220
T. Ruman et al. / Polyhedron 23 (2004) 219–223
addition of 120 mg of NaTp00 dissolved in toluene into
the equimolar amounts of [(COD)RhCl)]2 [14] or
[(NBD)RhCl)]2 [15] in toluene. The reaction mixtures
were stirred at room temperature for 4 h under atmo-
sphere of nitrogen, filtrated by passing through short bed
of celite, the solvent was partially removed, the solutions
layered with heptane and allowed to stand at 4 °C until
formation of yellow crystals of 1 (yield 85%) or 2 (yield
80%).
Table 1
Crystal data and structure refinement
Empirical formula
Formula weight
T (K)
C36H42BN6Rh
672.48
100(2)
0.71073
ꢁ
k (A)
Crystal system
Space group
triclinic
ꢂ
P1
ꢁ
a (A)
12.197(2)
15.876(3)
17.120(3)
102.42(3)
102.73(3)
90.88(3)
3151.1(10)
4
ꢁ
b (A)
ꢁ
c (A)
a (°)
b (°)
c (°)
2.2. Analytical data
3
ꢁ
V (A )
1: Elemental analysis: Calc. for C36H42N6BRh (MW
672.48): C, 64.30; H, 6.29; N, 12.50. Found: C, 64.55; H,
6.16; N, 12.43%.
1H NMR (toluene-d8, 298 K): 8.01 (4H, m, o-H(3-Ph));
7.25 (4H, m, m-H(3-Ph)); 7.16 (2H, m, p-H(3-Ph)); 6.31
(2H, s, 4-H(3-Ph,5-iPrpz)); 5.58 (1H, s, 4-H(3,5-diMepz));
3.33 (6H, septet + broad singlet, CH(5-iPr) + 20, 30, 50, 60-
H(NBD)); 2.94 (2H, s, 10, 40 –H(NBD)); 2.31 (3H, s, 3(5)-
Z
Dcalc (Mg mꢁ3
)
1.418
0.578
l (mmꢁ1
F ð000Þ
)
1400
0.17 ꢀ 0.15 ꢀ 0.15
Crystal size (mm)
h Range for data collection (°) 3.43–28.41
Ranges of h, k, l
)15 to 16, )20 to 20, )22 to 21
21 925
Reflections collected
Independent reflections
Data/parameters
13 848 (0.0561)
13 848/806
0.952
CH3); 2.14 (3H, s, 5(3)-CH3); 1.29 (6H, d, J
Hz, 2ꢀCH3(5-iPr)); 1.21(6H, d, J
¼ 6:6
ðCH3–CHÞ
ðCH3–CHÞ
Goodness-of-fit (F 2)
Final R1=wR2 indices
(I > 2rðIÞ)
¼ 6:6 Hz,
2ꢀCH3(5-iPr)); 0.59 (2H, s, 70-H(NBD)).
0.0549/0.0738
IR (KBr): m(BH) 2534, 2474 cmꢁ1
.
Extinction coefficient
Largest diffraction peak/hole
0.00015(10)
0.569/)0.734
2: Elemental analysis: Calc. for C37H46N6BRh (MW
688.53): C, 64.54; H, 6.73; N, 12.21. Found: C, 64.62; H,
6.86; N, 12.13%.
ꢁ3
ꢁ
(e A
)
1H NMR (toluene-d8, 273 K): 8.10 (4H, m, o-H(3-
Ph)); 7.25 (4H, m, m-H(3-Ph)); 7.10 (2H, m, p-H(3-Ph));
6.45 (2H, s, 4-H(3-Ph,5-iPrpz)); 5.56 (1H, s, 4-H(3,5-
diMepz)); 4.10 (4H, s, 10, 20, 50, 60-H(COD)); 3.19 (2H,
septet, CH(5-iPr)), 2.34 (3H, s, 5-CH3); 2.22 (3H, s, 3-
CH3); 1.87 (4H, s, 30, 40, 70, 80-Hexo (COD)); 1.39 (6H, d,
the Oxford Diffraction (Poland) Sp. z o.o (formerly
Kuma Diffraction Wrocław, Poland) programs. The
structure was solved by direct methods (program
SHELXS-97 [17]) and refined by the full-matrix least-
squares method on all F 2 data using the SHELXL-97 [17]
programs. Non-hydrogen atoms were refined with an-
isotropic displacement parameters; hydrogen atoms
were included from geometry of molecules and Dq maps.
During refinement they were fixed.
J
J
) ¼ 6.6 Hz, 2ꢀCH3(5-iPr)); 1.20 (10H, d,
ðCH3–CHÞ
ðCH3–CHÞ
) ¼ 6.6 Hz, 2ꢀCH3(5-iPr) + overlapped s, 30, 40,
70, 80-Hendo (COD)).
IR (KBr): m(BH) 2478 cmꢁ1
.
2.3. Methods
3. Results and discussion
The 1H NMR spectra were recorded with Bruker
AMX 300 spectrometer. Standard COSY and NOESY
experiments were performed with repetition time 1.0 and
mixing time 0.3 s (NOESY).
The heteroscorpionate ligand used in these studies,
composed of two 3-phenyl-5-isopropylpyrazolyl and 3,5-
dimethylpyrazolyl residues ([HB(3-Ph,5-iPrpz)2(3,5-
diMepz)]ꢁ) is more sterically demanding in comparison
with homoscorpionates TpMe [10], Tp [11], or TpMe2 [12],
which coordinate in j3 fashion to the rhodium(I) metal
ion in their Tp0Rh(LL) complexes. On the other hand it is
probably slightly less demanding than TpiPr2, which
forms Tp00Rh(diene) complexes with j3 hapticity, when
dien ¼ NBD and j2 hapticity in case of diene ¼ COD
[13]. Other sterically demanding Tp0 ligands, like TpPh
[18] and Tp4-OMePh [19], as well as [HB(pz)4]ꢁ [20] coor-
dinate in j2 fashion in their Tp0Rh(diene) complexes. We
have synthesized two compounds: [HB(3-Ph,5-iPrpz)2
(3,5-diMepz)]Rh(NBD) (1) and [HB(3-Ph,5-iPrpz)2(3,5-
Crystal data are given in Table 1, together with re-
finement details. All measurements of crystal were per-
formed at low temperature using an Oxford Cryosystem
device on a Kuma KM4CCD j-axis diffractometer with
graphite-monochromated Mo Ka radiation. The crystal
was positioned 65 mm from the CCD camera. 612
frames were measured at 0.75° intervals with a counting
time of 20 s. Accurate cell parameters were determined
and refined by least-squares fit of 5950 of the strongest
reflections. The data were corrected for Lorentz and
polarization effects. No absorption correction was ap-
plied. Data reduction and analysis were carried out with