COMMUNICATION
between the iron and inverted pyrrolic C-H bond is likely.
The axial ligand dependent core geometries are controlled
by the basicity of ligands consistent with having an agostic
interaction.12 Still, little information is available for the
mechanism of conformational change from a nonplanar NCP
core to a planar NCP geometry in NCP metal complexes. In
this paper we report that in the Mn(II) oxidation state, the
NCP adopted the tilted geometry similar to the iron
complexes; however, the inverted pyrrolic C-H bond can
be activated when Mn(II) is oxidized to Mn(III) to form a
planar NCP manganese complex.
Figure 1. Molecular structure of MnII(NCHPP)Br (3). Important bond
lengths (Å) and angles (deg): Mn(1)-C(3) 2.437(7); Mn(1)-N(2) 2.164-
(5); Mn(1)-N(3) 2.085(4); Mn(1)-N(4) 2.151(5); C(3)-C(4) 1.383(9);
C(4)-N(1) 1.377(7); N(3)-Mn(1)-C(3) 140.9(2); N(3)-Mn(1)-Br(1)
115.58(13).
When the free base NCP was treated with MnBr2 in
the mixed solvent of 2:1 CH3CN/THF in the presence of a
few drops of lutidine under anaerobic conditions,
MnII(NCHPP)Br (3)13 was isolated in 82% yield. The
electronic spectrum of 3 in CH2Cl2 gives a Soret type
absorption band at 462 nm while the Q bands are located at
715 and 782 nm. The pattern of the electronic spectrum is
distinct from the free base NCP but resembles other
nonplanar N-confused porphyrin complexes such as methy-
lated (NCP)Ni7 and Fe(NCP)Br.11 The similar electronic
spectra suggest that these compounds exhibit identical ring
conformations. MnII(NCHPP)Br has a magnetic moment of
5.50 µB at room temperature from the SQUID magnetic
susceptibility measurement. The plot of 1/ø vs T is linear
between 5 and 300 K. The room temperature magnetic
5
moment suggested a high-spin Mn(II) (s ) /2) state in 3.
Figure 2. The time trace of absorption spectra for the oxidation reaction
The ESR spectrum of the MnII(NCHPP)Br in toluene glass
at 6.8 K gives an s ) 5/2 Mn(II) type high-spin axial spectrum
with g at 5.65 and g| at 2.01.
of MnII(NCHPP)Br in the presence of O2.
MnII(NCHPP)Br is stable in the solid state as well as in
solution under anaerobic conditions. Interestingly, the elec-
tronic spectrum changed immediately when 3 was exposed
to air. A time trace of the electronic spectra is shown in
Figure 2. The intensity of the Soret band at 462 nm for
MnII(NCHPP)Br decreases and is accompanied by an in-
crease in a Soret type peak at 507 nm. The final product,
after 24 h, gives the electronic spectrum with the Soret band
at 507 nm and the Q band at 754 and 825 nm. The isolated
product gives an effective magnetic moment of 4.87 µB at
room temperature from SQUID and suggests a one-electron
oxidation of the MnII(NCHPP)Br to give MnIII(NCPP)Br
(4).17 4 is stable in the solid state as well as in solution under
aerobic conditions. No further variation was observed when
the absorption spectra were traced under aerobic conditions
for 72 h.
X-ray single-crystal analysis confirms the solid-state
conformation of MnII(NCHPP)Br. As shown in Figure 1, the
N-confused porphyrin ring adopts a nonplanar geometry with
inverted pyrrole ring tilted away from the mean plane de-
fined by the tripyrrole unit. The comparison of the bond
distances and bond angles in the porphyrin ring with the
theoretical values14 agrees that the porphyrin core in the
MnII(NCHPP)Br adopts the higher energy resonance form
as in 2. The distance of 2.437(7) Å between Mn and inner
core carbon in the inverted pyrrolic ring is much longer than
the normal Mn-C bond.15 The Mn atom sits 0.77 Å atop
the mean porphyrin plane, resembling other five-coordinated
porphyrin complexes. Finally, the Mn-Br bond distance of
2.491 Å is almost identical to 2.490 Å in the five-coordinated
Mn(TPP)Br.16
(12) The distance between iron and inner core C-H hydrogen in
Fe(NCTPP)Br is 1.971 Å while in Fe(NCTPP)(S-C7H7) the corre-
sponding bond distance increases to 2.334 Å.
(15) Brookhart, M.; Lamanna, W.; Humphrey, M. B. J. Am. Chem. Soc.
1982, 104, 2117.
(16) Turner, P.; Gunter, M. J.; Skelton, B. W.; White, A. H. Aust. J. Chem.
1998, 51, 835.
(13) MnII(NCHPP)Br: absorption spectrum (CH2Cl2) [λmax, nm (log ꢀ, M-1
cm-1)] 352 (4.69), 462 (5.14), 782 (4.41), 715 (4.06), 598 (3.54), 656
(3.7). Anal. Calcd for C44H29N4BrMn‚0.8CH2Cl2: N, 6.86; C, 65.90;
H, 3.78. Found: N, 6.74; C, 65.88; H, 4.04. MnBrN4C44H29: calcd
mass 748.582, obsd 667 (M - H - Br, FAB). Crystallographic data
for 3: C45.50H30BrCl3MnN4, T ) 295(2) K, MW ) 875.93, monoclinic,
space group P2/c, a )13.2250(11) Å, b ) 13.8871(11) Å, c )
22.5276(18) Å, R ) 90°, â ) 92.651(2)°, γ ) 90°, V ) 4132.9(6)
(17) MnIII(NCPP)Br: absorption spectrum (CH2Cl2) [λmax, nm (log ꢀ, M-1
cm-1)] 340 (4.39), 394 (4.46), 454 (4.31), 507 (4.70), 583 (3.64), 754
(3.66), 825 (3.91). Anal. Calcd for MnBrN4C44H28‚0.5THF‚0.1CH2-
Cl2: N, 7.07; C, 69.90; H, 4.10. Found: N, 7.27; C, 69.87; H, 4.26.
MnBrN4C44H28: calcd mass 747.574, obsd 667 (M - Br, FAB).
Crystallographic data for 4: C44H28BrMnN4, T ) 293(2) K, MW )
747.55, monoclinic, space group P21/n, a ) 10.2386(6) Å, b )
15.8204(9) Å, c ) 20.9468(13) Å, R ) 90°, â ) 90.000(1)°, γ )
90°, V ) 3392.9(3) Å3, Z ) 4, Dc ) 1.463 Mg/m-3, λ ) 0.71073 Å,
µ ) 1.606 mm-1, F(000) ) 1520. Data were collected on a Bruker
Smart 1000 diffractometer for 1.61° < θ < 27.54°. The structure was
solved by direct methods and refined by least-squares against F2 to
R1 ) 0.0753 (wR2 ) 0.1734) and SGOF ) 0.732.
Å3, Z ) 4, Dc ) 1.408 Mg/m-3, λ ) 0.71073 Å, µ ) 1.517 mm-1
,
F(000) ) 1776. Data were collected on a Bruker Smart 1000
diffractometer for 1.54° < θ < 27.57°. The structure was solved by
direct methods and refined by least-squares against F2 to R1 ) 0.0545
(wR2 ) 0.1051) and SGOF ) 1.136.
(14) Szterenberg, L.; Latos-Grazynski, L. Inorg. Chem. 1997, 36, 6287.
Inorganic Chemistry, Vol. 41, No. 13, 2002 3335