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The Journal of Neuroscience, June 15, 2001, 21(12):4162-4172
Channel-Lining Residues of the AMPA Receptor M2 Segment:
Structural Environment of the Q/R Site and Identification of the
Selectivity Filter
Thomas
Kuner1, 2,
Christine
Beck1,
Bert
Sakmann2, and
Peter H.
Seeburg1
1 Abteilung Molekulare Neurobiologie,
2 Abteilung Zellphysiologie, Max-Planck Institut für
Medizinische Forschung, 69120 Heidelberg, Germany
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ABSTRACT |
In AMPA receptor channels, a single amino acid residue
(Q/R site) of the M2 segment controls permeation of calcium
ions, single-channel conductance, blockade by intracellular polyamines,
and permeation of anions. The structural environment of the Q/R site
and its positioning with regard to a narrow constriction were probed
with the accessibility of substituted cysteines to positively and
negatively charged methanethiosulfonate reagents, applied from the
extracellular and cytoplasmic sides of the channel. The accessibility
patterns confirm that the M2 segment forms a pore loop with the Q/R
site positioned at the tip of the loop (position 0) facing the
extracellular vestibule. Cytoplasmically accessible residues on the N-
and C-terminal sides of position 0 form the ascending -helical ( 8
to 1) and descending random coil (+1 to +6) components of the loop,
respectively. Substitution of a glycine residue at position +2 with
alanine strongly decreased the permeability of organic cations,
indicating that position +2 contributes to the narrow constriction. The
anionic 2-sulfonatoethyl-methanethiosufonate reacted with a
cysteine at position 0 only from the external side and with cysteines
at positions +1 to +4 only from the cytoplasmic side. These results
suggest that charge selectivity occurs external to the constriction
(+2) and possibly involves interactions of ions with the negative
electrostatic potential created by the dipole of the -helix formed
by the ascending limb of the loop.
Key words:
glutamate receptor; AMPA; narrow constriction; pore loop; SCAM; organic cations; polyamines
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INTRODUCTION |
Glutamate receptor channels of the
AMPA subtype exist as
Ca2+-permeable and
Ca2+-impermeable variants in functionally
different sets of synapses (Geiger et al., 1995 ; Dingledine et al.,
1999 ; Liu and Cull-Candy, 2000 ). Ca2+
permeability in these channels is defined by the identity of a single
amino acid residue at the Q/R site located in the pore-lining M2
segment: glutamine renders channels permeable to
Ca2+, whereas arginine prevents the
permeation of Ca2+ (Hume et al., 1991 ;
Verdoorn et al., 1991 ; Burnashev et al., 1992 ). Additionally, the Q/R
site defines at least three more permeation properties of the pore.
Channels containing only glutamine at the Q/R site are blocked in a
strongly voltage-dependent fashion by polyamines present in the
cytoplasm of cells (Bowie and Mayer, 1995 ; Donevan and Rogawski, 1995 ;
Isa et al., 1995 ; Kamboj et al., 1995 ; Koh et al., 1995 ),
they exhibit single-channel conductances in the range of 7-8 pS
(Swanson et al., 1996 , 1997 ), and they are impermeable to anions
(Burnashev et al., 1996 ). In contrast, channels containing only
arginine at the Q/R site are insensitive to polyamine block, have
single channel conductances of ~300 fS, and are slightly permeable to
anions. Heteromeric channels containing both glutamine and arginine
show intermediate functional profiles with a dominating contribution of
the arginine residue (Dingledine et al., 1999 ). Therefore, a single
amino acid residue at the Q/R site controls four fundamental ionic
properties of the AMPA receptor (AMPAR) channel pore, and,
consequently, the function that these channels perform in the synapse.
Despite the early discovery of this critical amino acid residue (Hume
et al., 1991 ; Verdoorn et al., 1991 ), the structural environment of the
Q/R site and its relation to the overall structural design of the M2
segment remained poorly characterized.
AMPAR channels form large pores with a diameter of the narrow
constriction estimated to be 0.78 nm (Burnashev et al., 1996 ). Interestingly, the diameter of the constriction is not affected by the
identity of the residue at the Q/R site (Burnashev et al., 1996 ). In
addition to the Q/R site, an aspartate residue four positions
downstream has been shown to play a prominent role in defining
permeation properties of the AMPAR pore (Dingledine et al., 1992 ;
Blaschke et al., 1993 ). Knowing the positioning of these residues
relative to the constriction will further our understanding of the
structural basis of ion permeation in AMPAR channels.
In this paper, we identify channel-lining residues of the AMPAR M2
segment using the substituted-cysteine-accessibility method (Akabas et
al., 1992 , 1994 ). Our results confirm that the AMPAR channel M2 segment
forms a pore loop with the functionally critical Q/R site located at
the external entrance to the narrow constriction formed by position
G589. Furthermore, we show that charge selectivity occurs within a
small region external to the constriction, possibly involving an
electrical potential created by the dipole of the -helix formed by
the ascending limb of the loop.
Parts of this work have been published previously (Kuner et al.,
1997 ).
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MATERIALS AND METHODS |
Materials
The methanethiosulfonate (MTS) reagents were purchased from
Toronto Research Chemicals (Ontario, Canada). Enzymes were obtained from New England Biolabs (Schwalbach, Germany), Boehringer Mannheim (Mannheim, Germany), Stratagene (Heidelberg, Germany), or Promega (Madison, WI). All other chemicals were purchased from either Sigma
Chemicals (St. Louis, MO) or Merck (Darmstadt, Germany).
Molecular biology
All experiments were performed using expression constructs of
AMPAR subunits optimized for expression in Xenopus oocytes. The coding region of the GluR-Di was subcloned
into a vector derived from pSP6 (Kuner and Schoepfer, 1996 ); noncoding
regions were removed. Two silent restriction sites (ApaI,
BspEI) flanking the M2 region were introduced by
PCR-based methods (Ausubel et al., 1995 ). Mutants were generated by PCR
replacing the 105 bp fragment defined by ApaI and
BspEI. All constructs were sequenced over the entire length
of the replaced fragment. Capped cRNA was transcribed with SP6 RNA
polymerase and injected into Xenopus laevis
oocytes as described (Kuner and Schoepfer, 1996 ). In some instances,
wild-type cRNA was coinjected with mutant cRNA to improve current yields.
Electrophysiology
Whole-cell recordings were performed on a two-microelectrode
voltage-clamp system modified for automatic execution of recording protocols and solution exchange (Kuner and Schoepfer, 1996 ) (EggWorks, NPI Electronics, Tamm, Germany). The external solution consisted of (in
mM): 115 Na, 2.5 KCl, 1.8 Ca2+, and 10 HEPES. Solutions were
adjusted to pH 7.5 with NaOH. All drugs were applied with the bath solution.
Currents in oocyte patches were recorded with the patch-clamp technique
(Hamill et al., 1981 ) using an EPC-9 amplifier with PULSE software
(HEKA Electronics GmbH, Lambrecht, Germany). Solutions were applied
using a Piezo-driven double-barrel application system (Colquhoun et
al., 1992 ).
Giant inside-out patches were excised from Xenopus oocytes
as described (Kuner et al., 1996 ). Symmetrical potassium solution contained (in mM): 100 KCl, 10 HEPES, 10 EGTA
(external), or 10 EDTA (internal), pH adjusted to 7.2 with KOH. Data
were low-pass-filtered at 100 Hz and digitized at 500 Hz. Pipettes were
pulled from borosilicate glass and had resistances of 300-500 k
when measured in potassium solution.
Outside-out patches were excised from Xenopus oocytes. The
external solution was identical to that used for two-microelectrode voltage-clamp recordings. Pipettes were filled with a potassium solution and had resistances of 2-10 M .
Substituted-cysteine-accessibility method
Mutant channels were probed from the extracellular and
cytoplasmic sides of the membrane with three differently sized
methanethiosulfonate (MTS) derivatives:
2-aminoethyl-methanethiosufonate (MTSEA, positive charge),
2-trimethylammonioethyl-methanethiosufonate (MTSET, positive charge),
and 2-sulfonatoethyl-methanethiosufonate (MTSES, negative charge).
These reagents can covalently link their charged
-S-CH2-CH2-R groups
to the thiolate of cysteines exposed to the water-accessible surface of the channel. We assume that covalent modification of cysteine positioned in a narrow region of the channel persistently alters current flow. The accessibility of substituted cysteines to
reaction with the MTS reagents was assayed as a persistent change of
the glutamate-activated current and current rectification after
exposure to MTS reagents in the presence of glutamate. MTS reagents
were added to the solution at 1-3 mM (MTSEA), 1-2
mM (MTSET), and 10 mM (MTSES). Solutions either
were prepared immediately before the experiment or kept on ice
(maximally 2 hr) before use.
Experimental protocols and data analysis
Probing cysteine substitution mutants from the
extracellular side. Oocytes were held at 70 mV, and the baseline
current amplitude (Ipre) was
established by three consecutive applications of kainate (300 µM) for 60 sec. Voltage ramps ( 120 to +40 mV
in 2 sec) were applied before and at the end of kainate application.
Immediately after the third application, solution was switched to
solution containing MTS reagents for 120 sec in the continued presence of kainate. After exposure to MTS reagents, the current amplitude (Ipost) was determined with three
kainate applications. Individual applications were separated by 120 sec
washes. Currents before and after application of the reagents were
averaged, and percentage change was calculated as
%change = (1 Ipost/Ipre)*100.
Current amplitudes were corrected for rundown when appropriate.
Probing cysteine substitution mutants from the cytoplasmic
side. Kainate (100 µM) and cyclothiazide
(50 µM) were present in the pipette, and
voltage ramps were applied from 110 to 110 mV (within 2 sec). The
leak currents were in the range of 20-50 pA at 100 mV (~2-5 G )
as determined from patches containing no channels or after complete
block of the current by MTS reagents. The baseline current amplitude
was established by 6-12 consecutive ramps at an interval of 5 sec. MTS
reagents were applied for 60 sec, and ramps were applied continuously
every 10 sec. Voltage ramps (3-20) were applied after removal of MTS
reagents. Data were analyzed using Igor Pro (WaveMetrics, Lake Oswego,
OR). The current amplitude at 100 mV was determined and plotted against
time. When required, currents were corrected for rundown. Percentage
inhibition was calculated as %inh = (1 Ipost/Ipre)*100.
Apparent reaction rates. Reaction rates were determined by
fitting an exponential function to the decay of the current in the
presence of the reagents (Beck et al., 1999 ). To determine rate
constants for reactions of MTS reagents applied from the extracellular
side, the decay of the inward current could be fitted directly, because
MTS reagents caused only a weak open-channel block of
GluR-Di channels with the concentrations used
here. In contrast, MTS reagents block GluR-DiS
channels reversibly in a voltage-dependent manner when applied from the
cytoplasmic side. Therefore, rate constants for reaction from the
cytoplasmic side could not be determined from the decay of outward
currents but were inferred from the decay of the inward current, which
is only weakly blocked by the reagents (see Fig. 1). To accurately
determine reaction rates, low concentrations (20-200
µM) of the reagents were used.
Permeability of organic cations. The following organic
cations were used to probe the size of the narrow constriction:
dimethylammonium (DMA), trimethylammonium (TriMA), tetramethylammonium
(TMA), tetraethylammonium (TEA), and tetrapropylammonium (TPA).
External solutions contained 150 mM of the
organic cation and 10 mM HEPES (TMA, TEA, TPA) or 10 mM histidine (DMA, DEA, TriMA) adjusted to pH
7.2 with the respective hydroxide of the organic cation or HCl,
respectively. The internal solution consisted of (in
mM): 150 NaCl, 10 HEPES, and 10 EGTA, adjusted to
pH 7.2 with NaOH. Molecular dimensions are taken from Villarroel et al.
(19950 and Burnashev et al. (1996) and are summarized in Table 3. The
dimensions of TPA were taken from a simulated model of TPA using
SwissPdbViewer (Glaxo-Wellcome). Liquid junction potentials are
listed in Table 3. Permeability ratios were calculated from the
Goldmann-Hodgkin-Katz equation for cation-selective channels:
Px/PNa = ([Na+]i/[X+]o)exp(FVrev/RT),
where Vrev is the measured reversal
potential, [Na+]i
is the concentration of Na+ in the
pipette, [X+]o is
the concentration of the organic cation applied to the patch, and
F, R, and T have their usual
thermodynamic meanings. Assuming a simple hydrodynamic model
(Dwyer et al., 1980 ), the permeability of an organic cation is related
to the mean diameter of the pore according to the equation:
PX = k(1 (dorganic/dpore))2.
Dose-response analysis. Peak current responses
to 1, 10, 30, 100, and 300 µM kainate were
recorded at a holding potential of 70 mV and plotted against the
kainate concentration. The EC50 for kainate was
determined from fits of the Hill equation to the data.
Permeability to Ca2+. Outside-out patches
were held in symmetric 100 mM
K+ solution and briefly exposed to 100 mM Ca2+ external
solution in the presence of glutamate at membrane potentials ranging
from 50 to +100 in increments of 10 mV. The current-voltage (I-V) relation was constructed from the
peak currents corrected for leak, and a polynomial function was fitted
to the data. The reversal potential was determined from the
intersection of the fit with the abscissa corrected for the junction potential.
Fast desensitization. Glutamate was applied to outside-out
patches using a fast piezo-driven device. Desensitization time constants were determined from exponential fits to the decaying phase
of the current in the presence of glutamate, as described in Mosbacher
et al. (1994) .
Statistical analysis. One-way ANOVA was performed for each
of the six different experimental groups (extracellular MTSEA, extracellular MTSET, extracellular MTSES, cytoplasmic MTSEA,
cytoplasmic MTSET, cytoplasmic MTSES), and significance levels were
calculated with the Newman-Keuls multiple comparison test using the
GB-STAT software (Dynamic Microsystems, Silver Spring, MD).
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RESULTS |
Effects of MTS reagents on GluR-Di
wild-type channels
Figure 1A shows
kainate-activated currents recorded from a Xenopus oocyte
expressing homomeric GluR-Di channels. The
inset illustrates a current-response elicited by kainate at
a membrane potential of 70 mV, with arrows indicating the
application of voltage ramps. The I-V relations
show a strong inward rectification caused by a voltage-dependent block
of the channels by polyamines present in the oocyte. To probe for the
presence of reactive cysteine residues in the conduction pore, channels
were exposed to MTS reagents (MTSET, MTSEA, MTSES; see Materials and
Methods). The effect of these reagents on channel function was assessed
from persistent changes of the current amplitudes. Figure
1B shows a plot of current amplitudes isolated at
100 mV as a function of time. Kainate was applied three times to
establish the baseline (a), inward currents were weakly
blocked by MTSET (b), and after washout of the reagent the
current amplitudes returned to baseline (c). In four
independent experiments, the relative change of the current amplitude
(Ipost/Ipre)
was 1 ± 4%, and the current rectification remained unchanged.
Similar results were obtained with MTSEA ( 5 ± 7%;
n = 5) and MTSES ( 3 ± 6%; n = 3), none of which persistently changed the current amplitude or current
rectification. These results suggest that the extracellular part of the
pore of GluR-Di wild-type channels does not
contain functionally relevant pore-lining cysteine residues.

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Figure 1.
Effects of MTS reagents on GluR-Di
wild-type channels. A,
I-V relations recorded from an oocyte
expressing homomeric GluR-Di subunits before
(a), during (b), and after
(c) application of 2 mM MTSET from
the extracellular side. Currents were elicited with 300 µM kainate (inset, thin
bar); MTSET was applied for 1 min (inset,
thick bar). Applications of control and test voltage
ramps ( 120 to +40 mV) are marked with arrows.
Calibration (inset): 100 nA, 120 sec. B,
Current amplitudes extracted from the experiment shown in
A at 100 mV plotted against the time. Kainate was
applied three times before ( ) and after ( ) exposure to MTSET
(asterisk). Small letters denote
amplitudes extracted from the respective
I-V relations shown in A.
C, I-V relations recorded
from a giant inside-out patch containing GluR-Di channels
subunits before (a), during
(b), and after (c)
application of 2 mM MTSET from the cytoplasmic side.
Voltage ramps were applied in the continuous presence of kainate in the
pipette. D, Current amplitudes extracted from the
experiment shown in C at +100 mV plotted against the
time. Six ramps were applied before ( ), 6 were applied during
(asterisks), and 20 were applied after ( ) exposure to
MTSET. E, As in C, but the patch
containing GluR-Di channels with the native cysteine at
position +3 was substituted by serine (DiS). Interestingly,
the block by cytoplasmically applied MTSET was slightly voltage
dependent, showing a current rectification reminiscent of polyamine
block (b). F, As in
D, but the patch contained GluR-DiS
channels. Voltage ramps were applied 12 times before ( ) and 12 times
after ( ) exposure to MTSET (asterisks). The rundown
of the current amplitude is within the range typically found for
GluR-Di wild-type and cysteine-substituted channels.
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Figure 1C shows I-V relations
recorded from a giant inside-out patch containing
GluR-Di channels. In symmetrical divalent-free potassium solution, in the nominal absence of polyamines on the cytoplasmic side, GluR-Di-mediated currents were
outwardly rectifying (Fig. 1C, a). Current
amplitudes extracted at +100 mV and plotted against the time are shown
in Figure 1D. After the baseline was established
(a), application of MTSET from the cytoplasmic side resulted
in a strong block of both inward and outward currents (b).
Surprisingly, the current remained persistently blocked (93 ± 3%; n = 4) after washout of MTSET (c).
Cytoplasmic application of MTSEA yielded a similar result (96 ± 5%; n = 6). Exposure of the channels to MTSES
persistently blocked the current by 82 ± 11% (n = 4), but the onset of block was markedly slower in comparison to MTSET
and MTSEA (see below). These results suggest that MTS reagents applied
to the cytoplasmic side of homomeric GluR-Di channels reacted with a pore-lining cysteine residue, which was not
accessible, however, from the extracellular side.
The GluR-Di subunit contains cysteine at position
+3 (C590) of the M2 segment, a residue present only in AMPAR subunits
but in none of the other GluR subunits (Fig.
2). We substituted the cysteine residue
with serine, an amino acid of similar size occupying the homologous
position in kainate receptors. Probing a
GluR-Di(C+3S) channel with MTSET from the
cytoplasmic side revealed that this channel was rendered insensitive to
persistent modification by MTSET (Fig.
1E,F). After the baseline
was established (a), application of MTSET strongly blocked
the channel (b), and the current amplitude returned to
baseline during washout (c). From this result we infer that
the native cysteine residue at position +3 mediates inhibition of
wild-type GluR-Di and hence is exposed in the
lumen of the channel. Consequently, GluR-Di
wild-type subunits cannot be used to identify pore-lining residues of
the M2 segment using the substituted-cysteine-accessibility method.
However, the serine-substituted GluR-Di(C+3S)
subunit could be used as a host for cysteine substitutions, given that this mutant channel is near wild-type in its structural and functional properties. Indeed, we did not find differences in maximal whole-cell currents, EC50 of kainate, fast desensitization,
permeability to Ca2+, and diameter of the
pore (Table 1). Hence,
GluR-Di(C+3S) subunits can be used in place of
wild type as a host for cysteine substitutions.

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Figure 2.
Alignment of selected GluR M2 segments and
positions where cysteine was substituted. Schematic representation of a
GluR subunit (thick line) with the black
boxes denoting the four hydrophobic domains.
Numbers (579-593) refer to
positions of the amino acid residues of the M2 segment in the mature
GluR-Di subunit. To facilitate comparisons between
subunits, we use a relative numbering system with negative numbers
denoting positions N terminal to position 0 (Q/R site) and positive
numbers on the C-terminal site (Kuner et al., 1996 ). DiS
refers to a subunit in which the native cysteine residue at position +3
was replaced with a serine residue. This subunit was used for cysteine
substitutions at positions 8 to +6.
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Cysteine-substitutions in the GluR-Di(C+3S) subunit
Cysteine was substituted at positions 8 to +6 in the M2 segment
of the GluR-Di(C+3S) subunit, herein referred to
as "DiS" subunit (Fig. 2). Most of the 14 cysteine-substituted
channels yielded current amplitudes comparable with wild-type; only
four mutations, W-8C, F-7C, Q+1C, and G+2C, gave rise to maximal
current amplitudes smaller than 0.5 µA at 100 mV (Table
2). Within the narrow region of the
channel, engineered cysteine residues of adjacent subunits might be
positioned close to each other, possibly allowing the formation of
disulfide bridges, which could interfere with the function of the
channel. However, DTT treatment (10 mM; 5 min) did not lead
to an increase of the current amplitudes elicited by 300 µM kainate, suggesting that other mechanisms are responsible for the small current amplitudes produced by these mutant
channels (data not shown). To avoid experimental problems associated
with mutant channels yielding only small current amplitudes, mutant
subunits were coexpressed with the DiS subunit at a 1:1 cRNA ratio,
which in all instances increased current amplitudes significantly
(Table 2, lower section). Furthermore, assuming that heteromeric
channels were formed, this approach allowed us to titrate the average
number of cysteine residues present at a defined position in the pore
of a population of channels by coinjecting different ratios of cRNAs
coding for the DiS subunit and the cysteine-substituted subunit.
Effects of MTS reagents applied from the extracellular side
Application of MTS reagents on the extracellular side of the
cysteine-substituted channels revealed persistent changes of the
current amplitude in 4 of 15 positions tested (Figs.
3, 4; summarized in Fig. 5). Channels with
cysteine at position 0 (=Q/R site) were strongly blocked by 1 mM MTSET (Fig. 3A, inset). After washout of MTSET, a slow recovery from the block was observed (Fig.
3B), a behavior different from that of the other mutants tested (see below). However, the current amplitudes reached a steady-state level within ~20-30 min, indicating that covalent modification of the cysteine had occurred. Homomeric DiS(G+ 2C) channels were not persistently modified by MTSET (Fig. 3C,
b); only when coexpressed with DiS channels did a persistent
block of the current develop (Fig. 3D, b),
suggesting that the two subunits formed heteromeric channels.
Interestingly, currents passed by G+2C channels were only weakly
rectifying (Fig. 3C), suggesting that polyamine block was
abolished in homomeric G+ 2C channels. Coexpression of G+2C with DiS
channels resulted in an increased current rectification, suggesting a
partial restoration of polyamine block in channels likely to contain
both cysteine and glycine at position +2 (Fig. 3D,
a). Currents mediated by DiS(D+4C) channels were
persistently decreased after exposure to MTSET (Fig.
3E,F). In summary, 3 of 15 positions tested were accessible to covalent modification by
extracellularly applied MTSET: Q0C, G+2C, and D+4C (Fig.
5A).

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Figure 3.
Extracellular application of MTSET to
cysteine-substituted GluR-DiS channels. A,
I-V relations recorded from an oocyte
expressing homomeric GluR-DiS(Q0C) channels before
(a), during (b), and after
(c, d) application of 2 mM
MTSET. Currents were elicited with 300 µM kainate
(inset, thin bar, 90 sec), MTSET was
applied for 60 sec (inset, thick bar).
Current shown in the inset is 4 µA at 70 mV.
B, Current amplitudes of the
I-V relations shown in A
extracted at 100 mV plotted against the time. Kainate was applied 9 times before ( ) and 13 times after ( ) exposure to MTSET
(asterisk). The box denotes the duration
of a typical experiment as shown for all other cysteine-substituted
channels. C, I-V relation
recorded from an oocyte expressing homomeric GluR-DiS(G+2C)
channels (a). The currents remained unchanged
during and after exposure to 2 mM MTSET
(b). D,
I-V relation recorded from an oocyte
injected with a 1:1 ratio of cRNAs encoding GluR-DiS and
GluR-DiS(G+2C) subunits (a). In
heteromeric channels, MTSET (2 mM) persistently reduced the
current amplitude (b). E, As in
A, but recorded from an oocyte expressing homomeric
GluR-DiS(D+4C) channels. Current shown in the
inset is 4 µA at 70 mV. F, As in
B, but three applications of kainate before and after
exposure to MTSET.
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Figure 4.
Extracellular application of MTSEA to
GluR-DiS(Q+1C) channels. A, Currents
recorded from an oocyte expressing homomeric GluR-DiS(Q+1C)
channels. Current shown in the inset is 2.5 µA at 70
mV. For clarity, curve b has been removed.
B, Current amplitudes extracted at 100 mV plotted
against the time.
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Figure 5.
Effects of extracellularly applied MTS reagents on
cysteine-substituted GluR-DiS channels.
A-C, Mean change of the current
amplitude after exposure to MTSET, MTSEA, and MTSES applied from the
extracellular side. Black bars denote current
inhibition, and shaded bars represent current
potentiation after exposure to the reagents. Shown is the mean
change ± SD of 3-10 experiments. For a binary interpretation of
the data based on statistical analysis, see Figure 9.
Asterisks indicate coexpression with
GluR-DiS subunits.
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A similar pattern was found using the smaller MTSEA (Fig.
5B). Unlike MTSET, MTSEA revealed an additional residue
accessible to covalent modification. When DiS(Q+1C)/DiS channels (1:1
cRNA ratio) were exposed to MTSEA, the current amplitude recorded at 100 mV did not change significantly (Fig. 4). However, the
I-V relation was less outwardly rectifying after
covalent modification (Fig. 4A), suggesting an
interference of the modified cysteine with polyamine block. Reaction of
the smaller MTSEA, but not the larger MTSET, with the cysteine at
position +1 may suggest that steric constraints limit the accessibility
of the side chain at position +1.
The negatively charged MTSES reacted only with DiS(Q0C) mutant channels
(Fig. 5C). In summary, all three reagents reacted with a
cysteine at position 0, but only the positively charged MTSEA and MTSET
reacted with residues on the C-terminal side of position 0. These
results suggest that anions can reach as far down into the pore as
position 0, but a charge selectivity barrier may prevent the negatively
charged MTSES from reacting with G+2C and D+4C. Given that the size of
MTSES is in between that of MTSEA and MTSET, it should have reacted
with cysteine residues at these positions if steric constraints were
the limiting factor.
In conclusion, channels with substitutions Q0C, Q+1C, G+ 2C, and D+4C
exhibited persistent changes in current amplitudes after extracellular
application of MTS reagents and hence line the pore of
GluR-Di receptor channels.
Effects of MTS reagents applied from the cytoplasmic side
About half of the mutant channels were susceptible to covalent
modification when the MTS reagents were applied from the cytoplasmic side. A cysteine at position 0, which was accessible to all three reagents from the extracellular side, was modified only by
cytoplasmically added MTSEA, not by MTSET or MTSES (Fig.
6A,B;
summary in Fig. 7). MTSEA applied after
exposure to MTSET or MTSES resulted in irreversible inhibition,
suggesting that MTSET and MTSES did not react silently with the
cysteine (data not shown). The possibility remains that the neutral
form of MTSEA, which can passively diffuse through membranes (Holmgren
et al., 1996 ), reacted from the extracellular side. However, 10 mM cysteine in the pipette did not affect the reaction of MTSEA with the cysteine at position 0, suggesting that
MTSEA could access it directly through the channel. These observations
may suggest that the larger MTSET could not react because of steric
constraints, possibly imposed by a narrow constriction, and that the
negatively charged MTSES could not cross the selectivity filter.
Substituted cysteines on the C-terminal side of position 0, Q+1C, G+2C,
and D+4C were modified by all three reagents (Figs. 6, 7), suggesting a
sterically and electrostatically unrestricted access pathway. Because
homomeric DiS(Q+ 1C) and DiS(G+2C) channels yielded only low current
amplitudes, these subunits were coexpressed with DiS subunits. Figure
6C shows irreversible modification by MTSET of cysteine in
channels formed by DiS(G+2C) and DiS subunits coinjected with a 1:1
cRNA ratio. Given the heteromeric nature of this channel, this result
suggests that the modification of a number of cysteine residues less
than the number of subunits forming the channel is sufficient to
strongly inhibit the current. A cysteine at position +4 created a
change of the intrinsic current rectification and resulted in an
inwardly rectifying current in the absence of polyamines and divalent
ions (Fig. 6E). Exposure to MTSET produced a strong
and irreversible inhibition of the current amplitudes (Fig.
6F). On the N-terminal side of position 0, only A-3C,
G-4C, and F-7C were accessible to the reagents (Fig. 7). The large
MTSET reacted only with cysteines at positions 7 and 4, whereas the
two smaller reagents, MTSEA and MTSES, in addition reacted with a
cysteine at position 3. It remained unclear whether a cysteine at
position 8 is exposed to the pore, because expression of W-8C
subunits did not yield detectable currents (Table 2). Therefore, mutant
subunits with a W-8C substitution may not form heteromeric channels
when coexpressed with the DiS subunit. In summary, cysteine-substituted
channels F-7C, G-4C, A-3C, Q0C, Q+1C, G+2C, D+4C, and S+6C were
persistently inhibited by cytoplasmically applied MTS reagents (Fig. 7)
and thus contribute part of the channel wall in
GluR-Di receptor channels.

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Figure 6.
Cytoplasmic application of MTS reagents to
cysteine-substituted GluR-DiS channels. A,
I-V relations recorded from a giant
inside-out patch containing homomeric GluR-DiS(Q0C)
channels before (a), during
(b), and after (c)
application of 2 mM MTSEA. Currents were elicited with 300 µM kainate in the pipette. B, Current
amplitudes extracted from the experiment shown in A at
+100 mV are plotted against the time. Kainate was applied 12 times
before ( ) and 12 times after ( ) exposure to MTSEA
(asterisk). Letters a-c
denote amplitudes extracted from the experiment shown in
A. C, As in A, with
channels containing GluR-DiS(G+2C) and GluR-DiS
subunits and using MTSET instead of MTSEA. D, As in
B, with experiment shown in C.
E, As in A, with
GluR-DiS(D+4C) channels. The intrinsic current
rectification was altered by the mutation. F, As in
B, with experiment shown in E.
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Figure 7.
Effects of cytoplasmically applied MTS reagents on
cysteine-substituted GluR-DiS channels.
A-C, See legend to Figure 5.
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Reaction rates of MTS reagents with substituted cysteines
We determined apparent reaction rates for covalent modification of
exposed cysteine residues by MTS reagents from the decay of the current
in the presence of the reagents (Fig. 4, inset) (see
Materials and Methods). When applied from the extracellular side, MTSET
and MTSEA showed rather slow reaction rates, with no significant
differences between exposed cysteines Q0C, G+2C, and D+4C (Fig.
8). Reaction of MTSES with a cysteine at
position 0 was markedly slower than reaction of the positively charged MTSET and MTSEA (Fig. 8), suggesting that a negative
electrostatic potential close to position 0 may limit accessibility to
a negatively charged reagent. MTSET applied from the cytoplasmic side
reacted up to ~100 times faster, with G +2C and D+4C showing the
fastest reaction rates (Fig. 8, black bars). Similar rate
constants were found for MTSEA (gray bars), although
with cysteine at position +2 or +3, MTSEA showed a faster reaction rate
than MTSET, suggesting that accessibility to positions +2 and +3 may be
sterically restricted. MTSES exhibited low reaction rates (~1-5
M 1 sec 1) throughout (white
bars), consistent with restricted access of anions to the narrow
region of a cation-selective channel. However, MTSES reacted ~100×
faster with a cysteine at position +4, suggesting that this position
may be located at the internal opening to the narrow region. In
conclusion, the reaction rates observed for covalent modification of
the substituted cysteines are in agreement with a location at the
aqueous surface lining the lumen of the channel.

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Figure 8.
Apparent reaction rates of MTS reagents with
substituted cysteines. Reaction rates of MTSET (black
bars), MTSEA (gray bars), and MTSES
(white bars). Rate constants for reactions from the
extracellular side are shown in the top panel; those for
reactions from the cytoplasmic side are shown in the bottom
panel. Values are plotted as mean ± SEM of three to five
experiments.
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Location of the narrow constriction
Figure 9 summarizes the
accessibility patterns in a binary fashion and compares the different
reagents and relative sidedness of accessibility. A simple pattern is
found for MTSES: position 0 was accessible from the external side,
whereas positions flanking 0 were accessible from the internal side.
Assuming that MTSES is impermeant, such a pattern is expected if the
selectivity filter is located between positions -3 and 0 or 0 and +1. A
common pattern emerged for the two positively charged reagents: several
positions from 0 to +4 were accessible from either side of the channel, whereas positions on the C- and N-terminal sides were accessible only
from the cytoplasmic side. Furthermore, covalent modification of
cysteines at positions 0 to +4 had the strongest effects on current
amplitudes, intrinsic rectification, and polyamine block. These
findings suggested that a narrow region of the channel may form between
residues 0 and +4. To test this hypothesis further, we examined the
effects of mutations in this stretch of residues on the size of the
narrow constriction estimated from the permeability of organic cations
relative to sodium. Residue G+2 seemed particularly interesting,
because polyamine block was almost abolished and a cysteine at this
position was inaccessible in homomeric G+2C channels (Fig.
3C), but accessible in channels containing both G+2C and
DiS subunits (Fig. 3D). A strong decrease in the
size of the constriction by the G+2C substitution may explain both observations: the constriction might be too small for polyamines to
bind, and MTSET could not react because of steric constraints. To
create a mutant channel with only a small change in pore size compared
with wild type, we substituted the glycine residue at position +2 with
an alanine residue. Reversal potentials in bi-ionic conditions were
recorded from outside-out patches containing channels assembled from
DiS or DiS(G+2A) subunits. Figure
10A shows
current-responses mediated by homomeric DiS channels in outside-out
patches at different voltages. The bath solution contained 100 mM TMA with 100 mM
Na+ in the pipette. The reversal potential
under these conditions was 32.1 ± 3 mV (n = 11). In DiS(G+2A) channels (Fig. 10B), the reversal
potential was strongly shifted leftward to 75.5 ± 2.5 mV
(n = 4), suggesting that the dimensions of the narrow
constriction are much smaller in DiS(G+2A) channels than in DiS
channels. To quantify the change in the dimension of the pore, reversal
potentials of DMA, TriMA, TEA, and TPA were determined (Table
3). The relative permeability of organic
cations over the permeability of Na+ was
plotted against the mean diameter of the organic cations, and the data
were fitted to the hydrodynamic equation (Fig. 10C) (see
Materials and Methods). In this analysis, the diameter of the pore of
DiS channels was ~0.75 nm, in close agreement with previous results
obtained from wild-type GluR-A channels (Burnashev et al., 1996 ). The
diameter of the pore of DiS(G+2A) channels was markedly smaller,
measuring only ~0.58 nm. These results demonstrate that the residue
at position G+2 contributes to the narrow constriction of
GluR-Di channels.

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Figure 9.
Binary representation of cysteine accessibility
patterns: channel-lining residues of the GluR-Di M2
segment. The results shown in Figures 4 and 6 were analyzed with an
ANOVA test, and significance levels were calculated using the
Newman-Keuls procedure. Positions at which cysteine substitution led
to a persistent change of the current amplitude or current
rectification are shown as filled circles, whereas
positions that remained unchanged after exposure to the reagents are
shown as open circles. Externally accessible positions
are grouped in the top part of the Figure and
internally accessible residues are shown on the bottom
part. The accessibility patterns found for the three MTS
reagents were translated to a pattern of exposed residues
(diamonds). Numbers denote residue
position relative to the position 0 (Q/R site).
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Figure 10.
Determinants and dimensions of the narrow
constriction. A, Glutamate-induced currents recorded
from an outside-out patch containing GluR-DiS channels.
Glutamate (1 mM) was applied for 50 msec (thick
bar) at different voltages with 100 mM NaCl in the
pipette and 100 mM TMA in the bath. Peak currents are
plotted against the voltage (right panel,
diamonds). Continuous lines in the
right panel are the I-V
relations recorded before and after switching to TMA solution.
B, As in A, but recording from a patch
containing GluR-DiS(G+2A) channels. C, The
permeability ratio of organic cations versus sodium plotted against the
mean diameter of the organic cation, which are, from
left to right, DMA
(square), TriMA (circle), TMA
(triangle), and TEA (diamond). Only
organic cations with unambiguous reversal potentials are included
(Vrev > 100 mV). The data could be
described with the hydrodynamic equation (lines). The
intercept with the abscissa was taken as an estimate of the mean pore
diameter.
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 |
DISCUSSION |
The present work elucidates the structural environment of the
functionally critical Q/R site in AMPAR channels. We demonstrate that
the M2 segment of the GluR-Di subunit forms a
pore loop originating on the cytoplasmic side of the membrane, with the
Q/R site located at its tip (position 0), and the narrow constriction
formed by position +2 (Fig. 11). To
infer that a residue contributes to the lining of the channel, we
assume the following: first, substitution with a cysteine does not
change the gross structure of the channel; second, only residues
exposed in the water-filled lumen of the channel are accessible to
rapid covalent modification; and third, a persistent change in channel
function indicates that covalent modification of the introduced
cysteine had occurred.

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Figure 11.
Models of the GluR-Di M2 segment and
structural comparisons with NMDAR subunits. A,
Two-dimensional representation of the M2 loop. Upward-pointing
triangles denote positions accessible to extracellularly
applied MTSES; downward-pointing triangles denote
positions accessible to cytoplasmically applied MTSES.
B, As in A, but showing accessibility
patterns for MTSET (shaded triangles) and MTSEA
(shaded and open triangles).
C, Structural model of the M2 segment, location of the
narrow constriction, and positioning of the residues occupying the Q/R
site (black side chains). The asterisk
denotes the projection point of the helix dipole.
Numbers denote positions relative to the Q/R site.
D, Comparison of the patterns of exposed residues in
GluR-Di, NR1, and NR2 subunits. Exposed residues are
printed boldface. A consensus pattern of exposed
residues for GluRs is shown below the alignment; filled
diamonds denote channel-lining positions.
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The M2 segment of the GluR-Di subunit forms a
pore loop
As originally shown in K channels (MacKinnon and Yellen, 1990 ),
re-entrant loop segments are defined by a characteristic pattern: a
residue at the tip of the loop only interacts with impermeant reagents
applied from one side of the membrane, whereas flanking residues
interact only with reagents applied from the opposite side. Such a
pattern is present in the accessibility profile of the negatively
charged MTSES (Fig. 11A), confirming that the M2 segment of the GluR-Di subunit forms a loop. The
patterns found for the positively charged reagents MTSEA and MTSET are
consistent with a pore loop structure as well, although the two-sided
accessibility (Fig. 11B, diamonds) of
several residues, which could be explained if MTSEA and MTSET permeated
through the channel, complicates the interpretation of the results.
Attempts to measure the permeability of the MTS reagents in bi-ionic
conditions with concentrations of up to 150 mM
MTS reagent failed to demonstrate permeability of the reagents, because
GluR-DiS channels were persistently inactivated on exposure to such high concentrations of the reagents (data not
shown). On the basis of size, both MTSEA (1 × 0.48 × 0.48 nm) and MTSET (1 × 0.58 × 0.58 nm) should permeate through
a pore with the smallest diameter of 0.75 nm and react with cysteines exposed on the opposite side of the selectivity filter. However, we
found two-sided accessibility only for cysteines at the tip and at
positions +1, +2, and +4, but not for cysteines located farther away
from the tip. One possible explanation for this discrepancy could be
that the flux rate of the reagents through the channel is low and that
the reagents may become rapidly diluted after passing the narrow region
of the channel, resulting in concentrations too low to produce covalent
modification. Alternatively, the presence of polyamines in the oocyte
whole-cell experiments performed to probe extracellular accessibility
may prevent permeation of the reagents but still allow reaction with
the residues at or close to the narrow constriction. Interestingly, the
larger MTSET showed a similar pattern of two-sided accessibility in
AMPAR as the smaller MTSEA did in NMDAR channels, consistent with the
different dimensions of the pore in the two GluR subtypes.
Secondary structure of the M2 loop
The pattern of exposed residues suggests that the ascending limb
of the loop, on the N-terminal side of the Q/R site, forms an
-helix, whereas the descending limb, on the C-terminal side of the
Q/R site, forms an unstructured random coil. Inferring the secondary
structure of a protein segment from the accessibility of substituted
cysteines requires caution: the nonreactive positions may be exposed
but not accessible to the reagents because of sterical constraints or
particulars of the chemical microenvironment. Another possibility is
that a reaction occurred without affecting the function of the protein.
In addition, the patterns shown in Figures 9 and 11 may arise from two
different activation states of the channel each having a distinct
pattern of exposed residues, because the reagents were applied in the
presence of agonist when channels exist in both open and closed
conformations. Although in this study only kainate was used to
activate GluR-Di channels, other agonists may
produce distinct accessibility patterns that may arise from different
degrees of closure of the agonist-binding domain (Armstrong and Gouaux,
2000 ), consistent with the observation that different subconductance
levels are elicited by the agonists glutamate and kainate (Swanson et
al., 1997 ).
Location of the narrow constriction and positioning of the
Q/R site
The results demonstrate that the narrow constriction in AMPAR
channels is located at and adjacent to the +2 position. The main
evidence derives from the finding that adding a methyl group at the +2
position led to a decrease in pore diameter by ~0.17 nm. Methyl
groups projecting into the lumen perpendicularly to the channel axis
predict a decrease of the pore diameter by ~0.3 nm. The difference
between the predicted and the measured diameters suggests that the
methyl side chains are positioned at an angle, or that they produce a
local conformational change within the random coil that could result in
the repositioning of main chain carbonyl groups facing the pore. Such a
location of the narrow constriction is consistent with the
accessibility patterns of the MTS reagents, although they suggest that
a narrow region may extend from positions +1 to +3.
Position 0 (Q/R site) is located on the external side of the narrow
constriction, providing the possibility that the side chain of the
residue at the Q/R site projects into the extracellular vestibule of
the channel (Fig. 11C). Such an arrangement is consistent with the finding that the diameter of the pore is independent of the
identity of the residue present at the Q/R site (Burnashev et al.,
1996 ). In our model, the Q/R site overlooks the entrance to the narrow
constriction (Fig. 11C) and is therefore ideally positioned
to control passage of ions into the constriction. Position +4 may line
the internal side of the narrow constriction, consistent with the
observation that the MTS reagents reacted most rapidly with a cysteine
residue at position +4 when applied from the cytoplasmic side. Hence,
the narrow constriction seems to be bracketed by two functionally
important positions: the Q/R site on its external side and an aspartate
residue at position +4 on its internal side.
Charge selectivity and anion permeability
The negatively charged MTSES reacted with positions at the narrow
constriction, suggesting that anions can enter deep into the
cation-selective AMPAR channel. This is consistent with the finding
that AMPAR channels with an arginine residue at position 0 exhibit a
weak permeability for Cl (Burnashev et
al., 1996 ). MTSES reacted with a cysteine at position 0 only from the
extracellular side and with a cysteine at position +1 only from the
cytoplasmic side, suggesting that charge selectivity occurs slightly
external to the narrow constriction. One intriguing possibility could
be that in analogy to potassium channels (Doyle et al., 1998 ), the
negative dipole (Roux and MacKinnon, 1999 ) of the pore helix (here
formed by residues on the N-terminal side of position 0) projects into
the space just external to the narrow constriction, where the side
chains of the residues at position 0 might be located (Fig.
11C). With a glutamine residue at position 0, the negative
electrostatic potential would attract cations to the selectivity filter
and repel anions. In contrast, arginine side chains at position 0 would
neutralize the negative electrostatic potential and even create a net
positive potential, thereby facilitating anion permeation. The negative
electrostatic potential of the helix dipole could be thought of as
stabilizing the argininyl group within the space slightly external to
the narrow constriction (Fig. 11C), preventing divalent and
attenuating monovalent ion flux. Such a configuration of the pore loop
raises the possibility that the selectivity filter of AMPAR channels is
formed by two additive mechanisms: an electrostatic mechanism operating
external to a narrow constriction to confer charge selectivity and a
size-selective mechanism operating at the narrow constriction to select
among cations.
Comparison with NMDAR channels
The patterns of exposed residues in the M2 segment of the
GluR-Di subunit are similar to those found in the
NR1 and NR2 subunits (Fig. 11D). In both AMPAR and
NMDAR subunits, the N-terminal region of position 0 is consistent with
an -helical pattern, whereas the C-terminal region suggests a random
coil. A consensus pattern of exposed residues for the M2 segment of the
glutamate receptor family is shown in Figure 11D
(diamonds). The subunits show a similar positioning of the
residue at the 0 position, two-sided accessibility at positions +1 to
+4, and restricted accessibility at position 3. Nevertheless, the
GluR-D pattern is more similar to the NR2 pattern than to the NR1
pattern, consistent with a specialized role of the NR1 subunit in
creating an asymmetric pore (Kuner et al., 1996 ). In conclusion, AMPARs
possess pore loops with a structural design similar to that of NMDAR
channels but different sets of amino acid residues creating different
functional profiles in the two receptor subtypes.
 |
FOOTNOTES |
Received Oct. 11, 2000; revised March 10, 2001; accepted March 22, 2001.
This work was funded by Grant SFB 317/B9 of the Deutsche
Forschungsgemeinschaft to P.H.S. We thank Dr. Johannes Mosbacher for
measuring fast desensitization in GluR-DiS channels, Dr.
Lonnie P. Wollmuth for critically reading this manuscript, Nicole
Bender and Bernhard Sakmann for help with mutagenesis in an early stage of the project, and Annette Herold for DNA sequencing.
Correspondence should be addressed to Dr. Thomas Kuner, Abteilung
Molekulare Neurobiologie, Max-Planck Institut für Medizinische Forschung, Jahnstrasse 29, 69120 Heidelberg, Germany. E-mail: kuner{at}mpimf-heidelberg.mpg.de.
 |
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