After 118 years, the isolation of two common radical anion reductants as simple, stable solids

Article abstract of DOI:10.1039/b815272a

Two common radical anion reductants, potassium benzophenone ketyl (K(Ph₂CO)) and potassium naphthalenide (K₂(C ₁₀H₈)₂(THF)), have been isolated and characterized for the first time in solvent-free for

Full text of DOI:10.1039/b815272a

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After 118 years, the isolation of two common radical anion reductants as
simple, stable solidsw
Thomas A. Scott,a Betty A. Ooro,a David J. Collins,a Michael Shatruk,b Andrey Yakovenko,c
Kim R. Dunbarc and Hong-Cai Zhou*ac
Received (in Berkeley, CA, USA) 2nd September 2008, Accepted 14th November 2008
First published as an Advance Article on the web 20th November 2008
DOI: 10.1039/b815272a
Two common radical anion reductants, potassium benzo-
phenone ketyl (K(Ph2CO)) and potassium naphthalenide
(K2(C10H8)2(THF)), have been isolated and characterized for
the first time in solvent-free form or with low solvent content,
allowing their use as pure solid reactants in preparative redox
chemistry in accurate stoichiometric amounts.
located on a two-fold axis. The structure can be represented
by a dinuclear unit. As shown in Fig. 1, the naphthalenide
anions occupy two unique bonding environments. One is a
[Z12-C10H8]ꢀ anion that bridges two K+ centers from distinct
dimer units through cation–p interactions. The other is a
[Z16-C10H8]ꢀ anion, which bridges four K+ centers forming
two dimetal units through cation–p interactions. These
multiple cation–p interactions between the radical anions
and K+ cations lead to the formation of an extended 3D
network and fulfill the coordination sphere of K+ ions.
The K+ cations are arranged asymmetrically with respect to
the ring centers of the naphthalene radicals. Distances between
K+ cations and [Z12-C10H8]ꢀ anions vary in the range of
3.088(3)–3.447(2) A, the shortest distance being K(1)–C(2).
The K–C distances between the [Z16-C10H8]ꢀ anions and
K+ anions fall in the range of 2.995(3)–3.523(2) A. In the
[Z16-C10H8]ꢀ anion the peripheral carbon atoms C(8) and C(9)
also form extra K+–p interactions (Fig. 1) at distances of
3.095(3) and 3.533(4) A, respectively. These results are
consistent with the observation made by Stucky.8
The reactions of aromatic hydrocarbons with alkali metals
have long been recognized as forming organic radical
species,1–3 the first reported being benzophenone ketyl in
1891.4 These radical species are synthetically useful and have
subsequently been used in a variety of organic5 and organo-
metallic reactions6 as strong reductants.7 They are formed by
the one-electron reduction of ketones or aldehydes using
reducing metals, such as sodium and potassium. EPR solution
studies of these anionic radicals suggest that they exist as
monomeric and dimeric species.8 Despite the long existence
and common usage of these radical species, structurally-
characterized examples are very few due to their high
reactivity, making them difficult to isolate.
Single-crystal X-ray diffraction studies reveal that
K(Ph2CO) crystallizes in the non-centrosymmetric tetragonal
Several naphthalenide compounds have been previously
isolated with Li+ and Na+,8,9 while benzophenone ketyl
+
compounds have been reported containing Sm3+10 Ca2+11
,
,
ꢀ
space group I4.z Four K cations and four m3-O atoms from
and Na+.12 In these cases, however, there are large amounts of
solvent ligands that serve to stabilize the metal centers by
completing the coordination sphere. To date, no solvent-free
alkali–metal organic radical compound has been isolated. In
this communication we report, for the first time, the isola-
tion and characterization in the solid state of solvent-free
potassium benzophenone ketyl, K(Ph2CO), and of potassium
naphthalenide, K2(C10H8)2(THF), with low solvent content.
Results obtained from single-crystal X-ray diffraction show
that K2(C10H8)2(THF) crystallizes in the monoclinic space
group C2/c.z The asymmetric unit consists of one K+ cation,
two symmetrically independent naphthalenide anions, which
are located on inversion centers, and a bridging THF molecule
the benzophenone radicals form a K4O4 cubane-type struc-
ture, which is centered on a four-fold rotoinversion axis, as
illustrated in Fig. 2(a). In the K4O4 fragment, each K atom
form two long (2.735(3) and 2.766(4) A) and one short
(2.658(4) A) K–O bonds leading to a D2d distortion of the
K4O4-fragment from ideal Td symmetry.
a Department of Chemistry and Biochemistry, Miami University,
Oxford, OH 45056, USA. E-mail: zhouh@muohio.edu;
Fax: +01 513 5290452; Tel: +01 513 5298091
b Department of Chemistry and Biochemistry, Florida State
University, Tallahassee, FL 32306, USA
c Department of Chemistry, Texas A&M University, College Station,
TX 77842, USA
w Electronic supplementary information (ESI) available: Detailed
experimental procedures, cyclic voltammetry, magnetic measurements,
and UV-visible spectra. CCDC 689226 and 689227. For ESI and
crystallographic data in CIF or other electronic format see DOI:
10.1039/b815272a
Fig. 1 A dinuclear unit of K2(C10H8)2(THF); A ꢀx + 0.5, ꢀy + 0.5,
ꢀz + 1; B ꢀx + 1, ꢀy, ꢀz + 1; C ꢀx + 1, y, ꢀz + 1.5. Thermal
ellipsoids are shown at 50% probability level; hydrogen atoms are
omitted for clarity.
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constant from 300 to 30 K, then abruptly increases and
decreases again in a narrow temperature range below 30 K,
as illustrated in Fig. 3(b).
Such magnetic behavior indicates that K2(C10H8)2(THF)
undergoes long-range antiferromagnetic ordering below 30 K.
To test this hypothesis, AC magnetic susceptibility and
zero-field-cooled vs. field-cooled (ZFC/FC) magnetization
studies were performed on samples of K2(C10H8)2(THF). A
sharp out-of-phase signal was observed for the imaginary part
(w00) of the AC susceptibility (Fig. S1, ESIw). The signal
maximum occurs at 28.6 K, and its position is independent
of the frequency of the applied AC magnetic field. The ZFC
and FC curves are essentially superimposable below 30 K
(Fig. S2, ESIw), which, along with the AC susceptibility
measurements, supports the conclusion that long-range
antiferromagnetic ordering occurs in K2(C10H8)2(THF), with
a Neel temperature of TN = 28.6 K.
Fig. 2 (a) K(Ph2CO) cubane-type structure; C = grey, K = blue,
O = red. Thermal ellipsoids are shown at 50% probability level;
hydrogen atoms are omitted for clarity. (b) Formation of a 1D chain
through cation–p interactions between adjacent K(Ph2CO) cubanes.
A comparison of benzophenone13 and K(Ph2CO) reveals
that there is an elongation of the CQO bond from 1.222 to
1.311(5) A and a shortening of the C–CPh bond from 1.495
to 1.460(6) A and from 1.497 to 1.460(7) A. There are no
significant changes in the average phenyl ring distances, indicat-
ing the additional electron is localized in the trigonal-planar
C3O moiety.
The room-temperature wT value for K(Ph2CO) is
0.33 emu molꢀ1 K, which is close to the theoretically expected
value of 0.375 emu molꢀ1 K for an isolated S = 1/2 organic
radical. As the temperature decreases, the value of wT
decreases slowly (Fig. 4), and then more abruptly below
100 K, essentially reaching zero below 10 K. Such behavior
is indicative of antiferromagnetic interactions between benzo-
phenone ketyl radicals. An examination of the AC magnetic
susceptibility data revealed no signature of magnetic ordering.
The differences in the magnetic behavior of
K2(C10H8)2(THF) and K(Ph2CO) is attributed to their crystal
structures. In the former case, the [C10H8]ꢀ radical anions
exhibit interactions with K+ cations in all three dimensions. It
is reasonable to suggest that magnetic coupling is mediated
by these cation–p interactions which serve to bring the
spin centers closer and hence increase dipolar interactions;
the result is magnetic ordering for K2(C10H8)2(THF) at
TN = 28.6 K.
Cubane formation can be viewed as the condensation of two
dimers in the solid state, since ketyls are thought to exist as dimers
in solution14 and have been isolated as dimeric species.15 The
cubane structure is similar to that obtained by Hou for potassium
fluorenone ketyl ([K(C13H8O)(HMPA)]4(m-HMPA)),12 in which
the K+ cations were stabilized by hexamethylphosphoric triamide
(HMPA) coordination. In this case, however, there is an addi-
tional HMPA molecule bridging two K+ cations above one face
of the cubane causing distortion from ideal Td symmetry. Hou
also described the structurally similar benzophenone ketyl species
(Na3(Ph2CO)3(HMPA)4),12 in which the ketyl O atoms bridge
Na+ cations; one [Ph2CO]ꢀ anion contains a m3-O atom, and the
other two contain m2-O atoms. The three Na+ cations are each
stabilized by HMPA coordination with an additional bridging
HMPA preventing cubane formation, resulting in a cuboidal-type
structure. This example clearly illustrates that coordinating
solvents affect the structure of these compounds.
In contrast, the packing motif in the crystal structure of
K(Ph2CO) is such that the cation–p interactions produce a
one-dimensional architecture. As previously mentioned, the
K+ cations form cubane-type units with O atoms of the
[Ph2CO]ꢀ anions, and these units are further connected into
infinite chains. The [Ph2CO]ꢀ anions project outward from the
K4O4 cubane units, illustrated in Fig. 5. Such an arrangement
prevents close cation–p contacts in the other two dimensions
hence magnetic coupling between the [Ph2CO]ꢀ radicals
that belong to different chains is negligible and long-range
magnetic ordering does not occur in K(Ph2CO).
In the crystal of K(Ph2CO), the K(Ph2CO) cubanes form
chains along the c-axis via four K+–p interactions between
phenyl rings and the nearest K+ centers located in the
adjacent K(Ph2CO) cubane (Fig. 2(b)). The average K–C
distance is 3.231(6) A, with a range of 3.118(5)–3.351(5) A.
The cubanes are oriented 901 to each other to allow these
interactions, which stabilize the structure by fulfilling the K+
coordination sphere.
The redox potentials of these isolated complexes agree
with previously published values.15 The UV-Vis absorption
spectrum of K(C10H8) exhibits bands at 364 and 434 nm, and
a broad feature centered at 800 nm, in agreement with
previously published values.16 The UV-Vis absorption spec-
trum of K(Ph2CO) exhibits bands at 326, 376 and 656 nm,
giving this radical its intense blue color. These bands have
been assigned to a D0 - D1 transition.17,18
The magnetic properties of the compounds were also
investigated. The wT value at 300 K for K2(C10H8)2(THF) is
0.71 emu molꢀ1 K, which is slightly lower than the value
of 0.75 emu molꢀ1 K expected for two non-interacting
S = 1/2 organic spins. The wT curve decreases gradually with
decreasing temperature and then abruptly increases below
30 K to a maximum value of 1.69 at 27 K; below this
temperature wT abruptly decreases to zero as shown in
Fig. 3(a). Similar behavior is observed for the temperature
dependence of magnetic susceptibility, which remains nearly
In conclusion, the compounds K2(C10H8)2(THF) and neat
K(Ph2CO) have been isolated and characterized in the solid
state for the first time. Naphthalenide and benzophenone ketyl
radical species are useful as strong reductants in preparative
chemistry, but they have a limited shelf life in solution;
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Fig. 3 Magnetic properties of K2(C10H8)2(THF). (a) Temperature dependence of wT; (b) temperature dependence of magnetic susceptibility (w).
Inset: the expanded 0–50 K region of the w vs. T dependence.
Notes and references
z Data reduction, structure solution and refinement calculations were
performed using the Bruker SAINT+ and SHELXTL NT program
packages. Crystal data for K(Ph2CO), C13H10KO, Mr = 221.31,
ꢀ
tetragonal, space group I4, a = 16.927(4), c = 7.271(2) A, V =
.
2083.3(9) A3, T = 213(2) K, Z = 8, l = 0.71073 A, m = 0.475 mmꢀ1
5597 reflections, 1767 unique (Rint = 0.088). Final R values: R1 =
0.0664 [I 4 2s(I)], wR2 = 0.0996 (all data). Flack parameter: 0.05(8).
Crystal data for K2(C10H8)2(THF), C24H24K2O, Mr = 406.63, mono-
clinic, space group C2/c, a = 17.865(3), b = 10.2540(15), c =
11.5701(16) A, b = 97.655(4)1, V = 2100.6(6) A3, T = 213(2) K,
Z = 4, l = 0.71073 A, m = 0.461 mmꢀ1. 5599 reflections, 1861
unique (Rint = 0.027). Final R values: R1 = 0.0417 [I 4 2s(I)],
wR2 = 0.0910 (all data).
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