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Article

Structural Insights into the Intracellular Region of the Human Magnesium Transport Mediator CNNM4

by
Paula Giménez-Mascarell
1,†,
Iker Oyenarte
1,†,
Irene González-Recio
1,
Carmen Fernández-Rodríguez
1,
María Ángeles Corral-Rodríguez
1,
Igone Campos-Zarraga
1,
Jorge Simón
1,
Elie Kostantin
2,
Serge Hardy
2,
Antonio Díaz Quintana
3,
Mara Zubillaga Lizeaga
4,
Nekane Merino
4,
Tammo Diercks
4,
Francisco J. Blanco
4,5,
Irene Díaz Moreno
3,
María Luz Martínez-Chantar
1,6,
Michel L. Tremblay
2,
Dominik Müller
7,
Dritan Siliqi
8 and
Luis Alfonso Martínez-Cruz
1,*
1
Liver Disease Laboratory, Center for Cooperative Research in Biosciences (CIC bioGUNE), Bizkaia Science and Technology Park Bld 801A, 48160 Derio, Spain
2
Department of Biochemistry and Goodman Cancer Research Centre, McGill University, Montreal, QC H3A 1A3, Canada
3
Instituto de Investigaciones Químicas (IIQ), Centro de Investigaciones Científicas Isla de la Cartuja (cicCartuja), Universidad de Sevilla—CSIC. Avda. Americo Vespucio 49, 41092 Sevilla, Spain
4
Structural Biology Unit, Center for Cooperative Research in Biosciences (CIC bioGUNE), Bizkaia Science and Technology Park Bld 800, 48160 Derio, Spain
5
IKERBASQUE, Basque Foundation for Science, María Díaz de Haro 3, 48013 Bilbao, Spain
6
Centro de Investigación Biomédica en Red de Enfermedades Hepáticas y Digestivas (CIBERehd), 48160 Derio, Spain
7
Department of Pediatric Gastroenterology, Nephrology and Metabolic Disorders, Charité Universitäts medizin, 13353 Berlin, Germany
8
Istituto di Cristallografia, Consiglio Nazionale delle Ricerche (CNR), Via G. Amendola 122/O, 70126 Bari, Italy
*
Author to whom correspondence should be addressed.
These authors contributed equally to this work.
Int. J. Mol. Sci. 2019, 20(24), 6279; https://doi.org/10.3390/ijms20246279
Submission received: 26 November 2019 / Revised: 5 December 2019 / Accepted: 10 December 2019 / Published: 12 December 2019
(This article belongs to the Special Issue Structure and Function of Membrane Proteins)

Abstract

:
The four member family of “Cyclin and Cystathionine β-synthase (CBS) domain divalent metal cation transport mediators”, CNNMs, are the least-studied mammalian magnesium transport mediators. CNNM4 is abundant in the brain and the intestinal tract, and its abnormal activity causes Jalili Syndrome. Recent findings show that suppression of CNNM4 in mice promotes malignant progression of intestinal polyps and is linked to infertility. The association of CNNM4 with phosphatases of the regenerating liver, PRLs, abrogates its Mg2+-efflux capacity, thus resulting in an increased intracellular Mg2+ concentration that favors tumor growth. Here we present the crystal structures of the two independent intracellular domains of human CNNM4, i.e., the Bateman module and the cyclic nucleotide binding-like domain (cNMP). We also derive a model structure for the full intracellular region in the absence and presence of MgATP and the oncogenic interacting partner, PRL-1. We find that only the Bateman module interacts with ATP and Mg2+, at non-overlapping sites facilitating their positive cooperativity. Furthermore, both domains dimerize autonomously, where the cNMP domain dimer forms a rigid cleft to restrict the Mg2+ induced sliding of the inserting CBS1 motives of the Bateman module, from a twisted to a flat disk shaped dimer.

Graphical Abstract

1. Introduction

The Cyclin and CBS domain divalent metal cation transport mediators (CNNMs) are the most recently identified proteins involved in magnesium cation (Mg2+) transport across the cell membranes [1,2,3]. The four known members (CNNM1 to CNNM4) encoded in the human genome are integral membrane proteins with strong homology to CorC, a bacterial magnesium/cobalt efflux protein [4]. Despite a remarkable sequence similarity and domain architecture, the CNNMs show an expression pattern that varies significantly in different organs (https://www.proteinatlas.org/search/CNNM) [2,5,6]. For example, CNNM1 is mostly present in the brain, while CNNM2 has also been detected in kidney and liver [4]. In turn, the ubiquitous CNNM3 is additionally expressed in the heart, but scarcely in the skeletal muscle [4], while CNNM4 is predominant in the brain, bone marrow, immune system, and especially abundant in the intestinal tract [4,7]. Since their discovery [4,8], the actual function of CNNM proteins has remained controversial [9,10,11,12,13]. For example, CNNM1 appears to act as a cytosolic copper chaperone [14], while CNNM2 and CNNM4 are commonly considered as basolateral Mg2+ extruders (likely Na+/Mg2+ exchangers) in the renal and intestinal epithelia, respectively [3,15]. Some authors have alternatively proposed them as Mg2+ sensors [2] or homeostatic factors that regulate the activity of other still unknown Mg2+ transporters [9,16]. Yet, their key role in maintaining Mg2+ homeostasis and their involvement in the development of Mg2+-related pathologies are undoubted. For example, mutations in CNNM2 or CNNM4 cause recessively inherited dominant hypomagnesemia and renal Mg2+ wasting [2] or Jalili Syndrome, respectively [17,18,19,20,21,22,23]. Other disorders related to their altered activity include infertility [24,25], impaired brain development [26] along with neuropsychiatric disorders [27,28,29,30], and abnormal blood pressure levels [31]. On the other hand, CNNM3 and CNNM4 are involved in cancer progression [15,32] by associating with the highly oncogenic phosphatases of the regenerating liver (PRLs) and by promoting intracellular Mg2+ accumulation that favors tumor growth and metastasis [6,32,33,34].
Structurally, the CNNMs are complex multidomain proteins that consist of four independent domains connected by linkers of different length (Figure 1). The N-terminal region includes one transmembrane α-helix and an extracellular β-sheet domain with one glycosylation site [2]. A subsequent membrane spanning DUF21 domain (Pfam code PF01595) includes three or four transmembrane α-helices and presumably facilitates Mg2+ transport across the cell membrane [2]. The intracellular region is directly attached by a long α-helix (H0) [5] and comprises two distinct domains, a Bateman module and a cyclic nucleotide monophosphate binding-like domain (cNMP domain). The Bateman module consists of two intertwined cystathionine β-synthase (CBS) motifs (CBS1 and CBS2) and binds ATP and Mg2+ ions. This triggers important conformational changes that are transmitted to the preceding transmembrane region via the connecting H0 helix and are thought to regulate the transport activity of CNNMs [5,6,35]. The second CBS2 motif features a unique extended loop with a conserved aspartate at its tip. In CNNM2 and CNNM3, this aspartate is solvent exposed and provides the key docking site for stable complex formation with phosphatases of regenerating liver (PRL). Formation of the CNNM2·PRL-1 complex involves structural modifications in both proteins: in PRL-1, the loops defining the entrance to its catalytic cavity shift to interact with the conserved aspartate at the tip of the CNNM2 loop, resulting in a closure of the cavity with inhibition of the phosphatase activity [6,33,34,36]. In CNNM2, electrostatic attraction between surface residues in both proteins causes a displacement of its complementary CBS1 motifs, resulting in a flattening of the complete CBS module [6]. This disk flattening is known to also occur upon MgATP binding that is likely favored by the interaction with the phosphatase [6]. Finally, the C-terminal cNMP domain, also known as cyclic nucleotide binding homology domain (CNBDH), is similar to that present in ion channels and cNMP-dependent kinases [37], and is followed by a long and likely unstructured C-terminal tail (from now on designated as C-tail) with unknown function.
To increase our understanding of the molecular mechanisms underlying CNNM mediated Mg2+ transport, analyzed structure and ligand binding of the intracellular region of human CNNM4 (UniProtKB/Swiss-Prot code Q6P4Q7) both in the presence and absence of its known interaction partner, PRL-1 [15]. Thus, we significantly extend the scarce structural data available, which may help in designing new antitumoral drugs to modulate the activity of CNNM/PRL complexes in specific organs.

2. Results

A careful analysis of the human CNNM4 amino acid sequence using bioinformatic tools (e.g., Phyre2 [38] and Psipred [39]) predicted the presence of large unstructured stretches in the intracellular region that might impede the crystallization process: (i) a linker connecting the two intracellular domains (residues 512–544), (ii) the C-terminal segment following the cNMP domain (residues 731–775), (iii) a long loop linking the last two β-strands of the CBS2 motif in the Bateman module (residues 480–486), and (iv) an internal loop (residues 639–699) within the core of the cNMP domain. Based on these predictions, we opted for a “divide and conquer” strategy to facilitate crystallization using the following protein constructs: (i) CNNM4BAT (residues 359–511) including the Bateman module and the preceding α-helix H0 connecting it to the DUF21 transmembrane domain in the full-length protein; (ii) CNNM4cNMP-Ctail (residues 545–775) containing the cNMP domain and subsequent C-terminal tail (residues 731–775); (iii) CNNM4cNMP (residues 545–730) containing only the cNMP domain. In addition, we designed constructs comprising both Bateman module and cNMP domain: (iv) CNNM4BAT-cNMP-Ctail (residues 356–775); (v) CNNM4BAT-cNMP (residues 356–730). Of note, we maintained the long loop within the cNMP domain core due to its unknown structural and functional role.

2.1. Crystal Structure of CNNM4BAT

Crystals of CNNM4BAT were grown as described previously [40]. All crystallographic parameters and refinement statistics are listed in Table 1. The CNNM4BAT domain is formed by two consecutive CBS motifs, CBS1 (residues 371–435) and CBS2 (436–505), that present a αβαββα fold and contact each other via their three-stranded β sheets, resulting in an overall pseudo-C2 symmetric structure (upper left panel, Figure 1). As also found in the closest homolog, CNNM2, the strands in the β-sheet of CBS1 are shorter, the N-terminal helix HA1 adopts a stretched 310 conformation, and another 310 helix (H2) following strand β3 is split in two (H2A, H2B). The N-terminal connecting helix H0 packs against helices H3 and H4 of CBS2. Various polar side chains stabilize the Bateman module structure by forming either hydrogen bonds or salt bridges. The former occur more commonly within CBS motifs (i.e., D393-T396 at the N-terminus of helix H1; S388-E412 connecting strands β1 and β2; T495-D498 in the β5-H4 loop) than between CBS motifs (i.e., D426-Y445 connecting helices H2 and HB’, and N360-E463 tying the N-terminal helix H0 to H3). As in other CBS domain containing proteins [41,42], CNNM4BAT features two major symmetry-related clefts, S1 and S2, formed between their stacked β-sheets (central right panel, Figure 1). These clefts contain several basic residues to accommodate phosphonucleotides (Figure 1), although the likely location for their binding in site S1 comprises mainly bulky amino acids (Y423, L472, R407), possibly to prevent the binding of other small molecules here (lower left panel, Figure 1). This steric hindrance is not observed in cleft S2 (lower right panel, Figure 1) that features a hydrophobic environment for adenine binding (F384, M385, Y405, L493, V494) as well as a conserved aspartate (D498) and threonine (T495) for interaction with the ribose moiety. Of note, an acidic cluster (E497, D498, and E501) at the N-terminus of α-helix H4 in S2 replaces the positively charged residues found in S1 (R407, K425, H471, T406). A similar acidic cluster appears to function as a selective filter favoring MgATP over ATP binding in the closest homolog, CNNM2 [5,6]. There, an ATP bound Mg2+ cation reduces the electrostatic repulsion between its polyphosphate chain and the acidic cluster. Interestingly, this acidic cluster not only appears in the CNNMs but also in other CBS-containing proteins related with Mg2+ extrusion such as the Mg2+ tolerance factor SA0657 found in Staphylococcus aureus [43], or bacterial proteins CorB and CorC which have been proposed to mediate Mg2+ extrusion through bacterial Mg2+ channel CorA [44] (Supplementary Figure S1). In other CBS-containing proteins such as the bacterial Mg2+ channel MgtE [45,46] or the chloride channels CLCs [47], this acidic cluster is substituted by positively charged residues, which favor the interaction with the triphosphate chain of ATP.
As observed in other CBS-domain containing proteins, including CNNM2 [5,6] and CNNM3 [33], CNNM4BAT self-associates into a disk shaped head-to-head dimer commonly referred to as “CBS module” (upper and central right panels, Figure 1) where both CBS1 and CBS2 pack against their equivalent in the complementary subunit. A closer look at the CBS module in CNNM4BAT reveals some differences from the most common arrangement found in other proteins, in which both complementary Bateman modules lie within the same plane to form a “flat” disk. In CNNM4, this disk is semi-twisted and both CBS1 motifs are slightly separated (Supplementary Figure S2). This particular CBS module represents an intermediate state between the apo form of CNNM2 [5], where the separation between complementary CBS1 motifs is more pronounced (“twisted” conformation) [5], and its MgATP bound holo form, where the disk appears planar (“flat” conformation) (Supplementary Figure S2) [5]. In the semi-twisted conformation, the CNNM4BAT dimer interface is stabilized by an extensive network of hydrophobic interactions. The contacts between complementary CBS1 motifs are asymmetric, reflecting the intrinsically lower structural order and disruption of helix H2. A hydrophobic cage formed by side chains in helices H1 (F394, M397, M401) and H2 (V424, K425, L427, V430, P432) accommodates residues (A428, F429) in helix H2* of the complementary CBS1* motif. Contrarily, the interaction between both CBS2 motifs is largely symmetric, with reciprocal H3-H4*/H4-H3* helix contacts involving residues L462 in H3 and L496, I500, I503, I504 in helix H4. Upon dimerization, the H0 helices from complementary CNNM4BAT subunits lie crossed (upper right panel, Figure 1), as observed in the twisted conformation of CNNM2BAT [5], and participate in the CBS2 dimer interface via their residues N360, M361, I362, A365, and L368.

2.2. CNNM4BAT Interaction with ATP Depends on Mg2+

To clarify whether CNNM4BAT shares the Mg2+ and/or nucleotide binding ability observed for CNNM2 [5,6,35], we crystallized CNNM4BAT in the presence of ATP and/or different metal ions (Mg2+, Zn2+, Co2+, Ni2+), but the obtained crystals had insufficient diffraction quality. We therefore studied Mg2+ and ATP binding by solution state NMR spectroscopy, monitoring changes in the 2D 15N-HSQC NMR fingerprint spectrum of CNNM4BAT upon ligand addition.

2.2.1. NMR Titration Studies with Mg2+

The 2D 15N-HSQC spectrum of CNNM4BAT (0.1 mM) changed only marginally up to 10 mM MgCl2 added, but more substantially at higher stoichiometry (40 mM MgCl2) (Figure 2A and Figure S3A). Commonly, relative signal intensities decreased with increasing Mg2+ concentration, leading to strong attenuation or even complete disappearance of some signals at 40 mM MgCl2. As previously observed for CNNM2BAT [5], the signal attenuation was due to line broadening and/or multiple signal splitting, attesting to slow exchange between free and Mg2+ bound forms with significant conformational heterogeneity. Gradual shifting of some signals was also observed (Figure 2A). Overall, our NMR titration studies indicate that CNNM4BAT interacts very weakly with free Mg2+ ions, with a KD > 1 mM, on the order of the intracellular Mg2+ concentration.

2.2.2. NMR Titration Studies with ADPNP

Similar NMR titration experiments with ATP were compromised by its gradual hydrolysis that caused a continuous decrease of the pH, resulting in widespread false positive changes in the protein’s 2D 15N-HSQC spectra. We therefore used adenosyl-β,γ-imidodiphosphate (ADPNP) as a less hydrolysable analog of ATP and increased the HEPES buffer concentration to 100 mM. The chosen pH 7.2 then remained constant up to 6 mM ADPNP concentration and dropped marginally to 7.0 at 18 mM ADPNP concentration, causing only very small shifts of the pH sensitive HEPES 1H NMR signals. Compared to Mg2+, ADPNP addition produced more significant changes in the 15N HSQC spectrum of CNNM4BAT, and at distinctly lower concentrations (Figure 2B and Supplementary Figure S3B). Again, line broadening upon ADPNP addition was more prominent and common than signal shifting, with a maximal extent around 5 mM ADPNP concentration suggesting a KD in the range of the intracellular ATP concentration (1–10 mM) [48]. A substantial number of signals (≥20) also shifted gradually with increasing ADPNP concentration, corroborating the estimated KD (Figure 2B and Figure S3B). As described before for CNNM2 [5], and to further confirm ADPNP binding by CNNM4BAT, we also performed 1H→1H Saturation Transfer Difference (STD) NMR experiments that monitor direct polarization transfer from the protein to nearby protons of a reversibly binding ligand. The observed STD effects unambiguously confirmed specific ADPNP binding by CNNM4BAT despite the rather low affinity (Supplementary Figure S2D). Overall, ADPNP binding by CNNM4BAT is rather weak (estimated KD = 10−2 to 10−3 M), but clearly specific and localized, affecting approximately 15% of all resolved 15N HSQC signals (Figure 2B and Figure S3B). The commonly observed line broadening upon ADPNP addition derives from slow exchange between free and multiple bound forms. Of special note, most of the signals affected by ADPNP addition were distinct from those affected by Mg2+ addition (compare Figure 2A,B), suggesting different binding sites.

2.2.3. NMR Co-Titration Studies with Mg2+ and ADPNP

Adding Mg2+ to a mixture of CNNM4BAT and ADPNP (5.7 mM) produced only small further changes in the 15N HSQC fingerprint spectrum of CNNM4BAT that affected some 10–15 (i.e., 5%–8%) resolved signals (Figure 2C and Figure S3C). As with Mg2+ alone, signal widths and intensities were primarily affected, to a lesser extent also signal frequencies. Interestingly, the small spectral changes from Mg2+ co-addition made the 15N HSQC spectrum closely resemble the one obtained at very high ADPNP concentrations (18 mM). Thus, Mg2+ co-addition enhances and stabilizes the spectral effects of ADPNP binding to CNNM4BAT, suggesting a positive cooperative effect of Mg2+. Presumably, the increased conformational heterogeneity of CNNM4BAT induced by Mg2+ addition facilitates a conformational selection mechanism for ADPNP binding. Since binding of ADPNP and Mg2+ largely affect different sets of CNNM4BAT signals, their binding sites do not seem to overlap (Figure 2A–C). Based on the crystal structures of CNNM4BAT (presented here) and CNNM2BAT [5,6], we conclude that an elevated Mg2+ concentration neutralizes the charge repulsion between nucleoside phosphate groups and acidic residues at site S2 of CNNM4BAT, and contributes to stabilize the “flat” conformation of the CBS module.

2.3. Crystal Structure of CNNM4cNMP

Crystallization of the cNMP binding domain of CNNM4 was only possible using a CNNM4cNMP construct without the C-terminal tail. This segment is the most variable region in all known cyclic nucleotide binding domains (CNBD) and, in other proteins, usually contains a αC helix that helps to position a bound cyclic nucleotide. A secondary structure analysis predicted the C-tail to be unstructured in all CNNMs, thus explaining our failed crystallization attempts with the larger CNNM4cNMP-Ctail construct. Our final CNNM4cNMP model was refined to 3.7 Å resolution (Table 1 and Figure 3) and shows an overall fold similar to the CNBD domains in, e.g., PKA, cAMP activated exchange proteins, cyclic nucleotide gated (CNG) as well as hyperpolarization activated cyclic nucleotide gated (HCN) channels, and also in proteins containing CNBD homology domains (CNBDH) such as the KCNH voltage-dependent potassium channels [49,50,51]. As in these proteins, CNNM4cNMP features a central β-roll surrounded by helical elements at both its N- and the C-terminus. The two N-terminal helices αN1 and αA, preceding strand β1, run antiparallel (Figure 3). Helix αA furthermore packs antiparallel against the C-terminal helix αB that immediately follows strand β8. The β-roll contains the so-called phosphate binding cassette (PBC) [49] formed by strand β6, a helix turn (αP), and strand β7 (Figure 3). In CNNM4cNMP, a network of H-bonds between Y603 (β1), Y611 (β3), and Y639 (αP) as well as between Y639 (αP) and L602 (β1) stabilizes this motif and defines the separation between β-sheets, thus, the size of the main cavity. Another H-bond network formed by residues T633 (β5), G634, S637 (β6), and Y639 (αP) stabilizes a tight turn of the loop connecting strands β5 and β6.

2.3.1. The CNNM4cNMP Module Is Unable to Bind Cyclic Nucleotides

CNNM4cNMP has unique features that distinguish it from canonical CNBD and CNBDH domains. The first striking difference is the unusual length of the loop connecting strands β6 and β7 in the PBC, which is approximately 50 amino acid residues longer than in related proteins. This anomalously long loop, disordered and not visible in our crystal structure, is conserved in the four members of human CNNM family. The second unique feature in CNNM4cNMP is an abrupt turn of the polypeptide chain at residues 601–603 that distorts the otherwise canonical strand β2 and redirects the Y603 side chain towards the interior of the cavity, thus blocking the required space to accommodate a cyclic nucleotide like cAMP or cGMP (Figure 3). Two further structural details corroborate our assumption that the cNMP binding domain in CNNM4 (and, likely, in all CNNMs) neither binds nor is regulated by cyclic nucleotides: first, CNNM4cNMP does not contain a conserved buried arginine (e.g., R301 in PKG1, Supplementary Figure S4) to interact with the exocyclic phosphate of cAMP or cGMP, nor the glutamate to fix the orientation of their ribose 2”-OH (E292 in PKG1, Supplementary Figure S4). These residues are substituted by Ser/Pro and Thr/Val, respectively, in the human CNNMs (Figure 3 and Figure S4). Second, the base of the β-roll in CNNM4cNMP is occupied by a network of bulky residues (Y603, Y694, F698) that form a hydrophobic pocket along with residues L602, I613, V620, V622, and V700 (Figure 3 and Figure S4), which sterically hinders nucleoside binding inside the cavity. Analogous bulky residues are present in all known CNNM homologs, even from phylogenetically distant organisms (Supplementary Figure S5). To confirm the suggested inability of CNNM4cNMP to bind nucleotides we performed isothermal titration calorimetry (ITC) and titration studies by NMR. The thermograms and isotherms of cAMP or cGMP titration to CNNM4BAT-cNMP-Ctail (Supplementary Figure S6) show that the injection heat remains constant and low (as for simple water injection into water), indicating the absence of specific nucleotide-protein interactions under our experimental conditions. The absence of any saturation behavior in the isotherms made model fitting unnecessary. In agreement with these results, no significant spectral changes were observed in the 2D 15N HSQC spectra of CNNM4cNMP-Ctail upon addition of cAMP or cGMP (data not shown). Our results are in agreement with thermal shift assays (TSA) carried out by Chen et al., demonstrating the lack of cyclic nucleotide binding in the cNMP domains of CNNM2 and CNNM3 [52].

2.3.2. CNNM4cNMP Forms Symmetric Homodimers

A SEC-MALS analysis revealed that isolated CNNM4cNMP in solution exists as a concentration dependent mixture of monomers and dimers (Figure 4). Dimer formation was confirmed by small angle X-ray scattering (SAXS) (Figure 4, Table 2), which allows to assess macromolecular flexibility, shape, and assembly at low resolution [53]. The dimensionless Kratky plots and Porod exponent (2.3) revealed a well-folded, flexible, and elongated arrangement for CNNM4cNMP (Figure 4, Table 2). An analysis of all interfacing molecules in the CNNM4cNMP crystal structure also suggested homodimeric assemblies, where the intersubunit interface of 617 Å2 is mostly hydrophobic and involves residues E627, M629, F631, Y639, M642, and Y694 (Figure 4). M629 (in the loop preceding strand β5) points towards the hydrophobic pocket formed by F631 (β5), E627 (loop β4-β5) and, in the complementary subunit, V622, Y638 (β4), Y639 (loop β6-αP) (Figure 4). A network of H-bonds involving residues E627 (loop β4-β5), T633, G634, S637, Y639, Y694 (loop β6-β7), and K626 (loop β4-β5) as well as an additional salt bridge between K626 and D697 (loop β6-β7) contribute to stabilize the dimer. Interestingly, mutating the interface residue F631 to alanine yielded mostly monomers, highlighting its relevant role in stabilizing the dimer via π-stacking with its counterpart. A main feature in the dimer is the presence of two large symmetrical cavities of approximately 825 Å3, separated by complementary strands β4 and β5, whose walls are formed by both CNNM4cNMP subunits via their strands β4, β5, the loop following helix αP, and the N-terminal helix αN1 (Figure 4 and Supplementary movie S1).
Since the CNNM4BAT domain likewise dimerizes, we further investigated which of the two intracellular modules (Bateman or cNMP) governs the dimerization of the complete intracellular region. For this, we evaluated the impact of the aforementioned F631A mutation (in the cNMP domain) in the larger construct CNNM4BAT-cNMP-Ctail that, like CNNM4cNMP, also shows a concentration dependent mixture of monomers and dimers (Figure 4). In contrast to the latter, however, CNNM4BAT-cNMP-Ctail is barely affected by F631A (Figure 4) mutation indicating that the Bateman module (CNNM4BAT), rather than the cNMP domain (CNNM4cNMP), plays the more important role in CNNM4 dimer stabilization.

2.4. Structural Model of the Complete Intracellular Region of CNNM4

All our attempts to grow crystals from constructs containing both intracellular modules (i.e., CNNM4BAT-cNMP and CNNM4BAT-cNMP-Ctail) failed, presumably due to their monomer/dimer equilibrium in solution and the presence of disordered regions such as the interdomain linker, the long loop connecting strands β6 and β7, and the C-terminal tail following the cNMP binding domain. We therefore proceeded with a structural characterization by SEC-SAXS of the CNNM4BAT-cNMP-Ctail construct in the absence and presence of MgATP. In agreement with the crystallographic data from the isolated domains, the derived Rg, Dmax, and Mw values (estimated from the Porod volume) are consistent with a dimeric assembly under all experimental conditions (Table 2). The Porod exponent, used to estimate the flexibility of the protein, indicates a rather compact and rigid molecule (Table 2). The dimensionless Kratky plot (Supplementary Figure S7), used to assess the shape of a protein, shows a higher and right-shifted maximum compared to the reference BSA (maximum = 1.104 at 3 ), thus indicating a well-folded and elongated molecule (Supplementary Figure S7). Using the isolated crystal structures of CNNM4BAT and CNNM4cNMP, and the bead model (C-α low resolution model as described in §4.5) obtained from the SAXS experimental data, we next constructed a structural model of the whole intracellular region of CNNM4 (Figure 5). Three possible different scenarios were considered during the construction and refinement of such model: (1) in the first one, both CNNM4BAT and CNNM4cNMP dimers were treated as independent rigid bodies; (2) in the second, only CNNM4BAT dimers (CBS modules) were predefined while the CNNM4cNMP subunits were treated as independent, not necessarily interacting entities; (3) inversely, CNNM4cNMP dimers were predefined while the complementary CNNM4BAT modules were treated as independent, not necessarily interacting entities. The structure coordinates used for the CNNM4cNMP dimer were taken from our PDB entry 6G52. For scenarios (1) and (2), two possible conformations of the CBS module were considered: (i) a twisted disk, as observed in the closest homolog, CNNM2, in the absence of MgATP (PDB ID: 4IYS) [5]; (ii) a flat disk, as observed in the MgATP-CNNM2BAT complex (PDB ID: 4P1O) [5] (note: the MgATP-CNNM4BAT crystal structure remains unknown). We then explored all possible relative orientations of the intracellular domains without including the interdomain linker nor the C-terminal tail.
The arrangements that best fit the SAXS data were assemblies with 2-fold symmetry according to scenario (1), in which both CNNM4BAT and CNNM4cNMP associate with their corresponding counterparts. All models with an average Χ2 < 2 showed the CBS1 motifs above the large cavity between both CNNM4cNMP domains (Figure 5 and Figure 6). After determining the relative orientation of the intracellular domains, we progressively rotated the CNNM4cNMP dimer around the 2-fold axis relating both Bateman modules until the best fit was obtained. Of two different rotamers, both with Χ2 ≈ 1.3 but differing by 60°, one showed larger morphological complementarity between the two intracellular domains and was, therefore, selected as the final model (Figure 5 and Figure 6, Supplementary movies S1 and S2, Table 2). Finally, the relative distance between the dimerized CNNM4BAT and CNNM4cNMP domains along the 2-fold axis was refined, and the polypeptide chain connecting both intracellular domains as well as the C-terminal tail following CNNM4cNMP were modeled using the CORAL program [54].

2.5. Structural Model of the Full Intracellular Region of CNNM4 in Complex with PRL-1

CNNMs are known to interact with phosphatases of the PRL family [6,33,34,36] via the extended loop in their CBS2 motif and the catalytic cavity in PRL. Formation of the CNNM·PRL complex involves structural modifications in both proteins: in PRL, the loops defining the entrance to its catalytic cavity shift to interact with a conserved aspartate at the tip of the CNNM loop (D558 in CNNM2), resulting in a closure of the cavity with inhibition of the phosphatase activity [6,33,34,36]. In CNNM, electrostatic attraction between surface residues in both proteins causes a displacement of its complementary CBS1 motifs, resulting in a flattening of the complete CBS module [6]. This disk flattening is known to also occur upon MgATP binding that is likely favored by the interaction with the phosphatase [6]. Based on this knowledge, we therefore analyzed the complex formed by PRL-1 and the CNNM4BAT-cNMP-Ctail construct, both in the absence and in the presence of MgATP. As expected, the obtained Rg and Dmax values were very similar in both cases (48 and 185 Å vs. 47 and 183 Å, respectively). The Porod volume indicated that one CNNM4BAT-cNMP-Ctail dimer bound to two separate PRL-1 molecules (Table 2 and Figure 5) while the dimensionless Kratky plot showed a maximum higher than the BSA standard, consistent with a well-folded and elongated shape (Supplementary Figure S7, Table 2). To then model the CNNM4BAT-cNMP-Ctail·PRL-1 complex structure, we started from two building blocks: (i) the dimeric CNNM4BAT domain was replaced by the flat CBS module of the CNNM2∙PRL-1 complex (PDB ID: 5LXQ) [6] after substituting the 14 differing residues; (ii) the CNNM4cNMP dimer was taken from its isolated structure described here (PDB ID: 6G52). Both rigid building blocks were iteratively rotated against each other; the resulting complex structures where then analyzed with ZDOCK [55] and UCSF CHIMERA [56], and refined against the SAXS data. In a first round, all assemblies with Χ2 values < 2.5 (relative to the SAXS data) were selected as suitable candidates for subsequent refinement. We then explored all possible rotations between both building blocks in the dimeric assemblies, maintaining the 2-fold symmetry between monomers. The lowest Χ2 was obtained for two similar structure models differing by a 60° rotation angle of the CNNM4cNMP dimer around the 2-fold symmetry axis, of which we selected the model with the highest morphological complementarity between both building blocks (Figure 5). In a last step, we used CORAL [54] to model the linkers between the CNNM4BAT, CNNM4cNMP, and C-terminal tail regions. The resulting final structure model of the CNNM4BAT-cNMP-Ctail·PRL-1 complex (Figure 5, Supplementary movie S3) is a pseudo symmetric assembly in which the Bateman modules and cNMP binding domains are related by a 2-fold axis running between the interfacial helices of the Bateman domain. The cNMP binding domains localize close to the CBS1 motifs of the Bateman domains and away from their H0 helices that connect the intracellular region with the transmembrane DUF21 module. As expected [6], the PRL-1 molecules do not interact with the cNMP binding domains that, in turn, do not tightly pack against the Bateman modules (Figure 5, Supplementary movie S3).

3. Discussion

The biological relevance of CNNM proteins in cellular magnesium transport as well as their role in diverse pathological processes like magnesium wasting, neurological disorders, and cancer has become evident in recent years. Identification of some of their molecular partners and the metabolic and phenotypic effects resulting from their inhibition has shed some light on functional questions that arose immediately after their discovery. Despite significant experimental efforts, however, the actual role played by these homeostatic factors in different organs and cell types as well as the molecular mechanisms by which they (help to) mediate Mg2+ transport across the cell membranes remain a subject of intense debate. In this regard, high resolution structure information would be very helpful, but crystallization of these multimodular transmembrane proteins is greatly impeded by their intrinsically dynamic nature. By exploiting the structural independence of their different domains and applying a “divide and conquer” approach, we managed to obtain a structure model of the complete intracellular region of human CNNM4. The presented results provide broad structural insight on the CNNM family and reveal the relative orientation of their different domains in the absence and presence of PRL-1, an oncogenic phosphatase of regenerating liver that gets inhibited by CNNM binding and, inversely, inhibits their activity in Mg2+ transport. Our crystal structures show that the Bateman module of CNNM4 forms two main clefts, S1 and S2, where S2 may accommodate a bound nucleotide despite an unusually acidic surface rarely seen in typical ATP binding sites. The resulting electrostatic repulsion between the cluster of negatively charged residues in S2 and the ATP polyphosphate chain may explain the low nucleotide affinity and its increase by Mg2+ co-binding for charge compensation, as shown by our NMR titration experiments. While, in principle, the low ATP affinity of CNNMs is unexpected for Mg2+ transporters or sensors, it might be relevant for their sensor function in order to allow transport of Mg2+ cations only above a certain intracellular concentration (in the millimolar range). Of relevance in this regard, the Mg2+ dependence of ATP binding by CNNMs is exactly inverse to that by bacterial channels, which regulate the intracellular Mg2+ concentration by controlling the cation influx, rather than efflux. For instance, bacterial MgtE requires prior ATP binding to the Bateman module in order to enhance its Mg2+ affinity. This cooperative binding then promotes a conformational change leading to a closure of the MgtE membrane pore above a certain intracellular Mg2+ concentration [46,48].
Furthermore, as observed in most CBS domain containing proteins [41,42], our crystallographic and SEC-MALS data confirm that the Bateman module also plays a key role in CNNM4 dimerization. Remarkably, we found that the CNNM4BAT dimer assembles in a semi-twisted disk conformation resembling an intermediate state between the fully twisted and flat disks adopted by the CNNM2BAT dimer in the absence and presence of MgATP/Mg2+, respectively (Supplementary Figure S2) [5]. Considering the high sequence identity between CNNM2 and CNNM4 Bateman modules (where only 14 residues are different) it is reasonable to assume that, in solution, the intermediate state seen in the CNNM4BAT crystals also evolves into the fully twisted conformation in the presence of MgATP/Mg2+.
On the other hand, our crystal structure of CNNM4cNMP as well as ITC and NMR titration experiments reveal that this cyclic nucleotide binding-like domain (CNBH) actually cannot accommodate and/or be regulated by cAMP or cGMP, contrary to its name (Supplementary Figure S6). Interestingly, CNNM4cNMP associates in compact homodimers (Figure 4 and Supplementary movie S1) that are equally seen in the dimer structures of CNNM2 and CNNM3 [52]. Thus, and in line with these recent findings on the homologs, CNNM4cNMP appears to contribute importantly to the dimerization of the full-length protein while our SEC-MALS and SAXS data on the larger CNNM4BAT-cNMP-Ctail construct (containing both Bateman and cNMP domains) support a complementary and non-negligible role in dimer stabilization also for the Bateman module. Importantly, our SAXS derived structure model suggests that the CNNM4cNMP domain dimerization defines the morphological limits for the twisted-to-flat conformational change triggered within the Bateman module by MgATP binding in their S2 sites: we posit that the contiguous large cavity formed between both CNNM4cNMP monomers sets the limits for the induced shifting of the CBS1 motifs that insert into it (Figure 6 and Supplementary movies S1–S4). Supporting this important dimer stabilizing and motion restricting function by the cNMP domain, its removal inhibits Mg2+ transport by CNNM2 and CNNM3 [52]. We moreover found that mutation F631A (in its strand β5) induces the disassociation of CNNM4cNMP dimers, although dimers of larger constructs including also the Bateman module may still form.
In conclusion, we elucidated the overall architecture of the complete intracellular region of human CNNM4, alone and in complex with the binding partner PRL-1. Our data shows cooperative ATP and Mg2+ binding by the Bateman module (in site S2), providing a rationale for the observed Mg2+ concentration sensitivity, while the so-called cNMP binding domain is actually unable to bind cyclic nucleotides. Both modules dimerize autonomously, thus contributing to overall dimer stabilization in the full-length protein. Yet, while the Bateman module dimer is conformationally more flexible, the cNMP domain dimer is rigid and, thus, provides a stable framework delimiting the conformational changes induced in the former by MgATP binding. These results may pave new ways for designing drugs aimed at modulating the activity of CNNM4 and, by extension, of its closest family members.

4. Materials and Methods

4.1. Cloning and Protein Purification

The cDNA of human CNNM4 (hCNNM4) was purchased from OriGene (MD, USA; catalogue No. SC113208). The constructs hCNNM4BAT-cNMP-Ctail (residues 356–775), hCNNM4cNMP (residues 545–730), and hCNNM4cNMP-Ctail (545–775), were cloned into pHIS-Parallel2 [57], confirmed by sequencing, expressed in Escherichia coli BL21 (DE3), and grown in Luria–Bertani (LB) broth at 37 °C after induction at OD600 = 0.8 by adding 0.5 mM isopropyl-β-D-thiogalactopyranoside (IPTG). Cells containing the target proteins were harvested after 4 h of growth at 37 °C. Seleno-L-methionine (SeMet) derivates of the target proteins were similarly expressed in E. coli B834 (DE3) cells that were harvested, resuspended in SeMet medium base plus nutrient mix (Molecular Dimensions), and starved of methionine for 1 h. Then, 0.2 mM SeMet (Acros Organics, NJ, USA) and 0.5 mM IPTG were added to the medium and the cells were again harvested after 4 h of growth at 37 °C. The following purification steps were performed at 4 °C.
Both native and SeMet labeled proteins were purified by the same protocol, with few modifications. The cell pellet was resuspended in lysis buffer (50 mM Tris-HCl, pH 8, 300 mM NaCl, 50 mM imidazole, 1 mM DTT, 1 mM benzamidine, 0.1 mM PMSF) and lysed by sonication in a Labsonic P sonicator (Sartorius; 12 cycles of 15 s at 60% amplitude, with 60 s resting on ice between each cycle to prevent sample overheating). The lysate was clarified by ultracentrifugation at 250,000× g for 60 min at 4 °C and the supernatant was filtered through a 0.45 μm filter before injection onto a pre-equilibrated 5 mL HisTrap HP column (GE Healthcare), connected to an AKTA FPLC system (GE Healthcare) inside a cold room at 4 °C. The column was then washed with 10 column volumes of buffer A (50 mM Tris-HCl, pH 8, 300 mM NaCl, 50 mM imidazole, 1 mM DTT) and the bound protein was eluted with buffer B (50 mM Tris-HCl, pH 8, 300 mM NaCl, 300 mM imidazole, 1 mM DTT) using a linear gradient over 30 column volumes. Fractions containing the protein of interest (as confirmed by SDS-PAGE) were pooled and TEV protease was added to remove the N-terminal His-tag. The mixture was dialyzed overnight in 50 mM Tris-HCl pH 8, 150 mM NaCl, 1 mM DTT. A second Ni2+-NTA chromatography was carried out to remove cleaved 6xHis-tag and uncleaved protein. The cleaved protein was subsequently concentrated in an Amicon Ultra-15 (10,000 Da cutoff) centrifugal concentrator (Millipore) to a volume of ca. 2 mL, then loaded onto a HiLoad Superdex 75 16/60 Prep Grade gel filtration column (GE Healthcare) pre-equilibrated with 20 mM HEPES pH 7.4, 200 mM NaCl, 1 mM DTT, and eluted at a flow rate of 0.3 mL/min. Fractions containing pure protein were pooled and concentrated to 8–10 mg/mL using an Amicon Ultra-4 5000 Da cutoff concentrator (Millipore), and were flash frozen in liquid nitrogen and stored at −80 °C. The final concentration of all purified proteins was estimated by measuring the corresponding OD280 at 280 nm and applying the theoretical extinction coefficient.
Human CNNM4BAT was obtained by previously published protocols [40]. For NMR studies, an alternative construct of hCNNM4BAT, containing a N-terminal His6-tag with V5 epitope and Tobacco Etch Virus (TEV) proteinase cleavage site, was cloned in a pET151-D/TOPO vector (Invitrogen). The DNA sequence was then transformed into the E. coli strain BL21 CodonPlus (Stratagene) and the overexpression procedure was slightly modified from Marley’s protocol [58]. After growth at 37 °C to an OD600 of 0.6 in LB media containing 0.1 mg/mL ampicillin, the culture was concentrated threefold into M9 media with 15NH4Cl plus 0.2 % glucose to produce 15N-labeled His-hCNNM4BAT, and equilibrated at 20 °C for 30 min before overnight induction with 0.5 mM IPTG at 20 °C. Cells were then lysed by sonication in 25 mM HEPES pH 7.4, 400 mM NaCl, 20 mM imidazole, 1 μM β-mercaptoethanol, 0.1 mM PMSF, 1 mM benzamidine plus DNAse. After centrifugation at 35,000× g for 30 min, the extract was immediately subjected to affinity chromatography on a 1 mL HisTrap FF crude (GE Healthcare) column pre-equilibrated in the same buffer, but without DNAse. The protein was eluted by 25 mM HEPES pH 7.4, 0.4 M NaCl, 500 mM imidazole, 1 μM β-mercaptoethanol, 0.1 mM PMSF, 1 mM benzamidine. The eluted single peak fraction was subjected to gel filtration chromatography (HiLoad 16/60 Superdex-75 (GE Healthcare) equilibrated in 150 mM HEPES pH 7.4 buffer, 100 mM NaCl, 1 mM β-mercaptoethanol, 0.2 % NaN3, 1 mM benzamidine, 0.1 mM PMSF. Use of the metalloprotease inhibitor EDTA was avoided in order to prevent chelation of divalent cations (e.g., Mg2+) in subsequent titration studies. The resulting fractions containing target protein were concentrated in an Amicon-15 centrifugal filter device (Millipore) to a final concentration of 38 mg/mL.
Uniformly 15N enriched CNNM4cNMP-Ctail construct was similarly expressed in E. coli BL21 (DE3) grown in a modified auto-induction medium [59] with 2.5 g/L of 15NH4Cl as the only nitrogen source.

4.2. NMR Analysis

For our NMR titration studies we employed samples of U-15N labeled CNNM4BAT after buffer exchange from conventional PBS (containing phosphate that may compete with ATP for Mg2+ complexation) to HEPES. While 50 mM HEPES was sufficient for the titrations with MgCl2, we increased its concentration to 100 mM for titrations with ADPNP to compensate for any pH decrease from hydrolysis of its phosphate moieties. The preset pH 7.4 was verified at the end points of titration using a pH electrode while the very pH sensitive 1H NMR signals of HEPES (at 3.77, 3.08, 2.91, and 2.85 ppm) allowed to directly monitor the pH stability in situ. Thus, we confirmed that the pH did not drop by more than 0.1 units during titrations. The NMR samples furthermore contained 100 mM NaCl, 0.02% (w/v) NaN3, 1 mM benzamidine, and 0.1 mM PMSF to increase their long-term stability. All experiments were measured at 298 K on an 800 MHz BRUKER AVANCE III spectrometer equipped with a TCI cryoprobe. For each titration point we recorded a 1D 1H NMR spectrum (with water suppression by excitation sculpting) to monitor the pH on the HEPES signals and the amount of ADPNP added, and a high-resolution fast 2D 15N-HSQC (with water suppression by excitation sculpting and broad-band 1H polarization flip-back) to monitor ligand induced shifts of protein amide signals. We also confirmed ADPNP binding by recording 1Hprotein1HADPNP STD spectra (saturation transfer difference, measured in fully interleaved mode with alternating selective saturation of protein methyl resonances at 0.76 ppm during 1 to 3 s, a 100 ms T2 filter to suppress residual protein signal, and 3 s interscan recovery delay to avoid subtraction artifacts).
NMR titration experiments were similarly measured for U-15N labeled CNNM4cNMP-Ctail dissolved in a regular PBS buffer (pH 7.4, 5 % 2H2O, 0.01% NaN3, 20 µM DSS) since Mg2+ binding to this domain was not studied. Instead, we added up to an eightfold excess of cAMP or cGMP (800 to 100 µM CNNM4cNMP-Ctail) to test their possible binding, but could not detect any significant signal shifts in superpositions of the 2D 15N HSQC spectra of CNNM4cNMP-Ctail in the absence and presence of cNMP. TopSpin (Bruker) was used for NMR data processing and analysis. Chemical shifts were measured relative to internal DSS for 1H and calculated for 15N [60].

4.3. Size Exclusion Chromatography with Multiangle Light Scattering (SEC-MALS)

Static light scattering experiments were performed at 25 °C with a DAWN-HELEOS light scattering detector and Optilab rEX differential refractive index detector (Wyatt Technology, Santa Barbara, CA, USA) attached to a Superdex 200 10/300 GL column (GE HealthCare, Madrid, Spain). The column was equilibrated with running buffer (20 mM HEPES pH 7.4, 200 mM NaCl, 1 mM TCEP, 0.1 μm filtered) and the SEC-MALS system was calibrated with a 1 g/L BSA sample in the same buffer. Aliquots of 100 μL of each protein sample and at each concentration (1 and 10 g/L in the running buffer) were then injected into the column at a flow rate of 0.5 mL/min. ASTRA software (Wyatt Technology) was used for data acquisition and analysis. Based on repeated measurements with the BSA reference samples we estimated a 5% experimental error in the derived molar masses.

4.4. Isothermal Titration Calorimetry (ITC)

ITC experiments were performed with a Low-Volume NanoITC calorimeter (TA-Waters) using 50 μM protein solutions as analyte, except in titrations with Mg-ATP where the protein concentration was 40 μM. The titrant stock solutions were 10–13 times more concentrated than the analyte concentration to assure final titrant-to-analyte molar ratios above 3. Data were processed with Nanoanalyze (TA-Waters) and represented with Origin 2018 (Originlab, Northampton, MA, USA). The absence of any saturation behaviour in the thermograms made fitting unnecessary.

4.5. Small Angle X-Ray Scattering (SAXS)

SAXS data were collected in the bioSAXS beamline B21 at the Diamond Light Source (Harwell, UK) for the constructs CNNM4cNMP, CNNM4BAT-cNMP-Ctail, and the PRL-1/CNNM4BAT-cNMP-Ctail complex. The latter two samples were analyzed in both absence and presence of MgATP (5 mM). The protein samples (46 µL, 5 mg/mL) were injected onto a KW-403 size-exclusion column at 20 °C in 20 mM HEPES buffer pH 7.4, 200 mM NaCl, 1 mM DTT and the output from the Agilent HPLC was directed through a 1.6 mm diameter quartz capillary cell under vacuum at a flow rate of 0.08 mL/min. A total of 620 frames (3 s exposure time) were collected with a PILATUS 2M (Dectris, Switzerland) detector at a distance of 4.014 m from the sample; the two-dimensional images were subsequently corrected for variations in beam current, normalized for exposure time, and processed into 1D scattering curves using GDA and DAWN software (Diamond Light Source, UK). The background was manually subtracted using ScÅtter (available online: http://www.bioisis.net/scatter, accessed on 10 December 2019). All collected SAXS data and experimental parameters are summarized in Table 2.
The interpolated 1D SAXS curves were initially analyzed to judge the data quality and obtain basic structural information related to the protein size and shape (Figure 4 and Figure 5). One structural parameter is the radius of gyration, Rg, derived from the slope of the Guinier plot ln(Iq) vs q2 (q = 4πsin(θ)/λ is the scattering vector, 2θ the scattering angle, λ the wavelength). For globular proteins, this plot is expected to be linear at small q (i.e., q∙Rg < 1.3) and linearity of the Guinier plot is considered a quality measure of the data, but does not ensure ideality of the sample. SAXS curve analysis also provides an estimate of the protein’s molecular mass that, in turn, relates to its oligomeric state and approximately corresponds to half of its Porod volume (i.e., excluded volume of the hydrated protein), derived from the scattering intensity at larger q (Porod plot). Finally, the maximum size of a protein, Dmax, can be obtained by analyzing the SAXS data with a Pair-Distance Distribution Function, P(r), for all electrons in the protein. P(r) is obtained by indirect Fourier transformation [61] in a trial-and-error process, at the end of which the obtained Dmax corresponds to the smoothest positive distribution. Changes in the Dmax of a protein relate to conformational changes. It is also possible to calculate Rg from P(r) and compare its value with the one estimated from the Guinier plot. Low resolution structures derived from experimental scattering data were constructed by ab initio modelling using the program GASBOR [62] by aligning, averaging, and filtering 10 independently calculated dummy residue models (C-α models) [63]. All programs are included in ATSAS package [54]. The final SAXS models were deposited and are available at SASBDB [64] (corresponding access codes are listed in Table 2).

4.6. Protein Crystallization

The crystallizability of all protein constructs was evaluated with XtalPred [65]. CNNM4BAT crystals were obtained as described previously [40] while crystals of SeMet labeled CNNM4cNMP were grown by sitting drop vapor diffusion at 18 °C, mixing 0.5 μL protein (8 mg/mL) with 0.5 μL precipitant solution (0.5 M sodium formate, 5% (w/v) polyethylene glycol (PEG) 3350, 0.1 M Tris pH 7.2). All crystals were cryoprotected by immersion in mother liquor containing 20% (v/v) glycerol, and flash cooled in liquid nitrogen.

4.7. X-Ray Structure Determination and Refinement

All diffraction data were collected at the Diamond Light Source (Didcot, UK) beamline I03, and at the ALBA synchrotron (Barcelona, Spain) beamline BL13 (XALOC).
The anisotropy of the CNNM4359–511 diffraction data was corrected with the UCLA MBI Diffraction Anisotropy Server [66].
Diffraction intensities were indexed, integrated, scaled, and merged using XSCALE XDS [67]. Initial phases for CNNM4359–511 were determined by molecular replacement with Phaser [68], using CNNM2BAT (PDB ID 4IY4) [5] as search model. Non-crystallographic symmetry averaging over appropriate regions of independent monomers in the asymmetric units was applied. The crystal structure of SeMet labeled CNNM4545–730 was solved by single wavelength anomalous dispersion (SAD) for phase determination (Table 1) after allocating the selenium atoms for CNNM4545–730 with SHELXD [69]. Initial phases and density modification used Autosol in PHENIX [70] and an initial model was built with BUCCANEER [71]. Refinement with PHENIX and/or REFMAC5 [72] was alternated with manual modeling by COOT [73]. The geometric quality of the models was assessed with MolProbity [74]. All crystal characteristics and final refinement statistics are summarized in Table 1. Figures showing 3D protein structures were prepared with PyMOL (available online: http://www.pymol.org/, accessed on 10 December 2019) and Chimera [56]. For surface calculation we employed the PISA server [75].

Supplementary Materials

Supplementary materials can be found at https://www.mdpi.com/1422-0067/20/24/6279/s1.

Author Contributions

D.M., M.L.T. and L.A.M.-C. Conceived and coordinated the study and wrote the paper. P.G.-M., I.O., I.G.-R., I.C.-Z., C.F.-R. and J.S. purified the proteins and performed the crystallization and structural analysis. S.H. and E.K. cloned and overexpressed the proteins and performed directed mutagenesis. L.A.M.-C., I.O., M.Á.C.-R., M.Z.L., F.J.B. and T.D. performed the N.M.R. analysis. N.M. helped with SEC-MALS experiments. A.D.Q. and I.D.M. performed the ITC analysis. P.G.-M., L.A.M.-C. and D.S. performed the SEC.-SAXS. analysis. L.A.M.-C. and M.L.M.-C. Contributed to the study design and data analysis. All authors reviewed the results and approved the final version of the manuscript.

Funding

This work was supported by the Departamento de Educación, Universidades e Investigación del Gobierno Vasco [grant number PI2010-17], the Departamento de Industria, Innovación, Comercio y Turismo del Gobierno Vasco [grant numbers ETORTEK IE05-147, IE07-202], Diputación Foral de Bizkaia [grant numbers 7/13/08/2006/11, 7/13/08/2005/14], Ministerio Español de Ciencia e Innovación (MICINN) [grant numbers BFU2010-17857], Spanish Ministry of Economy and Competitiveness [BFU2013-47531-R, BES-2014-068464, BFU2016-77408-R and BES-2017-080435] (MINECO/FEDER, UE) and the MICINN CONSOLIDER-INGENIO 2010 Program [grant number CSD2008-00005] to LAMC. Structural studies were done under Block Allocation Group (BAG) 2019073624 (structural studies of macromolecular interactions relevant for infectious and metabolic diseases) from ALBA Synchrotron and BAG MX20113 (CIC bioGUNE Structural Biology Unit) from Diamond Light Source. The MLM-C’s work was funded by Gobierno Vasco-Departamento de Salud 2013111114, MINECO: SAF2017-87301-R integrated in the Plan Estatal de Investigación Cientifica y Técnica y Innovación, co-funded by Fondos FEDER, BIOEF (Basque Foundation for Innovation and Health Research): EITB Maratoia BIO15/CA/014, La CAIXA Foundation and Ayudas Fundación BBVA a Equipos de Investigación Cientifica 2018. Ciberehd_ISCIII_MINECO is funded by the Instituto de Salud Carlos III. We also thank MINECO for the Severo Ochoa Excellence Accreditation to CIC bioGUNE (SEV-2016-0644). TB and DM were supported by a Collaborative Research Grant (12.01.134/2bT4) of the Berlin Institute of Health. MLT, EK and SH were supported by the Canadian Institute for Health Research, operating grant #343439 (to MLT). The SAXS experiments where performed under proposal “Structural and mechanistic studies on different proteins related to diseases” numbers MX15832-9 and MX15832-10, beamline B21, Diamond Light Source. ADQ and IDM are thankful for support from the Spanish Ministry of Economy and Competitiveness (PGC2018-096049-B100), the Ramón Areces Foundation, the Biomolecular Interaction Platform (cicCartuja, Seville), and TA instruments. FJB, NM and MZL were funded by MINECO CTQ2017-83810-R.

Acknowledgments

We thank the staff of the BL13 (XALOC) beamline at ALBA (Barcelona, Spain), of the ESRF (European Synchrotron Radiation Facility, Grenoble, France) beamlines ID14-1, ID23-1, 2, and ID29, and of Diamond (Didcot, U.K.) beamline I04 and B21 (SAXS) for their valuable support during synchrotron data collection, as well as Adriana Rojas for maintaining our in house X-ray platform.

Conflicts of Interest

The authors declare no conflict of interest.

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Figure 1. Crystal structure of the hCNNM4 Bateman module. (A) (up) Domain architecture of the full length CNNM4 protein (the position of the Bateman module is highlighted in orange). (middle) CNNM4BAT adopts the overall fold of a Bateman module consisting of two consecutive CBS motifs (CBS1, CBS2). The long loop connecting strands β5 and β6 is disordered in most of the crystals. Of note, in CNNM2 and CNNM3 this loop mediates the interaction with all members of the PRL phosphatases family [6,32,33,34,36]. The N-terminal helix H0 connects the Bateman module to the preceding DUF21 transmembrane region in the full-length protein. (down) Sequence alignment of the Bateman modules from human CNNMs. The secondary structure elements (derived from the CNNM4BAT crystal structure) are shown above. (B) Two CNNM4BAT Bateman modules (colored vs. grey) associate into a disk shaped homodimer called CBS module. Each CNNM4BAT subunit presents two main clefts on opposite sides of the module (S1 and S2), of which only S2 can host a nucleotide [5,6]. (C) Residues forming the S1 and S2 clefts. CNNM4 residue T495 in S2, occupies a position equivalent to that of T568 in CNNM2, where mutation T568I causes hypomagnesemia [2].
Figure 1. Crystal structure of the hCNNM4 Bateman module. (A) (up) Domain architecture of the full length CNNM4 protein (the position of the Bateman module is highlighted in orange). (middle) CNNM4BAT adopts the overall fold of a Bateman module consisting of two consecutive CBS motifs (CBS1, CBS2). The long loop connecting strands β5 and β6 is disordered in most of the crystals. Of note, in CNNM2 and CNNM3 this loop mediates the interaction with all members of the PRL phosphatases family [6,32,33,34,36]. The N-terminal helix H0 connects the Bateman module to the preceding DUF21 transmembrane region in the full-length protein. (down) Sequence alignment of the Bateman modules from human CNNMs. The secondary structure elements (derived from the CNNM4BAT crystal structure) are shown above. (B) Two CNNM4BAT Bateman modules (colored vs. grey) associate into a disk shaped homodimer called CBS module. Each CNNM4BAT subunit presents two main clefts on opposite sides of the module (S1 and S2), of which only S2 can host a nucleotide [5,6]. (C) Residues forming the S1 and S2 clefts. CNNM4 residue T495 in S2, occupies a position equivalent to that of T568 in CNNM2, where mutation T568I causes hypomagnesemia [2].
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Figure 2. Ligand binding by hCNNM4BAT (100 μM), monitored by 2D 15N HSQC NMR spectra (zoom on a representative region). (A) Effect of Mg2+ addition to a final concentration of 0 mM (black, reference), 10 mM (light blue), 20 mM (blue), and 40 mM (dark blue). Signals shifting or diminishing due to addition of only Mg2+ or ADPNP (as in (B)) are marked with letters A or B, respectively, to emphasize differences in the affected signal sets, indicating non-overlapping binding sites. Arrows show the shift direction. (B) Effect of ADPNP addition to a final concentration of 0 mM (black, reference), 570 μM (yellow), 1.14 mM (orange), and 5.7 mM (red). (C) Effect of combined Mg2+ and ADPNP addition: Mg2+ plus 0 mM ADPNP (black, reference), 0 mM Mg2+ plus 5.7 mM ADPNP (orange), 0 mM Mg2+ plus 18 mM ADPNP (red), and 10 mM Mg2+ plus 5.7 mM ADPNP (blue). Moderate concentrations of ADPNP (5.7 mM) in the presence of Mg2+ produce an effect similar to the addition of high concentrations of ADPNP alone (18 mM; a representative signal is marked by an asterisk). The pertaining full spectra are shown in Figure S2A–C. Spurious t1 noise at 1H frequencies of ca. 8.2 and 8.4 ppm derive from protons H2 and H8 in the purine ring of ADPNP (see Figure S2D).
Figure 2. Ligand binding by hCNNM4BAT (100 μM), monitored by 2D 15N HSQC NMR spectra (zoom on a representative region). (A) Effect of Mg2+ addition to a final concentration of 0 mM (black, reference), 10 mM (light blue), 20 mM (blue), and 40 mM (dark blue). Signals shifting or diminishing due to addition of only Mg2+ or ADPNP (as in (B)) are marked with letters A or B, respectively, to emphasize differences in the affected signal sets, indicating non-overlapping binding sites. Arrows show the shift direction. (B) Effect of ADPNP addition to a final concentration of 0 mM (black, reference), 570 μM (yellow), 1.14 mM (orange), and 5.7 mM (red). (C) Effect of combined Mg2+ and ADPNP addition: Mg2+ plus 0 mM ADPNP (black, reference), 0 mM Mg2+ plus 5.7 mM ADPNP (orange), 0 mM Mg2+ plus 18 mM ADPNP (red), and 10 mM Mg2+ plus 5.7 mM ADPNP (blue). Moderate concentrations of ADPNP (5.7 mM) in the presence of Mg2+ produce an effect similar to the addition of high concentrations of ADPNP alone (18 mM; a representative signal is marked by an asterisk). The pertaining full spectra are shown in Figure S2A–C. Spurious t1 noise at 1H frequencies of ca. 8.2 and 8.4 ppm derive from protons H2 and H8 in the purine ring of ADPNP (see Figure S2D).
Ijms 20 06279 g002aIjms 20 06279 g002bIjms 20 06279 g002c
Figure 3. Crystal structure of the hCNNM4cNMP domain. (A) (left) The hCNNM4cNMP crystal structure shows two N-terminal helices (αN1, αA; in red), followed by a central seven-stranded β-roll (blue) and a C-terminal helix αB (green). The β-roll shows a cavity (marked by an asterisk) presenting the so-called phosphate binding cassette (PBC, in yellow) formed by a short helix (αP) and an extended loop (ca. 60 residues, invisible in the crystals) between strands β6 and β7. The domain architecture of the full length protein is shown above (the cNMP domain is highlighted in orange). (Right) Sequence alignment of cNMP domains in human CNNMs. The long β6-β7 loop is conserved throughout, but is larger in CNNM1 and CNNM2, intermediate in CNNM4, and shorter in CNNM3. A likely unstructured polypeptide segment following helix αB was not included in our CNNM4cNMP construct. The colors of the secondary elements correspond to those used in the crystal structure. (B) Stereo view of residues at the cavity opening of the β-roll in CNNM4cNMP. Residues within β-strands or the PBC motif are shown in blue or yellow, respectively. Residues Y603, F698, and Y694 (labeled in red and indicated by a red asterisk in the sequence alignment) invade the space usually occupied by a bound cyclic nucleotide in unrelated CNB containing proteins like PKA (a superimposed cAMP molecule is shown by transparent red sticks).
Figure 3. Crystal structure of the hCNNM4cNMP domain. (A) (left) The hCNNM4cNMP crystal structure shows two N-terminal helices (αN1, αA; in red), followed by a central seven-stranded β-roll (blue) and a C-terminal helix αB (green). The β-roll shows a cavity (marked by an asterisk) presenting the so-called phosphate binding cassette (PBC, in yellow) formed by a short helix (αP) and an extended loop (ca. 60 residues, invisible in the crystals) between strands β6 and β7. The domain architecture of the full length protein is shown above (the cNMP domain is highlighted in orange). (Right) Sequence alignment of cNMP domains in human CNNMs. The long β6-β7 loop is conserved throughout, but is larger in CNNM1 and CNNM2, intermediate in CNNM4, and shorter in CNNM3. A likely unstructured polypeptide segment following helix αB was not included in our CNNM4cNMP construct. The colors of the secondary elements correspond to those used in the crystal structure. (B) Stereo view of residues at the cavity opening of the β-roll in CNNM4cNMP. Residues within β-strands or the PBC motif are shown in blue or yellow, respectively. Residues Y603, F698, and Y694 (labeled in red and indicated by a red asterisk in the sequence alignment) invade the space usually occupied by a bound cyclic nucleotide in unrelated CNB containing proteins like PKA (a superimposed cAMP molecule is shown by transparent red sticks).
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Figure 4. Structure of the CNNM4cNMP dimer. (A) (left) Association of two CNNM4cNMP domains (blue and orange) in the crystal. The presence of such dimers in solution was confirmed by SAXS data that indicate a shape and volume consistent with the shown bead model (grey spheres). (A) (right) Residues (mostly hydrophobic) at the dimerization interface between CNNM4cNMP subunits, formed primarily by their strands β4 and β5. (B) SEC-MALS analysis of CNNM4cNMP (left) and CNNM4BAT-cNMP-Ctail (right). CNNM4cNMP (grey; Mw = 20936.78 Da monomer) yields an apparent Mw of 24,740 ± 60 Da and 33,920 ± 50 Da at concentrations of 1 mg/mL (dotted lines) and 10 mg/mL (solid lines), respectively, indicating prevalence of the dimer at higher concentration. For the F631A mutant (orange), smaller apparent MW of 21,730 ± 50 Da and 26,440 ± 50 Da are observed for 1 and 10 mg/mL, respectively, indicating that this mutation strongly impedes dimerization. CNNM4BAT-cNMP-Ctail (grey; MW = 47,861.17 Da monomer) similarly yields an apparent Mw of 51,120 ± 60 Da and 63,610 ± 100 Da for 1 and 10 mg/mL, respectively, again indicating prevalence of the dimer at higher concentration. For its F631A mutant (yellow), very similar MW of 49,230 ± 80 Da and 60,920 ± 90 Da are derived, indicating a negligible effect on CNNM4BAT-cNMP-Ctail dimerization. Thus, the disruption of CNNM4cNMP dimerization by this mutation (see left) is overridden by dimerization via the still intact Bateman module. (C) SAXS analysis of CNNM4cNMP. (left) Experimental SAXS data (orange) and scatter curve (black) for the best-fit bead model (Χ2 = 2.93) of CNNM4cNMP dimers in solution (shown in (A)). (right) The dimensionless Kratky plot (orange) indicates a well-folded, flexible, and elongated arrangement for CNNM4cNMP. The corresponding BSA reference peak is also shown.
Figure 4. Structure of the CNNM4cNMP dimer. (A) (left) Association of two CNNM4cNMP domains (blue and orange) in the crystal. The presence of such dimers in solution was confirmed by SAXS data that indicate a shape and volume consistent with the shown bead model (grey spheres). (A) (right) Residues (mostly hydrophobic) at the dimerization interface between CNNM4cNMP subunits, formed primarily by their strands β4 and β5. (B) SEC-MALS analysis of CNNM4cNMP (left) and CNNM4BAT-cNMP-Ctail (right). CNNM4cNMP (grey; Mw = 20936.78 Da monomer) yields an apparent Mw of 24,740 ± 60 Da and 33,920 ± 50 Da at concentrations of 1 mg/mL (dotted lines) and 10 mg/mL (solid lines), respectively, indicating prevalence of the dimer at higher concentration. For the F631A mutant (orange), smaller apparent MW of 21,730 ± 50 Da and 26,440 ± 50 Da are observed for 1 and 10 mg/mL, respectively, indicating that this mutation strongly impedes dimerization. CNNM4BAT-cNMP-Ctail (grey; MW = 47,861.17 Da monomer) similarly yields an apparent Mw of 51,120 ± 60 Da and 63,610 ± 100 Da for 1 and 10 mg/mL, respectively, again indicating prevalence of the dimer at higher concentration. For its F631A mutant (yellow), very similar MW of 49,230 ± 80 Da and 60,920 ± 90 Da are derived, indicating a negligible effect on CNNM4BAT-cNMP-Ctail dimerization. Thus, the disruption of CNNM4cNMP dimerization by this mutation (see left) is overridden by dimerization via the still intact Bateman module. (C) SAXS analysis of CNNM4cNMP. (left) Experimental SAXS data (orange) and scatter curve (black) for the best-fit bead model (Χ2 = 2.93) of CNNM4cNMP dimers in solution (shown in (A)). (right) The dimensionless Kratky plot (orange) indicates a well-folded, flexible, and elongated arrangement for CNNM4cNMP. The corresponding BSA reference peak is also shown.
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Figure 5. Solution structure of CNNM4BAT-cNMP-Ctail alone and in complex with PRL-1. (A) SAXS derived bead model of CNNM4BAT-cNMP-Ctail in the absence of MgATP, built from the crystal structures of the isolated CNNM4cNMP (PDB ID 6G52) and CNNM4BAT in twisted conformation (modeled from CNNM2BAT, PDB code 4IYS). (B) SAXS derived bead model of CNNM4BAT-cNMP-Ctail in the presence of MgATP, built from the independent crystal structures of the isolated CNNM4cNMP and CNNM4BAT in flat conformation (modeled from CNNM2BAT, PDB code 4P1O). The invisible disordered C-terminal tail of CNNM4cNMP is not represented for clarity. (C) SAXS derived bead model of the complex formed by PRL-1 and CNNM4BAT-cNMP-Ctail in the presence of MgATP. The model was built from the crystal structures of the homologous CNNM2BAT complexed with both PRL-1 and ZnATP (PDB ID: 5LXQ) and CNNM4cNMP (PDB ID: 6G52). In all structures shown, the disordered linker (green) between Bateman module and cNMP domain was modelled with CORAL [54], the putative position of the long loop within the cNMP domain is represented as a dotted line. The complementary monomer is distinguished by an asterisk. Panels to the right show the corresponding SAXS data and computed scatter curves (black) for the illustrated best-fit bead model.
Figure 5. Solution structure of CNNM4BAT-cNMP-Ctail alone and in complex with PRL-1. (A) SAXS derived bead model of CNNM4BAT-cNMP-Ctail in the absence of MgATP, built from the crystal structures of the isolated CNNM4cNMP (PDB ID 6G52) and CNNM4BAT in twisted conformation (modeled from CNNM2BAT, PDB code 4IYS). (B) SAXS derived bead model of CNNM4BAT-cNMP-Ctail in the presence of MgATP, built from the independent crystal structures of the isolated CNNM4cNMP and CNNM4BAT in flat conformation (modeled from CNNM2BAT, PDB code 4P1O). The invisible disordered C-terminal tail of CNNM4cNMP is not represented for clarity. (C) SAXS derived bead model of the complex formed by PRL-1 and CNNM4BAT-cNMP-Ctail in the presence of MgATP. The model was built from the crystal structures of the homologous CNNM2BAT complexed with both PRL-1 and ZnATP (PDB ID: 5LXQ) and CNNM4cNMP (PDB ID: 6G52). In all structures shown, the disordered linker (green) between Bateman module and cNMP domain was modelled with CORAL [54], the putative position of the long loop within the cNMP domain is represented as a dotted line. The complementary monomer is distinguished by an asterisk. Panels to the right show the corresponding SAXS data and computed scatter curves (black) for the illustrated best-fit bead model.
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Figure 6. Structure of the complete intracellular region, CNNM4BAT-cNMP-Ctail. The picture shows three orthogonal views in the absence (A) and presence (B) of bound MgATP. The structures were derived from SAXS and high resolution crystallography data. The CBS module, formed by two associated Bateman modules (red and orange), lies above their likewise dimerized CNNM4cNMP binding domains (dark and light blue), to which they are connected by an extended linker (dark and light green). The CBS1 motif in each Bateman module first into the large central cavity formed by the associated CNNM4cNMP domains. This contiguous and rigid cleft is morphologically complementary to both CBS1 motives and restricts their movement during the transition from twisted (as in (A)) to flat (as in (B)) conformations upon MgATP binding (at site S2 between connected CBS1 and CBS2 motives, see Figure 1). Helices H0, located distal from the central cavity, connect the Bateman modules to the preceding DUF21 transmembrane region.
Figure 6. Structure of the complete intracellular region, CNNM4BAT-cNMP-Ctail. The picture shows three orthogonal views in the absence (A) and presence (B) of bound MgATP. The structures were derived from SAXS and high resolution crystallography data. The CBS module, formed by two associated Bateman modules (red and orange), lies above their likewise dimerized CNNM4cNMP binding domains (dark and light blue), to which they are connected by an extended linker (dark and light green). The CBS1 motif in each Bateman module first into the large central cavity formed by the associated CNNM4cNMP domains. This contiguous and rigid cleft is morphologically complementary to both CBS1 motives and restricts their movement during the transition from twisted (as in (A)) to flat (as in (B)) conformations upon MgATP binding (at site S2 between connected CBS1 and CBS2 motives, see Figure 1). Helices H0, located distal from the central cavity, connect the Bateman modules to the preceding DUF21 transmembrane region.
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Table 1. Data statistics and refinement. One crystal was used per data set. Values in parentheses refer to the high resolution shell.
Table 1. Data statistics and refinement. One crystal was used per data set. Values in parentheses refer to the high resolution shell.
ProteinsCNNM4BATCNNM4cNMP
Data Collection and Process
BeamlineESRF, ID14-1DIAMOND, I03
Radiation wavelength (Å)0.9340.9794
Space group/PDB IDC2/6RS2P3221/6G52
a (Å)
b (Å)
c (Å)
91.39
141.36
87.89
116.74
116.74
243.46
Molecules per a.u.49
Resolution (Å)43.94–3.69 (3.76–3.69)243.46–3.69 (3.99–3.69)
Rsym a0.047 (0.437)0.179 (1.661)
Rmeas b0.052 (0.485)0.184 (1.707)
Rpim c0.023 (0.209)0.042 (0.387)
No. of observations62,620413,463
No. of unique reflections11,86421,343
Mean I/I21 (3.4)13.9 (2.8)
CC1/20.99 (0.91)0.99 (0.87)
Completeness (%)98.7 (90.7)99.7 (98.5)
Redundancy5.3 (5.2)19.4 (19.3)
Mosaicity (°)0.20.1
Refinement Statistics
No. of working/test reflections44,826/117820,676/1989
Rwork d/Rfree e0.23/0.280.2844/0.3026
No. of atoms
Protein45679252
Ligand--
Water--
Average B factors (Å2)
Protein105,94100
Ligand--
Water--
RMSDs
Bond lengths (Å)/angles (°)0.004/0.6830.003/0.748
Ramachandran plot statistics (%)
Residues in most favored regions97.599
Residues in additionally allowed regions2.51
Residues in disallowed regions00
One crystal was used per data set. Values in parentheses are for the highest resolution shell. Rsym a = Σhkl Σi |Ii (hkl) − <I(hkl)>I/Σhkl Σi Ii(hkl); Rmeas b = Σhkl Σi |Ii (hkl) − <I(hkl)>I/Σhkl Σi Ii(hkl); c Rpim= Rpim = Σhkl Σi |Ii (hkl) − <I(hkl)>I/Σhkl Σi Ii(hkl). Rwork d = Σ |Fo − Fc|/ΣFo. Rfree e = Σ |Fo − Fc|/ΣFo, calculated using a random 5 % of reflections that were not included throughout refinement. FMT = formate. N/A= Not applicable.
Table 2. Data collection and structural parameters by SAXS.
Table 2. Data collection and structural parameters by SAXS.
Data Collection Parameters
BeamlineB21, Diamond Light Source, Harwell (UK)
DetectorPilatus 2M
Beam size0.2 × 0.2 mm
Energy12.4 keV
Sample-to-detector distance (mm)4014
q range (A−1)0.0038–0.42
Exposure time (s)3
Number of frames620
Temperature (K)293
ModeSEC online
Structural Parameters
Protein constructCNNM4cNMPCNNM4BAT-cNMP-CtailCNNM4BAT-cNMP-Ctail + MgATPCNNM4BAT-cNMP-Ctail + PRL-1CNNM4BAT-cNMP-Ctail + MgATP + PRL-1
SASBDB access codeSASDER8SASDEQ8SASDES8SASDEP8SASDEN8
Concentration range (mg/mL)7.05.04.78.55.0
q Interval for Fourier inversion (Å−1)0.014–0.20180.007–0.1640.010–0.1090.09–0.1730.009–0.125
Rg [from P(r)] (Å)25.67 ± 1.3241.62 ± 2.1239.15 ± 1.3847.90 ± 5.2447.20 ± 2.55
Rg [from Guiner approximation] (Å)25.52 ± 1.6540.22 ± 0.5439.23 ± 1.9846.55 ± 0.8144.48 ± 1.42
sRg limits [from Guiner approx.]0.34–1.300.31–1.300.41–1.300.36–1.290.38–1.29
Dmax (Å)96166143185183
Porod volume estimate (nm3)102156149226216
Porod exponent2.33.23.33.13.1
Molecular Mass (kDa)
from Porod volume (×0.58)599086131125
from amino acid sequence2148486868
Software Employed
Primary data reductionDAWN pipeline (Diamond Light Source, UK)
Data processingScÅtter v3.1v
Ab initio modellingGASBOR
Validation and averagingDAMAVER/DAMCLUST
Computation of model intensitiesCRYSOL/CORAL
q = 4πsin(θ)/λ, where 2θ is the scattering angle and λ the wavelength.

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MDPI and ACS Style

Giménez-Mascarell, P.; Oyenarte, I.; González-Recio, I.; Fernández-Rodríguez, C.; Corral-Rodríguez, M.Á.; Campos-Zarraga, I.; Simón, J.; Kostantin, E.; Hardy, S.; Díaz Quintana, A.; et al. Structural Insights into the Intracellular Region of the Human Magnesium Transport Mediator CNNM4. Int. J. Mol. Sci. 2019, 20, 6279. https://doi.org/10.3390/ijms20246279

AMA Style

Giménez-Mascarell P, Oyenarte I, González-Recio I, Fernández-Rodríguez C, Corral-Rodríguez MÁ, Campos-Zarraga I, Simón J, Kostantin E, Hardy S, Díaz Quintana A, et al. Structural Insights into the Intracellular Region of the Human Magnesium Transport Mediator CNNM4. International Journal of Molecular Sciences. 2019; 20(24):6279. https://doi.org/10.3390/ijms20246279

Chicago/Turabian Style

Giménez-Mascarell, Paula, Iker Oyenarte, Irene González-Recio, Carmen Fernández-Rodríguez, María Ángeles Corral-Rodríguez, Igone Campos-Zarraga, Jorge Simón, Elie Kostantin, Serge Hardy, Antonio Díaz Quintana, and et al. 2019. "Structural Insights into the Intracellular Region of the Human Magnesium Transport Mediator CNNM4" International Journal of Molecular Sciences 20, no. 24: 6279. https://doi.org/10.3390/ijms20246279

APA Style

Giménez-Mascarell, P., Oyenarte, I., González-Recio, I., Fernández-Rodríguez, C., Corral-Rodríguez, M. Á., Campos-Zarraga, I., Simón, J., Kostantin, E., Hardy, S., Díaz Quintana, A., Zubillaga Lizeaga, M., Merino, N., Diercks, T., Blanco, F. J., Díaz Moreno, I., Martínez-Chantar, M. L., Tremblay, M. L., Müller, D., Siliqi, D., & Martínez-Cruz, L. A. (2019). Structural Insights into the Intracellular Region of the Human Magnesium Transport Mediator CNNM4. International Journal of Molecular Sciences, 20(24), 6279. https://doi.org/10.3390/ijms20246279

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