3906 Inorganic Chemistry, Vol. 38, No. 17, 1999
Catalan et al.
precipitated from solution by the addition of Et2O (5 mL); single crystals
were grown from a mixture of CH3CN/C6H5CH3. H NMR at 25 °C
X-ray crystallographic data for compounds 1 and 7 were collected on
a Siemens SMART diffractometer at -100 ( 1 °C with graphite
monochromated Mo ΚR (λR ) 0.710 73 Å) radiation and were corrected
for Lorentz and polarization effects. Calculations were performed on a
Silicon Graphics computer. The frames were integrated with the
Siemens SAINT software package, and the data were corrected for
absorption using the SADABS program.10 The structures of 1 and 7
were solved by direct methods using the SHELXS program in the
Bruker SHELXTL v. 5.05 software and11a refined by full-matrix least-
squares calculations on F 2 using the SHELXL-97 program.11b All
relevant crystallographic values and other pertinent information for
compounds 1, 5, 6, and 7 are listed in Tables 1-7.
1
(CD3CN) δ 1.25 (t, CH3), 1.95 (s, CH3CN), 2.25 (s, CH3), 2.33 (s,
CH3), 3.98-4.11 (m, CH2), 6.46 (d, tolyl), 6.76 (d, tolyl), 7.02 (d, tolyl),
7.09 (d, tolyl), 7.26 (s, NCHN), 7.68 (s, H2), 8.06 (s, H8), 8.63 (s,
1
H6). H NMR at -32 °C (CD3CN) δ 1.28 (t, CH3), 1.95 (s, CH3CN),
2.13 (s, H2O), 2.23 (s, CH3), 4.08 (m, CH2), 6.36 (d, tolyl), 6.46 (s,
H6), 6.78 (d, tolyl), 6.96 (d, tolyl), 6.99 (d, tolyl), 7.65 (t, NCHN),
1
7.68 (s, H2), 8.04 (s, H8). H NMR at 25 °C (acetone-d6) δ 1.30 (t,
CH3-9-EtAH), 1.88 (s, ax-CH3CN), 2.14 (s, H2O), 2.24 (s, CH3, tolyl),
4.15-4.19 (m, CH2-9-EtAH), 6.71 (d, tolyl), 6.86 (d, tolyl), 7.06 (d,
tolyl), 7.12 (d, tolyl), 7.73 (s, NCHN), 7.94 (s, H2), 8.63 (s, H8), 11.35
(s, H6). 1H NMR at -41 °C (acetone-d6) δ 1.27 (t, CH2-9-EtAH), 1.84
(s, ax-CH3CN), 2.13 (s, CH3, tolyl), 2.20 (s, CH3, tolyl), 4.17 (m, CH2-
9-EtAH), 6.76 (d, H6), 6.88 (d, tolyl), 7.03 (d, tolyl), 7.11 (d, tolyl),
7.20 (s, H1), 7.71 (s, NCHN), 7.99 (d, H2), 8.73 (s, H8), 11.57 (s,
H6).
Rh2(DTolF)2(O2CCF3)2(CH3CN)2 (1). An orange-red rectangular
platelet of dimensions 0.11 × 0.31 × 0.10 mm was selected from a
batch of crystals obtained from the evaporation of an acetonitrile
solution of the compound and mounted on the tip of a glass fiber with
Dow Corning grease. Indexing and refinement of 59 reflections selected
from a total of 45 frames with an exposure time of 10 s/frame gave
unit cell parameters for a monoclinic unit cell. A total of 1321 frames
were collected with a scan width of 0.3° in ω and an exposure time of
30 s/frame. The total data collection time was 13.5 h. The integration
of the frame data using a monoclinic B-centered unit cell yielded a
total of 25 160 reflections in the range h ) 14 f -14, k ) 27 f -28,
l ) 23 f -15 with a maximum 2θ angle of 56.78°. Of the 10 101
unique reflections, a total of 3761 reflections remained with I > 2σ(I)
and Rint ) 0.1116 and Rsig ) 0.1390 after data reduction. The positions
of all of the non-hydrogen atoms were located by direct methods and
refined anisotropically. Hydrogen atoms were calculated at fixed
positions. Final refinement of 506 parameters and 31 restraints gave
residuals of R1 ) 0.0451 and wR2 ) 0.0904. The goodness-of-fit was
0.717 with the maximum and minimum peak heights in the final
difference Fourier map being 0.649 and -0.994 e/Å3, respectively.
[Rh2(DTolF)2(CH3CN)6][BF4]2 (5). Large single crystals were
obtained from the slow diffusion of a concentrated acetonitrile solution
of the compound into toluene. The crystals grew as long orange-red
rectangles at the interface of the two solvents after 12 days. A suitable
single crystal, with the approximate dimensions 0.78 × 0.26 × 0.21
mm, was mounted on the tip of a glass fiber with Dow Corning grease
and cooled in a liquid nitrogen stream. Cell constants for an orthor-
hombic unit cell were obtained from a least squares refinement using
24 carefully centered reflections in the range 29 < 2θ < 37°. The
reflection data were collected in the range 4 e 2θ e 47°, by using the
ω scan method. Weak reflections (those with F < 10σ(F)) were
rescanned a maximum of 3 times, and the counts were accumulated to
ensure good counting statistics. Of the 8005 reflections which were
[Rh2(DTolF)2(9-EtGH)2(CH3CN)][BF4]2 (7). (a) A quantity of
9-ethylguanine (41.7 mg, 0.233 mmol) was added to a stirring solution
of [Rh2(DTolF)2(CH3CN)6][BF4]2 (115.4 mg, 0.116 mmol) dissolved
in 5 mL of CH3OH and 10 mL of CH3CN. The mixture was gently
refluxed for ∼2 h, during which time the orange-red mixture with the
suspended 9-ethylguanine became a clear green solution. The reaction
mixture was filtered, and the filtrate was evaporated in vacuo to yield
a green solid (60 mg, 47% yield).
(b) The aforementioned reaction was repeated in an acetonitrile/
acetone solvent mixture. Two equivalents of 9-EtGH (46 mg, 0.0257
mmol) were added to a solution of acetonitrile/acetone (5 mL/1 mL)
of 5 (138.5 mg, 0.0129 mmol). The mixture was stirred at constant
reflux for ∼3 h, filtered in air through a Celite plug, and finally reduced
1
to dryness in vacuo (110 mg, 78% yield). H NMR (CD3OD) δ 1.36
(t, CH3), 1.40 (t, CH3), 1.92 (s, CH3CN), 2.23 (s, CH3), 3.98 (q, CH2),
4.05 (q, CH2), 6.80 (m, tolyl), 6.89 (m, tolyl), 7.00 (m, tolyl), 7.50 (t,
NCHN), 7.55 (t, NCHN), 8.32, 8.35 (s, H8).
Physical Measurements. Infrared spectra were collected on a Nicolet
740 FT-IR spectrophotometer. All 1H NMR spectroscopic data including
the 2-dimensional experiments were collected on a either a 300 or a
500 MHz Varian spectrometer. Chemical shifts were referenced relative
to the residual proton impurities of the solvents used. Electrochemical
measurements were performed by using an EG&G Princeton Applied
Research model 362 scanning potentiostat in conjunction with a Soltec
model VP-6424S X-Y recorder. The cyclic voltammetric experiments
for compound 5 were carried out at r.t. in acetonitrile containing 0.1
M tetra-n-butylammonium hexafluorophosphate, TBAPF6, as supporting
electrolyte, while the experiments for 6 and 7 were performed with
0.1 M tetra-n-butylammonium tetrafluoroborate, TBABF4, as the
supporting electrolyte. E1/2 values, determined as (Ep,a + Ep,c)/2, were
referenced to the Ag/AgCl electrode without correction for junction
collected, 3865 reflections with Fo > 3σ(Fo)2 were used in the
2
measurement. Periodic measurement of three representative reflections
at regular intervals revealed that no loss of diffraction intensity had
occurred during data collection. An empirical absorption correction was
applied on the basis of azimuthal scans of 3 reflections with ø near
90°. The space group was determined to be Pbca on the basis of the
observed systematic absences. The positions of all non-hydrogen atoms
were obtained by the application of the direct methods programs
MITHRIL and DIRDIF followed by successive full-matrix least-squares
cycles9 and refined with anisotropic thermal parameters. Hydrogen
atoms were treated as fixed contributors at idealized positions and were
not refined. Final least-squares refinement of 567 parameters resulted
in residuals of R ) 0.046 and Rw ) 0.063 and a goodness-of-fit )
2.01. A final difference Fourier map revealed the highest peak to be
0.87 e-/Å3.
[Rh2(DTolF)2(9-EtAH)2(CH3CN)](BF4)2 (6). Single X-ray quality
crystals of 6 were grown from the slow diffusion of an acetonitrile
solution of 6 into toluene. A green rectangular crystal of approximate
dimensions of 0.31 × 0.23 × 0.18 mm was mounted on the tip of a
glass fiber with Dow Corning grease. Cell constants for the monoclinic
space group P21/c were obtained from a least-squares refinement of
potentials. The Cp2Fe/Cp2Fe+ couple occurs at E1/2 ) +0.46 V, E1/2
)
+0.53 V, and E1/2 ) +0.45 V for the cyclic voltammograms of
compounds 5, 6, and 7, respectively, under the same experimental
conditions in acetonitrile.
X-ray Crystallography and Structure Solution. Geometric and
intensity data for compound 5 were collected on a Rigaku AFC6S
diffractometer at -100 ( 1 °C. A hemisphere of crystallographic data
for compound 6 was collected at -100 ( 1 °C on a Nicolet P3/V
diffractometer upgraded to a Siemens P3/F with graphite-monochro-
mated Mo KR (λR ) 0.710 73 Å) radiation; the reflections were
corrected for Lorentz and polarization effects. All calculations for the
structure solution and the refinement of compounds 5 and 6 were
performed with Silicon Graphics computers on a cluster network in
the Department of Chemistry at Michigan State University using the
Texsan software package of the Molecular Structure Corporation.9 The
(9) (a) TEXSAN-TEXRAY Structure Analysis Package; Molecular Struc-
ture Corporation: The Woodlands, TX, 1985. (b) MITHRIL: Inte-
grated Direct Methods Computer Program, Gilmore, C. J. J. Appl.
Crystallogr. 1984, 17, 42. (c) P. T. DIRDIF: Direct Methods for
Difference Structures, An Automatic Procedure for Phase Extension;
Refinement of Difference Structure Factors; Beurskens, Technical
Report, 1984.
(10) SAINT & SADABS programs in the SHELXTL software, Bruker
AXS, Inc., Analytical X-ray Systems.
(11) (a) Sheldrick, G. SHELXS-97; University of Go¨ttingen: Go¨ttingen,
1990. (b) Sheldrick, G. SHELXL-97; 1997.