive nature of perchlorates.
2.3. Synthesis of the macrocycle L
Synthesis of the precursor ligand L1. The synthesis of
L1 was achieved following the literature method [11]. A
solution of ethylenediamine (0.67 ml, 10 mmol) was
added dropwise to a refluxing suspension of barium(II)
chloride dihydrate (1.22 g, 5 mmol) and 2,6-diformyl-
pyridine [12] (1.35 g, 10 mmol) in methanol (200 ml).
The mixture was refluxed for 4 h and the solution wasallowed to cool to room temperature. Sodium tetrahyd-
roborate (1.52 g, 40 mmol) was added slowly; after
30 min a second portion of NaBH4 (0.76 g, 20 mmol)
was added. The mixture was stirred for 1.5 h and con-
centrated to dryness under reduced pressure. The crude
solid was extracted with chloroform (3 · 100 ml) and a
brown oil was obtained. This oil was dissolved in meth-
anol and hydrobromic acid was added dropwise untilacidic pH. The tetrahydrobromide salt of the ligand L1
was isolated.
Synthesis of L. L1 (3 mmol, 2 g) was dissolved in
acrylonitrile (30 mL) and the solution refluxed for
24 h. The solution was filtered off and evaporated to
dryness. The residue was then extracted with water/chlo-
roform. The organic layer was dried over MgSO4 and
evaporated to yield an orange solid, which was recrystal-lized from acetonitrile to give the ligand L as a white
solid.
Anal. Calc. for C30H38N10 (MW: 538.70) C, 66.9; H,
7.1; N, 26.0. Found: C, 66.7; H, 7.0; N, 26.1%. Yield:
75%. IR (KBr, cm�1): 1594, 1457, [m (C@N)py and
m(C@C)], 2245 [m(C„N)]. (L-SIMS, m/z): [L1]+ 483. Col-
our: white.
2.4. Synthesis of the metal complexes – general procedure
The appropriate metal salt (0.37 mmol) was dissolved
in acetonitrile (10 mL) and added to a stirred solution of
Table 1
Crystal data and structure refinement for L, 1, 3, 4, 5 and 6
L [CoL][Co(NO3)4] ÆCH3CN (1)
[NiL](NO3)2 (3) [NiL](ClO4)2 ÆCH3CN Æ 3H2O (4)
[CuL][Cu(NO3)3(H2O)2] Æ(NO3) Æ H2O (5)
[CuL](ClO4)2 Æ2CH3CN (6)
Empirical formula C30H38N10 C32H41N15O12Co2 C30H38N12NiO6 C32H41N11O11Cl2Ni C30H38N14O15Cu2 C34H44N12O8Cl2Cu
Formula weight 538.70 945.66 721.43 885.37 961.82 883.25
Temperature (K) 298(2) 293(2) 293(2) 293(2) 293(2) 293(2)
Wavelength (A) 1.54184 0.71073 0.71073 0.71073 0.71073 0.71073
Crystal system monoclinic monoclinic monoclinic monoclinic triclinic monoclinic
Space group P21/c P21/n P21/n P21/n P�1 P21/n
Unit cell dimensions
a (A) 10.7475(8) 12.242(3) 10.7452(10) 11.154(2) 11.0370(9) 11.138(5)
b (A) 5.6114(9) 20.956(4) 15.3462(14) 25.914(6) 11.9928(10) 25.135(11)
c (A) 24.905(3) 15.515(3) 19.7356(18) 16.231(3) 15.9363(15) 16.148(7)
a (�) 90.964(7)
b (�) 92.293(7) 91.974(4) 92.415(2) 95.110(5) 93.125(7) 94.161(9)
c 96.950(7)
Volume (A3) 1500.8(3) 3978.0(14) 3251.5(5) 4673.2(17) 2090.2(3) 4509(3)
Z 2 4 4 4 2 4
Dcalc (mg/m3) 1.192 1.579 1.474 1.258 1.528 1.301
Absorption coefficient (mm�1) 0.593 0.915 0.660 0.590 1.099 0.661
F(000) 576 1952 1512 1840 988 1836
Crystal size (mm3) 0.28 · 0.20 · 0.08 0.65 · 0.61 · 0.51 0.36 · 0.18 · 0.05 0.46 · 0.28 · 0.27 0.31 · 0.22 · 0.13 0.40 · 0.40 · 0.35
h Range for data collection (�) 3.55–72.90 1.63–26.42 1.68–28.05 1.48–28.08 1.28–26.46 1.50–26.42
Index ranges �13 6 h 6 13,
�6 6 k 6 0,
�30 6 l 6 0
�15 6 h 6 15,
0 6 k 6 26,
0 6 l 6 19
�14 6 h 6 14,
�20 6 k 6 20,
�13 6 l 6 26
�14 6 h 6 14,
�27 6 k 6 34,
�21 6 l 6 17
�13 6 h 6 13,
�15 6 k 6 15,
0 6 l 6 19
�13 6 h 6 13,
0 6 k 6 31,
0 6 l 6 20
Reflections collected 3053 24489 17970 23947 25697 25036
Independent reflections [Rint] 2976 [0.0489] 8152 [0.0239] 7305 [0.0681] 10224 [0.1187] 8521 [0.0677] 9140 [0.0509]
Completeness to theta 100.0% (72.90�) 99.6% (26.42�) 92.6% (28.05�) 89.9% (28.08�) 99.2% (26.46�) 98.6% (26.42�)Absorption correction None SADABS SADABS SADABS SADABS SADABS
Maximum and minimum
transmission
0.9541 and 0.8515 0.6526 and 0.5878 0.9677 and 0.7969 0.8569 and 0.7730 0.8703 and 0.7268 0.8016 and 0.7779
Refinement method full-matrix least-
squares on F2
full-matrix least-
squares on F2
full-matrix least-
squares on F2
full-matrix least-
squares on F2
full-matrix least-
squares on F2
full-matrix least-
squares on F2
Data/restraints/parameters 2976/0/181 8152/0/551 7305/0/442 10224/0/500 8521/0/550 9140/6/517
Goodness-of-fit on F2 1.054 1.015 0.731 0.854 1.073 1.209
Final R indices [I > 2r(I)] R1 = 0.0719,
wR2 = 0.2188
R1 = 0.0481,
wR2 = 0.1306
R1 = 0.0462,
wR2 = 0.0644
R1 = 0.0884,
wR2 = 0.2132
R1 = 0.0692,
wR2 = 0.1914
R1 = 0.2051,
wR2 = 0.4910
R indices (all data) R1 = 0.1524,
wR2 = 0.2617
R1 = 0.0665,
wR2 = 0.1481
R1 = 0.1578,
wR2 = 0.0825
R1 = 0.2921,
wR2 = 0.2672
R1 = 0.1152,
wR2 = 0.2196
R1 = 0.2322,
wR2 = 0.5066
Extinction coefficient 0.0129(16)
Largest difference in peak
and hole (e A3)
0.397 and �0.235 1.765 and �0.850 0.277 and �0.239 0.646 and �0.465 0.976 and �0.783 3.586 and �1.596
2620
L.Valen
ciaet
al./Inorganica
Chim
icaActa
358(2005)2618–2628
L. Valencia et al. / Inorganica Chimica Acta 358 (2005) 2618–2628 2621
the ligand L (0.135 g, 0.25 mmol) in acetonitrile
(20 mL). The solution was stirred for 2 h. The low solu-
bility of the nitrate complexes at room temperature in
this solvent led to the formation of crystalline precipi-
tates immediately after addition of the metal salts. The
resulting solids were isolated, dried under vacuum andrecrystallized from hot acetonitrile or water. The solu-
tions of the perchlorate complexes were concentrated
in a rotary evaporator until the volume was ca. 5–
6 mL. The resulting products were filtered off, dried
and recrystallized from acetonitrile or water.
2.5. [CoL][Co(NO3)4] Æ CH3CN (1)
Anal. Calc. for C32H41N15O12Co2 (MW: 945.6): C,
40.6; H, 4.4; N, 22.2. Found: C, 39.7; H, 4.6; N,
21.9%. Yield: 49%. IR (KBr, cm�1): 1614, 1579, 1473
[m(C@N)py and m(C@C)], 2426, 2252 [m(C„N)], 1449,
1383, 1300 ½mðNO3�Þ�. MS (L-SIMS, m/z): 597 [CoL]+,
659 [CoL(NO3)]+. KM/X�1 cm2 mol�1 (in DMF): 180
(2:1). Colour: violet.
2.6. [CoL](ClO4)2 Æ 4H2O (2)
Anal. Calc. for C30H46N10O12Cl2Co (MW: 868.6): C,
41.5; H, 5.3; N, 16.1. Found: C, 41.1; H, 5.9; N, 16.8%.
Yield: 47%. IR (KBr, cm�1): 1609, 1583, 1456 [m(C@N)pyand m(C@C)], 2252 [m(C„ N)], 1100, 627 ½mðClO4
�Þ�. MS
(L-SIMS, m/z): 597 [CoL]+, 697 [CoL(ClO4)]+.
KM/X�1 cm2 mol�1 (in DMF): 153 (2:1). Colour: blue.
2.7. [NiL](NO3)2 (3)
Anal. calc. for C30H38N12O6Ni (MW: 721.4): C, 49.9;
H, 5.3; N, 23.3. Found: C, 49.5; H, 5.3; N, 23.1%. Yield:
65%. IR (KBr, cm�1): 1609, 1581, 1476 [m(C@N)py and
m(C@C)], 2426, 2250 [m(C„N)], 1454, 1384, 1343
½mðNO3�Þ�. MS (L-SIMS, m/z): 596 [NiL]+, 658 [NiL
(NO3)]+. KM/X�1 cm2 mol�1 (in DMF): 133 (2:1). Col-
our: blue.
2.8. [NiL](ClO4)2 Æ CH3CN Æ 3H2O (4)
Anal. Calc. for C32H47N11O11Cl2Ni (MW: 891.4): C,
43.1; H, 5.3; N, 17.3. Found: C, 43.1; H, 5.0; N, 17.2%.
Yield: 55%. IR (KBr, cm�1): 1610, 1582, 1475 [m(C@N)pyand m(C@C)], 2253 [m(C„N)], 1089, 625 ½mðClO4
�Þ�. MS
(L-SIMS, mz): 596 [NiL]+, 695 [NiL(ClO4)]+. KM/
X�1 cm2 mol�1 (in DMF): 161 (2:1). Colour: blue.
2.9. [CuL][Cu(NO3)3(H2O)2] Æ (NO3) Æ H2O (5)
Anal. Calc. for C30H44N14O15Cu2 (MW: 967.9): C,
37.2; H, 4.6; N, 20.3. Found: C, 37.6; H, 4.5; N,20.3%. Yield: 46%. IR (KBr, cm�1): 1616, 1579, 1474
[m(C@N)py and m(C@C)], 2426, 2251 [m(C„ N)], 1446,
1383, 1350 ½mðNO3�Þ�. MS (L-SIMS, m/z): 601 [CuL]+.
KM/X�1 cm2 mol�1 (in DMF): 172 (2:1). Colour: green.
2.10. [CuL](ClO4)2 Æ 2CH3CN (6)
Anal. Calc. for C34H44N11O8Cl2Cu (MW: 869.2): C,47.0; H, 5.1; N, 17.7. Found: C, 46.9; H, 5.0; N,
17.9%. Yield: 62%. IR (KBr, cm�1): 1617, 1579, 1475
[m(C@N)py and m(C@C)], 2250 [m(C„N)], 1120, 627
½mðClO4�Þ�. MS (L-SIMS, m/z): 601 [CuL]+. KM/
X�1 cm2 mol�1 (in DMF): 160 (2:1). Colour: green.
2.11. X-ray crystallographic study
Slow recrystallization from acetonitrile or water gave
crystals of [CoL][Co(NO3)4] Æ CH3CN (1), [NiL](NO3)2(3), [NiL](ClO4)2 Æ CH3CN Æ 3H2O (4), [CuL][Cu(NO3)3(H2O)2] Æ (NO3) Æ H2O (5) and [CuL](ClO4)2 Æ 2CH3CN
(6) suitable for X-ray diffraction. The details of the
X-ray crystal data, and the structure solution and refine-
ment for all complexes are given in Table 1. Measure-
ments were made on a Bruker SMART CCD 1000 areadiffractometer. All data were corrected for Lorentz and
polarization effects. Empirical absorption corrections
were also applied for all the crystal structures obtained
[13]. Complex scattering factors were taken from the pro-
gram package SHELXTL [14]. The structures were solved
by direct methods, which revealed the position of all
non-hydrogen atoms. All the structures were refined on
F2 by a full-matrix least-squares procedure using aniso-tropic displacement parameters for all non-hydrogen
atoms. The hydrogen atoms were located in their calcu-
lated positions and refined using a riding model. Molec-
ular graphics were generated using ORTEP-3 [15]. The
free nitrate and perchlorate ions present in 3, 4, 5 and
6 were refined with no disorder, giving bond distances
and angles typical for those ions.
3. Results and discussion
The macrocyclic ligand L1 was prepared by barium-
template condensation of ethylenediamine and 2,6-dif-
ormylpyridine followed by reduction with NaBH4 as
reported previously [11]. The tetracyanoethylated mac-
rocycle L was obtained by reaction of L1 with acryloni-trile under reflux for 24 h. The ligand L was isolated as
an air-stable white solid in 75% yield and was character-
ized by elemental analysis, FAB MS, IR and 1H NMR
spectroscopy. The infrared spectrum (KBr disc) of L
contains a strong band at 2245 cm�1 attributable to
m(C„N), a feature that supports the formation of the
tetracyanoethylated macrocycle. The other absorption
bands corresponding to m(C@N) and m(C@C) vibrationsfrom the pyridine groups appear in their expected posi-
tions at 1594 and 1457 cm�1, respectively.
2622 L. Valencia et al. / Inorganica Chimica Acta 358 (2005) 2618–2628
The FAB MS of L shows the parent peak at m/z 539,
further confirming the presence of the ligand. The 1H
NMR spectrum of L was recorded in deuterated aceto-
nitrile and confirms the integrity of the ligand and its
stability in solution. The spectrum shows that the four
quadrants of the macrocyclic ligand are chemicallyequivalent, as one would expect with this kind of system.
The pyridine hydrogens exhibit the expected triplet and
doublet splitting patterns and the chemical shifts are
also consistent with the proposed structure. Two singlets
appear in the aliphatic region of the spectrum and these
Fig. 1. (a) Crystal structure of the ligand L; (b) Packing of ligand L along the
along the a axis of the crystal.
correspond to Py–CH2–N and N–CH2–CH2–N at 3.58
and 2.53 ppm, respectively. The two triplets observed
at 2.46 and 2.84 ppm are attributable to the ethylenic
fragment of the pendants.
Recrystallization of L from acetonitrile yielded crys-
tals that were suitable for X-ray diffraction. The crystal-lographic summary is given in Table 1 and the molecular
structure is shown in Fig. 1(a). The crystal belongs to the
monoclinic space group P21/c. Bond lengths and angles
determined for the structure fall within the normal
ranges. The pyridine rings of the macrocyclic backbone
b axis in the crystal lattice to form nanotubes; (c) Chains of L molecules
L. Valencia et al. / Inorganica Chimica Acta 358 (2005) 2618–2628 2623
are parallel and the four amine nitrogen atoms are in a
plane. As in L1, the structure shows a markedly stepped
conformation, with a dihedral angle of 81.48(0.10)�(77.30 for L1) between the plane containing the pyridyl
groups and the plane that contains the four aliphatic
nitrogen atoms. The X-ray structural analysis of Lshows the formation of nanotubes along the b axis of
the crystal (Fig. 1(b)) stabilized by the presence of inter-
molecular p,p-stacking interactions, a situation that also
occurs in L2.
Analysis of the short intermolecular ring–ring inter-
actions in L reveals that side-on p,p-interactions partic-ipate in the molecular recognition process. The ligand L
forms chains along the a axis (Fig. 1c) by intermolecularslipped p,p-stacking interactions between pyridine rings
of adjacent ligands. The distance dc–c has a value of
5.22 A. The planes containing the pyridine rings of
two adjacent molecules lie parallel (a = 0�) and the inter-
planar distance is 3.16 A. The pyridine units are slipped
to a reasonable extent, with a slipping angle (b) (definedby the vector c1–c2 and the normal to the planes con-
taining the pyridine rings) of 52.7�.As far as the molecular recognition processes and
building of crystals are concerned, an intramolecular
p,p-stacking interaction does not exist between the pyr-
idine rings. These rings also lie parallel but the interpla-
nar distance of 4.32 A, with a dc–c value of 5.68 A, is too
high for a p,p-interaction to be considered between them
[16].
The coordination ability of ligand L towards hydratednitrate and perchlorate salts of Co(II), Ni(II) and Cu(II)
was studied. The reaction of L with the metal salts in a
1.5:1 metal-to-ligand ratio in acetonitrile led to the for-
mation of compounds with a 1:1 metal-to-ligand ratio
of the type [ML](X)2 Æ xCH3CN Æ yH2O (X ¼ NO3� or
ClO4�) for all metal salts, except when Co(NO3)2 and
Cu(NO3)2 were used. The microanalysis data suggest a
2:1 metal-to-ligand stoichiometry for the latter com-plexes. The ring size of L is insufficient for the formation
of endomacrocyclic dinuclear metal complexes, but the
presence of the nitrile groups can give rise to unexpected
coordination modes. Nevertheless, the resolution of the
crystal structures of [CoL][Co(NO3)4] Æ CH3CN and
[CuL][Cu(NO3)3(H2O)2] Æ (NO3) Æ H2O reveals the pres-
ence of independent cationic and anionic complexes of
the type [ML]2+ and [M(NO3)n Æ (H2O)m]y� in both cases.
The results of the L-SIMS MS of the complexes pro-
vide important evidence to confirm the 1:1 stoichiometry
of the complexes as they feature peaks attributable in all
cases to the mononuclear species [MLX]+ or [ML]+.
Molar conductivity data were measured at room tem-
perature using DMF as solvent (10�3 M solutions of the
complexes) due to the low solubility of some nitrate
complexes in acetonitrile. The molar conductivity valuesobtained for all complexes lie in the range previously ob-
served for 2:1 electrolytes [17].
4. Structural studies of the complexes
Crystals suitable for X-ray diffraction were obtained
by recrystallization of the products from acetonitrile
for 1, 3 and 6 or water for 4 and 5. The crystallographic
summary is given in Table 1 and selected bond lengthsand angles are given in Table 2. The ORTEP diagrams
are shown in Figs. 2–4 together with the atom notation
scheme adopted.
In all cases, the dication [ML]2+ is present. Each me-
tal ion in [ML]2+ displays a distorted octahedral coordi-
nation environment with the equatorial plane defined by
the four amine nitrogen atoms from the macrocycle. The
axial positions are occupied by the pyridinic nitrogenatoms. The distances Npy–M are shorter than those to
the tertiary amine nitrogen atoms (Nam–M), as one
would expect with this kind of ligand bearing pyridyl
rings in the macrocyclic framework [18]. The angle
Npy–M–Npy is always the closest to 180�.The structure of the ligand in those [ML]2+ ions
shows a �twist-wrap� conformation, where the ligand
wraps round the metal ion by twisting of the pyridylbridgehead units relative to each other. The macrocycle
adopts a helical shape, with an average value for the
rotation angle between pyridine rings of 74� [minimum
value 73.07� for [NiL](ClO4)2 Æ CH3CN Æ 3H2O and
maximum value 74.92� for [NiL](NO3)2]. The angles
Npy–M–Npy show that the macrocycles are not folded.
In all cases, the N atoms of the nitrile groups are not
coordinated to the metal due to their linear nature.Crystals of [CoL][Co(NO3)4] Æ CH3CN (1) also con-
tain the [Co(NO3)4]2� anion and an interstitial acetoni-
trile molecule. [Co(NO3)4]2� (Fig. 4) consists of four
nitrate ions around the Co(II) ion in a distorted trigonal
bipyramidal environment (s = 0.36) [19]. Three nitrate
ions act as monodentate groups, whilst the fourth one
chelates the Co(II) ion and acts as a bidentate group.
[CuL][Cu(NO3)3(H2O)2](NO3).H2O (5) contains themonoanion [Cu(NO3)3(H2O)2]
� (Fig. 4) where the
Cu(II) ion has a regular square pyramidal geometry
(s = 0.04) and is coordinated to three monodentate ni-
trate ions and two water molecules. The axial position
is occupied by one oxygen atom from one nitrate anion
and the equatorial plane defined by the four oxygen
atoms has a r.m.s. value of 0.0367. The distance of the
Cu(2) atom from the O4 coordination plane is 0.0513(0.0029) A, indicating that the metal is barely out of
the plane. The O atom that occupies the axial position
is 2.294(8) A away from the metal and the average value
for the O4–Cu(2) bond distance is 1.97 A, which is typ-
ical for this kind of bond [20,21].
In contrast, the perchlorate ions in complexes 4 and 6
are not coordinated to the metal ion.
Both centroid–centroid and interplanar distances areused as criteria to determine whether a p,p-interactionexists between aromatic rings, with interplanar distances
Table 2
Selected bond lengths and angles at the M(II) atom
[CoL][Co(NO3)4] ÆCH3CN (1)
[NiL]( NO3)2 (3) [NiL](ClO4)2 Æ CH3CN Æ 3H2O (4) [CuL][Cu(NO3)3(H2O)2] Æ (NO3) Æ H2O (5) [CuL](ClO4)2 Æ 2CH3CN (6)
N(1)–Co(1) 2.044(2) N(1)–Ni(1) 2.010(2) N(1)–Ni(1) 2.007(6) N(1)–Cu(1) 1.974(5) N(1)–Cu(1) 1.981(13)
N(2)–Co(1) 2.271(2) N(2)–Ni(1) 2.229(2) N(2)–Ni(1) 2.208(6) N(2)–Cu(1) 2.292(5) N(2)–Cu(1) 2.346(11)
N(3)–Co(1) 2.248(2) N(3)–Ni(1) 2.232(2) N(3)–Ni(1) 2.249(6) N(3)–Cu(1) 2.303(5) N(3)–Cu(1) 2.243(13)
N(4)–Co(1) 2.055(2) N(4)–Ni(1) 2.006(3) N(4)–Ni(1) 1.999(6) N(4)–Cu(1) 1.965(5) N(4)–Cu(1) 1.958(13)
N(5)–Co(1) 2.262(2) N(5)–Ni(1) 2.254(2) N(5)–Ni(1) 2.232(6) N(5)–Cu(1) 2.295(5) N(5)–Cu(1) 2.248(13)
N(6)–Co(1) 2.247(2) N(6)–Ni(1) 2.238(2) N(6)–Ni(1) 2.220(6) N(6)–Cu(1) 2.289(5) N(6)–Cu(1) 2.318(13)
O(1N)–Co(2) 2.033(3) N(4)–Ni(1)–N(1) 179.85(12) N(4)–Ni(1)–N(1) 179.1(3) O(1W)–Cu(2) 1.968(5) N(4)–Cu(1)–N(1) 178.5(5)
O(4N)–Co(2)#1 2.108(3) N(4)–Ni(1)–N(2) 102.28(10) N(4)–Ni(1)–N(2) 102.2(2) O(2W)–Cu(2) 1.977(5) N(4)–Cu(1)–N(3) 78.7(5)
O(8N)–Co(2)#2 2.023(4) N(1)–Ni(1)–N(2) 77.76(10) N(1)–Ni(1)–N(2) 77.9(2) O(6N)–Cu(2) 1.972(5) N(1)–Cu(1)–N(3) 102.6(5)
O(9N)–Co(2)#2 2.366(6) N(4)–Ni(1)–N(3) 77.74(10) N(4)–Ni(1)–N(6) 103.1(2) O(7N)–Cu(2) 1.963(5) N(4)–Cu(1)–N(5) 77.7(5)
O(10N)–Co(2) 2.112(5) N(1)–Ni(1)–N(3) 102.41(10) N(1)–Ni(1)–N(6) 76.9(2) O(10N)–Cu(2) 2.294(8) N(1)–Cu(1)–N(5) 101.0(5)
N(2)–Ni(1)–N(3) 83.22(9) N(2)–Ni(1)–N(6) 154.8(2) N(4)–Cu(1)–N(1) 178.30(19) N(3)–Cu(1)–N(5) 156.4(4)
N(1)–Co(1)–N(4) 177.94(10) N(4)–Ni(1)–N(6) 102.99(9) N(4)–Ni(1)–N(5) 77.9(2) N(4)–Cu(1)–N(6) 101.07(18) N(4)–Cu(1)–N(6) 103.1(5)
N(1)–Co(1)–N(6) 77.26(9) N(1)–Ni(1)–N(6) 76.97(10) N(1)–Ni(1)–N(5) 102.9(2) N(1)–Cu(1)–N(6) 77.92(18) N(1)–Cu(1)–N(6) 77.5(5)
N(4)–Co(1)–N(6) 103.73(9) N(2)–Ni(1)–N(6) 154.72(9) N(2)–Ni(1)–N(5) 102.0(2) N(4)–Cu(1)–N(2) 102.81(18) N(3)–Cu(1)–N(6) 105.5(4)
N(1)–Co(1)–N(3) 104.82(9) N(3)–Ni(1)–N(6) 101.50(9) N(6)–Ni(1)–N(5) 84.1(2) N(1)–Cu(1)–N(2) 78.20(18) N(5)–Cu(1)–N(6) 81.3(5)
N(4)–Co(1)–N(3) 76.78(10) N(4)–Ni(1)–N(5) 77.39(10) N(4)–Ni(1)–N(3) 77.4(2) N(6)–Cu(1)–N(2) 156.12(17) N(4)–Cu(1)–N(2) 101.6(4)
N(6)–Co(1)–N(3) 103.29(9) N(1)–Ni(1)–N(5) 102.46(10) N(1)–Ni(1)–N(3) 101.8(2) N(4)–Cu(1)–N(5) 78.07(17) N(1)–Cu(1)–N(2) 77.8(5)
N(1)–Co(1)–N(5) 102.03(9) N(2)–Ni(1)–N(5) 102.91(9) N(2)–Ni(1)–N(3) 83.1(2) N(1)–Cu(1)–N(5) 103.03(17) N(3)–Cu(1)–N(2) 81.1(4)
N(4)–Co(1)–N(5) 76.38(9) N(3)–Ni(1)–N(5) 155.11(9) N(6)–Ni(1)–N(3) 101.7(2) N(6)–Cu(1)–N(5) 80.30(17) N(5)–Cu(1)–N(2) 102.4(4)
N(6)–Co(1)–N(5) 82.65(9) N(6)–Ni(1)–N(5) 83.32(9) N(5)–Ni(1)–N(3) 155.3(2) N(2)–Cu(1)–N(5) 104.77(17) N(6)–Cu(1)–N(2) 155.2(4)
N(3)–Co(1)–N(5) 153.15(9) N(4)–Cu(1)–N(3) 77.60(17)
N(1)–Co(1)–N(2) 76.54(9) N(1)–Cu(1)–N(3) 101.27(17)
N(4)–Co(1)–N(2) 102.48(10) N(6)–Cu(1)–N(3) 103.77(17)
N(6)–Co(1)–N(2) 153.79(9) N(2)–Cu(1)–N(3) 81.36(17)
N(3)–Co(1)–N(2) 82.87(9) N(5)–Cu(1)–N(3) 155.67(17)
N(5)–Co(1)–N(2) 103.46(9) O(7N)–Cu(2)–O(1W) 92.4(2)
O(8N)#2–Co(2)–O(1N) 111.60(13) O(7N)–Cu(2)–O(6N) 90.2(2)
O(8N)#2–Co(2)–O(4N)#3 120.32(15) O(1W)–Cu(2)–O(6N) 177.2(2)
O(1N)–Co(2)–O(4N)#3 97.78(12) O(7N)–Cu(2)–O(2W) 174.9(2)
O(8N)#2–Co(2)–O(10N) 140.98(18) O(1W)–Cu(2)–O(2W)87.6(2)
O(1N)–Co(2)–O(10N) 94.62(18) O(6N)–Cu(2)–O(2W)89.7(2)
O(4N)#3–Co(2)–O(10N) 81.95(13) O(7N)–Cu(2)–O(10N) 98.2(3)
O(8N)#2–Co(2)–O(9N)#2 55.57(16) O(1W)–Cu(2)–O(10N) 90.3(3)
O(1N)–Co(2)–O(9N)#2 162.87(18) O(6N)–Cu(2)–O(10N) 90.3(3)
O(4N)#3–Co(2)–O(9N)#2 82.06(15) O(2W)–Cu(2)–O(10N) 86.9(3)
O(10N)–Co(2)–O(9N)#2 102.3(2)
2624
L.Valen
ciaet
al./Inorganica
Chim
icaActa
358(2005)2618–2628
Fig. 3. ORTEP drawing of the molecular structure of the dication from 6, [CuL]2+.
Fig. 2. ORTEP drawing of the molecular structure of the dication from 4, [NiL]2+.
L. Valencia et al. / Inorganica Chimica Acta 358 (2005) 2618–2628 2625
in the range 3.3–3.8 A commonly accepted for face to
face stacks of aromatic units with approximately paral-
lel molecular planes [16].
The crystal lattices of the cobalt(II) and nickel(II) ni-
trate complexes 1 and 3 contain nitrate ions that are sit-
uated close to the pyridine rings but are slightly tiltedwith respect to them. In these cases, the dihedral angles
between the planes are 18.09 (0.31)� and 14.76 (0.19)�for 1 and 3, respectively. In the copper(II) nitrate com-
plex 5, the nitrate ions are more tilted with respect to
the pyridine rings than in the other complexes and, in
this case, the dihedral angles are 44.39� and 45.69� [be-tween the nitrate ion of N2ni and the pyridine rings of
N1 and N4 (I = x, y � 1, z)].
Table 3 suggests the possibility of a p,p-stackinginteraction between nitrate ions and pyridine rings inthe crystal structure of complexes 1, 3 and 5.
In this case, we can consider the distance between the
centroid of the pyridine and the N atom of the nitrate
group as analogous to the centroid–centroid distance.
Fig. 4. ORTEP drawing of the molecular structure of: (a) [CoL][Co(NO3)4] Æ CH3CN (1); (b) [NiL](NO3)2 (3); (c) [CuL][Cu(NO3)3(H2O)2]
(NO3) Æ H2O (5), showing the intermolecular atom–atom distances [A] shorter than 3.5 A between nitrate ions and pyridine and nitrile groups.
Table 3
Intermolecular atom–atom distances [A] shorter than 3.5 A for 1, 3
and 5
[CoL][Co(NO3)4] ÆCH3CN (1)
[NiL](NO3)2] (3) [CuL][Cu(NO3)3(H2O)2(NO3) ÆH2O (5)
C11–O11n 3.221 C10–O2n 3.167 C13–O9n 3.247
C14–O12n 3.492 C11–O2n 3.148 N7–O9n 3.175
C13–O12n 3.526 C11–N1n 3.104 C14–O9n 3.346
C10–O11n 3.427 C10–N1n 3.423 N7–N3n 3.393
N10–O11n 3.394 C12–O3n 3.297 C4–O6n_$1 3.0815
N10–O2n 3.443 C2–O4N_$1 3.3764
C30–O2n 3.349 N9–N2N_$1 3.2392
$1 = x, y � 1, z.
2626 L. Valencia et al. / Inorganica Chimica Acta 358 (2005) 2618–2628
]
This distance (dc–N) is 3.6, 3.4 and 3.5 A, respectively.
However, as these two planes are tilted, atom–atom con-
tacts provide a better criterion and supply more suitableinformation about possible contacts between these
groups. In all cases (see Table 3), the intermolecular
atom–atom distances are shorter than the sum of the
van der Waals radii for these atoms [22]. These results
reveal that p,p-interactions exist in these complexes be-
tween nitrate ions and pyridine fragments from the li-
gand L. Although a CSD search reveals that this sort
of p,p-interaction between pyridine rings and nitrateions is present in previously reported structures
L. Valencia et al. / Inorganica Chimica Acta 358 (2005) 2618–2628 2627
[23,24], to the best of our knowledge, it was not previ-
ously described in the literature. Only Sanchez-Moreno
et al. [25] reported nitro-benzyl p,p-interactions in two
mixed Cu(II) complexes with N-(p-nitrobenzyl)iminodi-
acetic acid (NBIDA).
Table 3 also contains some atom–atom distances be-tween the nitrate ions and the nitrile groups on the pen-
dants present in the ligand. These distances are shorter
than the sum of the van der Waals radii for these atoms,
again suggesting an interaction between the nitrate ion
and the p-shell of the nitrile pendant group, which has
not been described either in the literature, although a
new CSD search reveals the existence of that in some
deposited crystal structures [26].
5. Spectroscopic and magnetic studies
The IR spectra of the complexes were recorded using
KBr discs. The spectra exhibit medium to strong bands
at ca. 1610, 1580 and 1470 cm�1, as expected for the
m(C@C) and m(C@N) pyridine ring vibrations. Thesebands are shifted to higher wavenumbers when com-
pared to those in the free ligand, suggesting coordina-
tion to the metal atom [27,28].
Perchlorate complexes exhibit a medium intensity
band in the region 2248–2253 cm�1 and this is attributed
to the m(C„N) mode of the pendant groups. These
bands are in the same position as in the free ligand L
spectrum, indicating that coordination of the nitrilegroups to the metal does not occur. On the other hand,
the IR spectra of the nitrate complexes show in all cases
two equal intensity bands at 2251 and 2426 cm�1. The
2251 cm�1 band is similar to the free ligand vibration
(2245 cm�1). However, the presence of the second band
(2426 cm�1) is surprising given that the crystal struc-
tures do not show any interaction between the nitrile
groups and the metal ions. The presence of this secondband only in the nitrate complexes is consistent with
the p,p-interaction shown in the solid state structure
of the nitrate complexes between those counterions
and the nitrile groups. The crystal structures of 1, 3
and 5 reveal the presence of a p,p-interaction between
the nitrate ions and the pyridine rings. These nitrate ions
were in all complexes in a middle position between the
pyridine ring and one nitrile pendant group, a situationthat could even give rise to an interaction between these
three p-systems. The shortest atom–atom distances are
reported in Table 3.
The IR spectra of the perchlorate complexes feature
absorptions attributable to ionic perchlorate at
1100 cm�1. The lack of splitting of this band indicates
that these groups are not coordinated to the metal cen-
tres [29,30]. However, the IR spectra of the nitrate com-plexes show the presence of several bands in the region
associated with nitrate vibrations, indicating the pres-
ence of coordinated nitrate groups. In addition, all spec-
tra show the presence of the vibration associated with
ionic nitrate groups at 1383 cm�1 [31].
The solid state electronic spectra were obtained at
room temperature for all complexes. The reflectance
spectrum of [CoL](ClO4)2 Æ 4H2O (2) shows two d–dtransition bands at ca. 10838 and 16666 cm�1, which
are due to the 4T2g 4T1g and4T1g(P) 4T1g(F) transi-
tions, respectively, and are of the type expected for dis-
torted octahedral high spin Co(II) complexes [32]. In the
case of [CoL][Co(NO3)4] Æ CH3CN (1), the spectrum is
complicated and shows five bands at 8636, 15300,
18000, 19685 and 21552 cm�1. These bands must be
attributable to the presence of both octahedral and a tri-gonal bipyramidal arrangement for the Co(II) ions [33].
The reflectance spectra of the nickel complexes
[NiL](NO3)2 (3) and [NiL](ClO4)2 Æ CH3CN Æ 3H2O (4)
show three bands at ca. 10415, 17540 and
31250 cm�1. These bands are attributable to the3T2g 3A2g,
3T1g(F) 3A2g and3T1g(P) 3A2g tran-
sitions, respectively, and are indicative of octahedral
Ni(II) compounds. One absorption band at ca.15150 cm�1is also present and is probably due to the
spin forbidden transition 1Eg 3A2g usually observed
in Ni(II) complexes [34].
The X-ray structure of [CuL][Cu(NO3)3(H2O)2] Æ(NO3) Æ H2O (5) shows two metal ions having different
coordination numbers and geometries. In [CuL]
(ClO4)2 Æ 2CH3CN (6), the solid state structure shows a
mononuclear complex in a distorted octahedral environ-ment, but no difference was found in the solid state UV–
vis spectra of these two complexes. The UV spectra
show a broad band with a maximum at 13570 cm�1and
a shoulder at 7350 cm�1, which are typical of octahedral
Cu(II) complexes [35].
The values of the room temperature magnetic mo-
ments of the compounds [CoL](ClO4)2 Æ 4H2O (4.8
BM), [NiL](NO3)2(2.9 BM), [NiL](ClO4)2 Æ CH3CN Æ3H2O (2.8 BM) and [CuL](ClO4)2 Æ 2CH3CN (1.8 BM)
lie within the range usually observed for high-spin octa-
hedral Co(II), and octahedral Ni(II) and Cu(II) com-
plexes. The magnetic moment values obtained for
[CoL][Co(NO3)4] Æ CH3CN and [CuL][Cu(NO3)3(H2O)2] Æ (NO3) Æ H2O are 8.3 and 3.4 BM, respectively.
These values are consistent with the presence of high
spin octahedral and pentacoordinated Co(II) and Cu(II)ions [36].
6. Conclusion
The new macrocyclic ligand L, which contains two
pyridine rings in the ligand skeleton and bears four
cyanoethyl pendant groups, has been synthesized byreaction of the precursor L1 with acrylonitrile. In the
solid state, L presents a nanotubular structure arranged
2628 L. Valencia et al. / Inorganica Chimica Acta 358 (2005) 2618–2628
by p,p-stacking interactions between the pyridine
groups. The complexation capacity of the ligand L to-
ward a range of first row transition metals has been stud-
ied. The crystal structures of [CoL][Co(NO3)4] Æ CH3CN
(1), [NiL](NO3)2 (3), [NiL] (ClO4)2 Æ CH3CN.3H2O (4),
[CuL][Cu(NO3)3(H2O)2] (NO3) Æ H2O (5) and [CuL](ClO4)2 Æ 2CH3CN (6) were determined, and in all cases
the dication [ML]2+ is present. The X-ray structure of
the nitrate complexes reveals a new and unexpected
simultaneous p,p-interactions between a pyridine ring,
a nitrate ion and a nitrile group.
7. Supplementary material
Crystallographic data (excluding structure factors) for
the structures reported in this paper have been deposited
with the Cambridge Crystallographic Data Centre as
supplementary publication: CCDC 234001 for L, CCDC
234002 for [CoL][Co(NO3)4] Æ CH3CN, CCDC 234003
for [NiL](NO3)2, CCDC 234004 for [NiL](ClO4)2 ÆCH3CN Æ 3H2O, CCDC 234005 for [CuL][Cu(NO3)3-(H2O)2](NO3) Æ H2O and CCDC 234006 for [CuL]-
(ClO4)2 Æ 2CH3CN. Copies of the data can be obtained
free of charge on application to the Cambridge Crystal-
lographic Data Centre, 12 Union Road, Cambridge CB2
IEZ, UK [fax: (internat.) +44 (0)1223 336033; e-mail:
Acknowledgements
We thank Xunta de Galicia (PGIDT01PXI20901PR)
for financial support. Intensity measurements were per-
formed at the Unidade de Raios X. RIAIDT. University
of Santiago de Compostela, SPAIN.
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