3217
Baoming Ji et al[
Table 0[ The crystallographic data and re_nement par!
Chemical and physical measurements
ameters
Melting points were measured on a WC!0 apparatus
and are uncorrected[ Transition metal ion contents
were determined by EDTA complexometric titration
method[ Microanalyses "C\ H and N# of the adducts
were carried out on a Carlo!Erba 0095 elemental ana!
lyzer[ The IR spectra were recorded on a Shimadzu
324 spectrometer in KBr pellets[ UVÐVIS spectra were
Empirical formula
Formula weight
Crystal color\ habit
Crystal dimensions "mm#
C15H17N5O10Cu
713[97
green\ prismatic
9[19×9[19×9[29 mm
9[21
Omega scan peak width at
half!height ">#
Ä
a "A#
02[431"2#
06[923"6#
6[461"0#
Ä
measured with a Shimadzu UV!1099 spectrometer[ b "A#
Ä
c "A#
Conductivity measurements were performed with a
DDS!00A conductometer with acetone as solvent at
14>C[
a ">#
b ">#
g ">#
89[30"1#
099[43"0#
097[20"1#
0515[3"7#
−2
Ä
V "A
#
¹
Space group
Z
p0 "(1#
1
General procedure for the preparation of the adducts
Dcalc "g cm−2
F"999#
#
0[572
735[99
6[63
34[9
The adducts were prepared by dissolving a 0]1
molar ratio of hydrated metal picrate and B04C4 in a
1]1]0 "v:v:v# mixed solvent of MeCN\ EtOH and H1O\
and the resulting solutions were _ltered and allowed
to stand over several days until the crystalline prod!
ucts of the adducts were separated[ A green single
crystal of copper"II# adduct suitable for X!ray struc!
tural analysis was obtained by recrystallization using
the same mixed solvent[
m "MoKa# "cm−0
1umax ">#
#
Total No[ of re~ections measured 3059
No[ observations ðI×2[99 s "I#Ł
R
Rw
Maximum peak "e A
Minimum peak "e A
2501
9[921
9[938
9[49
−
−2
Ä
Ä
#
−
−2
#
−9[30
X!ray crystal structure determination of Cu adduct
All measurements were made on a Rigaku AFC6R
di}ractometer with graphite monochromated MoKa
radiation and a 01 kW rotating anode generator[ Cell
constants and orientation matrix for data collection
were obtained from a least!squares re_nement using
the setting angles of 08 carefully centered re~ections
in the range of 12[12³1u³15[62>[ The data were cor!
rected for Lorentz and polarization e}ects and empiri!
cal absorption[
The structure was solved by direct methods and
expanded using Fourier techniques[ The nonhydrogen
atoms were re_ned anisotropically[ Hydrogen atoms
were included but not re_ned[ All calculations were
performed on a Micro VAX2099 computer using
teXsan crystallographic software package of Molec!
ular Structure Corporation "0874 and 0881#[ Neutral
atom scattering factors were taken from Cromer and
Waber[ Atomic coordinates and anisotropic tem!
perature factors for all nonhydrogen atoms were
re_ned by full!matrix least!squares[
sition metal picrate and ligand in a molar ratio of 0]1
was used[
All the adducts possess similar IR spectra\ indi!
cating that they have similar coordination pattern[
The IR spectra of the adducts revealed that the molec!
ular symmetric vibration absorption of the ligand at
ca[ 879 cm−0 disappears and that the nARÐOÐC absorp!
tion at 0149 cm−0 does not undergo any changes in
the adducts[ The intensity of the nas"CÐOÐC# absorption
at 0019 cm−0 for the adducts decreases obviously in
comparison with that of the free ligand[ These results
implied that some interaction between hydrated tran!
sition metal picrates and aliphatic ether oxygen atoms
rather than the phenolic ether oxygen atoms occurs in
the adducts[ This conclusion will be further con_rmed
by the X!ray crystal structure analysis of the copper"II#
adduct[ The strong absorption bands at 2199Ð2499
cm−0 in the adducts show the presence of the water
molecules\ which is consistent with that of micro!
analysis[
The crystallographic data and re_nement par!
ameters are listed in Table 0[ The selected bond dis!
tances and angles are given in Table 1
The measurements of the UVÐVIS spectra of the
adducts show that all the adducts possess the similar
absorption pattern[ The absorption for the picrate
anion at 219Ð229 nm does not show much di}erence
before and after the formation of the adducts[ This
RESULTS AND DISCUSSION
The elemental analysis data as shown in Table 2 implies that the coordination pattern of the hydrated
indicate that all the adducts prepared have a 0]0 metal transition metal picrates does not undergo a pro!
picrateÐligand stoichiometry with two or four water nounced conformational change after the adducts
molecules\ although a mixture of the hydrated tran! were formed and as a result the central transition