The pyrrolyldipyrrin motif is found in several naturally occurring prodigiosin pigments. The potential roles of the interactions of prodigiosins with transition metals and the properties of metal-bound pyrrolyldipyrrins, however, have been difficult to assess because of the very limited number of well-characterized stable complexes. Here, we show that the introduction of a meso-aryl substituent and an ethyl ester group during the sequential assembly of the three heterocycles affords a pyrrolyldipyrrin of enhanced coordinating abilities when compared to that of natural prodigiosins. UV-visible absorption studies indicate that this ligand promptly binds Zn(II) ions with 2:1 ligand-to-metal stoichiometry and Cu(II) ions with 1:1 stoichiometry. Notably, no addition of base is required for the formation of the resulting stable complexes. The crystal structures reveal that whereas the tetrahedral zinc center engages two nitrogen donors on each ligand, the pseudosquare planar copper complex features coordination of all three pyrrolic nitrogen atoms and employs the ester group as a neutral ligand. This first example of coordination of a redox-active transition metal within a fully conjugated pyrrolyldipyrrin framework was investigated spectroscopically by electron paramagnetic resonance to show that the 1:1 metal-to-ligand ratio found in the crystal structure is also maintained in solution.
The pyrrolyldipyrrin motif is found in several naturally occurring prodigiosin pigments. The potential roles of the interactions of prodigiosins with transition metals and the properties of metal-bound pyrrolyldipyrrins, however, have been difficult to assess because of the very limited number of well-characterized stable complexes. Here, we show that the introduction of a meso-aryl substituent and an ethyl ester group during the sequential assembly of the three heterocycles affords a pyrrolyldipyrrin of enhanced coordinating abilities when compared to that of natural prodigiosins. UV-visible absorption studies indicate that this ligand promptly binds Zn(II) ions with 2:1 ligand-to-metal stoichiometry and Cu(II) ions with 1:1 stoichiometry. Notably, no addition of base is required for the formation of the resulting stable complexes. The crystal structures reveal that whereas the tetrahedral zinc center engages two nitrogendonors on each ligand, the pseudosquare planar copper complex features coordination of all three pyrrolic nitrogen atoms and employs the ester group as a neutral ligand. This first example of coordination of a redox-active transition metal within a fully conjugated pyrrolyldipyrrin framework was investigated spectroscopically by electron paramagnetic resonance to show that the 1:1 metal-to-ligand ratio found in the crystal structure is also maintained in solution.
Oligopyrrolic compounds
are essential to all forms of life and play a critical role in the
chemistry of transition metals in living systems. The coordination
chemistry of porphyrins and other oligopyrrolic macrocycles has been
investigated intensely; however, linear oligopyrroles and particularly
dipyrrolic fragments are gaining increasing attention.[1,2] Presenting an electron-rich scaffold and an array of pyrrolic nitrogendonors, linear oligopyrrolic fragments are typically well-poised for
metal coordination. In addition, these fully or partially conjugated
compounds can offer diverse coordinating abilities toward transition
metals in multiple oxidation states, as well as highly tunable, potentially
redox-active, ligand behavior. Such properties have been observed
in studies of reactivity and catalytic applications of complexes of
dipyrranes,[3,4] dipyrrins,[1,5−9] and other linear oligopyrrolic ligands.[10−14] Herein, we examine in the context of metal coordination
a tripyrrolic scaffold found in several naturally occurring pigments
of bacterial origin.The pyrrolyldipyrrin motif characterizes
the natural product prodigiosin (1 in Chart 1, showing the common letter designation of the three
pyrrole rings), a red pigment produced by certain Serratia, Streptomyces, and Bacillus bacteria strains.[15,16] This tripyrrolic species is the parent compound of a large family
of natural and synthetic analogues, termed prodigiosenes (or less
commonly prodiginines), which are currently undergoing intense scrutiny
in medicinal chemistry studies because of their diverse biological
activity profiles. Multiple studies document the efficacy of numerous
pyrrolyldipyrrins as immunosuppressive,[17,18] antimicrobial,[19] antimalarial,[20] and
anticancer[21−24] agents. The reported ability of prodigiosenes to induce apoptosis
has been connected to DNA intercalation,[25] perturbation of intracellular pH through H+/Cl– symport[26] and/or Cl–/HCO3– antiport[27,28] mechanisms, and oxidative DNA damage.[29−31]
Chart 1
Natural Prodigiosin
and Selected Metal Complexes of Its Analogues
Prodigiosin cleaves double-stranded DNA in the presence
of O2 and Cu(II) cations without the need of an added reductant.[29] Both metal binding and redox interplay between
the electron-rich tripyrrole and the redox-active cation, possibly
resulting in formation of a ligand-based π-radical cation, have
been proposed to explain the observed nuclease activity.[29,32] Consistently, modifications of the prodigiosin scaffold that rendered
the ligand less coordinating or harder to oxidize decreased DNA cleavage
activity.[29,32,33] In spite of
the interest in the role of metal binding and redox chemistry in the
biological activity of prodigiosenes, however, the coordination chemistry
of these tripyrrolic fragments remains rather unexplored, and copper
complexes of pyrrolyldipyrrins have been elusive.Bidentate
coordination modes to the dipyrrin unit of prodigiosin analogues have
been observed in fluorescent boron difluoride complexes,[34−36] and two such compounds are available commercially as longer-wavelength
members of the BODIPY family of fluorescent dyes (Molecular Probes).
Similarly, several homoleptic zinc complexes of pyrrolyldipyrrins,
such as 2 (Chart 1),[22,23,37] share the characteristics of
other complexes within the large family of simple dipyrrins, which
coordinate as bidentate monoanionic ligands. The additional pyrrolic
ring on the prodigiosin-type scaffolds behaves as a ligand in fluorescent
dialkyl and diaryl tin(IV) complexes such as 3 (Chart 1),[38] for which structural
characterization revealed tridentate coordination of all nitrogendonors on the fully conjugated pyrrolyldipyrrin scaffold. A similar
tridentate coordination mode was recently proposed for a Zn(II) complex,
which was not characterized fully but was inferred from UV–visible
absorption data and computational work.[39]Studies aimed at Cu(II) coordination of prodigiosin led to
the isolation of complex 4 (Chart 1) following reaction of the free ligand with cupric chloride in the
presence of potassium tert-butoxide in tert-butyl alcohol.[37] Notably, the tripyrrolic
scaffold behaves as a tridentate ligand, but oxidation of pyrrole
ring C yielded an sp3-hybridized hydroxyl-bound carbon
atom in 4 and confirmed the occurrence of ligand-centered
redox reactivity in solution. Additional coordination studies conducted
on a C-ring modified analogue of prodigiosin indicated copper–ligand
binding interactions of 1:1 and 1:2 stoichiometry, as inferred by
spectrophotometric titrations and mass spectrometry, but the resulting
copper complexes were not isolated.[22] Interestingly,
oxidative degradation was also observed during Cu(II) insertion in
another tripyrrolic ligand, a tripyrrane that was found to undergo
oxidation at the methylene bridges.[14]In spite of their electron-rich scaffold featuring an array of three
pyrrolic nitrogendonors, pyrrolyldipyrrins are not associated with
a well-established coordination chemistry. Herein, we describe the
design and synthesis of a pyrrolyldipyrrin ligand of enhanced metal-coordinating
ability when compared to that of natural systems and current synthetic
analogues. Binding of divalent zinc is observed as well as the prompt
and hitherto elusive coordination of divalent copper ions in the absence
of bases and without oxidative degradation of the ligand. The spectroscopic
and structural characterization of the resulting complexes documents
two available coordination modes for the tripyrrolic fragment. The
reported synthetic findings will offer access to new classes of prodigiosin
analogues; concurrently, our prototype ligand system provides a new
platform for the study of metal-bound pyrrolyldipyrrins and their
potential applications in medicinal chemistry, small-molecule activation,
and catalysis.
Results and Discussion
Ligand Design and Synthesis
Aiming to build a pyrrolyldipyrrin of higher metal-binding affinity
when compared to that of natural systems, we introduced two electron-withdrawing
groups in the first-generation scaffold H2PD1 (Scheme 1): (i) a phenyl group in the meso-type position and (ii) an ethyl ester group on the C-ring. These
substituents were expected to increase the acidity of the pyrrolic
N–H protons in order to facilitate deprotonation and coordination
of metal cations. In addition, the α-ester functionality was
envisioned as an additional ligand to contribute to metal coordination
with a neutral oxygendonor, as previously observed for α-substituted
dipyrrins.[9,40] Further supporting our ligand design featuring
two electron-withdrawing substituents, H2PD1 presents a
stabilized π system when compared to naturally occurring analogues.
As such, we anticipated that such construct would be less prone to
the type of oxidative degradation observed in complex 4 (Chart 1) in the presence of redox-active
transition metal species such as Cu(II) ions.[37]
Scheme 1
Synthesis of a meso-Aryl Pyrrolyldipyrrin with an
Ester Group on the C-Ring
meso-Aryl pyrrolyldipyrrin scaffolds
have recently appeared in studies on the preparation of pyrrolylBODIPY
dyes. Specifically, substitution reactions[34,36] onmeso-aryl dipyrrin substrates and the one-pot
reaction[35] of acyl chlorides with excess
pyrrole under an oxygen atmosphere afford boron pyrrolyldipyrrins.
Demetalation of these dyes can then be employed to prepare free pyrrolyldipyrrin
ligands.[36,41] Alternatively, a recent synthetic route
to this class of compounds requires the low-yielding acylation of
2,2′-bipyrrole, leading to a mixture of products.[39] These synthetic methods for the preparation
of meso-aryl pyrrolyldipyrrin, however, generally
afford modest-to-moderate yields and have not been employed on α-substituted
pyrroles. Our stepwise assembly of the three pyrrolic rings is designed
to provide flexibility of substitution patterns for the overall structure.Similar to several reported preparations of C-ring-modified prodigiosenes,[22−24] our synthetic pathway begins with the heterocycle that will become
the C-ring in the final product. The pyrrolic precursor ethyl 5-benzoyl-1H-pyrrole-2-carboxylate 5, which carries the
desired ethyl ester substitution and a benzoyl group for further functionalization,
was reduced with NaBH4 to give alcohol 6.
This reactive species was utilized promptly upon isolation, and the
B-ring was introduced by condensation with excess pyrrole under acidic
conditions.[42] Alternatively, asymmetric
dipyrrane 7 could be prepared via known methods requiring
synthesis of a 5-substituted dipyrran and subsequent Grignard-mediated
acylation using a pyridyl carbonothioate (Mukaiyama reagent).[43] These transformations, however, are typically
characterized by low-to-moderate yields and challenging purifications.Because bromodipyrrins are reliable precursors in the synthesis
of prodigiosenes,[22−24] dipyrromethane 7 was brominated with N-bromosuccinimide and then oxidized with 2,3-dichloro-5,6-dicyano-1,4-benzoquinone
(DDQ) to afford asymmetric bromodipyrrin 9. Compound 9 is susceptible to rapid decomposition under acidic conditions,
and the addition of a base during the oxidation reaction proved to
be critical. The A-ring completing the pyrrolyldipyrrin scaffold was
then introduced using a protected pyrrole-2-boronic acid through a
Suzuki–Miyaura coupling reaction, giving the target tripyrrolic
pigment H2PD1.A full assignment of the pyrrolic
proton resonances for the pyrrolyldipyrrin ligand was performed by
COSY and NOESY 2D NMR techniques (see Supporting
Information). These experiments also indicated that free base
H2PD1 exists in solution as the rotamer shown in Scheme 2. Although three alternative rotameric structures
are available for this scaffold, this pyrrolyldipyrrin is best represented
by the structure featuring all three pyrrolic nitrogen atoms on the
inner side of the cleft. This rotamer is also the one observed experimentally
by 2D NMR experiments and was found to be most stable by DFT analysis
in a recent study on a close analogue of natural prodigiosin.[44] In addition, our 2D NMR data allowed identification
of the NH proton on ring A (Figure S3, ) but left undetermined
the position of the other NH proton, which was not observed, likely
because of rapid exchange equilibrium between the two tautomeric forms
of the dipyrrin moiety (Scheme 2). The NMR
data summarized above indicate that free base H2PD1 maintains
the orientation of pyrrolic nitrogendonors in a tridentate array
poised for metal coordination and/or multiple hydrogen-bonding interactions,
two aspects of its solution chemistry that have been invoked in the
biological mechanisms of action of prodigiosin analogues.
Scheme 2
Tautomeric
Equilibrium of H2PD1 in CDCl3 Showing Key NOESY
Correlations for the Assignment of the Rotameric Structure
Metal Binding Studies and
Structural Characterization
Pyrrolyldipyrrin H2PD1 is a dark red pigment characterized by an intense visible absorption
band at λmax 476 nm (ε, 29 600 M–1 cm–1 in CH3OH); thus,
the coordination of metal cations could be monitored by UV–vis
absorption spectroscopy. Addition of 0.5 equiv of Zn(OAc)2·2H2O to a solution of H2PD1 in methanol
(Figure 1) or THF led to prompt formation of
a new metal complex featuring two red-shifted absorption bands. Clear
isosbesticity was maintained over the course of the metal-binding
study, and further additions of zinc salt did not elicit any changes
in the absorption spectra; therefore, the formation of a single complex
of 2:1 ligand-to-metal stoichiometry was inferred. Because absorbance
values changed almost linearly with metal ion additions, and hence
the fraction of ligand-bound metal approached 100%, these binding
studies of zinc and copper (see below) ions revealed binding stoichiometry
but did not allow reliable determination of the high-affinity equilibrium
constants.
Figure 1
Spectral changes and binding isotherms observed upon addition of
Zn(OAc)2·2H2O (left panel) or Cu(OAc)2·H2O (right panel) to pyrrolyldipyrrin H2PD1 (36 μM) in methanol at 298 K.
Spectral changes and binding isotherms observed upon addition of
Zn(OAc)2·2n class="Chemical">H2O (left panel) or Cu(OAc)2·H2O (right panel) to pyrrolyldipyrrin H2PD1 (36 μM) in methanol at 298 K.
Complex Zn(HPD1)2 was isolated and first characterized
by NMR spectroscopy. The proton spectrum displayed a single set of
resonances for the tripyrrolic ligand, consistent with a 1:1 stoichiometry
of binding or with formation of a symmetric 2:1 complex. Two-dimensional
experiments allowed identification of the proton on the pyrrolic nitrogen
atom on ring A (Figures S5–S6, Supporting
Information), which is shifted downfield with respect to the
corresponding resonance in the free ligand (at 9.75 vs 9.35 ppm in
H2PD1) and does not participate in metal binding. In addition,
a NOESY crosspeak between the α C–H proton on ring A
and the phenyl multiplet was identified as a correlation between two
ligands held in close proximity by coordination to the zinc center
and therefore consistent with 2:1 ligand-to-metal binding stoichiometry.
The expected coordination of the zinc(II) ion to two ligands through
the bidentate dipyrrin moieties was confirmed in the solid state by
X-ray diffraction analysis on a single crystal of complex Zn(HPD1)2 (Figure 2).
Figure 2
Crystal structure of
zinc complex Zn(HPD1)2 showing a partial labeling scheme.
For clarity, the two pyrrolyldipyrrin ligands are shown in different
colors, and the hydrogen atoms in calculated positions are shown only
for one of the ligands. Anisotropic thermal displacement ellipsoids
are set at the 50% probability level (CCDC 994299).
Crystal structure of
zinc complexZn(HPD1)2 showing a partial labeling scheme.
For clarity, the two pyrrolyldipyrrin ligands are shown in different
colors, and the hydrogen atoms in calculated positions are shown only
for one of the ligands. Anisotropic thermal displacement ellipsoids
are set at the 50% probability level (CCDC 994299).The crystallographic metric parameters of complex
Zn(HPD1)2 are similar to those of the zinc complex of natural
prodigiosin 1,[37] in which
the zinc center coordinates with tetrahedral geometry to two bidentate
monoanionic dipyrrin units. Interestingly, the noncoordinating A-ring
of one of the ligands in the structure of Zn(HPD1)2 features
a pyrrolic NH group pointing away from the zinc center and hence is
in a different rotameric structure when compared to that of the free
ligand. This packing effect is attributed to an intermolecular hydrogen-bonding
interaction with the carbonyl group of a neighboring complex (Figure
S7, Supporting Information) and is not
observed in chloroform solution according to our 2D NMR data.Partly because copper is a biologically relevant metal and partly
because of the documented interplay of Cu(II) ions and natural prodigiosin
in the cleavage of double-stranded DNA,[29,45,46] the copper binding properties of pyrrolyldipyrrin
scaffolds have been previously investigated. Nevertheless, copper-bound
prodigiosenes have remained elusive, and coordination studies reported
oxidative degradation of the ligand in complex 4 (Chart 1)[37] or formation of multiple
complexes that could not be isolated and fully characterized.[22] Because ligand H2PD1 was designed
for enhanced metal-binding properties, we sought to investigate its
coordination of the Cu(II) cation.The reaction of H2PD1 with Cu(OAc)2·H2O could be monitored
by UV–vis spectrophotometry in CH3OH (Figure 1, right panel) or THF. The spectral changes observed
upon addition of the copper salt presented a clear isosbestic point,
and full saturation of the ligand was reached when the concentration
of Cu(II) ions amounted to 1 equiv, therefore indicating formation
of a single copper complex of high affinity and 1:1 binding stoichiometry.
H2PD1 is an excellent receptor for copper coordination,
and, unlike previously reported binding studies,[22,37] complex formation in this case did not require addition of a base
to facilitate deprotonation of pyrrolic NH groups.The solid-state
structure of the isolated copper complex Cu(PD1) was investigated
by single-crystal X-ray diffraction analysis. Although the refinement
was complicated by the presence of disordered solvent molecules (see Experimental Section), this analysis allowed for
the determination of the copper coordination mode in the complex (Figure 3). PyrrolyldipyrrinPD12– behaves
as a tetradentate dianionic ligand, and the copper center exhibits
a slightly distorted square planar coordination geometry in the resulting
neutral complex. All three pyrrolic nitrogen atoms are engaged as
donor groups, and the ester group on the C-ring assumes the expected
role of neutral ligand through the carbonyl oxygen atom to complete
the copper coordination sphere. The Cu–Npyrrole (1.900(8)–1.931(9)
Å) and Cu–Ocarbonyl (2.074(7) Å) bond
lengths compare well with those found in Cu(II) complexes of prodigiosin[37] and α-substituted dipyrrin ligands.[9] The copper center is closer to the dipyrrin unit
and the Cu–N bond distance to pyrrole ring A (1.931(9) Å)
is longer than those to rings B and C (1.909(8) and 1.900(8) Å,
respectively). In addition, C–N and C–C bond metric
comparisons with free pyrrolyldipyrrin ligands[26,36,47,48] and with Zn(II)
complex Zn(HPD1)2 confirm a fully conjugated tripyrrolic
scaffold in Cu(PD1). Such considerations, together with the absence
of counterions, indicate that Cu(II) ions bind to deprotonated ligand
PD12– without complications arising from interfering
redox events.
Figure 3
Top and side views of the crystal structure of copper(II)
complex Cu(PD1) showing a partial labeling scheme. Anisotropic thermal
displacement ellipsoids are scaled to the 50% probability level (CCDC
994298).
Top and side views of the crystal structure of copper(II)
complex n class="Gene">Cu(PD1) showing a partial labeling scheme. Anisotropic thermal
displacement ellipsoids are scaled to the 50% probability level (CCDC
994298).
EPR Characterization of
Cu(PD1)
The coordination environment of the copper center
in Cu(PD1) was investigated in solution by electron paramagnetic resonance
(EPR) spectroscopy. The X-band (∼9.5 GHz) continuous-wave (CW)
EPR and the Ka-band (∼30 GHz) electron
spin echo (ESE) field-sweep spectra (Figure 4) are characterized by nearly axial g and A tensors (where A denotes the hyperfine interaction (hfi) of the
central Cu nucleus) with (g∥, g⊥) = (2.188, 2.043) and (ACu∥, ACu⊥) ≈
(17.6, <4) mT, indicative of the unpaired electron predominantly
localized in the d2–2 orbital.
Figure 4
(a) X-band CW EPR and
(b) Ka-band two-pulse ESE field-sweep
spectra of a Cu(PD1) solution in toluene. The asterisk in panel b
indicates the EPR position where the pulsed ENDOR measurements (Figure 5) were performed. Experimental conditions: (a) Microwave
frequency, 9.450 GHz; microwave power, 2 mW; magnetic field modulation
amplitude, 0.2 mT; temperature, 77 K. (b) Microwave frequency, 30.360
GHz; microwave pulses, 24 and 42 ns; time interval between microwave
pulses, τ = 400 ns; temperature, 15 K.
(a) X-band CW EPR and
(b) Ka-band two-pulse ESE field-sweep
spectra of a Cu(PD1) solution in toluene. The asterisk in panel b
indicates the EPR position where the pulsed ENDOR measurements (Figure 5) were performed. Experimental conditions: (a) Microwave
frequency, 9.450 GHz; microwave power, 2 mW; magnetic field modulation
amplitude, 0.2 mT; temperature, 77 K. (b) Microwave frequency, 30.360
GHz; microwave pulses, 24 and 42 ns; time interval between microwave
pulses, τ = 400 ns; temperature, 15 K.
Figure 5
14N Davies ENDOR spectrum of a Cu(PD1) solution in toluene (top panel)
and integrals under the ENDOR features belonging to different 14N ligand nuclei (bottom panel). The experiment was performed
in a 2D fashion, νRF vs the RF pulse length, tRF, and then the 2D set was integrated over tRF to obtain the 1D spectrum shown in the top
panel. Experimental conditions: microwave frequency, 30.360 GHz; magnetic
field, B0 = 970 mT (marked by an asterisk
in Figure 4b); microwave pulses, 160, 80, and
160 ns; time interval between the first and second microwave pulses,
36 μs; time interval between the second and third microwave
pulses, 400 ns; tRF variation range, 2–32
μs; temperature, 15 K.
The 14N hyperfine splittings in the CW EPR spectrum
(Figure 4a) are not sufficiently resolved to
permit the determination of the number and detailed parameters of
the 14N ligands. In order to reveal the (relative) number
of copper-bound nitrogen atoms in Cu(PD1) in solution, we employed
a pulsed electron–nuclear double resonance (ENDOR) technique
due to Davies,[49] which is particularly
suitable for detecting the strong (tens of megahertz) hfi of 14N in Cu(II) complexes.Because we were mostly
interested in quantification of the 14N nuclei, we performed
only the measurements at the low-field g∥ turning point of the EPR spectrum (marked by an asterisk in Figure 4), which corresponds to a single-crystal-like situation
and to the highest resolution in the ENDOR spectra. The relevant theoretical
background and the experimental details are given in the Experimental Section. Here, we will mention only
that the microwave (mw) pulses used were sufficiently long to make
the Davies ENDOR response independent of the hfi constants
of the detected 14N nuclei. In addition, to minimize the
dependence of the 14N ENDOR line amplitudes on the transition
probabilities, the experiment was performed in a 2D fashion (Figure
S8, Supporting Information): radiofrequency
(RF) versus the RF pulse length, tRF,
and then the 2D set was integrated over tRF to obtain the 1D spectrum.The obtained 14N Davies
ENDOR spectrum (Figure 5) shows three pairs of features attributable to 14N nuclei (labeled Na, Nb, and Nc in Figure 5), with the splitting within each
pair equal to twice the Zeeman frequency of 14N: 2νN ∼ 6 MHz in the applied magnetic field, B0 ∼ 1 T. The smaller quadrupole splittings are
poorly resolved because of the line broadening. These three pairs
of lines are centered at the frequencies of 12.6, 21.9, and 30.2 MHz,
resulting in the 14N hfi constants AN∥ = 25.2, 43.8, and 60.4 MHz, respectively.14N Davies ENDOR spectrum of a Cu(PD1) solution in toluene (top panel)
and integrals under the ENDOR features belonging to different 14N ligand nuclei (bottom panel). The experiment was performed
in a 2D fashion, νRF vs the RF pulse length, tRF, and then the 2D set was integrated over tRF to obtain the 1D spectrum shown in the top
panel. Experimental conditions: microwave frequency, 30.360 GHz; magnetic
field, B0 = 970 mT (marked by an asterisk
in Figure 4b); microwave pulses, 160, 80, and
160 ns; time interval between the first and second microwave pulses,
36 μs; time interval between the second and third microwave
pulses, 400 ns; tRF variation range, 2–32
μs; temperature, 15 K.In order to estimate the relative numbers of nitrogen nuclei
contributing to each pair of 14N ENDOR features, we have
integrated the spectrum within the regions occupied by each line group
(Figure 5, bottom panel). The similar areas
under each feature correspond to three types of copper-bound nitrogendonors in equal numbers. We conclude, therefore, that the solution
structure of Cu(PD1) is similar to that determined by single-crystal
X-ray diffraction analysis (Figure 3), with
a single PD12– ligand coordinated in tetradentate
fashion to the Cu(II) center. Alternative structures formally having
three types of nitrogen ligands in equal numbers can be discarded:
three-coordinate Cu(II) complexes are quite unusual, and they exhibit ACu∥ ∼ 9–13 mT,[50,51] significantly lower than that found in our case, whereas Cu(II)
complexes with six nitrogen ligands have g∥ values in excess of 2.23,[52] significantly
greater than that observed in this work.The hfi constants AN∥ found in this work
are within the range known for 14N ligands in Cu(II) complexes.[53] The largest hfi constant, AN∥ = 60.4 MHz (Nc in Figure 5), is close to those found in Cu(II) complexes of
tetraphenylporphyrin (TPP) (four equivalent nitrogendonors with AN∥ = 54.2 MHz)[54] and N-confused TPP (NcTPP) (two of the larger hfi constants AN∥ = 60 MHz).[55] For pyrrolic nitrogens coordinated trans to oxygen ligands, hfi constants are reduced to
∼40 MHz,[9,56] and AN∥ of Nb is of similar magnitude (43.8 MHz). The remaining AN∥ = 25.2 MHz (Na) found in
this work appears to be much smaller than the hfi constants found for pyrrole or imidazole ligands of Cu(II) in nitrogen–oxygen
coordination environments[53] to be explained
by electronic factors only. Because the Cu–N1 bond distance
is longer than the other nitrogen contacts in the crystal structure
of Cu(PD1) (see structural characterization and Figure 3 above), we tentatively assign Na to N1, whereas
Nb and Nc are assigned to N2 and N3, respectively.Together with the visible absorption data, the EPR and ENDOR spectroscopic
analysis of the paramagnetic complex Cu(PD1) indicated that prodigiosin
analogue H2PD1 coordinates Cu(II) ions with 1:1 stoichiometry,
employing all three nitrogendonors on the ligand in the absence of
any added base in organic solvents.
Conclusions
The
electron-rich tripyrrolic scaffold and preorganized array of nitrogendonor groups of pyrrolyldipyrrin motifs have made them long-standing
candidates for binding of transition metals. In spite of these features,
these oligopyrrolic fragments are not characterized by a rich coordination
chemistry. Here, we report a molecular design of the substitution
pattern on this tripyrrolic motif that leads to the construction of
an effective platform for metal coordination. Specifically, the addition
of a meso-aryl group and an ester group on the C-ring
resulted in ligand system H2PD1, which not only maintains
the known monoanionic bidentate binding mode shown in complex Zn(HPD1)2 but also offers an unprecedented dianionic tetradentate coordination
mode for Cu(II) in a pyrrolyldipyrrin complex. The latter was established
by X-ray crystallography in the solid state and confirmed in solution
by pulsed ENDOR. The described spectroscopic analysis provides a basis
for the study of metal-bound pyrrolyldipyrrins in other paramagnetic
complexes.The modular construction of meso-substituted pyrrolyldipyrrins described herein is anticipated to
produce a class of ligands featuring high tunability of donor capacity
and redox potentials. In addition, lacking the rigid structure of
porphyrin and other pyrrole-based macrocycles, tripyrrolic ligands
enable the formation of complexes in which the metal center is possibly
more accessible for substrate coordination in catalytic applications.
These expectations reflect recent reports on the coordination compounds
of several linear oligopyrroles that testify to the rich redox chemistry[3,9] and catalytic applications[8] of transition
metal complexes of this class of ligands. Our findings offer new opportunities
in the construction and untapped reactivity of metal complexes of
pyrrolyldipyrrin ligands. These studies could provide insight into
the involvement of transition metals in the biological activities
of prodigiosin compounds and their synthetic analogues.
Experimental Section
Materials and Methods
All reactions
were carried out under an inert (N2 or Ar) atmosphere using
dry solvents unless otherwise noted. Tetrahydrofuran (THF), methanol
(MeOH), pentane, diethyl ether (Et2O), and dichloromethane
(CH2Cl2) were dried by passage through a Vacuum
Atmospheres solvent purifier. 1,2-Dimethoxyethane (DME) was freshly
distilled from CaH2. Flash column chromatography was carried
out using SiliaFlash P60 silica (40–63 μm particle size,
230–400 mesh, SiliCycle) or Brockmann grade I neutral aluminum
oxide (58 Å, 60 mesh, Alfa Aesar). Reactions were monitored by
thin-layer chromatography (TLC) on silica gel plates (aluminum-backed,
60 W F254s, EMD Millipore). All other reagents were obtained commercially
and used as received.1H and 13C NMR spectra
were recorded at the University of Arizona NMR Facility on Bruker
DRX-600, DRX-500, or AVIII-400 instruments and calibrated using residual
undeuterated solvent or tetramethylsilane as an internal reference.
Low- and high-resolution mass spectra were acquired at the University
of Arizona Mass Spectrometry Facility. Elemental analyses were performed
by Numega Resonance Laboratories, San Diego, CA. UV–vis spectra
were recorded on an Agilent 8453 UV–vis spectrophotometer,
and solutions were freshly prepared in MeOH. The EPR measurements
were performed at the University of Arizona EPR facility (see the
section below for details).
Ethyl
5-benzoyl-1H-pyrrole-2-carboxylate[57,58] (1.72 g, 7.07 mmol) was dissolved in MeOH (15 mL) in a round-bottomed
flask at 0 °C. NaBH4 (0.802 g, 21.2 mmol) was added
to the flask in three portions over 30 min. The reaction mixture was
warmed to room temperature and stirred for 8 h. The reaction mixture
was then cooled to 0 °C and carefully quenched by adding saturated
aqueous NaHCO3. The aqueous layer was extracted three times
with ethyl acetate (20 mL), and the combined organic layers were washed
with brine (10 mL) and dried over anhydrous Na2SO4. Following solvent evaporation under reduced pressure, crude product 6 was used directly in the next step without further purification
(1.47 g, 6.01 mmol, 75%). 1H NMR (500 MHz, CDCl3, δ): 9.69 (s, 1H), 7.44–7.33 (m, 5H), 6.85 (dd, J = 3.8, 2.6 Hz, 1H), 5.98–5.96 (m, 1H), 5.92 (d, J = 4.1 Hz, 1H), 4.29 (q, J = 7.1 Hz, 2H),
3.23 (d, J = 4.1 Hz, 1H), 1.35 (t, J = 7.1 Hz, 3H). 13C NMR (125 MHz, CDCl3, δ):
161.57, 141.74, 139.21, 128.71, 128.30, 126.60, 122.31, 115.80, 108.36,
60.46, 14.46. LRMS-ESI+m/z (relative intensity): 228.0 (100%).
Compound 7 (0.100 g, 0.340 mmol) was dissolved in THF (6 mL) at −78
°C. n class="Chemical">N-Bromosuccinimide (61 mg, 0.340 mmol) was
added to the reaction flask in one portion, and the mixture was stirred
at −78 °C for 30 min. The reaction mixture was diluted
with hexanes (5 mL) and with water (5 mL). The aqueous layer was extracted
three times with ethyl acetate (20 mL), and the combined organic layers
were washed with brine (10 mL) and dried over anhydrous Na2SO4. Solvent evaporation under reduced pressure afforded
compound 8 as a brown oil (0.114 g, 0.241 mmol, 90%),
which was used directly in the next step without further purification.
(Note that in order to obtain the desired compound in high yields
and free of side products, this reaction could not be conducted on
more than 0.150 g of 7.) 1H NMR (500 MHz,
CDCl3, δ): 8.79 (s, 1H), 7.82 (s, 1H), 7.40–7.32
(m, 3H), 7.24–7.20 (m, 2H), 6.87 (dd, J =
3.7, 2.5 Hz, 1H), 6.11 (dd, J = 3.6, 2.7 Hz, 1H),
6.01 (ddd, J = 3.6, 2.7, 0.7 Hz, 1H), 5.88 (ddd, J = 3.7, 2.5, 0.9 Hz, 1H), 5.44 (s, 1H), 4.31 (q, J = 7.1 Hz, 2H), 1.36 (t, J = 7.1 Hz, 3H). 13C NMR (125 MHz, CDCl3, δ): 161.71, 140.36,
137.84, 132.19, 128.65, 128.14, 127.34, 122.29, 116.01, 110.47, 109.97,
109.45, 97.54, 60.47, 44.21, 14.35. LRMS-ESI+m/z (relative intensity): 372.1 (33%), 327.0 (100%).
Compound 8 (0.114 g, 0.241 mmol) was dissolved in THF (6.7 mL) at 0
°C. 2,3-Dichloro-5,6-dicyano-1,4-benzoquinone (DDQ, 55 mg, 0.241
mmol) was dissolved in THF (1.4 mL) and added dropwise. 1,5-Diazabicyclo(4.3.0)non-5-ene
(DBN, 30 μL, 0.241 mmol) was added, and the mixture was stirred
at room temperature for 7 h. The reaction mixture was quenched by
adding saturated aqueous NaHCO3 (10 mL), and the aqueous
layer was extracted three times with CH2Cl2 (10
mL). The combined organic layers were washed with brine (10 mL) and
dried over anhydrous Na2SO4. Solvent evaporation
under reduced pressure resulted in a brown oil. The crude product
was redissolved in 1:1 mixture of ethyl acetate/hexanes and filtered
through a silica pad in order to give compound 9 (75
mg, 0.202 mmol, 84%) as a yellow oil. 1H NMR (500 MHz,
CDCl3, δ): 7.55–7.45 (m, 5H), 6.87 (dd, J = 4.1, 2.4 Hz, 1H), 6.76 (d, J = 4.5
Hz, 1H), 6.52 (d, J = 4.5 Hz, 1H), 6.33 (dd, J = 4.1, 2.4 Hz, 1H), 4.43 (q, J = 7.1
Hz, 2H), 1.46 (t, J = 7.1 Hz, 3H). 13C
NMR (125 MHz, CDCl3, δ): 160.54, 150.17, 149.00,
139.47, 137.00, 135.65, 134.87, 130.65, 129.57, 128.39, 127.99, 121.63,
115.54, 60.76, 14.26. LRMS-ESI+m/z (relative intensity): 370.9 (19%), 325.1 (100%).
Compound 9 (75 mg, 0.202 mmol), LiCl (30 mg, 0.707 mmol), pyrrole-2-boronic
acid (64 mg, 0.303 mmol), and Pd(PPh3)4 (23
mg, 10 mol %, 20.2 μmol) were dissolved in 1,2-dimethoxyethane
(6.1 mL), and the solution was degassed for 2 h. A degassed solution
of aqueous Na2CO3 (2 M, 0.5 mL) was added dropwise,
and the mixture was refluxed for 2 h. The reaction mixture was cooled
to room temperature and diluted with water (10 mL). The aqueous layer
was extracted three times with CH2Cl2 (10 mL).
The combined organic layers were washed with brine (10 mL) and dried
over anhydrous Na2SO4. Solvent evaporation under
reduced pressure afforded the crude product, which was dissolved in
CH2Cl2 (10 mL). The solution was cooled to 0
°C, and trifluoroacetic acid (0.8 mL) was added dropwise. The
mixture was stirred at room temperature for 8 h, cooled to 0 °C,
and carefully quenched with saturated aqueous NaHCO3 (20
mL). The mixture was extracted three times with CH2Cl2 (10 mL), and the combined organic layers were washed with
brine (10 mL) and dried over anhydrous Na2SO4. Solvent evaporation followed by flash chromatography (neutral alumina,
10–30% ethyl acetate in hexanes) gave pyrrolyldipyrrin H2PD1 as a dark red solid (38 mg, 0.107 mmol, 48%). (Note that
this reaction gives lower yields when conducted on more than 0.100
g of 9.) 1H NMR (400 MHz, CDCl3, TMS δ): 9.35 (bs, 1H), 7.49–7.41 (m, 5H), 7.10 (bs,
1H), 6.92 (d, J = 4.7 Hz, 1H), 6.90 (d, J = 4.7 Hz, 1H), 6.85–6.83 (m, 2H), 6.40–6.37 (m, 1H),
6.24 (d, J = 4.0 Hz, 1H), 4.41 (q, J = 7.1 Hz, 2H), 1.46 (t, J = 7.1 Hz, 3H). 13C NMR (125 MHz, CDCl3, δ): 160.30, 153.05, 138.25,
137.70, 136.68, 132.58, 132.11, 131.51, 131.23, 129.92, 128.69, 125.46,
122.69, 122.24, 122.15, 117.59, 113.82, 61.48, 14.40. HRMS-MALDI (m/z): [M + H]+ calcd for [C22H20N3O2], 358.1555; found,
358.1536. UV–vis (MeOH) λmax (ε), 476
nm (29 600 M–1 cm–1).
Zn(II) Complex Zn(HPD1)2
Pyrrolyldipyrrin H2PD1 (20 mg, 5.6 μmol) was dissolved in THF (6 mL), and
Zn(OAc)2·2H2O (6.0 mg, 2.8 μmol)
was added. The reaction progress was monitored by UV–vis spectroscopy.
Upon completion, the solvent was removed under high vacuum, and the
resulting crude solid was dissolved in dichloromethane (0.5 mL). Filtration
through a Celite pad to remove any unreacted zinc salt followed by
evaporation of the solvent and recrystallization from THF/pentane
gave the zinc complex as a dark orange/red powder (10 mg, 1.3 μmol,
46%). Single crystals for X-ray diffraction analysis and elemental
analysis were grown from THF/pentane mixtures. 1H NMR (400
MHz, CDCl3, TMS δ): 9.75 (bs, 2H), 7.58–7.48
(m, 10H), 6.96 (d, J = 4.0 Hz, 2H), 6.85 (d, J = 4.7 Hz, 2H), 6.79 (d, J = 4.7 Hz, 2H),
6.67 (ddd, J = 3.8, 2.5, 1.4 Hz, 2H), 6.58 (td, J = 2.7, 1.4 Hz, 2H), 6.45 (d, J = 4.0
Hz, 2H), 6.14 (dt, J = 3.7, 2.4 Hz, 2H), 4.05–3.98
(m, 4H), 0.98 (t, J = 7.1 Hz, 6H). HRMS (m/z) [M + H]+ calcd for [C22H17N3O2Zn], 777.2168; found,
777.2163. UV–vis (MeOH) λmax (ε): 512
nm (56 607 M–1 cm–1), 544
nm (50 200 M–1 cm–1). Anal.
Calcd for C44H37N6O4Zn·2THF·4H2O: C, 62.80; H, 6.08; N, 8.45%. Found: C, 62.20; H, 5.56;
N, 8.70%.
Cu(II) Complex Cu(DP1)
Pyrrolyldipyrrin H2PD1 (20 mg, 5.6 μmol) was dissolved in THF (6
mL), and Cu(OAc)2·H2O (11 mg, 5.6 μmol)
was added. The reaction progress was monitored by UV–vis spectroscopy.
Upon completion, the solvent was removed under high vacuum and the
resulting crude solid was dissolved in THF (0.5 mL). Filtration through
a Celite pad followed by slow evaporation of the solvent gave the
copper complex as a dark blue microcrystalline powder (12 mg, 2.9
μmol, 52%). Crystals for X-ray diffraction analysis and elemental
analysis were grown in Et2O/n-hexane mixtures.
HRMS-MALDI (m/z): [M + H]+ calcd for [C22H17N3O2Cu], 418.0617; found, 418.0611. UV–vis (MeOH) λmax (ε): 586 nm (18 200 M–1c
m–1). Anal. Calcd for C44H37N6O4Cu·n-hexane·Et2O·2H2O: C, 62.70; H, 6.04; N, 8.13%. Found:
C, 62.80; H, 5.92; N, 7.87%.
X-ray Diffraction Analysis
Data
were collected at the University of Arizona X-ray Diffraction Facility.
Crystals were mounted onto a MiTeGen micromount under a protective
film of Paratone oil, and diffraction data for both crystals were
measured using a Bruker Kappa APEX II DUO diffractometer with graphite-monochromated
Mo Kα radiation (λ = 0.71073 Å) generated by a sealed
tube and an APEX II CCD area detector. The diffractometer was fitted
with an Oxford Cryostream low-temperature device, and the data sets
were collected using the APEX2 software package.[65] The data were corrected for absorption effects using a
multiscan method in SADABS.[66] Experimental
details of the structure determinations are given in Table S1 (see Supporting Information). All structures were
solved by direct methods (SHELXS-97), and developed by full least-squares
refinement based on F2 (SHELXL).[59] Crystallographic figures were prepared using
Mercury[60] and POV-Ray.[67]
Structure Refinement of
Zn(HPD1)2.
Data were collected, solved, and refined
in the triclinic space group P–1. The asymmetric
unit contains one full complex molecule with no other significant
peaks in the Fourier map. All non-hydrogen atoms were located in the
Fourier map and refined anisotropically, whereas all hydrogen atoms
were placed in calculated positions and refined using a riding model.
The highest residual Fourier peak is 0.7 e Å–3, located 1.0 Å from Zn(1), and the deepest Fourier
hole is −0.45 e Å–3, located 0.93 Å from Zn(1).
Structure Refinement of
Cu(PD1)
Although multiple crystallizations were attempted
under different conditions, the best single crystals obtained for
this complex diffracted significantly only to 2θmax = 40° and presented substantial solvent disorder, which further
complicated the analysis. Data were collected, solved, and refined
in the monoclinic space group P21/c. The asymmetric unit contains one full complex molecule
and a solvent channel running parallel to (100) filled with electron
density that refined reasonably as three partially occupied oxygen
atoms of a water molecule (labeled O(3A), O(3B), and O(3C)). Two of
these were modeled with molar occupancies of 20% and one with 15%.
Alternative solvent molecules of crystallization were tentatively
fitted in this solvent channel but failed to offer a stable refinement
possibly because of the low observed data/parameter ratio (6.8).All fully occupied, crystallographically ordered non-hydrogen atoms
were refined anisotropically. Carbon atom C(10) was refined with a
rigid bond restraint because this atom continually refined as nonpositive
definite without restraints. All hydrogen atoms were placed in calculated
positions and refined using a riding model.A SQUEEZE analysis[61,62] of a model containing only the complex molecule identified 330 Å3 of total void space, equivalent to 16.3% of the unit cell
volume. These voids contained 73 electrons per unit cell, or approximately
18 per asymmetric unit. This could equate approximately to one molecule
of hexane (50 electrons each) and one-half molecule of diethyl ether
(42 electrons each) or seven molecules of water (10 electrons each)
per unit cell, or a combination of all three with partial molar occupancies.
Because only three partially occupied molecules of water could be
positively identified in the Fourier map, a formula of complex·1.8(H2O) was used for the density and F(000)
calculations. The highest residual Fourier peak of 0.9 e A–3 is located within the solvent accessible void,
and the deepest residual Fourier hole of −0.5 e A–3 is located 1.1 Å from N(3).
EPR and
Pulsed ENDOR Spectroscopy
The X-band (∼9 GHz) CW EPR
experiments were performed at room temperature and 77 K using a Bruker
E500 (Elexsys) spectrometer. The pulsed EPR measurements were performed
on a Ka-band (26–40 GHz) pulsed
EPR spectrometer[63] at 15 K. In order to
establish the relative number of copper-bound nitrogen ligands in
Cu(PD1), Ka-band pulsed (Davies) ENDOR
spectroscopy was used.Here, we briefly describe the ENDOR spectra
expected for 14N ligands in Cu(II) complexes under our
experimental conditions. The 14N transition lines in such
spectra are located at the frequencieswhere AN is the diagonal part of the 14N hfi (predominantly isotropic), νN ∼ 3 MHz is the 14N Zeeman frequency in
the applied magnetic field, B0 ∼
1 T, and QN is the diagonal part of the 14N nqi: QN ∼
−0.9 MHz for the pyrrole14N at g∥.[54] For the nitrogen
ligands in Cu(II) complexes, AN is on
the order of tens of megahertz. Therefore, under our experimental
conditions, the relationship between the various terms in eq 1 is AN/2 > νN > QN. Without the nqi, the ENDOR pattern for the 14N nucleus would
consist of two lines centered at ν = AN/2, with the splitting between them equal to 2νN ∼ 6 MHz. The nqi will split each
of these lines into a doublet, with the splitting equal to 2QN (∼1.8 MHz at g∥). However, a broadening of the individual lines caused
by even an insignificant degree of structural disorder can result
in a partial or complete loss of the quadrupolar splitting and observation
of only two broader lines for each 14N nucleus at the frequencies
ν = AN/2 ± νN. Such a situation is observed in the spectrum of Cu(PD1) (Figure 5).In order to make the Davies ENDOR response
independent of the hfi constants of the detected
nuclei, one has to ensure that the amplitudes of the mw pulses were
much smaller than that of the hfi constants while
keeping the spin flip angles close to optimal (π for the preparation
(inversion) pulse and π/2 and π for the two-pulse detection
sequence).[64] The hfi constants
of 14N ligands in Cu(II) complexes are on the order of
tens of megahertz and therefore this requirement is easily satisfied
for mw pulses with durations ∼100 ns (the mw amplitude ∼5
MHz).Because of the strong hfi and non-negligible
nuclear quadrupole interaction (nqi), the probabilities
of transitions of nonequivalent 14N nuclei, and even different
transitions of the same 14N nucleus, induced by the RF
field are expected to be noticeably different. Therefore, to approximately
equalize the contributions of different nitrogens to the ENDOR spectrum,
a 2D experiment was performed, with one dimension being the radiofrequency,
and the other being the RF pulse duration. The 2D data set was then
integrated over the RF pulse duration to obtain the 1D ENDOR spectrum
with the relative intensities of the 14N lines reflecting
relative numbers of nuclei rather then relative transition probabilities.
The 2D ENDOR data set (from which the 1D spectrum in Figure 5 was obtained) is shown in Figure S8 (Supporting Information).
Authors: Kancharla Papireddy; Martin Smilkstein; Jane Xu Kelly; Shaimaa M Salem; Mamoun Alhamadsheh; Stuart W Haynes; Gregory L Challis; Kevin A Reynolds Journal: J Med Chem Date: 2011-07-08 Impact factor: 7.446
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