Communications
binding site, but also at the internal entrance to the selectivity
The current–voltage (I/V) curve further indicates that
AAQ acts at the internal TEA binding site and shows that
block by AAQ is distinctly voltage-dependent, so that Iss is
blocked more effectively at more depolarized membrane
potentials (Figure 2c). Under irradiation at 380 nm, the
current increases linearly with voltage once the channels are
fully activated (gray line). Under irradiation at 500 nm, the
current is predominantly blocked at all membrane potentials
(black line). However, irradiation at 420 nm, which produces
only partial conversion to the cis isomer, reveals voltage-
dependent block (dashed black line), as indicated by the
decline in Iss at potentials more positive than + 10 mV
(Figure S4a in the Supporting Information shows the raw
current responses). This result is typical of positively charged
intracellular K+ channel blockers.[10,22] Just as depolarization
provides a driving force for positively charged K+ ions to flow
in the outward direction, internal alkyl ammonium ions are
driven into their binding site within the membrane electric
field and block more effectively as membrane depolarization
is increased.
filter.[12–15] Charged blockers of the internal but not external
TEA binding site exhibit “open-channel block”, wherein pore
occupancy does not occur until after the voltage gate has
opened.[9,10,16] This effect is most easily observed in Shaker IR
(Sh-IR) and other channels that lack the fast-inactivating
N-terminal peptide.[17,18] In response to step depolarization,
some ionic current initially flows through the unbound
channel, but this flow quickly decays over tens of milliseconds
as the blocking molecules bind to the pore.
Figure 2a shows the current responses to depolarizing
voltage steps of a HEK293 cell expressing Sh-IR that has been
treated with 400 mm AAQ. Under irradiation at 380 nm, the
As K+ ions move through the permeation pathway of K+
channels in a single file, high concentrations of external K+
([K+]o) electrostatically repel intracellular charged blockers
to accelerate their exit rate from the channel and thereby
reduce their blocking potency.[23,24] Accordingly, the extent of
AAQ block correlates inversely with the extracellular potas-
sium concentration [K+]o , as revealed by the current values
shown in Figure 2d. After establishing a voltage clamp in
standard external buffer ([K+]o = 1.5 mm) and measuring Iss
under irradiation at 380 and 500 nm, cells were locally
perfused with solutions containing 0.3 mm and 20 mm [K+]o .
We controlled for the change in maximal current, which
results from the altered K+ driving force, by measuring
currents at 380 nm, which completely unblocks the channels.
This trend of lower efficiency was consistent across the range
of voltages that activate Sh-IR (Figure S4b in the Supporting
Information).
Consistent with this mode of action, direct application of
AAQ to the internal TEA binding site in both the inside-out
patch (Figure 3) and whole-cell recordings (Figure S5a in the
Supporting Information) also produced photoswitchable
open-channel block. Because inclusion in the patch pipette
does not permit solution exchange at the cytosolic interface,
inside-out patches were pulled from HEK293 cells expressing
Sh-IR to allow AAQ application, followed by washout. In this
Figure 2. AAQ is an open-channel blocker of the Sh-IR internal TEA-
binding site. a,b) Whole-cell current responses to 200 ms depolarizing
voltage steps from À70 to +40 mV under irradiation at 380 nm (gray
line) or 500 nm (black line). a) Open-channel block is apparent in
AAQ-treated Sh-IR channels (scale bar: 6 nA, 25 ms). b) Open-channel
block is absent in MAQ-treated SPARK channels (scale bar: 0.5 nA,
25 ms). c) Steady-state I/V curves under 380 nm (gray line), 420 nm
(black dashes) and 500 nm (black line) irradiation. I/V curves from
each of four cells were normalized to the current measured at 380 nm
and +60 mV. d) Dependence of AAQ block on [K+]o . Whole-cell
current responses of a cell to depolarizing voltage steps from À70 to
+40 mV under irradiation at 380 nm (gray line) or 500 nm (black line)
at the indicated [K+]o value. Similar results were obtained in two other
cells (Scale bar: 5 nA, 50 ms.)
channels are not blocked by AAQ (gray trace). However,
when the channels are blocked by AAQ under irradiation at
500 nm, an initial transient current remains (Ipk), which
rapidly decays so that nearly all of the steady-state current
(Iss) is blocked (black trace). This effect is not observed during
blockade of SPARK channels,[19] which contain an extracel-
lular cysteine residue for covalent attachment of the male-
imide analogue MAQ (2; Figure 2b).
The data obtained suggest that AAQ acts predominantly
at the internal TEA binding site of Sh-IR, while MAQ acts on
the external TEA binding site of the SPARK channels.[20,21]
A
more extensive characterization of the open-channel block
observed with AAQ is provided in Figure S3 in the Support-
ing Information. These experiments directly demonstrate the
requirement for channel opening to occur before AAQ is able
to block the pore, and reveal that pore occupancy is
correlated with the frequency of channel opening.
Figure 3. AAQ is a PCL for the internal-TEA binding site of Sh-IR. a) Iss
recorded from inside-out patches as AAQ was applied at the indicated
concentrations (mm). b) Dose-response relationships for AAQ applied
to inside-out patches under 500 nm (black line) and 380 nm (gray line)
irradiation.
ꢀ 2009 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim
Angew. Chem. Int. Ed. 2009, 48, 9097 –9101