Journal of the American Chemical Society
Article
(
50 mL), water (50 mL), saturated NaHCO (50 mL), and brine (50
the internal standard 1,4-difluorobenzene (−124.27 ppm), 1 (−153.02
ppm), and 1a (−153.74 ppm) were integrated. At various points
throughout the course of the reaction, the same NMR tube was heated
in a steam bath, cooled, and analyzed by 19F NMR spectroscopy as
3
mL). The organic fraction was dried (Na SO ) and concentrated to
afford a syrupy residue. The protected HFIP solvolysis product (R =
0
2
4
f
.29) and 2,3,4-tri-O-acetyl-1,6-anhydro-β-D-glucopyranose (R = 0.13)
f
were purified via column chromatography [3:7 (v/v) EtOAc/hexanes].
Each product was treated with freshly prepared NaOMe in MeOH
described above. The resultant fraction of reaction (F ) and individual
1
peak areas were analyzed using a nonlinear least-squares fit to eq 1. Of
note, the intense 19F signal corresponding to HFIP (−78.66 ppm)
does not overlap or interfere with the peaks of interest. All other KIEs
(
∼0.5 M, 10 mL). The reaction mixtures were neutralized with
+
Amberlite IR-120+ resin (H form), filtered, and concentrated to
2
afford 4 (α-GluHFIP) and 5 (1,6-anhydro-β-D-glucopyranose).
were determined relative to the α- H KIE using eq 2
1
,1,1,3,3,3-Hexafluoropropan-2-yl α-D-glucopyranoside (4): mp
2
0
1
R
R
0
1
25−126 °C; [α] = +89.8 (c 0.017, H O); H NMR (600 MHz,
(1/KIE−1)
D
2
= (1 − F1)
D O) δ 5.20 (d, J = 3.3, 1 H, H-1), 5.10 [m, 1 H, OCH(CHF ) ], 3.76
(1)
2
3
2
(
3
m, 1 H, H-6), 3.74−3.64 (m, 3 H, H-3, H-6′, H-5), 3.57 (dd, J = 10.0,
.8, 1 H, H-2), 3.40 (t, J = 9.5, 1 H, H-4); C NMR (151 MHz, D O)
13
1D
2
KIE
= k
H
δ 121.84 (q, JCF = 62.6, −CF ), 119.97 (q, J = 65.5, −CF ), 100.31
KIE = Rel
3
CF
3
k
(2)
(
6
3
C-1), 72.54, 72.00 (septet, JCF = 32.4, −CHCF ) 71.67, 70.34 (C-2),
KIE
x
3
+
8.55, 59.70 (C-6); HRMS (M + Na ) C H F O requires m/z
9 12 6 6
where 1DKIE is the α- H isotope effect (k
k ) is the relative isotope effect measured in the competitive
experiment between 1a and another labeled α-GluF. In these
calculations, 1a is treated as the “heavy” isotopologue such that the
ratio of 1DKIE and KIE will give the KIE for x (i.e., x = 1b). All
calculations of standard deviations on KIE values computed using eq 2
involved standard propagation of the errors associated with the
2
/k ) and RelKIE (kx/
unlabeled 1D
53.0430, found m/z 353.0443.
,6-Anhydro-β-D-glucopyranose (5): [α]
20
1D
1
= −67.6 (c 0.017,
D
22
1
H O) (lit. = −66.0); H NMR (600 MHz, D O) δ 5.38 (s, 1 H, H-
2
2
1
), 4.56 (d, J = 5.7, 1 H, H-5), 4.02 (d, J = 7.7, 1 H, H-6), 3.69 (m, 1
Rel
13
H, H-6′), 3.62−3.59 (m, 2 H, H-3, H-4), 3.45 (s, 1 H, H-2); C NMR
151 MHz, D O) δ 100.96 (C-1), 75.78 (C-5), 72.01 (C-3), 70.32 (C-
), 69.69 (C-2), 64.71 (C-6); HRMS (M + Na ) C H O requires m/
z 185.0420, found m/z 185.0420.
(
4
2
+
6 10 5
1D
Rel
23
measured values of KIE and KIE.
Simultaneous Measurement of Three KIEs. A 5 mm NMR tube
was charged with a solution of 1 (∼0.3 mg), 1a (∼0.3 mg), 1b (∼0.3
mg), and 1f (∼0.6 mg) in DMSO-d (50 μL), 1,4-difluorobenzene (0.2
6
μL), 2,6-lutidine (4.8 μL), and HFIP (600 μL). A protocol identical to
2
2
13
that described above was used to measure 1- H, 2- H, and 1- C KIEs
simultaneously.
Solvent KIE. A solution of 1 (16 mg) in DMSO-d (75 μL) was
6
Solvolysis Product Stability. To show that α-GluHFIP is stable
to the solvolysis conditions, α-GluHFIP (10 mg) was dissolved in
HFIP (2 mL) and the solution sealed in an ampule that was heated in
added to a flask charged with HFIP (12 mL) and 2,6-lutidine (25 μL).
The solution was distributed evenly into 14 prescored ampules that
were subsequently sealed. Samples containing HFIP-d were prepared
in an identical manner. These two sets of ampules were heated in a
steam bath, and every 5 min, samples were removed and cooled in an
ice bath. The observed rate constants were calculated as described in
Activation Parameters.
1
a steam bath for 12 h. Subsequent H NMR spectroscopic analysis in
D O of the nonvolatiles showed no 1,6-anhydroglucose. In addition,
2
1
,6-anhydroglucose was shown to be stable under the reaction
conditions by being heated a sealed ampule containing it (∼1 mg),
DMSO (15 μL), and 2,6-lutidine (4 μL) in HFIP (600 μL) at 100 °C
for 2 h. After removal of the volatiles, the residue was dissolved in
1
THEORETICAL CALCULATIONS
D O, and analysis by H NMR spectroscopy showed that no reaction
2
■
had occurred.
Computational Analysis. Calculations for the HFIP
solvolysis of α-GluF were performed using Gaussian 09 and
the B3LYP method with a 6-31G* basis set. All TS structures
were calculated in the gas phase at 373 K. The α-GluF ground
Activation Parameters. Ampules were charged with 1 (1 mg) in
DMSO (5 μL), HFIP (1 mL), and 2,6-lutidine (1.5 μL). After being
sealed, the ampules were heated in a “reflux chamber” equipped with a
still pot containing an appropriate solvent. The temperature
dependence of the reaction was determined by monitoring the rate
of solvolysis at 56, 65, 82, and 100 °C by suspending the ampules in
the vapors of boiling acetone, methanol, 2-propanol, and water,
respectively. Samples were removed after various time intervals and
cooled in an ice bath. The contents were transferred to a flask, from
24
4
state structure was optimized beginning from several C
1
conformations to ensure that the calculated structure is a
local minimum. In addition, ground state structures with a
hydrogen bond between the C2 hydroxyl group and the
anomeric fluorine atom were not considered to ensure that the
intramolecular H−O···H hydrogen bonding arrangement,
which mainly results from the system being calculated in
vacuo, is the same in the TS as it is in the ground state. With
regard to the TS structures for ionization of α-GluF, an HFIP
which the volatiles were removed under reduced pressure. The residue
1
was dissolved in D O (650 μL) and analyzed by H NMR
2
spectroscopy. The anomeric proton chemical shifts for 1 (5.62
ppm), 4 (5.19 ppm), and 5 (5.38 ppm) were integrated and
normalized. The normalized ratio of 1 was fit to a standard exponential
one-phase decay using a nonlinear regression algorithm.
́
molecule was positioned 4 Å from the fluoride leaving group
2
19
and allowed to optimize. Subsequently, the C−F bond distance
was incrementally increased and constrained to locate TS
structures that had one imaginary frequency. In addition, a TS
structure with an HFIP catalyzing the departure of the fluoride
KIE Measurements. The α- H KIE was determined via F NMR
2
0
spectroscopy on a Bruker AVANCE III 500 MHz spectrometer. A 5
mm NMR tube was charged with 1 (∼1.5 mg), 1a (∼1.5 mg), DMSO-
d (15 μL), 1,4-difluorobenzene (1.5 μL), 2,6-lutidine (4.8 μL), and
6
HFIP (650 μL). The NMR tube was flame-sealed, and an initial NMR
in a backside S 2 reaction that generates 1,6-anhydro-β-D-
N
spectrum was recorded with the sample temperature maintained at 298
glucopyranose was located by constraining the O6−C1
distance, a protocol that was necessary to prevent re-formation
of the starting material. The ground state for 1,6-anhydroglu-
cose was optimized from several starting geometries.
Calculations were performed using the same conditions and
level of theory. All TS structures were recalculated at the
MP2(full)/6-31G* level of theory using the B3LYP geometric
19
K. Each quantitative proton-decoupled and -coupled F NMR
spectrum was acquired using a gated pulse sequence. Spectra
consisting 128 scans (acquisition time of 0.35 s) were recorded with
a recycle delay of 2.5 s between scans (6.1 min per spectrum). The
baseline was corrected to remove baseline distortions that are typically
associated with 19F spectra using the Whittaker Smoother method
19
found in MestReNova version 6.2. The F signals corresponding to
1
214
dx.doi.org/10.1021/ja209339j | J. Am. Chem.Soc. 2012, 134, 1212−1220