John SA and Weiss JN (1999), Novel gating mechanism of polyamine block in th...

XB-ART-13267

J Gen Physiol 1999 Apr 01;1134:555-64.

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Novel gating mechanism of polyamine block in the strong inward rectifier K channel Kir2.1.

Lee JK , John SA , Weiss JN .

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Inward rectifying K channels are essential for maintaining resting membrane potential and regulating excitability in many cell types. Previous studies have attributed the rectification properties of strong inward rectifiers such as Kir2.1 to voltage-dependent binding of intracellular polyamines or Mg to the pore (direct open channel block), thereby preventing outward passage of K ions. We have studied interactions between polyamines and the polyamine toxins philanthotoxin and argiotoxin on inward rectification in Kir2.1. We present evidence that high affinity polyamine block is not consistent with direct open channel block, but instead involves polyamines binding to another region of the channel (intrinsic gate) to form a blocking complex that occludes the pore. This interaction defines a novel mechanism of ion channel closure.

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Species referenced: Xenopus laevis
Genes referenced: kcnj2 tbx2

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	Figure 2. Competitive inhibition of polyamine block by polyamine toxins. (A) Representative traces from the same giant excised inside-out patch showing block of wild-type Kir2.1 channel by various concentrations of spermine (S) in the absence (left) or presence (right) of 30 nM philanthotoxin (T). Recording conditions and voltage-clamp protocol as in Fig. 1. (B–D) Dose–response of outward currents at +40 mV (after 200 ms) to spermine in Kir2.1 wild type (B), D172N (C), and E224G (D), in the absence (○) or presence (•) of philanthotoxin. The gray crosses show the normalized data for philanthoxin + spermine, to better illustrate the shift in K0.5. The superimposed curves are least-squares fits to the Hill equation. Hill coefficients ranged from 0.7 to 0.9. (E) Dose–response curves for wild-type Kir2.1 currents to spermidine (Spd) in the absence (○) and presence (•, gray crosses, normalized) of 30 nM philanthoxin. Hill coefficients ranged from 0.42 to 0.51. (F) Dose–response curve of wild-type Kir2.1 currents at +40 mV to spermine in the absence (○) or presence (•, gray crosses, normalized) of 10 nM argiotoxin (AT). Hill coefficients ranged from 0.77 to 0.99. Data points in B–F represent the mean ± SEM for n = 4–6 patches.
	Figure 3. Long pore plugging model of inward rectification. (A) Reaction scheme for the “long pore” model of direct open channel block by spermine (S) proposed by Lopatin et al. (1995) (shaded area), modified to include direct competitive block by philanthotoxin (T). Cartoons illustrate states in which the channel pore is open (O), blocked by spermine (B1–B3), philanthotoxin (B4), or both spermine and philanthotoxin (B5). K1–5 represent equilibrium constants (kreverse/kforward) for the various transitions. See text for details. (B–C) Fits of the direct block model in A to the experimental data for the spermine–philanthotoxin interaction in wild-type Kir2.1 shown in Fig. 3 B, where ○ are spermine alone, • are spermine + philanthotoxin, and gray crosses are normalized spermine + philanthotoxin. Model parameters in B: K1 = 7.75 × 10−5 M, K2 = 7.75 × 10−5 M, K3 = 7.75 × 10−5 M, K4 = 47 × 10−9 M, K5 = 47 × 10−9 M. In C, the B5 state was disabled by increasing K5 to 103 M. In neither case could the model reproduce quantitatively the increase in K0.5 for spermine in the presence of philanthotoxin.
	Figure 4. Time course of inactivation of outward currents in wild-type Kir2.1 channels. (A) Macroscopic currents were recorded from a giant inside-out patch excised from a Xenopus oocytes expressing wild-type Kir2.1 channels, while superfusing with Mg and polyamine-free bath solution. At the times indicated after patch excision, outward wild-type Kir2.1 currents elicited by voltage clamp pulses to +60 mV from a holding potential of −30 mV showed progressively slower inactivation, reaching a steady state after 5 min. Despite identical amplitudes of inward current at −30 mV (indicating complete unblock), endogenous polyamines still remained available to reblock the current upon depolarization to +30 mV, albeit at a slower rate (e.g., 1- vs. 3-min traces). (B) Rate of inactivation of outward current in four patches. Fraction of noninactivating current (Ifinal/Ipeak) at the end of a 60-ms voltage clamp to +40 mV is plotted for each patch. The rate of inactivation reached steady state by 5 min of washout. (C) Hypothetical schema of channel block by polyamines (left) or polyamine toxins (right) using an intrinsic gate mechanism. Unlike spermine, it is assumed that the hydrophobic head of the toxin molecule is too large to block the pore when its polyamine end is tethered to the intrinsic gate. Conjectured locations of two negatively charged residues D172 and E224 are shown at the pore docking site and at the polyamine-binding site on the intrinsic gate, respectively.
	Figure 5. Intrinsic gate model of inward rectification. (A) The simplest reaction scheme showing spermine (S) and philanthotoxin (T) competition for an intrinsic gate and a pore-docking site in the Kir2.1 channel. Cartoons illustrate the blocked states (B1–B7) and the O3 state in which the toxin is bound to the intrinsic gate, preventing spermine's access to its high affinity blocking pathway (O1 → O2 → B1). K1–5 represent equilibrium constants (kreverse/kforward) for the various transitions. Shaded area represents states involved in spermine block in the absence of toxin, see Fig. 3 A for comparison. See text for further details. (B–D) Fits of the intrinsic gate model in A to the experimental data for the spermine–philanthotoxin interaction shown in Fig. 3, B–D, where ○ are spermine alone, • are spermine + philanthotoxin, and gray crosses are normalized spermine + philanthotoxin. Model parameters for wild-type Kir2.1 (B): K1 = 7.75 × 10−5 M, K2 = 7.75 × 10−5 M, K3 = 5.8 × 10−9 M, K4 = 6 × 10−9 M, K5 = 47 × 10− 9M; for D172N (C): K1 = 7.75 × 10−5 M, K2 = 115 × 10−5 M, K3 = 132 × 10−9 M, K4 = 89 × 10−6 M, K5 = 1,220 × 10−9 M; for E224G (D): K1 = 103 M, K2 = 103 M, K3 = 103 M, K4 = 6,030 × 10−9 M, K5 = 7,090 × 10−9 M.

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