The RCK1 domain of the human BK_Ca channel transduces Ca²⁺ binding into structural rearrangements

Abstract

Large-conductance voltage- and Ca²⁺-activated K⁺ (BK_Ca) channels play a fundamental role in cellular function by integrating information from their voltage and Ca²⁺ sensors to control membrane potential and Ca²⁺ homeostasis. The molecular mechanism of Ca²⁺-dependent regulation of BK_Ca channels is unknown, but likely relies on the operation of two cytosolic domains, regulator of K⁺ conductance (RCK)1 and RCK2. Using solution-based investigations, we demonstrate that the purified BK_Ca RCK1 domain adopts an α/β fold, binds Ca²⁺, and assembles into an octameric superstructure similar to prokaryotic RCK domains. Results from steady-state and time-resolved spectroscopy reveal Ca²⁺-induced conformational changes in physiologically relevant [Ca²⁺]. The neutralization of residues known to be involved in high-affinity Ca²⁺ sensing (D362 and D367) prevented Ca²⁺-induced structural transitions in RCK1 but did not abolish Ca²⁺ binding. We provide evidence that the RCK1 domain is a high-affinity Ca²⁺ sensor that transduces Ca²⁺ binding into structural rearrangements, likely representing elementary steps in the Ca²⁺-dependent activation of human BK_Ca channels.

INTRODUCTION

Ca²⁺ plays a central role as a ubiquitous signaling molecule in fundamental physiological processes and can directly or indirectly modulate the activity of a large number of proteins (Clapham, 1995; Carafoli and Klee, 1999), including several families of ion channels. In some cases, ion channels acquire Ca²⁺ sensitivity by associating with Ca²⁺-binding proteins, such as calmodulin, that in turn modulate channel properties (Pitt, 2007). In contrast, the large-conductance voltage- and Ca²⁺-activated K⁺ (BK_Ca or MaxiK) channels (Marty, 1981; Pallotta et al., 1981; Latorre et al., 1982), which regulate a multitude of physiological processes including smooth muscle tone, uresis, immunity, and neurotransmission (Tang et al., 2004b; Lu et al., 2006; Salkoff et al., 2006; Cui et al., 2009), appear to be directly modulated by intracellular Ca²⁺ that binds to specialized intracellular modules known as regulator of K⁺ conductance (RCK) domains (Pico, 2003; Niu et al., 2004; Lingle, 2007; Yusifov et al., 2008; Yuan et al., 2010; Wu et al., 2010).

It has been proposed that RCK domains operate as chemo-mechanical transducers that convert the free energy of Ca²⁺ binding (or other ligands) into mechanical work that ultimately opens the channel pore (Jiang et al., 2001, 2002; Niu et al., 2004; Chakrapani and Perozo, 2007). Significant insights into the structure and function of these domains were provided by crystallographic data of bacterial RCKs (Jiang et al., 2001, 2002). Sequence analysis suggests that two tandem regions of the large cytoplasmic domain of eukaryotic BK_Ca channels’ protein conformation, RCK1 and RCK2, are structurally homologous to bacterial RCK domains (Jiang et al., 2002; Pico, 2003; Roosild et al., 2004; Fodor and Aldrich, 2006, 2009; Kim et al., 2006, 2008; Latorre and Brauchi, 2006; Yusifov et al., 2008). Indeed, the large BK_Ca cytosolic C terminus, recently visualized at 17–20-Å resolution by cryo-electron microscopy (Wang and Sigworth, 2009), is thought to comprise a hetero-octameric assembly of RCK1 and RCK2 domains akin to the gating ring of prokaryotic channels. This view is supported by two recent studies that report on the atomic structure of the cytoplasmic domain of the BK_Ca channel (Wu et al., 2010; Yuan et al., 2010). Tandem RCK1 and RCK2 domains interact with each other within the same subunit; these four RCK1/RCK2 pairs assemble in a gating ring structure through “assembly” interfaces (Wu et al., 2010; Yuan et al., 2010).

RCK domains in BK_Ca channels are thought to be involved in high-affinity Ca²⁺ sensing (Niu et al., 2004; Latorre and Brauchi, 2006; Qian et al., 2006; Lingle, 2007; Yusifov et al., 2008). In the RCK2 domain, high-affinity Ca²⁺ sensing is endowed by a Ca²⁺-binding region termed the “Ca²⁺ bowl” consisting of five consecutive aspartates (894–898) (Schreiber and Salkoff, 1997; Schreiber et al., 1999), which are critical for Ca²⁺ binding (Bian et al., 2001; Braun and Sy, 2001; Bao et al., 2004; Sheng et al., 2005; Yuan et al., 2010) and Ca²⁺-induced conformational changes (Yusifov et al., 2008). In RCK1, mutations of aspartates 362/367 or methionine 513 reduce the high-affinity Ca²⁺ sensitivity of the channel (Bao et al., 2002; Xia et al., 2002; Zeng et al., 2005; Sweet and Cox, 2008). Indeed, the concomitant neutralization of D362/367 (RCK1) and the Ca²⁺ bowl (RCK2) to alanine residues completely abolishes the high-affinity Ca²⁺ dependence of BK_Ca channels (Xia et al., 2002; Zeng et al., 2005; Sweet and Cox, 2008). However, no Ca²⁺-binding sites within the RCK1 domain have yet been observed (Wu et al., 2010; Yuan et al., 2010). Thus, the molecular details of Ca²⁺ sensing in the RCK1 domain remain unknown.

To shed light on the molecular basis for Ca²⁺-dependent channel activation, we have expressed and purified the cytosolic part of the BK_Ca channel corresponding to the RCK1 region and interrogated its function as a Ca²⁺ sensor, as previously performed for the RCK2 domain (Yusifov et al., 2008). We postulate that a Ca²⁺ sensor involved in the Ca²⁺-dependent activation of the channel must satisfy the following criteria: bind Ca²⁺; undergo Ca²⁺-dependent conformational transitions (to exert mechanical force to open the pore); operate in a physiologically relevant range of [Ca²⁺]; and, finally, mutations of critical residues involved in Ca²⁺-dependent channel activation should perturb either Ca²⁺ binding, the transduction mechanism, or both. We have used a combination of optical and biochemical methods to test these criteria for the RCK1 domain of the human BK_Ca (Slo1) channel.

MATERIALS AND METHODS

Expression and purification of the human BK_Ca RCK1 and RCK2 domains

Expression and site-directed mutagenesis of the human Slo1 RCK1 domain with flanking N- and C-terminal regions (³²²IIE…HDP⁶⁶⁷) and the BK_Ca RCK2 domain (⁶⁶⁵HDP…ALK¹⁰⁰⁵) were performed as described previously (Yusifov et al., 2008). The protein fractions were solubilized in 50 mM Tris-HCl and 8 M urea, pH 8.0. The supernatant was refolded by dialysis to 50 mM Tris and 2 mM EGTA, pH 7.5, and applied to a Ni-NTA affinity column. The protein fractions were eluted with 250 mM imidazole and dialyzed against 25 mM MOPS, 2 mM EGTA, and 120 mM KCl, pH 7.2. The purity of the expressed proteins was analyzed using a 12.5% SDS-PAGE. Protein concentrations were determined using the Biuret-Lowry assay.

Size-exclusion chromatography

The purified BK_Ca RCK1 or RCK2 domains were solubilized in 8 M urea. 500 µl of each sample was refolded onto a Superdex 200 10/300 column with a flow rate of 0.5 ml/min, equilibrated with a buffer containing 50 mM Tris and 5 mM EGTA, pH 8.4, or 20 mM MOPS and 2 mM EGTA, pH 7.2. The refolded protein fractions eluted between 10 and 11 ml were collected and reinjected into the sizing column and eluted in equilibrium buffer. The apparent mol wt of RCK1 and RCK2 was determined by constructing a calibration plot from the elution profiles of protein standards of known mol wt (MWGF1000; Sigma-Aldrich).

Multi-angle laser light scattering (MALLS)

MALLS experiments were performed with a DAWN-EOS MALLS detector coupled to an Optilab refractometer (Wyatt Technologies) and a UV-absorption spectrophotometer. The purified RCK1 domain (100 µl; 0.1 mg/ml) in 25 mM MOPS, 2 mM EGTA, and 120 mM KCl, pH 7.2, was loaded onto a QC-PAK GFC 300 column (Tosoh Bioscience). Light-scattering data were acquired from 14 detectors (detectors 1–4 were disabled, as they are unreliable for aqueous solutions) and fit by the following equation based on the Zimm formalism, using the Astra 5.3.4 program (Wyatt Technologies):

$$\left(K\text{*}c\right)/R\left(\theta \right)=\text{1}/[\mathit{M}W\times P(\theta \left)\right],$$

where K* is an optical parameter equal to 4π²n²(dn/dc)²/(${\lambda }_0^4$ N_A), where n is the solvent refractive index, dn/dc is the refractive index increment (0.185), λ is the wavelength of the scattered light in vacuum (cm), and N_A is Avogadro’s number. Parameter c is the sample concentration in g/ml, R(θ) is the excess intensity of scattered light at DAWN angle θ, MW is the weighted-average mol wt, and P(θ) describes the angular dependence of the scattered light. The proportion of eluted protein, determined by UV absorption at 280 nm, was binned according to mol wt, as determined by light scatter analysis.

Circular dichroism (CD) spectroscopy

CD spectra and free [Ca²⁺] were obtained as described previously (Yusifov et al., 2008). CD data are presented in units of molar ellipticity per residue. Computational analysis of the far-UV CD spectra of the purified proteins was done using the SELCON3 algorithm of the CDPro software package (Sreerama and Woody, 2004). Secondary structure composition was estimated using SMP56 (IBasis 10). Normalized root mean-square deviation is defined as

$${\left[{\displaystyle \sum {({\theta }_{\text{exp}}-{\theta }_{\mathit{cal}})}^2/{\displaystyle \sum {\left({\theta }_{\text{exp}}\right)}^2}}\right]}^{1/2},$$

where θ_exp and θ_cal is the experimental and calculated molar ellipticity per amino acid residue, respectively. The number of the α-helix secondary structure segments (n_α) was calculated by dividing the number of residues included in the distorted α-helix structure by a factor of four and in the distorted β structure (n_β) by a factor of two.

Time-resolved fluorescence

The time-resolved fluorescence decay of endogenous tryptophan was recorded with a spectrofluorometer (Fluorolog-3; HORIBA) using the time-correlated single-photon counting method at 22°C with a pulsed nanoLED at λ_ex = 296 nm. Ludox was used as scatter solution. The fluorescence intensity decay data were fit with a sum of three exponential functions, using the DAS6 v6.4 software (HORIBA):

$$I\left(t\right)={\displaystyle \sum _{i=1}^n{\alpha }_i\hspace{0.17em}}\text{exp}(-t/{\tau }_i),$$

where I is the fluorescence intensity and α_i and τ_i are the normalized preexponential factors and decay times, respectively. The average fluorescence lifetimes (τ_avg) for three exponential iterative fittings are calculated from the decay times and preexponential factors using equations

$${\tau }_{\mathit{avg}}={\displaystyle \sum _{i-1}^n{f}_i{t}_i,}$$

where f_i shows the fractional contribution of each decay time to the steady-state intensity, which is given by

$$f_i={\alpha }_i{\tau }_i/{\displaystyle \sum {\alpha }_j}{\tau }_j.$$

The goodness of the fit was determined from its χ² value and the variance of the weighted residual distribution.

Steady-state fluorescence

Intrinsic tryptophan fluorescence spectra were recorded with protein concentrations of 0.1 mg/ml in 25 mM MOPS, 2 mM EGTA, and 120 mM KCl, pH 7.2. Fluorescence measurements were obtained using excitation/emission slit widths of 5 nm each, with λ_ex = 295 nm. The tryptophan emission fluorescence spectra were collected in the wavelength range of 300–400 nm. Experiments were fit with a Hill function in the form:

$$F_{\mathit{330}}=\left(F_{\mathit{max}}-F_{\mathit{min}}\right)/{\left(1+\left(\left[{\text{Ca}}^{2+}\right]\right)/K_{\mathit{1/2}}\right)}^{\text{n}}+F_{\mathit{min}}.$$

⁴⁵Ca²⁺-binding assay

Purified wild-type (WT) and D362/367A-RCK1 (30 µg each) were centrifuged at 13,000 rpm for 5 min and then blotted onto nitrocellulose membranes prestained with 0.1% Ponceau S and 5% acetic acid (Morçöl and Subramanian, 1999). 10 µg troponin and 10 µg glutathione S-transferase (GST) were used as positive and negative controls, respectively. After protein blotting, the membranes were stained again with Ponceau S and washed five times with distilled water to remove nonspecific staining and estimate the relative protein abundance. The membranes were then probed by ⁴⁵Ca²⁺ overlay as reported previously (Levitsky et al., 1994). In brief, the membranes were placed in a wash solution containing 60 mM KCl, 10 mM imidazole, and 2 mM MgCl₂, pH 7.2, for 30 min, followed by a 60-min wash in the same solution supplemented with 115 µM CaCl₂, and different concentrations of EGTA to obtain the desired free [Ca²⁺]. Then, 6 µC/ml ⁴⁵Ca²⁺ (PerkinElmer) was added to this solution, and the membrane was washed for an additional 10 min. The free [Ca²⁺] was estimated with WebMaxC and measured with a Ca²⁺-selective electrode (WPI) or by using a calibration curve constructed from the fluorescent Ca²⁺-sensitive Ca²⁺ green 5N dye (Takahashi et al., 1999). The membranes were then washed twice in distilled water, dried, and exposed to a phosphor storage screen for 1–3 d. Relative binding was obtained by dividing the pixel values of the ⁴⁵Ca²⁺ signal of each protein by the pixel values of its Ponceau S staining using the ImageJ 1.43S program (http://rsb.info.nih.gov/ij/).

Cleavage of N-terminal 6xHis tag of the purified WT-RCK1 domain was performed using the TAGZyme system (QIAGEN). In brief, 50 µg RCK1 was incubated in the presence of 5 U/ml dipeptidyl aminopeptidase I (DAPase) enzyme mixed with 2 mM cysteamine-HCl (QIAGEN) for several time intervals at 37°C. Reaction efficiency of 6xHis tag cleavage was analyzed using InVision His tag in-gel stain (Invitrogen). The WT-RCK1 domain lacking the 6xHis tag was separated from undigested 6xHis-tagged RCK1 and DAPase using NI-NTA immobilized metal affinity chromatography (IMAC; QIAGEN).

RESULTS

Expression and purification of the C terminus region of the human BK_Ca channel corresponding to the RCK1 domain

To directly investigate the structure and Ca²⁺-sensing properties of the human BK_Ca RCK1 domain in solution, we expressed and purified the region of the human BK_Ca channel C terminus corresponding to the amino acid sequence ³²²IIE…HDP⁶⁶⁷ (Wallner et al., 1995), which includes the S6-RCK1 linker (³²²IIE…GRK³⁴³), the RCK1 domain (³⁴⁴HIV…FYC⁶¹²), and part of the RCK1-RCK2 interconnecting linker (⁶¹³KAC…HDP⁶⁶⁷) (Yuan et al., 2010). In spite of the poor amino acid sequence similarity between the BK_Ca channel RCK1 domain and the MthK RCK domain (<25%), they share structural similarities (Fig. 1 A).

Figure 1.

Purification of the RCK1 domain of the human BK_Ca channel. (A) Structure-based sequence alignment of the BK_Ca channel (GI, 507922) C terminus (encompassing the RCK1 domain) with the MthK (GI, 2622639) RCK domain. The α helices are depicted as bars, and β strands are shown as arrows. The secondary structures (obtained from the DSSP reference set) above the sequences (blue) are obtained from the atomic structure of the BK_Ca C-terminal domain (Protein Data Bank accession no. 3MT5) (Yuan et al., 2010) and below the sequences (orange) are obtained from the atomic structure of the MthK RCK domain (Protein Data Bank accession no. 2AEF) (Dong et al., 2005). Light blue and light orange bars correspond to 3₁₀ helices. Dotted lines are unresolved regions in the respective crystal structures. Semi-conserved residues within ordered structures are highlighted yellow. Residues known to be involved in high-affinity Ca²⁺ sensitivity in the BK_Ca RCK1 domain (D362/D367 and M513) are highlighted red. (B) 12.5% SDS-PAGE of purified WT-RCK1 and D362/367A-RCK1 stained with Coomassie blue. Both proteins migrate as an ∼40-kD band, consistent with their expected mol wt (41 kD).

We also expressed and purified a RCK1 mutant carrying the D362A/367A mutations to probe the role of these residues, which are known to be critical for high-affinity Ca²⁺ sensitivity (Xia et al., 2002; Zeng et al., 2005; Sweet and Cox, 2008). The purity of the two proteins was assessed by SDS-PAGE. The WT and D362/367A-RCK1 domains both migrate as a 40-kD band in denaturating conditions, close to their theoretical mol wt of a monomeric RCK1 domain (41 kD; Fig. 1 B).

The secondary and quaternary structures of the RCK1 domain in solution share similarities with bacterial RCK domains

The secondary structure of the purified RCK1 domain was probed by CD spectroscopy, a powerful technique for the determination of secondary structure composition and ligand-induced conformational changes of proteins in solution (Kelly et al., 2005; Greenfield, 2006). The far-UV CD spectrum of WT-RCK1 in nominal Ca²⁺ (free [Ca²⁺] = 0.00058 µM) is presented in Fig. 2 A. The CD spectrum of WT-RCK1 shows an inflection at 210 nm and a minimum at 220 nm, characteristic of significant α-helical content (Sreerama and Woody, 2004; Turk et al., 2006). The analysis of the CD spectrum of WT-RCK1 in solution suggests a secondary structure composition of ∼28% α helix and ∼23% β strand, organized in ∼10 α helices and ∼15 β strands. RCK1’s folding pattern, analyzed using the cluster algorithm (Sreerama et al., 2001), revealed an α/β fold (in a consecutive β–α–β pattern; Table I), a common structural motif of the Rossmann fold (Rao and Rossmann, 1973), and an important structural feature of the RCK domains (Jiang et al., 2001, 2002; Wu et al., 2010; Yuan et al., 2010).

Figure 2.

Structural analysis of WT and D362/367A RCK1. (A) Far-UV CD spectra of WT-RCK1 and D362/367A-RCK1 domains obtained in nominal free [Ca²⁺] (0.00058 µM). The CD spectrum of WT-RCK1 exhibits a strong signal at 220 nm, whereas D362/367A displays different spectral properties with a red-shifted minimum at 223 nm (relative to WT-RCK1), suggesting that the double D362/367A mutation altered its secondary structure. (B) Characteristic size-exclusion column profile of the purified WT-RCK1 domain reveals an elution peak at ∼10.5 ml. (C) A calibration curve is established by plotting the log (mol wt) of proteins with known mol wt versus their elution peak (R² = 0.91). The purified WT-RCK1 domain is calculated to elute with an apparent mol wt of 341 ± 10.0 kD (n = 7), suggesting a homo-octameric assembly of RCK1 domains (theoretical octameric mol wt = 328 kD).

Table I.

Estimated secondary structure composition of RCK domains

	CD spectroscopy			X-ray diffraction
	BKCa RCK1, 0 Ca2+	BKCa RCK1, 35 µM Ca2+	BKCa RCK1-D362/367A	BKCa RCK1	MthK RCK	MthK RCK Ca2+ bound
Amino acids	322IIE…HDP667, 346 aa			343KHI…IEY570, 577SRI…YCK613, 265 aa	116RHV…ISA336, 221 aa
Reference		This study		Yuan et al., 2010	Ye et al., 2006	Jiang et al., 2002
α helix (%)	28.1 ± 0.751	19.3 ± 0.557	24.8 ± 0.0882	39.6 (30)	40.9	38.2
nα helix	10.3 ± 0.415	7.81 ± 0.288	9.26 ± 0.0302	14	12	13
β strand (%)	23.2 ± 0.318	30.2 ± 0.731	25.4 ± 0.208	18.5 (14)	22.3	22.3
nβ strand	15.4 ± 0.181	18.3 ± 0.582	14.6 ± 0.396	12	12	12
Turn + unordered (%)	48.9 ± 0.503	46.8 ± 0.689	48.7 ± 0.306	41.9 (56)	36.8	39.5
NRMSD	0.0630 ± 0.00900	0.0827 ± 0.0123	0.115 ± 0.00762
Fold	α/β	α/β	α/β	α/β	α/β	α/β

Secondary structure composition of the BK_Ca RCK1 and MthK RCK domains. Deconvolution of far-UV CD spectra performed on the purified WT-RCK1 in the presence and absence of Ca²⁺ and D362/367A-RCK1 into percent secondary structural contributions. The WT-RCK1 domain in 0.00058 µM Ca²⁺ has higher α-helical content than D362/367A-RCK1. The addition of Ca²⁺ to WT-RCK1 changes the secondary structure fractions of the RCK1 domain, decreasing the α-helix content and increasing the β-strand content (see Fig. 6). Secondary structure fractions of the crystallized BK_Ca RCK1 domain (Protein Data Bank accession no. 3MT5 estimated from the resolved regions ³⁴³KHI…IEY⁵⁷⁰ and ⁵⁷⁷SRI…YCK⁶¹³) and the MthK RCK domain in the presence (Protein Data Bank accession no. 1LNQ) or absence (Protein Data Bank accession no. 2FY8) of Ca²⁺ are provided for reference, obtained from the DSSP reference set. Note that the purified RCK1 domain in this study is composed of 346 amino acids (³²²IIE…HDP⁶⁶⁷, which amounts to an 81–amino acid difference between the RCK1 domain in this study and the BK_Ca RCK1 x-ray structure, and a 126–amino acid difference with respect to the two MthK RCK domains). This region includes the flanking S6-RCK1 linker and part of the RCK1-RCK2 linker, which were not included or resolved in the BK_Ca crystal structure. The structure fractions reported in parentheses were estimated by assuming the unresolved RCK1 flaking linker regions possessed no additional α or β structures. Errors represent standard errors of the mean (n = 3). NRMSD, normalized root mean-square deviation.

The oligomeric state of the purified RCK1 domain was investigated using size-exclusion chromatography. Fig. 2 B shows the elution profile of purified RCK1 on a Superdex 200 10/300 column. The elution peak (10.4 ± 0.08 ml; n = 7 elutions; errors represent standard errors of the mean) correlates to an apparent mol wt of 341 ± 10.0 kD, very close to the expected mol wt of a RCK1 octamer (theoretical RCK1 × 8 = 328 kD), according to a calibration curve constructed with protein standards of known mol wt (Fig. 2 C). These data suggest that the WT-RCK1 domain in solution preferentially self-assembles into octamers. A MALLS analysis (Wen et al., 1996; Folta-Stogniew and Williams, 1999; Philo, 2006) performed on the RCK1 domain in solution confirms its octameric organization. The elution profile of the WT-RCK1 domain is shown in Fig. 3 A. The corresponding mol wt distribution, estimated from light-scattering analysis, is shown superimposed (red circles). A representative Debye plot of light-scattering data with Zimm formalism, taken from the elution slice 2.893 ml, is shown in Fig. 3 B. The inverse of the y-axis intercept of the fit yields a molecular mass of ∼331 kD (Fig. 3 B). A histogram of the relative abundance of mol wts of the eluted protein between volumes 2.6 and 3.3 ml is shown in Fig. 3 C. The majority of eluted WT-RCK1 (76.3%) had mol wts between 316 and 398 kD (mean = 352 ± 24.2 kD). Thus, the purified RCK1 domain preferentially assembles in solution into homo-octamers, similar to bacterial RCK domains (Jiang et al., 2002; Parfenova et al., 2007).

Figure 3.

Mol wt determination using MALLS. (A) The normalized absorption at 280 nm (continuous line) of eluted WT-RCK1 is superimposed with its mol wt distribution (red circles) calculated from light-scattering data. (B) A Debye plot with Zimm formalism is shown using the light-scattering data from 14 detectors for the sample at elution volume 2.893 ml. Extrapolation of the fit to zero angle reveals a mean mol wt of eluted protein corresponding to 331 kD. (C) Relative protein abundance (calculated from UV absorbance) of samples eluted between volumes 2.6 and 3.3 ml binned according to mol wt, calculated from MALLS analysis. According to this cumulative distribution, 76.3% of eluted protein had mol wt between 316 and 398 kD, with a mean of 352 ± 24 kD.

The neutralization of D362 and D367 alters the structure of the RCK1 domain

Within the RCK1 domain, two aspartates (D362 and D367) are critical for the BK_Ca channel’s Ca²⁺ sensitivity in the µM range (Xia et al., 2002; Zeng et al., 2005; Sweet and Cox, 2008). To investigate the structural and functional roles of these residues on RCK1, we introduced mutations D362/367A and probed the secondary structure of the purified D362/367A-RCK1 in solution. Its CD spectrum (shown in Fig. 2 A) is altered as compared with the WT-RCK1 domain. Specifically, a red-shifted minimum from 220 to 223 nm suggests a change in the secondary structure. The analysis of D362/367A-RCK1 CD spectrum reveals that its β content increased from 23 ± 0.3% to 25 ± 0.2%, whereas the α-helix fraction was reduced from 28 ± 0.7% to 25 ± 0.1% compared with WT-RCK1 (Table I). An increase in the β content of proteins has been related to oligomerization (Rotondi and Gierasch, 2006; Zimmer et al., 2006). Interestingly, although WT-RCK1 preferentially self-assembles into an octameric state (Figs. 2, B and C, and 3), we found from size-exclusion chromatography that the D362/367A-RCK1 domain has an apparent mol wt higher than 670 kD (>16-mer). These results suggest that although D362/367A-RCK1 remains soluble and displays an ordered structure, its conformation and oligomeric state are altered.

Time-resolved fluorescence spectroscopy distinguishes between the conformational states of the apo- and Ca²⁺-bound states of the RCK1 domain

To investigate the Ca²⁺-dependent properties of the RCK1 domain, we took advantage of the three RCK1 endogenous tryptophan residues (W475/477/524) that can serve as fluorescent probes to resolve possible Ca²⁺-induced conformational changes. Tryptophan fluorescence lifetime is sensitive to its local environment; therefore, different conformational states of proteins have been reported (Lakowicz, 2006). We used time-correlated single-photon counting spectroscopy to record the excited-state fluorescence lifetime measurements of the endogenous tryptophan residues in the RCK1 domain. The fluorescence intensity decay of WT-RCK1 and D362/367A-RCK1 in the absence and presence of Ca²⁺ are shown in Fig. 4.

Figure 4.

Ca²⁺-induced conformational changes revealed by the intrinsic tryptophan fluorescence lifetime. Intrinsic tryptophan fluorescence intensity decay of (A) WT-RCK1 and (B) D362/367A-RCK1 recorded in the absence (free [Ca²⁺] = 0.00058 µM; blue) and presence (35 µM; red) of Ca²⁺. Black solid curves are the best fit to a triple-exponential decay (Table II). Residuals are shown below the decay curves. The intensity decay of a scattering solution (IRF) is shown in gray. The goodness of the fit was determined from its χ² value and the variance of the weighted residual distribution. The triple-exponential analyses gave a χ² value close to unity (χ² of ∼0.86–0.95), whereas fitting the fluorescence decays to the sum of four exponential functions did not improve the accuracy of the fit.

The decay of the fluorescence intensity was well fit by the sum of three exponential functions. Mean with standard error fluorescence decay parameters for WT-RCK1 and D362/367A RCK1 in the presence and absence of Ca²⁺ are shown in Table II. The decay of WT-RCK1 fluorescence in the absence of Ca²⁺ (free [Ca²⁺] = 0.00058 µM) is dominated by the intermediate (τ = 2.0 ± 0.068 ns) and the long-lived components (τ₃ = 5.4 ± 0.049 ns) that have fractional contributions of f₂ = 49% and f₃ = 37% of the total fluorescence intensity, respectively (Table II). The fraction of the shortest-lived component (τ₁ = 0.62 ± 0.040 ns) is f₁ = 14% (n = 3; ±SEM).

Table II.

Time-resolved fluorescence lifetime parameters

RCK1	WT		D362/367A
	−Ca2+	+Ca2+	−Ca2+	+Ca2+
τ1 (ns)	0.62 ± 0.040	0.70 ± 0.018	0.68 ± 0.096	0.71 ± 0.025
τ2 (ns)	2.0 ± 0.068	1.6 ± 0.011	2.0 ± 0.14	1.9 ± 0.033
τ3 (ns)	5.4 ± 0.049	5.1 ± 0.030	5.4 ± 0.10	5.4 ± 0.023
α1	0.42 ± 0.032	0.29 ± 0.020	0.46 ± 0.054	0.45 ± 0.017
α2	0.45 ± 0.026	0.64 ± 0.018	0.44 ± 0.052	0.45 ± 0.016
α3	0.12 ± 0.0052	0.068 ± 0.0020	0.10 ± 0.0021	0.10 ± 0.0012
f1	0.14 ± 0.021	0.13 ± 0.0088	0.18 ± 0.040	0.18 ± 0.013
f2	0.49 ± 0.011	0.65 ± 0.0062	0.50 ± 0.033	0.50 ± 0.010
f3	0.37 ± 0.010	0.22 ± 0.0027	0.32 ± 0.0073	0.31 ± 0.0028
τavg (ns)	3.1 ± 0.010	2.3 ± 0.067	2.8 ± 0.049	2.8 ± 0.0037
χ2	0.95 ± 0.0053	0.86 ± 0.0092	0.95 ± 0.018	0.95 ± 0.0069

Triple-exponential fitting parameters of fluorescence lifetime. Lifetime fluorescence was recorded at λ_em = 330 nm (λ_ex = 296 nm). Fractional preexponential factors α_i correspond to lifetimes τ_i, respectively. f_i is fractional contribution of each decay time, and τ_avg · χ² values indicate goodness fit. Errors represent standard errors of the mean (n = 3).

In contrast, the WT-RCK1 domain in the Ca²⁺-bound state (free [Ca²⁺] = 35 µM) has an intermediate component with a faster time constant of τ₂ = 1.6 ± 0.011 ns and an increased fractional component to f₂ = 65% when compared with WT-RCK1 in nominal [Ca²⁺]. Furthermore, the time course of the longest-lived component remained practically unchanged (τ₃ = 5.1 ± 0.030 ns), but its fractional contribution decreased to f₃ = 22%. The time course and fractional contribution of the shortest-lived component remained practically unchanged (τ₁ = 0.7 ± 0.018 ns; f₁ = 13%). Also, as shown in Fig. 4 A and Table II, the average excited-state lifetime time constant of the Ca²⁺-bound protein (free [Ca²⁺] = 35 µM; τ_avg = 2.3 ± 0.067 ns; n = 3) is markedly lower than the apo–WT-RCK1 (τ_avg = 3.1 ± 0.010 ns), suggesting a Ca²⁺-induced conformational change. On the contrary, the fluorescence lifetime parameters for D362/367A-RCK1 remain similar with the addition of Ca²⁺, indicating that D362 and D367 are necessary for Ca²⁺ binding, functional transduction of Ca²⁺ binding into conformational rearrangements of the RCK1 domain (Fig. 4 B), or both. We have further explored the effects of these mutations on the Ca²⁺-sensing properties of RCK1.

Steady-state tryptophan fluorescence reports Ca²⁺-induced conformational changes in the RCK1 domain

The results from the fluorescence lifetime experiments suggest that the conformational state of RCK1 domain in solution is [Ca²⁺] dependent (Fig. 4). As BK_Ca channels operate in micromolar [Ca²⁺], we sought to resolve the Ca²⁺ dependence of the observed conformational changes in the following experiments. We recorded changes in steady-state tryptophan fluorescence intensity with increasing [Ca²⁺] to determine RCK1’s apparent affinity for Ca²⁺. The fluorescence emission spectrum of WT-RCK1 (λ_ex = 295 nm) displays a peak at 330 nm, which undergoes significant Ca²⁺-dependent quenching as the free [Ca²⁺] is raised from 0.00058 to 35 µM, suggesting the presence of Ca²⁺-induced conformational rearrangements (Fig. 5 A). On the other hand, the emission spectrum of D362/367A-RCK1 remains practically unchanged up to 35 µM of free [Ca²⁺] (Fig. 5 B) (similar to albumin, which was used as a negative control), confirming the results from fluorescence lifetime experiments. The apparent Ca²⁺ affinity of RCK1 was estimated by fitting the fluorescence intensity at 330 nm in increasing [Ca²⁺] to a Hill function. The mean of the parameters of the best fit are: K_1/2 = 1.7 ± 0.26 µM with n = 1.3 ± 0.19 (n = 3; errors represent standard errors of the mean) (Fig. 5 C).

Figure 5.

Tryptophan fluorescence reports WT- and D362/367A-RCK1 Ca²⁺ sensitivity. The intrinsic steady-state tryptophan fluorescence emission spectra of (A) WT and (B) D362/367A RCK1 recorded in increasing free [Ca²⁺]. As free [Ca²⁺] increases, the fluorescence intensity of WT-RCK1 decreases (A), whereas the fluorescence emission of D362/367A (B) shows no significant sensitivity to [Ca²⁺]. (C) The normalized fluorescence intensity at λ_330nm and free [Ca²⁺] = 0.00058 µM, plotted against free [Ca²⁺] for WT-RCK1 (red circles), D362/367A-RCK1 (blue triangles), and albumin (BSA) (black squares). The continuous curve is the least-squares fit to a Hill function, the parameters of which are shown in the panel. Errors represent standard errors of the mean.

The results from both time-resolved and steady-state fluorescence experiments are in agreement and provide evidence for the existence of apo- and Ca²⁺-bound states of the RCK1 domain, revealing Ca²⁺-induced structural rearrangements of the RCK1 domain occurring in physiologically relevant [Ca²⁺]. Moreover, evidence is provided that the residues D362 and D367 are required for Ca²⁺-induced conformational rearrangements.

Ca²⁺-induced conformational transitions of the BK_Ca RCK1 domain

We used CD spectroscopy to characterize the structural changes in terms of the protein’s secondary structure. Far-UV CD spectra of the purified WT-RCK1 domain were recorded in increasing [Ca²⁺] (Fig. 6). As free [Ca²⁺] was increased from 0.00058 to 35 µM, the CD spectra of WT-RCK1 displayed a decrease in overall molar ellipticity associated to a red shift of the minimum from 220 to 223 nm (Fig. 6 A). The estimated secondary structure fractions of WT-RCK1 plotted as a function of free [Ca²⁺] are presented in Fig. 6 B. The elevation of free [Ca²⁺] resulted in an increase of β-strand content (from ∼23 to 30%), accompanied by a decrease in the α-helical fraction (from ∼28 to 19%), whereas the fraction of turns and unordered secondary structures remain practically unchanged (Fig. 6 B and Table I). The apparent Ca²⁺ affinity of the structural transitions was estimated by fitting the α-helical and β-strand fractions with a Hill function (K_{1/2_α-helix} = 1.6 ± 0.30 µM; n = 1.4 ± 0.39; and K_{1/2_β-strand} = 1.2 ± 0.34 µM; n = 1.2 ± 0.04). Intriguingly, the apparent affinity of the Ca²⁺-dependent structural transitions is in the same range of [Ca²⁺] relevant to physiological BK_Ca channel activation (Bao et al., 2002; Xia et al., 2002; Zeng et al., 2005; Latorre and Brauchi, 2006).

Figure 6.

CD spectroscopy reveals Ca²⁺-dependent conformational changes in the WT-RCK1 domain. (A) Far-UV CD spectra of the BK_Ca WT-RCK1 domain obtained in increasing free [Ca²⁺]. The spectra exhibit decreased overall amplitude with increasing [Ca²⁺], and a red shift in the ellipticity minimum from 220 to 223 nm, indicating Ca²⁺-dependent structural alterations. (B) Estimated secondary structure fractions of WT-RCK1 as a function of free [Ca²⁺]. The α-helix and β-sheet fraction data obtained at different [Ca²⁺] are fitted to a Hill function. (C and D) As in A and B, respectively, for purified D362/367A-RCK1. The double mutant exhibits little change in secondary structure up to 35 µM of free [Ca²⁺].

Unlike WT-RCK1, the CD spectrum of D362/367A-RCK1 was practically unaffected by free Ca²⁺ (Fig. 6, C and D) up to 35 µM. This is in agreement with fluorescence spectroscopy experiments and further supports the premise that residues D362 and D367 are necessary for Ca²⁺-induced rearrangements in the µM range.

Both WT-RCK1 and D362/367A-RCK1 bind Ca²⁺

We have presented evidence that RCK1 undergoes Ca²⁺-induced structural changes and that these conformational rearrangements are no longer detected after the neutralization of residues D362 and D367. An important question is whether these negatively charged aspartates are involved in Ca²⁺ binding. We directly probed the Ca²⁺-binding properties of both WT-RCK1 and D362/367A-RCK1 (Fig. 7). Both proteins were blotted onto nitrocellulose membranes along with GST and troponin (for negative and positive controls, respectively) and analyzed for ⁴⁵Ca²⁺ binding from 2.1 to 115 µM of free [Ca²⁺]. Fig. 7 A shows a nitrocellulose membrane stained with Ponceau S (for protein quantification) and its corresponding ⁴⁵Ca²⁺ overlay, for 2.1 µM of free Ca²⁺. Both WT-RCK1 and D362/367A-RCK1 show ⁴⁵Ca²⁺ binding at physiologically relevant [Ca²⁺], whereas GST displays practically no binding. The ratio of WT- to D362/367A-RCK1 ⁴⁵Ca²⁺ binding is plotted versus free [Ca²⁺] in Fig. 7 B. Although low-affinity Ca²⁺-sensing sites E374 and E399 are present in RCK1 (Shi et al., 2002; Zeng et al., 2005; Lingle, 2007; Yang et al., 2007, 2008; Cui et al., 2009), they are unlikely to be responsible for the strong positive ⁴⁵Ca²⁺ signal, as they exhibit Ca²⁺ sensitivity in the mM range (Xia et al., 2002; Zeng et al., 2005).

Figure 7.

⁴⁵Ca²⁺ binds to both WT and D362/367A-RCK1 domains. (A) Protein (Ponceau S) staining blotted on nitrocellulose membrane (left) and ⁴⁵Ca²⁺ overlay phosphor image of the same blot (right) in 2.1 µM of free [Ca²⁺]. Signal intensity is proportional to protein amount (left) and Ca²⁺ binding (right). (B) The ratio of WT to D362/367A-RCK1 Ca²⁺ binding (normalized by protein amount) is plotted versus free [Ca²⁺]. (C) Enzymatic removal of the 6xHis from the WT-RCK1 domain. The purified 6xHis-WT-RCK1 is incubated with 5 U/ml DAPase, and then separated on a 12.5% SDS-PAGE and stained with either Coomassie Brilliant Blue (top strip) or InVision His tag in-gel stain (Invitrogen) (bottom strip). Troponin and GST are positive and negative controls, respectively. Note that the removal of the histidine tag did not reduce Ca²⁺ binding.

To exclude the involvement of the N-terminal 6xHis tag (used for purification of the WT-RCK1 domain) in ⁴⁵Ca²⁺ binding, we have enzymatically removed it from the purified protein. Fig. 7 C shows the time-dependent digestion efficiency of the 6xHis tag in WT-RCK1 with DAPase. The ⁴⁵Ca²⁺-binding activity of the 6xHis tag–cleaved WT-RCK1 domain is conserved, as presented in Fig. 7 A. We conclude that the 6xHis tag is not responsible for ⁴⁵Ca²⁺ binding.

DISCUSSION

The human BK_Ca RCK1 domain shares structural homology with the bacterial RCK domain

Multiple primary sequence alignments across several species, as well as biochemical and electrophysiological experiments, have suggested that the cytosolic region of the BK_Ca channel is composed of two modules termed the RCK1 and RCK2 domains (Jiang et al., 2001, 2002; Pico, 2003; Kim et al., 2006; Latorre and Brauchi, 2006; Yusifov et al., 2008). The x-ray structures of the cytoplasmic domain of the BK_Ca channel have confirmed this view and revealed the structural organization of the RCK1 and RCK2 domains, which form a hetero-octameric superstructure referred to as the gating ring (Wu et al., 2010; Yuan et al., 2010). In addition to Ca²⁺, this intracellular region has been shown to confer sensitivity to other small signaling molecules, such as carbon monoxide (Hou et al., 2008b), Zn²⁺ (Hou et al., 2010), Mg²⁺(Shi et al., 2002; Yang et al., 2007, 2008), H⁺ (Hou et al., 2008a), heme (Tang et al., 2003; Horrigan et al., 2005), and reactive oxygen species (Tang et al., 2004a), which modulate channel activation.

Here, we have probed the structure and investigated the functional properties of the purified BK_Ca RCK1 domain in solution under conditions physiologically relevant to the operation of BK_Ca channels. In addition to the α/β fold shared with its bacterial counterparts (Jiang et al., 2001, 2002; Yuan et al., 2010), the human RCK1 domains preferentially self-assemble into octameric structures (Figs. 2, B and C, and 3), as observed for RCK domains of MthK and TvoK channels (Jiang et al., 2002; Parfenova et al., 2007). Although RCK1 homo-octamers likely do not occur in functional BK_Ca channels, this property of RCK1 domains highlights structural and functional similarities among these ligand-binding domains, emphasizing their significance as modular components of gating ring superstructures. Indeed, the purified human BK_Ca RCK2 domain was also found to preferentially self-assemble into octamers (Fig. 8). On the other hand, in the intact BK_Ca channel, structurally homologous RCK1 and RCK2 domains can form a hetero-octameric gating ring complex (Wu et al., 2010; Yuan et al., 2010), which likely represents an evolutionary divergence from prokaryotic channel gating rings.

Figure 8.

The purified BK_Ca RCK2 domain forms a homo-octamer in solution. (A) 12.5% SDS-PAGE analysis of purified RCK2 reveals a single band with a mol wt of ∼40 kD, consistent with its expected size (39 kD). (B) Size-exclusion profile of the purified RCK2 domain. RCK2 elutes at 10.15 ml on a Superdex 200 10/300 column. (C) The oligomeric state of the purified RCK2 domain was determined using a calibration curve constructed from protein standards. The purified RCK2 domain corresponds to a mol wt of 333 ± 14 kD (n = 8), consistent with a homo-octameric structure of RCK2 (theoretical mol wt = 312 kD). R² of fit = 0.97.

Secondary structure of RCK1 in solution

The RCK1 domain used in this study spans 346 amino acids, including RCK1 flanking regions (S6-RCK1 linker and a portion of the RCK1-RCK2 linker), which are likely unordered. The CD data of this polypeptide obtained under physiological conditions predicted a secondary structure composition of ∼28% α helix and ∼23% β strand (Table I). This region, with the exception of the flanking linkers, was recently resolved at 3-Å resolution (Yuan et al., 2010). The proportion of α-helical structure (considering the unordered RCK1 flanking sections) is in agreement with the CD data (∼30% α-helical structure) (Table I). However the β-strand content in the crystal structure (14%) is reduced compared with the solution structure. Several factors may account for this discrepancy, including differences in experimental conditions (e.g., buffer, pH, and ionic composition); limited resolving power of CD spectroscopy for β strand (Whitmore and Wallace, 2008); and structural changes resulting from the homo-octameric assembly of RCK1 domains.

Ca²⁺-induced conformational transitions in the RCK1 domain

Here, we have provided evidence that the purified RCK1 domain undergoes Ca²⁺-induced structural rearrangement. Our steady-state and time-resolved spectroscopic data (Figs. 4 and 5) reveal Ca²⁺-induced conformational transitions that correlate with an increase in overall β-sheet content (Fig. 6). Although Ca²⁺-induced structural preference to β sheet has been observed in other proteins (Hilge et al., 2006; Yousefi et al., 2007; Fan et al., 2008), the physiological meaning of this transition in the RCK domains is unknown. Based on the accepted notion that a gain in β-sheet content (regardless of the cause) may lead to oligomerization or molecular recognition events (Rotondi and Gierasch, 2006; Zimmer et al., 2006), we speculate that in the RCK1 domain, the α-to-β transition may favor or strengthen intra- and/or inter-subunit interactions and possibly the association with other channel partners (Lu et al., 2006). Intriguingly, BK_Ca RCK2 domains, where Ca²⁺ binding has been observed in a recent crystal structure (Yuan et al., 2010), also undergo a similar decrease in α/β ratio in solution upon [Ca²⁺] elevation (Yusifov et al., 2008). Thus, although crystallographic data have not revealed Ca²⁺ binding to BK_Ca RCK1, both BK_Ca RCK1 and RCK2 domains appear to possess similar Ca²⁺-sensing properties. It is possible that the RCK1 domain is more likely to bind and respond to Ca²⁺ under conditions resembling those of the cytosolic environment, as those used in this study.

Although Ca²⁺-induced changes in α/β ratio are exhibited by both BK_Ca RCK1 and RCK2 domains, such conformational transitions were not observed in the crystal structures of the MthK RCK domain (Jiang et al., 2002; Ye et al., 2006) (Table I), possibly indicating that gating rings in BK_Ca and MthK channels exhibit different Ca²⁺-dependent activation mechanisms. The large difference in their Ca²⁺ sensitivity, which is three orders of magnitude lower in the MthK channel (Li et al., 2007), may also support this view.

Do D362 and D367 participate in a Ca²⁺-biding site?

Electrophysiological evidence has highlighted the role of aspartates 362 and 367 in the high-affinity Ca²⁺-dependent activation of BK_Ca channels. Interestingly, residues D362 and D367 have also been shown to be important for the modulation of BK_Ca channels by other ligands (Hou et al., 2008a,b); however, the mechanisms by which they exert their function are unknown. The affinity of the putative RCK1 Ca²⁺-binding site was inferred by allosteric models of BK_Ca activation to be ∼1–20 µM (depending on the pore state and the membrane potential) (Bao et al., 2002; Xia et al., 2002; Zeng et al., 2005; Sweet and Cox, 2008; Cui et al., 2009), whereas neutralization of D362/367 reduced it into the millimolar range (Xia et al., 2002). Indeed, this view is recapitulated by the apparent Ca²⁺ sensitivity estimated from steady-state tryptophan fluorescence and CD spectroscopy of the purified WT-RCK1 (K_1/2 ≈ 1.5 µM Ca²⁺) and the evidence that D362/367-RCK1 exhibited no response to Ca²⁺, as no conformational changes were detected up to 35 µM Ca²⁺ (Figs. 4–6). Although it is reasonable to consider their involvement in a Ca²⁺-binding site, the ⁴⁵Ca²⁺ assay revealed that the neutralization of D362/367 alone was not sufficient to alter the Ca²⁺-binding activity of RCK1 in the range of 2.1–115 µM of free Ca²⁺ (Fig. 7). The minimal [Ca²⁺] assayed (2.1 µM) is near the experimental K_1/2 for the Ca²⁺-induced conformational changes (Figs. 5 and 6); therefore, conceivably, a change in Ca²⁺ affinity would have been resolved. The data points in Fig. 7 B exhibit a trend that suggests that WT-RCK1 may have slightly higher Ca²⁺ affinity than the mutant; however, statistical significance was not achieved. Thus, WT and mutant RCK1 seem to bind Ca²⁺ with indistinguishable affinity. Collectively, the results favor the hypothesis that D362 and D367 have a major structural role in RCK1, determining their ability to transduce Ca²⁺ binding into conformational rearrangements. Nevertheless, it cannot be ruled out that D362 or D367 is also an element of a Ca²⁺-binding site with multiple coordinating residues, so that its neutralization does not substantially impair Ca²⁺ binding. Furthermore, it cannot be excluded that the RCK1 homo-oligomers in solution possess different Ca²⁺-dependent properties from RCK1 domains incorporated into the BK_Ca gating ring, allosterically linked with the pore domain and voltage-sensing apparatus (Horrigan and Aldrich, 2002; Sweet and Cox, 2008).

Structural consequences of D362/367 neutralization

The neutralization of residues D362 and D367 seems to alter the secondary and quaternary structure of the RCK1 domain. The differences in the secondary structure composition of D362/367A-RCK1 relative to the WT are based only on the comparison of the experimental CD data that suggest an increase in β-strand content associated to a decrease in α helix (Fig. 2 A and Table I). CD cannot provide molecular details or information about the region(s) of the protein undergoing this transition, or discriminate between a change occurring in the length of α helices and β strands or in their number, or both. Mutations inducing structural changes that perturb the α/β composition of proteins in solution have been described. For example Ulrih et al. (2008) report a drastic increase in α-helix content after a Tyr>Ala mutation in α synuclein. An Ala>Val mutation greatly increased β-sheet content in N-terminal troponin C (Pinto et al., 2009). In the N-terminal domain of a viral capsid protein, a Pro deletion or Asp>Ala mutation increased the α-helix content by 5% and decreased the β-sheet content by 3–4% (Macek et al., 2009). Increasing the hydrophobicity of residue side chains (as in the D362/367A mutation) can in some cases induce α helix to β-sheet conversion, as reported in a study modeling the energetics of these transitions in simple polypeptides (Imamura and Chen, 2007).

In summary, although a causal relation between the higher β content and loss of Ca²⁺-induced conformational change is not yet established, the altered structural state of the double mutant retains the ability to bind Ca²⁺ with high affinity but fails to transduce the free energy of ligand association into structural rearrangements. We speculate that in the intact BK_Ca channel, these mutations lock RCK1 domains in a conformation state unresponsive to ligand binding, thus hampering the propagation of conformational changes of ligand binding to the gating apparatus.

Both RCK1 and RCK2 are Ca²⁺ sensors with similar biophysical properties

Investigations of the Ca²⁺-dependent conformational changes of the purified BK_Ca RCK1 and RCK2 domains revealed that these two Ca²⁺ sensors exhibit a different Ca²⁺ affinity: RCK1 has less apparent affinity for Ca²⁺ (K_1/2 ≈ 1.5 µM) relative to the Ca²⁺ bowl in RCK2 (K_1/2 ≈ 0.4 µM) (Yusifov et al., 2008). In spite of this difference, the RCK1 and RCK2 domains share structural similarity (Wu et al., 2010; Yuan et al., 2010). Here, we report that the nature of Ca²⁺-induced conformational changes of the RCK1 domain are similar to those described for the purified RCK2 domain (Yusifov et al., 2008). Furthermore, the purified RCK2 domain (Fig. 8 A) also preferentially assembles into homomeric octamers in solution (Fig. 8, B and C), similar to RCK1 (Figs. 2, B and C, and 3). Thus, the RCK1 and RCK2 domains share functional and structural similarities.

In summary, we have presented evidence that Ca²⁺-induced conformational rearrangements take place within the RCK1 region of the BK_Ca channel at physiologically relevant [Ca²⁺]. The Ca²⁺-dependent properties of this structure seem to correlate well with Ca²⁺-induced BK_Ca channel activation. The agreement between the Ca²⁺ dependence of conformational changes (apparent K_1/2 values obtained from CD and tryptophan fluorescence spectroscopy of ∼1.5 µM) with the values obtained from electrophysiological experiments (Bao et al., 2002; Xia et al., 2002; Sweet and Cox, 2008) supports this view. We have demonstrated that the D362/367A mutation, previously shown to impair high-affinity Ca²⁺ sensing (Xia et al., 2002), causes a structural change in the RCK1 domain, preventing Ca²⁺-dependent conformational rearrangements.