3204
K. Takano et al. / Inorganica Chimica Acta 362 (2009) 3201–3207
The reaction of VCl3 with Hqn in acetonitrile–water or acetoni-
3.2. X-ray structures
trile–concentrated HCl gives mononuclear V(IV) species 1, which
turns to dinuclear V(IV) species 2, when coordination of qnꢁ oc-
curs. Smaller amounts of water and higher acidity retard the reac-
tion rate from 1 to 2. Probably deprotonation of H2qn+ is one of the
important processes. 1 ꢀ 2H2qn ꢀ 2Cl ꢀ CH3CN is very hygroscopic
and becomes liquefied within a few seconds when the crystals
are taken out of the mother liquid in the air, and therefore the com-
position is according to that determined by X-ray crystallography.
Electronic spectral change of 1 to 2 was observed by dissolving
1 ꢀ 2H2qn ꢀ 2Cl ꢀ CH3CN in acetonitrile under dinitrogen atmo-
sphere (Fig. 1). Further oxidation of 2 proceeds to give V(V) species
in the air (Fig. 2), but the rate is low and any air-free technique is
required to obtain crystals of 2.
Addition of propanol or butanol in the synthesis of 2 ꢀ Hqn
results in the formation of alcohol-coordinated species
[V2O2Cl2(qn)2(ROH)2] (R = C3H7, 3; C4H9, 4), respectively, which
are air-oxidized to give V(V) species much more easily than the
water-coordinated complex 2, and a mild air-free condition is re-
quired for the isolation of 3 and 4; leaving the solution containing
the crystals of iso-propanol-coordinated species 3 for a few days
longer causes resolution of the deposited crystals and change of
color of the solution from pale-green to dark red. This indicates
the formation of V(V) complex [3–5]. The use of HClqn (5, 6, 7,
and 8) or HFqn (9 and 10) instead of Hqn gave respective
complexes.
ORTEP drawings of 1 ꢀ 2H2qn ꢀ 2Cl ꢀ CH3CN, 3, 4, 6, 7, 8, and 10
are shown in Fig. 3. Atomic distances are listed in Tables 3 and
4, respectively. Fig. 3a. 1 ꢀ 2H2qn ꢀ 2Cl ꢀ CH3CN shows that
a
crystallographic mirror plane passes through V1, O1, O2, O3,
C21, C22, N21, and H221. A feature of this compound is that
coordination of Hqn to vanadium does not occur; however, pro-
tonation to Hqn occurs to give H2qn+, which is linked to [VOCl2-
(H2O)] through hydrogen bonding: H10ꢀ ꢀ ꢀCl2, 2.32 Å; Cl2ꢀ ꢀ ꢀH2,
2.15 Å.
X-ray structures of five compounds containing the mononuclear
vanadium complex, [VOCl2(H2O)] (1), have been reported so far:
1 ꢀ 2Et2O [16], 1 ꢀ 15-crown-5 [17], 1 ꢀ benzo-15-crown-5 [17],
1 ꢀ 18-crown-6 [18], and 1 ꢀ 2C10H10N3 ꢀ Cl2 (C10H10N3 = bis{2-
(2-pyridylamino)pyridinium}) [23], where diethyl ethers (in the
former four complexes) connect 1’s through hydrogen bonding,
which cause interaction between the complexes. The dimensions
of 1 in 1 ꢀ 2H2qn ꢀ 2Cl ꢀ CH3CN are not so different from those of
the reported complexes (see Table 4).
Complexes 3, 4, 6, 7, 8, and 10 are dimeric species having four
membered anti-coplanar (V–O)2 rings. Possible structures of
[VO(l
-OR)2VO]2+ are shown in (Chart 3). Crystallographic (4, 7,
and 8) or pseudo crystallographic (3, 6, and 10) centers of symme-
try reside on the centers of the rings. The V–O distances trans to
the terminal oxo ligands are substantially longer than those cis
to the terminal oxo ligands (Table 3) due to V@O trans effect.
The V–V distances will be discussed in the magnetic properties sec-
tion below.
Electronic spectral data of 1–10 are shown in Table 2. Electronic
spectral change of 1 to 2 was observed by means of dissolving
1 ꢀ 2H2qn ꢀ 2Cl ꢀ CH3CN in acetonitrile under dinitrogen atmo-
sphere (Fig. 1); coordination of 8-quinolinol (Hqn) to 1 gives 2,
which accompanies the peak shift from 720 to 670 nm. Further
electronic spectral change indicates slow air oxidation of 2 ꢀ Hqn
to give V(V) species in acetonitrile (Fig. 2).
3.3. Magnetic properties
The magnetic data of 3, 4, 6, 7, and 10 were treated by applying
the Bleaney–Bowers equation [24] (Eq. (1)), calculated for two
S = 1/2 centers under a 2JS1 ꢂ S2 spin Hamiltonian, using a non-
linear least-squares fitting routine (N
a
, 0.0001).
1.0
0.8
0.6
0.4
0.2
0
ꢀ
ꢁ
2Ng2b2
kT
1
vM
¼
þ N
a;
where x ¼ expðꢁJ=kTÞ
ð1Þ
3 þ x2
The results are summarized in Table 5. The compounds in solid
state are experiencing a very weak antiferromagnetic interaction
between the metal centers, and the effective magnetic moments
are close to spin only value (2.44) of the d1–d1 system. Fig. 4 shows
temperature dependence of magnetic susceptibility of 3. ESR spec-
trum of 3 at 270 K in THF and its simulation (Fig. 5) indicate that
the dimeric species 3 dissociates to give monomeric species; the
g value (2.03) obtained in the solution differs distinctly from that
obtained in solid state (Table 5).
Much discussion has focused on the magnetic properties of
dinuclear oxo-vanadium complexes, and it is suggested that me-
tal–metal interactions of complexes with syn-orthogonal, syn-
coplanar, and twist structures are strong, while those of complexes
with anti-coplanar ones are weak [11,12,13]. The complexes 3, 4, 6,
7, and 10 are of anti-coplanar structure, and the above discussion is
well applied.
400
600
800
1000
Wavelength/nm
Fig. 2. Electronic spectral change in the course of the air oxidation of 2 ꢀ Hqn in
acetonitrile (every 30 min).
Table 2
Electronic spectral data of 1–10 in acetonitrile.
Compound
kmax,
(e )
/Mꢁ1 cmꢁ1
nm
4. Conclusion
1 ꢀ 2H2qn ꢀ 2Cl ꢀ CH3CN
355 (6220), 720 (40.4)
372 (5560), 670 (108)
375 (4570), 672 (103)
393 (5960), 675 (113)
375 (4590), 673 (99.3)
390 (5660), 671 (97.5)
401 (6210), 679 (120)
374 (4550), 670 (105)
380 (5490), 672 (98.0)
2
Reaction of vanadium(III) chloride with 8-quinolinol (Hqn) gave
a mononuclear vanadium(IV) complex, 1 ꢀ 2H2qn ꢀ 2Cl ꢀ CH3CN, and
three dinuclear vanadium(IV) complexes: 2 ꢀ Hqn, 3, and 4. Reac-
tion of vanadium(III) chloride with 5-chloro-8-quinolinol (HClqn)
gave four dinuclear vanadium(IV) complexes: 5 ꢀ 2HClqn, 6,
7, and 8 ꢀ 2 t-BuOH. Reaction of vanadium(III) chloride with 5-flu-
oro-8-quinolinol (HFqn) gave two dinuclear vanadium(IV)
3
4
6
7
8 ꢀ 2C4H9OH
9
10