metal-organic compounds
Table 1
Selected geometric parameters (A, ).
sponding occupancies around atom B2 converged to 0.60 (1) and
0.40 (1). Aromatic and amide H atoms, after location from ÁF
syntheses, were placed geometrically and re®ned with a riding model,
for which the CÐH and NÐH distances were constrained to be 0.95
Ê
and 0.88 A, respectively, and Uiso(H) = 1.2Ueq(C, N). Methyl H atoms
were located and treated similarly, with CÐH distances constrained
ꢀ
Ê
Cu1ÐN1
Cu1ÐN2
Cu1ÐN11
1.945 (3)
2.316 (3)
1.964 (3)
Cu1ÐN22
Cu1ÐN62
2.024 (3)
2.026 (3)
N1ÐCu1ÐN2
N1ÐCu1ÐN11
N1ÐCu1ÐN22
N1ÐCu1ÐN62
N2ÐCu1ÐN11
93.41 (12)
171.42 (13)
78.87 (12)
78.80 (11)
95.12 (12)
N2ÐCu1ÐN22
N2ÐCu1ÐN62
N11ÐCu1ÐN22
N11ÐCu1ÐN62
N22ÐCu1ÐN62
93.70 (14)
93.29 (14)
101.55 (12)
99.67 (12)
156.94 (11)
Ê
to be 0.98 A and Uiso(H) = 1.5Ueq(C)
Data collection: IPDS (Stoe & Cie, 1995); cell re®nement: IPDS;
data reduction: IPDS; program(s) used to solve structure: SIR92
(Altomare et al., 1994); program(s) used to re®ne structure:
SHELXL97 (Sheldrick, 1997); molecular graphics: CAMERON
(Watkin et al., 1996); software used to prepare material for publica-
tion: SHELXL97 and PLATON (Spek, 2002).
Table 2
Hydrogen-bonding geometry (A, ).
ꢀ
Ê
The authors thank the University of Nottingham for
®nancial support (to MAW).
DÐHÁ Á ÁA
DÐH
HÁ Á ÁA
DÁ Á ÁA
DÐHÁ Á ÁA
N17ÐH17AÁ Á ÁF11Ai
N17ÐH17BÁ Á ÁF11Aii
N17ÐH17BÁ Á ÁF11Bii
N17ÐH17AÁ Á ÁF12Ai
N17ÐH17AÁ Á ÁF12Bi
C5ÐH5Á Á ÁO17iii
0.88
0.88
0.88
0.88
0.88
0.95
0.95
2.60
2.09
2.01
2.12
2.03
2.22
2.36
3.334 (6)
2.900 (6)
2.866 (7)
2.971 (5)
2.885 (7)
3.140 (5)
3.221 (4)
142
152
163
163
163
162
151
Supplementary data for this paper are available from the IUCr electronic
archives (Reference: GG1141). Services for accessing these data are
described at the back of the journal.
C65ÐH65Á Á ÁO17iii
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Re®nement on F2
R[F2 > 2ꢄ(F2)] = 0.059
wR(F2) = 0.175
S = 1.01
6613 re¯ections
401 parameters
H-atom parameters constrained
w = 1/[ꢄ2(Fo2) + (0.115P)2]
where P = (Fo2 + 2Fc2)/3
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3
Ê
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3
È
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0.74 e A
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=
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The tetra¯uoroborate anions are affected by disorder; this was
modelled by allowing alternative positions for each F atom, with
extensive restraints applied to BÐF distances and FÐBÐF angles.
Around atom B1, the major and minor orientations re®ned to
occupancies of 0.57 (2) and 0.43 (2), respectively, while the corre-
ꢁ
m544 Gerhard Baum et al.
[Cu(C2H3N)(C11H9N5)(C6H6N2O)](BF4)2Á2C2H3N
Acta Cryst. (2002). C58, m542±m544