The Electron as a Protecting Group. 3
J. Am. Chem. Soc., Vol. 123, No. 18, 2001 4191
organic layer was washed with water, 1 M HCl, water, saturated
NaHCO , and saturated NaCl, and then dried over MgSO and
3 4
Scheme 1. Synthesis of Acenaphthyne Radical Anion (9)
concentrated by rotary evaporation. The crude product was purified
by flash chromatography with hexanes as the eluting solvent to afford
1
0
.31 g (81%) of a yellow oil. H NMR (300 MHz, CDCl
3
) δ 7.87 (d,
J ) 8.1 Hz, 1H), 7.79 (d, J ) 8.1 Hz, 1H), 7.70 (d, J ) 6.6 Hz, 1H),
.62 (d, J ) 6.9 Hz, 1H), 7.61 (dd, J ) 8.1 and 6.9 Hz, 1H), 7.51 (dd,
7
1
3
J ) 8.1 and 6.6 Hz, 1H), 7.16 (s, 1H); C NMR (75 MHz, CDCl
1
1
3
) δ
38.3, 138.0, 129.0, 128.6, 128.0, 127.7, 127.1, 123.7, 123.5, 122.3,
20.8, 119.2; IR (neat) 3039, 1427, 1262, 1029, 832, 765, 727 cm
-
1
;
+
HRMS-CI (4% ammonia in methane mixture) (M + H) calcd for
C
12
H
1
8
Br 230.9809, obsd 230.9802.
-Trimethylsilylacenaphthylene (15). 1-Bromoacenaphthylene (0.59
g, 2.6 mmol) was dissolved in 60 mL of anhydrous THF and cooled to
78 °C. n-Butyllithium (2.5 M in hexanes, 1.1 mL) was added and
-
the mixture was stirred for 1 h. Chlorotrimethylsilane (0.9 g, 8 mmol)
was then added and the reaction was allowed to slowly warm to room-
temperature overnight. The crude product was diluted with hexanes
and washed with 1 M HCl and water. The organic material was dried
over MgSO and concentrated by rotary evaporation. Purification by
4
column chromatography with hexanes afforded 0.49 g (85%) of the
desired silane as a yellow oil. For the gas-phase experiments, the
compound was further purified by medium-pressure liquid chroma-
1
tography again using hexanes as the eluent. H NMR (300 MHz, CDCl
3
)
δ 7.79 (d, J ) 8.1 Hz, 2H), 7.74 (d, J ) 6.9 Hz, 1H), 7.66 (d, J ) 6.6
Hz, 1H), 7.55 (dd, J ) 8.1 and 6.9 Hz, 1H), 7.53 (dd, J ) 8.1 and 6.6
1
3
Hz, 1H), 7.25 (s, 1H), 0.39 (s, 9H); C NMR (75 MHz, CDCl
3
) δ
nature of stationary points was investigated by a full vibrational analysis.
Zero-point-energy corrections were made in all cases, and for computing
acidities the energies were adjusted to 298 K. The structures of
acenaphthyne (1) and cyclopentyne (16) and their alkene analogues
1
1
9
43.4, 143.2, 140.5, 137.9, 130.4, 128.5, 127.83, 127.77, 127.3, 126.9,
24.8, 123.6, -0.15; IR (neat) 3037, 2954, 1482, 1427, 1249, 1150,
31, 838, 770, 755 cm-1; HRMS-EI (M) calcd for C15
+•
H16Si 224.1021,
obsd 224.1042.
(10H and 17) were also investigated at the CAS(4,4)/cc-pVDZ and
Gas-Phase Experiments. All work was carried out in a dual cell
Finnigan Model 2001 Fourier transform mass spectrometer (FTMS)
equipped with a 3 T superconducting magnet and interfaced with a
custom-built Analytica electrospray ionization (ESI) source. Acenaph-
thylene dicarboxylate was sprayed (3 µL/min) into the gas phase from
a 750 µM solution of the diacid in methanol-water (35:65 v/v) which
contained 2 equiv of cesium hydroxide (pH 8-9). Ions were ac-
cumulated for 0.5 s in the hexapole of the ESI source and then allowed
to travel to the FTMS cell during a 45 µs period (time-of-flight). The
following typical settings for the ESI source were found to give optimal
signal of acenaphthylene dicarboxylate: cylinder (needle housing) 2.6
kV, end plate 3.6 kV, capillary 6.0 kV (front) and -36 V (back),
skimmer cone -11 V, acceleration lenses 319 V, deceleration lenses
CAS(2,2)/cc-pVDZ levels of theory, respectively, and the energies were
corrected with zero-point energies from BPW91/cc-pVDZ optimized
42,43
geometries.
For these calculations, the active space was comprised
of the C1-C2 π bonding and antibonding orbitals. Dynamic electron
correlation was accounted for by carrying out CASPT2 calculations
44
on the CAS structures.
Results and Discussion
We have generated the radical anion of acenaphthyne (9) in
a Fourier transform mass spectrometer (FTMS) and explored
its reactivity and thermochemistry to gain insight into the
corresponding neutral cyclopentyne (i.e., 1). A methodology
1
9.0 V, and high voltage element in acceleration/deceleration lens stack
.35 kV. Fluoride ion was prepared by electron ionization of carbon
recently developed in our laboratory was used to prepare 9
1
31
(
Scheme 1). Specifically, dicarboxylate 12 (m/z 119) was
tetrafluoride at 6 eV and used to generate 10 and 13 upon reaction
with 1-trimethylsilylacenaphthylene and acenaphthenone, respectively.
In general, ions of interest were isolated by ejecting unwanted species
sprayed from a basic solution of diacid 11 into our FTMS where
it was isolated and then fragmented by sustained off-resonance
45
3
8
39
irradiation (SORI). This technique involves kinetically exciting
an ion by applying energy to its cyclotron frequency off-
resonance in the presence of an inert collision gas. In this case,
application of 1.3 eV (lab) of energy for 30 ms concurrent with
with a SWIFT waveform or a chirp broad band excitation for low
-
5
masses and were vibrationally cooled with pulses of argon (10 Torr).
Neutral reagents were introduced via slow leak or pulsed valves, and
all reactions were monitored as a function of time.
Computations. All calculations were performed with Gaussian9840
installed on IBM and SGI workstations. Geometries were optimized
by using the B3LYP functional and the 6-31+G(d) basis set,41 and the
-5
a pulse of argon (∼10 Torr) led to the loss of carbon dioxide
and an electron (m/z 194). Further excitation (1.1 eV (lab) for
1
0 ms) afforded the desired ion 9 (m/z 150, Scheme 1, and
Figure 2). On-resonance irradiation of 12 gives 9 directly, but
the efficiency of this process is considerably lower than that of
the stepwise route. In addition to the loss of an electron and
carbon dioxide, electron detachment of dicarboxylate dianion
(
38) Wang, T. C. L.; Ricca, T. L.; Marshall, A. G. Anal. Chem. 1986,
5
8, 2935-2938.
(
39) Marshall, A. G.; Roe, D. C. J. Chem. Phys. 1980, 73, 1581-1590.
(40) Frisch, M. J.; Trucks, G. W.; Schlegel, H. B.; Scuseria, G. E.; Robb,
M. A.; Cheeseman, J. R.; Zakrewski, V. G.; Montgomery, J. A., Jr.;
Stratmann, R. E.; Burant, J. C.; Dapprich, S.; Millam, J. M.; Daniels, A.
D.; Kudin, K. N.; Strain, M. C.; Farkas, O.; Tomasi, J.; Barone, V.; Cossi,
M.; Cammi, R.; Mennucci, B.; Pomelli, C.; Adamo, C.; Clifford, S.;
Ochterski, J.; Petersson, G. A.; Ayala, P. Y.; Cui, Q.; Morokuma, K.; Malick,
D. K.; Rabuck, A. D.; Raghavachari, K.; Foresman, J. B.; Cioslowski, J.;
Oritz, J. V.; Baboul, A. G.; Stefanov, B. B.; Lui, G.; Liashenko, A.; Piskorz,
P.; Komaromi, I.; Gomperts, R.; Martin, R. L.; Fox, D. J.; Ketih, T.; Al-
Laham, M. A.; Peng, C. Y.; Nanayakkara, A.; Gonzalez, C.; Challacombe,
M.; Gill, P. M. W.; Johnson, B.; Chen, W.; Wong, M. W.; Andres, J. L.;
Gonzalez, C.; Head-Gordon, M.; Replogle, E. S.; Pople, J. A. Gaussian
1
2 without fragmentation to yield the corresponding radical
anion at m/z 238 is a minor dissociation pathway.
(42) (a) Becke, A. D. Phys. ReV. A 1988, 38, 3098-3100. (b) Perdew,
J. P.; Burke, K.; Wang, Y. Phys. ReV. B 1996, 54, 16533-16539.
(43) (a) Dunning, T. H., Jr. J. Chem. Phys. 1989, 90, 1007-1023. (b)
Kendall, R. A.; Dunning, T. H., Jr.; Harrison, R. J. J. Chem. Phys. 1992,
96, 6796-6806.
(44) Andersson, K.; Borowski, P.; Fowler, P. W.; Malmqvist, P.-Å.; Roos,
B. O.; Sadlej, A. J. Chem. Phys. Lett. 1992, 190, 367-373.
(45) Gauthier, J. W.; Trautman, T. R.; Jacobson, D. B. Anal. Chim. Acta
1991, 246, 211-225.
9
8, Revision A.7; Gaussian, Inc.; Pittsburgh, PA, 1998.
41) Becke, A. D. J. Chem. Phys. 1993, 98, 5648-5652.
(