Department of Pharmacology, University of Virginia,
Charlottesville, Virginia (J.C.G., E.P.-R.)
 |
Introduction |
Generalized,
or petit mal, absence epilepsies are characterized by periods of
synchronized neuronal activity, generating a 3-Hz spike-wave pattern on
the electroencephalogram. Considerable evidence suggests that
spike-wave discharges are produced by synchronized oscillations of
cortical, reticular thalamic, and corticothalamic neurons (Gloor and
Fariello, 1988
; Steriade et al., 1993
). Oscillatory firing of
corticothalamic neurons requires the activity of low threshold
Ca2+ spikes (LTS; Steriade and Llinas, 1988
;
McCormick and Bal, 1997
),which are produced by T-type
Ca2+ channels (Crunelli et al., 1989
; Suzuki and
Rogawski, 1989
).
Ethosuximide is considered the prototypical absence seizure drug that
works by inhibition of T-type channels. This hypothesis was based on
the finding that ethosuximide could partially block T-type currents in
thalamic neurons at therapeutically relevant concentrations (Coulter et
al., 1989a
). Support for this hypothesis came from studies with
related analogs: 1) T-type current block was also observed at
therapeutically relevant concentrations of methyl-phenylsuccinimide
(MPS), the active metabolite of methsuximide; and 2) no block was
observed using either the inactive analog succinimide or the convulsant
analog tetra-methylsuccinimide (Coulter et al., 1990a
). The
sensitivity of T-type channels to MPS has been confirmed using dorsal
root ganglion neurons (Todorovic and Lingle, 1998
). With one exception
(Kostyuk et al., 1992
), other studies have failed to confirm
ethosuximide block of T-type currents at therapeutically relevant
concentrations (Todorovic and Lingle, 1998
), leading to the suggestion
that block of other ionic channels may be more relevant (Leresche et
al., 1998
).
Many factors interfere with the pharmacological characterization of
native T-type channels, such as interference from other ionic
conductances, the lack of highly selective blockers, and adequate
voltage control. Most studies have been performed in isolated neurons
that have lost their dendritic trees and, hence, most of their T-type
channels (Destexhe et al., 1998
). We have recently cloned the cDNAs of
three T-type Ca2+ channels (
1G,
Cav3.1;
1H, Cav3.2; and
1I, Cav3.3), and we now report the cloning of
human
1I (Perez-Reyes, 1999
; Cribbs et al., 2000
). Expression of the
cloned channels in HEK-293 cells provides an excellent assay system to
test the pharmacology of T-type currents, since they contain very
little background currents under appropriate assay conditions. We
report for the first time the block of human T-type channels by two
succinimide antiepileptic drugs, ethosuximide and MPS, the active
metabolite of methsuximide. Our results show that block is
state-dependent, with less block observed at highly hyperpolarized
holding potentials. This finding may partially explain the controversy
of whether ethosuximide block of T-type currents is therapeutically relevant.
 |
Experimental Procedures |
Materials.
The following stably transfected HEK-293 cell
lines were used in this study: h
1G-Q39, containing the human
1G
channel, Cav3.1a (GenBank accession number
AF190860; Cribbs et al., 2000
); h
1H-Q31, containing the Hh7 plasmid
construct of human
1H, Cav3.2 (GenBank accession number AF073931; Cribbs et al., 1998
); and h
1I-14, containing the LT4 plasmid construct of
1I,
Cav3.3 (described below). All chemicals were from
either Sigma (St. Louis, MO) or Aldrich (Milwaukee, WI).
Cloning of a Human
1I-cDNA.
Human brain cDNA libraries
derived from either fetal brain or cerebellum (CLONTECH, Palo Alto, CA)
were screened using the rat
1I as probe. Screening was done by
filter hybridization according to the manufacturer's protocol. The
cDNA probes were synthesized using
[
-32P]dCTP and the Ready-To-Go labeling kit
(Amersham Pharmacia Biotech Piscataway, NJ). Positive clones were
plaque-purified and then subcloned into pUC18 for sequencing. BLAST
searches of the GenBank with the rat
1I identified the genomic DNA
encoding the human CACNA1I gene (AL022312), allowing us to design PCR
primers to clone the 5' end. Overlapping clones were selected and
ligated in the vector pcDNA3 (Invitrogen, Carlsbad, CA), generating the clone LT4. The nucleotide sequence of human
1I has also been reported by two groups (Mittman et al., 1999
; Monteil et al., 2000
).
The sequence of LT4 is similar to that reported in AF211189, in that it
lacks putative exon 9, but is longer at the 3' end, extending to
nucleotide 6214 of AF393329.
Generation of a Stably Transfected Cell Line.
Stable cell
lines expressing human
1I were constructed by transfecting HEK-293
cells with linearized LT4 plasmid. HEK cells were maintained in DMEM,
10% fetal bovine serum, 100 U/ml penicillin, and 100 µg/ml
streptomycin. Cells were plated at a density of 1 × 106 per 100-mm plate. One day later, fresh media
was added, and the cells were transfected with 10 µg of plasmid DNA
by the calcium phosphate method (CalPhos Maximizer Transfection Kit,
CLONTECH) according to the manufacturer's protocol. Following
transfection, the cells were selected in 1.0 mg/ml G-418 (Invitrogen)
for 2 to 3 weeks. Single colonies were isolated, expanded, and then screened electrophysiologically for the expression of T-type
Ca2+ current. One clone, h
1I-14, was selected
for further study.
Electrophysiological Analysis of HEK-293 Transfected Cells.
HEK-293 cells were dissociated by digestion with 0.25% trypsin plus 1 mM EDTA for 2 min and then diluted 20-fold with DMEM. The cells were
triturated, diluted 2-fold with DMEM, and then plated on cover slips.
The cells were incubated at least 4 h and up to 2 days before
electrophysiological studies. The standard internal pipette solution
contained 135 mM CsCl, 10 mM EGTA, 4 mM Mg-ATP, 0.3 mM
Na3GTP, and 10 mM HEPES, pH adjusted to 7.3 with
CsOH. Most experiments were performed using the following solution: 5 mM CaCl2, 155 mM tetraethylammonium (TEA)
chloride, and 10 mM HEPES, pH adjusted to 7.4 with TEA-OH. As noted in
the figure legends, some experiments were performed using
Ba2+ as charge carrier in 10 mM
BaCl2, 160 mM TEA chloride, 6 mM CsCl, and 10 mM
HEPES, pH adjusted to 7.4 with TEA-OH. Addition of 1 mM
Mg2+ to the external solution had no effect on
the block of either
1G or
1I produced by 3 mM MPS.
Whole cell currents were recorded from HEK-293 cells using the ruptured
patch method on two electrophysiological set-ups. One set-up consisted
of an Axopatch 200B amplifier, Digidata 1200 A/D converter, and pCLAMP
8.0 software (Axon Instruments, Foster City, CA). The second set-up
used an Axopatch 200A amplifier, Digidata 1200 A/D converter, and
pCLAMP 6.0 software (Axon Instruments). Data were digitized at 4 to 50 kHz and filtered at 1 to 5 kHz. Recording pipettes were made from
TW-150-6 capillary tubing (World Precision Instruments, Inc., Sarasota,
FL), using a model P-97 Flaming-Brown pipette puller (Sutter Instrument
Co., Novato, CA). Once filled with the internal solution the pipette
resistance was typically 1.5 to 2.5 M
. Series resistance (initially
between 2 and 5 M
) was compensated 70 to 80% and adjusted between
protocols if necessary. Leak currents were minimal; therefore leak
subtraction was not used. The average cell capacitance was ~25 pF.
All experiments were performed at room temperature.
Dose-Response Analysis.
Succinimide analogs were freshly
dissolved in external solution at a concentration of either 30 or 100 mM and then diluted in 10-fold increments. The recording chamber was a
RC-25 (Warner Instrument Corp., Hampden, CT), which has a volume of
0.15 ml. Each test solution was perfused at 1 to 3 ml/min.
Data Analysis.
Peak currents and exponential fits to
currents were determined using Clampfit software (Axon Instruments).
Dose-response analysis and graphing of the data were with Prism
(GraphPad, San Diego, CA). The following equation was used to fit
dose-response data
where X is the logarithm of concentration and
Y is the response. The voltage dependence of activation was
calculated using the solver function of Excel (Microsoft, Redmond, WA)
to minimize the residual sum of squares from the simultaneous fit of
the data with the Goldman-Hodgkin-Katz equation (Hille, 1992
)
and a Boltzmann equation
where PCa is the
Ca2+ permeability; z, the valence of
the Ca2+ ion; V, the test potential;
V1/2, the mid-point of activation; F, Faraday's constant; R, the gas constant;
T, absolute temperature; [Ca2+]i, intracellular
Ca2+ concentration (25 nM);
[Ca2+]o, extracellular
Ca2+ (5 mM); and k is the slope
factor. Values are reported as the means ± S.E.M.
 |
Results |
Cloning of a Human
1I-cDNA.
The human gene encoding
Cav3.3 (
1I), CACNA1I, was
identified using homology searches of the GenBank HTGS database (Lee et al., 1999a
). This sequence information was originally used to clone the rat
1I-cDNA. We then used the rat cDNA to screen human brain cDNA libraries. Overlapping cDNAs were assembled to produce a
6,268-base pair cDNA (LT4-pcDNA3) that encodes a protein of 220,706 Da.
The cloning of human
1I was previously reported by Monteil et al.
(2000)
. As noted under Experimental Procedures, our clone
contains additional coding sequence at the 3' end. Transient transfection studies indicated that LT4 encoded a functional low voltage-activated Ca2+ channel with similar
electrophysiological characteristics as observed with the rat (Lee et
al., 1999a
). The LT4 plasmid was then used to generate stably
transfected cell lines, and h
1I-14 was chosen for further study.
Ethosuximide Block of Cloned T-Type Ca2+ Channels.
The effect of ethosuximide was tested on human T-type currents using
whole cell recording from HEK-293 cell lines that were stably
transfected with Cav3.1 (
1G),
Cav3.2 (
1H), or Cav3.3 (
1I). Currents were measured using either 5 mM
Ca2+ or 10 mM Ba2+ as
charge carrier and Cs-based intracellular solutions that contain ATP.
Under these recording conditions the current density is approximately 40 pA/pF, such that the typically sized cell has 1000 pA of current during a test pulse to
30 mV. The size of the currents is quite stable for most recordings, although there is some run-up observed immediately after establishment of the whole cell clamp and some run-down after ~15 min of recording. Therefore, the stability of the
currents was monitored in all experiments, and results are only
presented for cells whose run-down rate was less than 2%/min. The
effects of compounds were tested by dissolving each compound directly
in external solution and then perfusing the compound over the
cell. Various concentrations were tested on each cell without
(Fig. 1, A and B) or with (Fig.
2) washout between concentrations. Little difference was
observed among the results obtained with these two protocols, so the
results have been pooled. The ethosuximide dose-response curve for
block of human
1G currents is shown in Fig. 1C. The data were fit
with the dose-response equation, yielding an apparent
IC50 of 10 ± 2 mM (n = 31 cells). Similar results were obtained using 5 mM
Ca2+ as the charge carrier
(IC50 = 12 ± 2 mM, n = 16 cells). The response to concentrations below 1 mM was greater than
expected from simple binding of a drug molecule to a single site on the
channel. Since the deviation occurred in the therapeutic range of
plasma ethosuximide concentrations (40-100 µg/ml or 0.3-0.7 mM;
Browne et al., 1975
), these measurements were repeated extensively.
Clear inhibitory effects of ethosuximide could be detected with
concentrations as low as 0.1 mM (Fig. 1D). The response to 100 mM also
deviated from the fit. Since such a high concentration alters the
osmolarity of the external solution and might cause a nonspecific
effect, we adjusted for this by reducing the TEA concentration. In
either case the block was 100%. Although the data are consistent with two binding sites, an alternative hypothesis is that ethosuximide block
is state-dependent (Hille, 1992
).

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Fig. 1.
Inhibition of human 1G T-type Ca2+
channels by ethosuximide. A, representative whole cell recordings
showing the effect of various concentrations of ethosuximide on T-type
currents. Whole cell Ba2+ (10 mM) currents recorded from an
HEK-293 cell stably transfected with 1G subunit in response to
voltage steps to 30 mV from a holding potential of 90 mV applied
every 10 s. B, time course of peak currents normalized to control
for the same cell shown in A. Ordinate axis, peak current during
steady-state exposure to ethosuximide, normalized by the peak current
before drug exposure, defined as the fraction of
IBa remaining. C, dose-response relationship
for ethosuximide block. Fraction of unblocked peak current is plotted
against drug concentration. Number of cells investigated for each
concentration is indicated near each data point. Data were fitted
(smooth line) using a Hill equation (see Experimental
Procedures). Note that data points representing drug
concentrations lower that 1 mM deviated significantly from the fitted
curve. D, inhibitory effect of 0.1 mM ethosuximide on peak currents
averaged from five cells.
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Fig. 2.
Inhibition of human T-type Ca2+ channels
by MPS. A, representative whole cell recordings showing the effect of
various concentrations of MPS on T-type currents. Whole cell
Ca2+ (5 mM) currents recorded from an HEK-293 cell stably
transfected with 1I subunit in response to voltage steps to 30 mV
from a holding potential of 90 mV applied every 10 s. B, time
course of peak current for the same cell shown in A. C, dose-response
relationship for MPS block on Ca2+ currents expressed by
1G, 1H, and 1I channels. Fraction of unblocked peak current is
plotted against drug concentration. IC50 values from fitted
data (smooth lines) using a Hill equation were: 1G, 1.95 ± 0.2 mM; 1H, 3.03 ± 0.26 mM; and 1I, 1.82 ± 0.16 mM.
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Methyl-Phenylsuccinimide Block of Cloned T-Type Channels.
The
antiepileptic drug methsuximide is rapidly demethylated to
N-desmethylmethsuximide, which is also called MPS.
Therapeutic plasma levels of MPS in well controlled patients range
between 10 and 40 µg/ml or 50 and 200 µM (Strong et al., 1974
;
Porter et al., 1979
; Wilder and Buchanan, 1981
). The sensitivity of
human T-type channels to block by MPS was measured as above. Figure 2
shows the time course of a typical experiment using
1I. MPS produced
a rapid block of current, which was rapidly and almost completely
reversed upon washout. The dose-response relationship of MPS block of
the three cloned human T-type channels was measured using the peak
Ca2+ current elicited during a pulse to
30 mV
(Fig. 2C) from a holding potential of
90 mV. The
1G and
1I
channels were equally sensitive, displaying apparent
IC50 values of 1.95 ± 0.19 (n = 7 cells) and 1.82 ± 0.16 mM
(n = 14 cells), respectively, whereas
1H channels were slightly less sensitive (IC50 = 3.0 ± 0.3 mM, n = 6 cells). The Hill coefficients were
significantly greater than one: ~1.3 for
1G and
1I and 1.7 for
1H. As observed with ethosuximide, these results suggested that
block was more complex than simple 1:1 binding of drug to
channel/receptor; therefore we investigated the mechanisms by which the
succinimide antiepileptics blocked the channels.
Block Is Voltage-Dependent.
Current-voltage relationships
(I-V curves) for
1I were measured using 500-ms step
depolarizations to varying potentials from a holding potential of
90
mV. Typical current traces are shown in Fig.
3A, measured before (C) and during (M)
exposure to 3 mM MPS. Average I-V curves are shown in Fig.
3B (n = 4 cells). The percent block of the peak current
was calculated, and then plotted as a function of the test potential
(Fig. 3C). MPS block was greatest during test potentials to
50 mV,
and then gradually decreased at more positive potentials. To calculate
the V1/2 of activation, the permeability of
the channels was estimated using constant field equations (Hille, 1992
)
and fit with a Boltzmann equation. MPS produced an apparent +7 mV
shift, which was reversed upon washout
(V1/2 in mV): control,
41 ± 1; MPS,
34 ± 1; and washout,
41 ± 2. Somewhat surprisingly, the
outward currents, which are due to Cs+ efflux
through the T-type channel (Lee et al., 1999a
), were hardly blocked at all. These results indicate that MPS affects the voltage dependence of gating, and that it interacts with the permeant ion.

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Fig. 3.
Voltage-dependent block of MPS. A, sample records
obtained at the indicated values of Vm from
a holding potential of 100 mV. Current traces were obtained from an
HEK-293 cell stably expressing 1I channels in the absence (C) and in
the presence of 3 mM MPS (M). Charge carrier was 5 mM Ca2+.
B, current-voltage relationships of 1I channels obtained before
( ), in the presence of 3 mM MPS ( ), and after washout the drug
( ). Data points are averages of five cells. The smooth lines are
spline curves fit to the calculated values of current using the product
of the Goldman-Hodgkin-Katz and Boltzmann equations (see
Experimental Procedures). C, percent block of peak
current as a function of test potential; from same cells shown in B. Data are not shown for voltages near the reversal potential.
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Closer inspection of the current traces revealed that MPS was capable
of affecting the decay of the
1I currents. To illustrate this
effect, the currents recorded during test pulses to
30 mV were scaled
and superimposed (Fig. 4A). Two effects
can be observed: 1) MPS accelerated the apparent inactivation rate; and
2) MPS totally abolished the sustained component of current. To
quantify the effect on kinetics, the entire current trace was fit with two exponentials, one corresponding to activation and the other to
inactivation. The inactivation
was plotted as a function of test
potential in Fig. 4B. MPS had no effect on the relatively slow
inactivation rate observed during test pulses to
50 mV, but
accelerated the rate greater than 2-fold during pulses in the range of
30 to +20 mV. Currents measured after washout of the drug inactivated
in the same manner as control. The MPS effect on inactivation was
dose-dependent, with less effect observed using 1 mM (Fig. 4C). MPS was
also capable of accelerating the apparent inactivation rate of
1G
and
1H in a dose-dependent manner (Fig. 4C).

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Fig. 4.
MPS accelerates decay of human T-type currents. A,
superimposed current traces at 30 mV from the same cell illustrated
in Fig. 3. MPS (3 mM) and wash traces were normalized to the amplitude
of the control trace. Current signals plotted with dots and solid lines
represent fits with two exponentials, one for the activation and the
other for the inactivation of the current. B, voltage dependence of the
inactivation in the three conditions. Current traces obtained in
response to an I-V protocol like in Fig. 3A were fitted
as mentioned above, and the respective inactivation time constant was
plotted as a function of voltage for the indicated experimental
conditions. C, concentration-dependent effect of MPS on inactivation
. Inactivation time constants were obtained as described in B for
1G, 1H, and 1I currents at 30 mV and were plotted versus the
concentration of MPS.
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In contrast to its effects on inactivation, MPS did not have a
significant effect on the rate of recovery from inactivation of
1G
(data not shown). Inactivation was induced by either short (100-ms)
prepulses to
30 mV or long (10-s) prepulses to
50 mV. Recovery at
100 mV was measured by changing the interval between the prepulse and
the test pulse. Recovery from short prepulses were well fit with a
single exponential in both control (87 ± 2 ms) and in the
presence of 3 mM MPS (86 ± 2 ms, n = 3 cells). Recovery from long prepulses was significantly better fit with two
exponentials in both the absence and presence of 3 mM MPS (
1 = 116 ms,
2 = 1.2 s, n = 3 cells). In both cases, the percent block at each time point was relatively constant, indicating that drug
bound channels remained blocked.
Ethosuximide also accelerated the decay of the current during a
depolarizing pulse. Representative current traces are shown in Fig.
5A and were scaled for comparison in Fig.
5B. Although both
1G and
1H exhibit measurable sustained currents
using Ca2+ as charge carrier (Klöckner et
al., 1999
; Serrano et al., 1999
), these currents are too small to
measure drug effects. The
1I currents display more of a sustained
component, and this component was extremely sensitive to both
succinimide antiepileptics (Figs. 2B, 4A, and 5B). To quantify this
effect, we measured the amount of ethosuximide block that occurs after
150 ms of depolarization, and compared that with the block of the peak
current. The ethosuximide dose-response relationships on block of
1I
channels are shown in Fig. 5C. The apparent IC50
for block of the persistent current was 13-fold lower, dropping from
8 ± 2 to 0.6 ± 0.2 mM (n = 8 cells).

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Fig. 5.
Ethosuximide accelerates decay of human T-type
currents. A, effect of increasing concentrations of ethosuximide on
Ba2+ currents recorded from a HEK-293 cell stably
transfected with 1I subunit in response to voltage steps to 20 mV.
Dotted line corresponds to the washout of the drug. B, same traces as
in A normalized to the control amplitude. C, dose-response relationship
for ethosuximide block of Ba2+ currents measured at peak
( ) and after 150 ms of depolarization ( ). Smooth lines represent
the fitted curve using the Hill equation. The calculated
IC50 values were 8 ± 2 and 0.6 ± 0.2 mM for the
peak and the sustained current, respectively.
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Block Is State-Dependent.
The modulated receptor hypothesis
was based on observations that drugs had varying affinities for
closed/rested and inactivated states. Binding to inactivated states is
an important property of drugs because it can provide selectivity to
their action, as clearly exemplified by dihydropyridines that
preferentially block smooth muscle L-type channels with little effect
on cardiac channels (Triggle, 1999
). Voltage-gated
Ca2+ channels do not need to open before
inactivating, and transitions from closed to inactivated states can be
measured using long prepulses at subthreshold potentials, commonly
referred to as the steady-state inactivation curve, or
h
. Drugs that bind and stabilize the
inactivated state shift the equilibrium from closed/rested to
inactivated states, and hence shift this steady-state inactivation curve to more negative voltages (Bean et al., 1983
). The effect of MPS
and ethosuximide on the inactivation curves of the three T-type
channels was estimated using prepulses of the following duration:
0.3 s for
1G (Fig. 6A); 5 s
for
1H prepulses (Fig. 6, C and D); and 30 s for
1I (Fig.
6B) and
1G (Table 1). In each case,
MPS was capable of shifting the curve 5 to 10 mV to more negative
potentials. The amount of shift was dose-dependent; 1 mM MPS shifted
the
1G curve
5.5 mV (data not shown), whereas 3 mM shifted it
9.5 mV (Table 1). Similar results were obtained using 10 mM
ethosuximide, which shifted the
1H inactivation curve 5 mV toward
more negative potentials (Fig. 6D). Reversal of this effect by washing
out the drug was in many cases incomplete. This is due in part to
time-dependent shifts in the inactivation curve, which can be largely
prevented by inclusion of ATP in the intracellular pipette solution
(Zhang et al., 2000
). The lack of full reversal may also be due to
residual drug in the bath.

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Fig. 6.
MPS and ethosuximide shift the voltage dependence of
steady-state inactivation of human T-type Ca2+ channels.
Steps lasting 0.3 s ( 1G), 5 s ( 1H), and 30 s
( 1I) to the indicated voltages were followed by 150-ms test pulses
to 30 mV in A and B or 20 mV in C and D. Protocols were run before
( ), during, and after ( ) exposure to 3 mM MPS ( ) or 10 mM
ethosuximide ( ). Charge carrier was 5 mM Ca2+ in A and
B, and 10 mM Ba2+ in C and D. Currents were normalized to
the value at 100 mV at each experimental condition. The smooth curves
are fits using the Boltzmann equation. The corresponding parameters are
shown in Table 1.
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TABLE 1
Effect of MPS on inactivation
The effects of MPS on the inactivation properties were determined using
a double pulse protocol (see Fig. 6). The prepulse duration is shown in
parenthesis. Data from each cell were collected before, in the presence
of 3 mM MPS, or after washout. The results from each cell were fit with
a Boltzmann equation and then averaged. All V1/2
values are in millivolts. Steady-state inactivation curves using 30-s
prepulses were also performed on cells that were preincubated (>4 min)
in 3 mM MPS before patching the cell and recorded in the continued
presence of drug. The double pulse protocol was run 2 min after
establishment of the whole cell configuration. As control for these
experiments, the protocol was run on other cells a similar time after
patching. The V1/2 and k values for the
curves of Fig. 6D were: control, 71.7, 3.8; 10 mM ethosuximide,
76.5, 3.9; wash, 74.0, 3.8; respectively. Charge carrier was 5 mM Ca2+ in 1G and 1I experiments and 10 mM Ba2+
in the case of 1H.
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An independent method for measuring binding to inactivated states of
the channel is to measure the dose-response relationship at various
holding potentials. We chose two potentials to measure the MPS dose
response:
110 mV, where all the channels should be in the
closed/rested state, and
75 mV, where 50% of the channels should be
in inactivated states (see Fig. 6). The potency of MPS for all three
T-type channels was enhanced more than 2-fold by holding at
75 mV
(Fig. 7 and Table 2).
As shown in Fig. 5 for ethosuximide, the potency of MPS was even
greater if block was measured on the sustained component (Fig. 7C;
IC50 = 0.4 ± 0.1 mM, n = 5 cells). Ethosuximide block was also dependent on the holding potential
(Fig. 7E), with the apparent IC50 decreasing 6-fold from 18.2 ± 1.2 at
100 mV to 3.2 ± 0.4 mM at
75
mV (n = 4 cells).

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Fig. 7.
Block by succinimide antiepileptic drugs is dependent
on the holding potential. Dose-response relationship for MPS block of
peak Ca2+ currents expressed by 1G (A), 1H (B), and
1I (C) channels. Data points were obtained by performing experiments
like those described in Fig. 2 (5 mM Ca2+ as charge
carrier), but using holding potentials of either 110 mV (open
symbols) or 75 mV (filled symbols). Smooth lines represent the fit to
the data using the Hill equation. The third set of data ( ) and the
corresponding fit in C indicate the block of the current measured after
150 ms of depolarization using a holding potential of 75 mV. The
calculated IC50 for each human T-type channel is plotted
against holding potential in D. The corresponding relationship for
ethosuximide block of 1G is shown in E; in this case, the holding
potentials were 100 mV ( ) and 75 mV ( ), and the charge
carrier was 10 mM Ba2+. F, estimated ethosuximide
IC50 values from the data shown in E and Fig. 1.
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TABLE 2
Apparent affinities of MPS for resting and inactivated channels
Apparent affinities are reported in units of millimolar.
KR was measured as the block of the peak current
elicited during pulses to 30 mV from a holding potential of 110 mV
(Fig. 7). The shift in the midpoint of the steady-state inactivation
curve ( h) was measured using 30-s prepulses.
KI was calculated using eq. 1. Kapp was measured as the block of the peak current
elicited during pulses to 30 mV from a holding potential of 75 mV
(Fig. 7). The value of h was determined for each cell by
dividing the baseline current obtained with a holding potential of 75
mV with that obtained previously at 110 mV. KI*
was calculated using eq. 2. Data were obtained using 5 mM Ca2+
as charge carrier in the external solution except for h
of 1H, which was measured in 10 mM Ba2+.
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An important property of T-type Ca2+ channels is
that they display "window currents", that is, there are voltages
where channels do not inactivate totally and are available to open.
This property is commonly defined by the presence of an overlap region
between the steady-state inactivation curve and the activation curve. The size and position of the window current region is subject to many
experimental variables. Short prepulses (<1 s) may not reach steady
state, such that increasing the duration of the prepulse shifts the
apparent inactivation curve to the left (Herrington and Lingle, 1992
).
Preliminary experiments with
1I indicated that at least 10 s
were required, so we performed experiments with a 30-s prepulse.
Activation curves have been estimated by fitting current data with a
Boltzmann equation, with the current data coming from either
I-V or tail current measurements. In addition, I-V data must take into account changes in driving force,
which can be done by either assuming a chord conductance or with
constant-field theory. Although these different methods yield different
values for V1/2 and k, they have
surprisingly little effect on the foot of the curve (data not shown)
and hence the window current region. We used constant-field theory,
which produced a good fit of the I-V data (Fig. 3). The
effect of 3 mM MPS on the window current region is shown in Fig.
8A. The fraction of
1I channels
available for opening in the window current region was reduced by 50%
in the presence of 3 mM MPS.

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Fig. 8.
Window currents are reduced by MPS and
ethosuximide. A, overlapping area of voltage-dependent activation
(lines originating from 80 mV) and steady-state inactivation curves
(lines ending at 40 mV) for 1I channels in the absence (solid
lines) and presence (dotted lines) of 3 mM MPS. All lines represent
Boltzmann function fits to experimental data, which have been omitted
for clarity purposes. MPS shifted the window current region ~5 mV to
more negative potentials and reduced the size of the region ~50%. B,
effect of 0.7 mM ethosuximide on Ca2+ current carried
through human 1G channels obtained in response to a mock
subthreshold LTS.
|
|
Another important property of T-type channels is that they
mediate LTS (Crunelli et al., 1989
; Suzuki and Rogawski, 1989
). To
study the effect of ethosuximide on such activity, we used a voltage
protocol that mimics a subthreshold LTS recorded from thalamic neurons
(Destexhe et al., 1998
). To investigate the effect of a therapeutically
relevant concentration, we tested the effect of 0.7 mM ethosuximide on
the Ca2+ current carried through human
1G
channels obtained in response to the LTS protocol. The voltage protocol
and the corresponding currents evoked from an HEK-293 cell expressing
the human
1G subunit are shown in Fig. 8B. Ethosuximide reduced the
peak LTS current 26 ± 7% (n = 3).
Our last series of experiments focused on the structure-activity
relationships of succinimide compounds. For this purpose, we
investigated the effect of two succinimide analogs that are not
antiepileptic drugs, succinimide and trimethylsuccinimide (TMS;
,
-dimethyl-
-methylsuccinimide). Figure
9A shows the effect of these two
compounds at the indicated concentrations on the peak current of a cell
expressing human
1H channels. Although tested concentrations were as
high as 10 mM (in the case of succinimide) the block of the current was
considerably weaker in comparison with the effect produced by MPS in
these same cells. To illustrate this observation, the fractional block
induced by succinimide, TMS, and MPS on the three human T-type
Ca2+ channels is compared in Fig. 9B. For
example, currents expressed for
1G were blocked 7.5 ± 4.7% by
10 mM succinimide, 30 ± 6% by 6 mM TMS, and 87 ± 2% by 3 mM MPS.

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Fig. 9.
Block of human T-type Ca2+ channels by
succinimide nonantiepileptic drugs is much less potent. A, time course
of peak current during exposure to trimethylsuccinimide and succinimide
recorded from a cell expressing human 1H channels. The insets show
representative Ca2+ current traces at 30 mV obtained
under the indicated experimental conditions. The holding potential was
90 mV, and the charge carrier was 5 mM Ca2+. B, fraction
of Ca2+ current blocked at 30 mV by succinimide (10 mM),
TMS (6 mM), and MPS (6 mM) for the three human T-type Ca2+
channels.
|
|
Analysis of Drug Block.
Both ethosuximide and MPS produced
measurable shifts in the h
curve of all
three cloned T-type channels. The shift in the mid-point of
inactivation (
h) can be used to calculate the apparent
affinity of the drug for the inactivated state,
KI (Bean et al., 1983
). Rearrangement of
this equation yields
where D represents the drug concentration, and
k represents the slope of the
h
curve estimated from Boltzmann fits to
the control data (Fig. 6). As shown in Table 2, the apparent affinity
of MPS for inactivated channels is 5- to 6-fold greater than
closed/rested channels. Similar results were obtained using the
h induced by either 1 mM ethosuximide or MPS, as
predicted by the model (Bean et al., 1983
).
Due to the difficulties in estimating steady-state inactivation, we
sought an independent method to estimate the affinity of the drugs for
inactivated states. Dose-response relationships were measured using a
holding potential that would cause approximately 50% of the channels
to inactivate. In comparison with the data obtained using a holding
potential of
110 mV (KR), the potency of
MPS to all three cloned T-type channels was increased approximately 2-fold by holding at
75 mV (Kapp).
Rearrangement of the equation derived by Bean, Cohen, and Tsien (Bean
et al., 1983
) yields
The values for KI* using this method
were similar to those calculated using eq. 1 (Table 2). The
KI* of MPS for the inactivated state of
1G and
1I was approximately 0.5 mM, which indicates that MPS has
a 4- to 5-fold higher affinity for inactivated channels. The
h
data in Table 2 for
1G were
measured with 30-s prepulses, however, identical values of
KI* were obtained using data from 0.3-s
prepulses (Fig. 6). The KI* of MPS for the
inactivated state of
1H was approximately 1.2 mM, which is only
2.6-fold higher than its affinity for closed/rested channels.
Ethosuximide also has different apparent affinities for closed/rested
and inactivated/open channel states of the three cloned T-type channels
(Figs. 5-7). The potency of ethosuximide to block
1G currents
increased 6-fold by changing the holding potential from
100 to
75
mV. Using eq. 2, the KI* for the
1G
inactivated states was calculated to be 1.9 mM. If a drug has higher
affinity for inactivated states, then it may produce biphasic
dose-response relationships when measured at holding potentials that
induce inactivation (Cai et al., 1997
). Since some
1G channels are
inactivated at
90 mV, this may partially explain the biphasic
response shown in Fig. 1, and the reduced Hill coefficient observed for
the data obtained at
70 mV (Fig. 7). Ethosuximide block of
1H was
also state-dependent. To calculate KI for
1H we used eq. 1,
h (Fig. 6), and the
KR value determined previously (Todorovic
et al., 2000
). The KI of ethosuximide for
the inactivated state of
1H was approximately 2.5 mM, which is
9-fold higher than its affinity for rested channels.
 |
Discussion |
This study describes the block of the cloned human T-type channels
1G,
1H, and
1I by succinimide antiepileptic drugs. Previous studies have used currents from rat or cat neurons (Coulter et al.,
1989a
, 1990a
; Leresche et al., 1998
; Todorovic and
Lingle, 1998
). The amino acid sequences of T-type channels are not
identical between rats and humans. For example, the human
1G
sequence is only 93% identical to the rat (Cribbs et al., 2000
). More
importantly, the pharmacology of human
1G also differs from the rat,
being 2-fold more sensitive to block by nickel (Lee et al.,
1999b
; Cribbs et al., 2000
). Considering the recent challenge to
the hypothesis that the mechanism of action of ethosuximide involves
blockade of T-type channels (Leresche et al., 1998
), we decided to
clone the human T-type channels and to test their sensitivity to these drugs. The main conclusions of this study are that block is observed at
clinically relevant concentrations and that block is state-dependent.
The present results indicate that the apparent potency of ethosuximide
and MPS is highly dependent on the recording conditions. Block is
greater at threshold potentials, if measured at the end of a
depolarizing pulse, and if the holding potential is more positive than
90 mV. T-type channels do not need to open to be blocked since there
is block of peak currents in the first pulse after drug treatment in
the absence of depolarizing pulses (data not shown). This result
indicates that there is substantial block of channels in deep rested
states. The affinities of the drugs for the closed/rested state were
estimated by measuring the dose-response relationship at a holding
potential of
110 mV (KR, Fig. 7).
Open Channel Block.
T-type channels, especially those formed
by
1I (Fig. 4), do not inactivate completely during a long
depolarizing pulse, leading to measurable persistent current, or
plateau. This property is difficult to measure with native channels
since plateau currents are often contaminated with currents through
high voltage-activated Ca2+ channels (Sayer et
al., 1993
). Block of the T-type channel increased during the pulse,
such that the plateau current was eliminated at doses that had little
effect on the peak current. This had a dramatic effect on the apparent
potency of ethosuximide, decreasing the apparent
IC50 13-fold to 0.6 mM (Fig. 5). However, at the pulse frequency used (0.1 Hz) there was little evidence of use dependence, indicating that channels recovered from this additional block when the holding potential was
90 mV or more negative. Two
possible explanations for the effect on kinetics are 1) antiepileptic drugs accelerate the transition from open to inactivated states and/or
2) that there is additional block of open states.
Two lines of evidence suggest that there was open channel block. 1)
Block of the peak current was greatest during test potentials to
50
mV, where inactivation was the slowest (Figs. 3 and 4). If block were
only occurring by binding to inactivated states, then one would expect
less block at these potentials. 2) At concentrations that blocked
Ca2+ influx, there was little block of outward
currents, which under these experimental conditions are carried by
Cs+ efflux (Fig. 3). Tail currents after pulses
that elicited outward currents showed less block than after pulses that
elicited inward currents (data not shown). This unidirectional block
suggests that the drugs physically plug the pore and that outward
currents partially unblock the channel.
Assuming that there is open channel block, then the on-rate of drug can
be estimated from the current kinetics. To estimate this rate, the
currents measured in the presence of MPS were fit with three
exponentials, with two of the
values fixed to that observed in
control. Thus, the third
corresponded to the difference between
control and MPS and reflected the on-rate of drug during the pulse.
From the data shown in Fig. 4 with
1I, this rate was calculated to
be 25 ms, and this rate did not vary with the test potential between
30 and 20 mV. Similarly, we estimated the on-rate for 30 mM
ethosuximide to be 15 ms during pulses to
30 mV. This on-rate may
explain the apparent voltage dependence of block, the effect on the
voltage dependence of activation, and their effect on inactivation
rate. Since cloned
1I channels activate very slowly during test
pulses in the range of
60 and
30 mV (e.g., at
50 mV,
act = 44 ± 6 ms), MPS block is nearly
complete before the peak is reached. At more positive potentials, the
peak is reached before block is complete (e.g., at +10 mV,
act = 4.0 ± 0.3 ms), and block occurs
during the inactivating phase, causing an apparent increase in the rate
of inactivation. Therefore, block of the peak current is greatest at
negative potentials and decreases at more positive test potentials,
causing an apparent shift in the position of I-V curve.
Alternatively, MPS block may be inherently voltage-dependent [even
though it is uncharged at physiological pH (Huffman, 1982
)]; it may
alter the voltage dependence of gating; and it may affect the
transition rate between open and closed channels. The observation that
block is greatest at
50 mV where MPS does not affect the inactivation
rate (Fig. 4) favors the simpler hypothesis that block occurs on
channels that are near or in the open state.
Preferential Binding to Inactivated States.
Two experiments
indicated that succinimide antiepileptic drugs preferentially blocked
inactivated states of the T-type channel: 1) the drugs shifted the
steady-state inactivation curve, and 2) potency was enhanced by
depolarizing shifts in the holding potential. Analysis of these
experiments allowed independent calculations of the drug affinity for
inactivated states (Table 2). For most channel subtypes these two
methods produced similar estimates for KI.
The selectivity for inactivated states over rested states of the
channel was modest, ranging from 3- to 9-fold. Changing the holding
potential also increases the potency of ethosuximide to block a mouse
1G (Lacinova et al., 2000
).
Ethosuximide Sensitivity of T-Type Channels.
Studies on the
dose response of human
1G indicated that therapeutically relevant
concentrations of ethosuximide were capable of producing modest block
(~15%). Since a small degree of run-down could complicate the
measurement of such a small effect, the experiment was repeated using a
variety of set-ups, external solutions (10 mM
Ba2+ or 5 mM Ca2+), and
flow rates. In each case, there was evidence for a plateau in the
response to concentrations ranging from 0.1 to 1 mM. The original
observation that ethosuximide could inhibit T-type channels in isolated
rat thalamic neurons also had similar results; block was partial (32%)
and appeared to plateau at 2 mM (Coulter et al., 1989a
). Higher
concentrations were not reported in that study. One study using
isolated rat dorsal root ganglion (DRG) neurons also found evidence for
ethosuximide block at low concentrations; block was complete and had an
apparent IC50 of 0.007 mM (Kostyuk et al., 1992
).
Subsequent studies on rat DRG neurons failed to confirm block at
concentrations below 1 mM, but did find block at higher concentrations
(Todorovic and Lingle, 1998
). The apparent IC50
was 23 mM. Recent studies on isolated and slice preparations of rat
thalamic neurons found no effect of 0.75 mM ethosuximide on the T-type
current (Leresche et al., 1998
). Although there are many differences in
the recording conditions used in these studies, one notable difference
is the holding potential. Since studies that reported no effect used
very negative holding potentials (
110 mV), we suggest these
experiments tested block of rested channels, which are less sensitive
to block. Preferential block of inactivated states can produce biphasic
dose-response curves (Cai et al., 1997
). Therefore, the partial block
originally observed in thalamic neurons (Coulter et al., 1989a
)
may have corresponded to block of inactivated channels.
Sensitivity of T-Type Channels to MPS.
In contrast to the
discrepant findings with ethosuximide, there is general agreement that
MPS is a potent blocker of rat T-type currents (Coulter et al.,
1990a
; Huguenard and Prince, 1992
; Todorovic and Lingle, 1998
).
The present results indicate that MPS is also a potent blocker of all
three cloned human T-type channels. Block was complete and had apparent
IC50 values between 2 and 3 mM. Similar results
were obtained previously with the rat
1G and human
1H (Todorovic
et al., 2000
). Block of thalamic T-type currents was also complete and
displayed a similar IC50 of 1.1 mM (Coulter et
al., 1990a
). Three millimolar MPS blocked 45% of the T-type currents recorded from thalamic neurons isolated from either the ventrobasal or the reticular nuclei (Huguenard and Prince, 1992
). In
situ hybridization studies indicated that
1G is the predominant isoform expressed in the rat ventrobasal nucleus, whereas
1H and
1I were expressed in the reticular nucleus (Talley et al., 1999
).
Therefore, MPS blocks both native and cloned channels with similar
potency. In contrast, MPS block of DRG T-type currents was only partial
(~30%), but occurred at lower doses (IC50 ~ 0.18 mM; Todorovic and Lingle, 1998
; Todorovic et al., 2000
). It is unclear why MPS produces only partial block of DRG currents, but complete block of currents from either thalamic neurons or cloned channels.
Structure-Activity Relationships of Succinimides.
Tetramethylsuccinimide has been reported to induce seizures in mice
(Klunk et al., 1982
). It was found to have no effect on either thalamic
T-type currents (1 mM) or their block by MPS (Coulter et al.,
1990a
). This result rules out a single binding site where compounds have agonist or antagonist properties (Klunk et al., 1982
).
Evidence indicates that this second site is on
-aminobutyric acid
receptors (Coulter et al., 1990b
). We were unable to test its
effect because it is no longer commercially available. In contrast to
ethosuximide, the trimethylsuccinimide analog
(
,
-dimethyl-
-methylsuccinimide) has been shown to be
ineffective at reducing spontaneous epileptiform discharges in rat
thalamocortical slices (1 mM; Zhang et al., 1996
). The present study
shows that trimethylsuccinimide is similarly ineffective at blocking
T-type currents. The base molecule, succinimide, has been reported to
be devoid of anticonvulsant activity (Ferrendelli and Kupferberg,
1980
). It is also ineffective at blocking rat thalamic T-type currents
(0.5 mM; Coulter et al., 1989b
), and at blocking epileptiform
discharges in thalamocortical slices (1 mM; Zhang et al., 1996
). The
present results indicate it was also ineffective in blocking the cloned
human T-type channels. These results confirm the correlation that only
succinimides that are capable of blocking T-type channels are effective anticonvulsants.
The present studies also show that MPS is 10-fold more potent than
ethosuximide. If the mechanism of action of these drugs involves
blockade of T-type channels, then MPS should be more potent.
Therapeutic plasma levels are consistent with this hypothesis; MPS
concentrations are approximately 0.1 mM, whereas ethosuximide concentrations range between 0.3 and 0.7 mM (Strong et al., 1974
; Browne et al., 1975
; Porter et al., 1979
; Wilder and Buchanan, 1981
).
Similar differences in potency were noted in the prevention of
pentylenetetrazol-induced seizures in rats (Chen et al., 1963
). More
striking were the differences in potency observed in the prevention of
maximal electroshock seizures in mice, where MPS was 25-fold more
potent than ethosuximide (Chen et al., 1963
). This result suggested
that methsuximide might be effective in a wider range of epilepsies.
Studies have shown that it was also effective in the treatment of
complex partial seizures (Wilder and Buchanan, 1981
; Browne et al.,
1983
). Unfortunately this drug had a small therapeutic window,
producing too many undesirable side effects at concentrations just
above those required for seizure prevention (Browne et al., 1983
).
Therefore, drugs that block T-type channels may be useful in a wide
variety of seizures. Evidence exists for the corollary of this
hypothesis, drugs such as phenytoin and zonisamide, which are useful in
the treatment of generalized tonic-clonic and complex partial seizures,
also block T-type channels (Twombly et al., 1988
; Kito et al., 1996
;
Todorovic et al., 2000
).
Therapeutic Implications of State-Dependent Block.
T-type
Ca2+ channels mediate low threshold
Ca2+ spikes in a number of neurons (Crunelli et
al., 1989
; Suzuki and Rogawski, 1989
). Such spikes play an important
pacemaker role in the initiation of burst firing of thalamic neurons,
and such firing underlies the spike-wave activity observed in the EEG
during absence seizures (McCormick and Bal, 1997
; Huguenard, 1999
).
Similar synchronized oscillations occur during slow wave sleep.
However, they are not observed during rapid eye movement sleep or in
wakeful states. In these states, the thalamus fires single
Na+-dependent spikes (tonic mode), because the
membrane potential of the neuron is depolarized to such an extent that
T-type channels are inactivated (Steriade and Llinas, 1988
). Therefore,
clinically relevant targets for antiepileptic drugs include T-type
channels in inactivated states, and blocking these states may prevent
the transition from tonic to burst firing. The present results show that both ethosuximide and MPS blocks are enhanced by holding the
membrane at a potential that is similar to the resting potential of
many neurons. We also found that block was greatest at threshold potentials. These two effects combine such that therapeutically relevant concentrations can cause significant block of current elicited
with mock LTS waveforms (Fig. 8).
The conclusion that a drug blocks at therapeutically relevant
concentrations is usually based on comparisons of the apparent IC50 for block observed in vitro with the plasma
concentrations reached in vivo. However, since T-type channels are
pacing Na+ channels that fire in an
all-or-nothing manner, even 10% block of the T-type current may lead
to a pronounced effect on firing (Huguenard and Prince, 1994
;
Narahashi, 2000
).
T-type window currents are thought to play an important role in
determining neuronal excitability (Williams et al., 1997
). Due to their
ability to shift inactivation to more negative potentials, we found
that ethosuximide and MPS reduced the window current region. The window
region is close to the resting membrane potential of many resting
neurons. Mutations in Na+ channels that affect
window currents have profound effects on excitability, leading to a
number of diseases including epilepsy (for review, see Lehmann-Horn and
Jurkat-Rott, 1999
). Due to the similarities in T-type channel gating,
it is interesting to speculate that mutations in human T-type channel
genes may also produce hereditary disease. Over-activity of T-type
channels in the thalamic reticular nucleus has been observed in a rat
model of absence epilepsy (Tsakiridou et al., 1995
), and this has been
attributed to an increase in expression of
1H mRNA (Talley et al.,
2000
). It should be noted that persistent currents are particularly
difficult to measure with native channels, since neurons contain other
Ca2+ channels that are capable of producing
plateau currents and that can activate even during relatively negative
test potentials (
30 mV; Avery et al., 1996
). Although
1G and
1H
display persistent currents, these currents are much more prominent in
1I channels (Figs. 2 and 4). Ethosuximide was 13-fold more effective
in blocking these persistent currents than block of the peak current,
displaying an apparent IC50 of 0.6 mM. Due to the
expression of
1I in the reticular nucleus of the thalamus (Talley et
al., 1999
) and the role of this nucleus in controlling thalamic
oscillations (Steriade and Llinas, 1988
), the present results are
consistent with the hypothesis that blockade of T-type channels may
underlie the therapeutic usefulness of succinimide antiepileptics.
T-type channel blockade may also be useful in a wide variety of
neurological disorders that are caused by thalamocortical dysrhythmias,
such as neuropathic pain (Llinas et al., 1999
).
We thank Qun Jiang for technical assistance. We thank Edward
Bertram for comments on the manuscript.
Supported in part by National Institutes of Health Grant
NS38691 and an Established Investigator Award of the American Heart Association (to E.P.R.).
Dr. Edward Perez-Reyes
Department of Pharmacology, University of Virginia Health System, P.O.
Box 800735, 1300 Jefferson Park Avenue, Charlottesville, VA 22908-0735. E-mail: eperez{at}virginia.edu