Abstract
Nanodiscs (ND) are discoidal phospholipid bilayers stabilized by a pair of membrane-scaffolding proteins (MSP). The macromolecular composition and size of ND are ideal for structural and functional studies of membrane and membrane-associated proteins. In this work, we investigate the assembly of ND from a galactosylceramide and dioleoyl phosphatidylserine (PS) lipid mixture with two different MSP and at four MSP-to-lipid ratios. This lipid composition has been optimized for structural and biophysical studies of membrane-bound blood clotting factors that require Ca2+ ions for function. We have demonstrated that CaCl2 induces reversible stacking of the ND that depends on the ND size and Ca2+ concentrations. Our biophysical and electron microscopy (EM) studies show a predominant ND population of ~12 nm in diameter for both the ND assembled from MSP1D1 to lipids ratio of 1:40 and from MSP1E3D1-to-lipids ratio of 1:80. Approximately half of the ND population assembled at MSP1E3D1-to-lipids ratio of 1:150 has a diameter of ~16 nm. These larger ND form ordered stacks at 5-mm Ca2+ concentrations, as shown by cryo-EM. The number and length of the ND stacks increase with the increasing in Ca2+ concentration. Adding millimolar concentrations of EDTA reverses the stacking of the ND.
1 Introduction
In the last 15 years, a new platform for functional and structural studies of membrane proteins has been developed based on the properties of the nascent discoidal high-density lipoprotein (HDL) particles, which are stabilized by two amphipathic apolipoproteins (apoA-I) of around 200 amino acid residues each [1], [2], [3]. These so-called lipid nanodiscs (ND) are a two-component lipid-protein system. The lipids are organized as a bilayer, and the membrane-scaffolding proteins (MSP) are organized as a belt that constrains the lipid bilayer. The MSP are predominantly alpha-helical proteins that can be genetically engineered as derivative of apoA-I. Changing the lipid composition, the length of the MSP, and the MSP to lipids ratio can alter the size and monodispersity of the ND. Numerous studies have been conducted to investigate how these parameters can affect the structure and physicochemical properties of the ND, showing that the MSP-to-lipid ratio and lipid composition are critical [2], [3], [4], [5]. For saturated phospholipids (PLs), such as dipalmitoylphosphatidylcholine, increasing the length of the MSP from 200 to 280 amino acid residues increases the diameter of the ND from 9.8 nm to 12.9 nm [2]. Size exclusion chromatography (SEC), dynamic light scattering (DLS), small-angle X-ray scattering (SAXS), and conventional electron microscopy (EM) are the methods of preference used to define the size and homogeneity of the assembled ND [2], [3], [6], [7], [8]. The melting enthalpy measured for the ND lipids’ phase transition is significantly lower than that for liposomes with the same lipid composition [5], indicating that there is a loss of cooperativity due to the small size of the ND (160–300 lipids per ND) and high fraction of boundary lipids. More than 40% of the ND lipids are boundary and do not participate in the phase transition as they are stabilized by the MSP. This value corresponds to that of the native cell membranes, where 60% of the lipids are boundary and constrained by the high content of membrane proteins [6], [9], [10]. Therefore, the physicochemical properties of the ND make them particularly suitable for the study of membrane-associated proteins at close to physiological lipid conditions.
The focus of this study is to characterize ND with a lipid composition found to be close to the activated platelet membrane surface and most suitable for structural studies of membrane-bound blood coagulation proteins by cryo-EM. These proteins assemble on the activated platelet surface during the propagation phase of coagulation [11]. Activated platelets are a critical component of the blood clotting system, and their physical interaction with the coagulation factors regulates the efficiency of the blood clotting process. The assembly of the clotting complexes requires elevated concentrations (1.2 mm) of free cytosolic Ca2+ and a negatively charged membrane surface that is provided by the activated platelets, which overexpose phosphatidylserine (PS) on the outside of the membrane (10–15 mol%) [11], [12]. Based on these facts and our previous work with Factor VIII bound to lipid nanotubes (LNT) [13], we have developed PS-rich galactosylceramide (GC) ND and shown that they are suitable for structure determination by single particle cryo-EM [7], [14]. The ND with a lipid composition of 80% PS and 20% GC were found to give the best size for single particle cryo-EM studies. This lipid composition (80%PS/20%GC) was previously found to bind FVIII in a stable conformation for helical organization on LNT [14], [15], [16]. Adding 5 mm Ca2+ to the ND assembled from 80%PS/20%GC in physiological buffer induces the formation of well-ordered stacks predominantly from ND with a diameter of ~16 nm. The length of the stacks increases proportionally with increasing the Ca2+ concentration from 0.1 to 10 mm. Above 10 mm Ca2+, the ND stacks begin to form bundles and Y-branched aggregates, without disturbing the ND order within the stacks. Adding mm concentrations of EDTA reversibly disassembles the ND stacks.
In this work, we have applied a combination of complementary biochemical, biophysical, and structural techniques to characterize ND assembled from different MSP and MSP-to-lipid ratio at a lipid composition optimized for the structure determination of membrane-bound blood-clotting proteins by cryo-EM. The developed approach can be applied and optimized for different lipid compositions and is suitable for biophysical and structural studies of membrane-associated proteins and complexes in addition to coagulation factors.
2 Materials and methods
2.1 Reagents
HEPES sodium salt, Na cholate, MSP1D1, and MSP1E3D1 scaffolding proteins were purchased from Sigma (Sigma-Aldrich, St. Louis, MO, USA). PS (1,2-dioleoyl-sn-glycero- 3-phospho-L-serine, sodium salt) and GC (D-galactosyl-β-1,1′ N-nervonoyl-D-erythro-sphingosine, d18:1/24:1) were purchased from Avanti Polar Lipids Inc. (Alabaster, AL, USA). All buffer solutions – HBS (150 mm NaCl, 20 mm HEPES, pH 7.4) and HBS-Ca (HBS with 5 mm CaCl2) – were filtered through a 0.22-μm Millex® GP filter (Millipore Co., Cork, Ireland).
2.2 ND assembly and SEC
ND were prepared following the procedure described in refs. [7], [17]. Briefly, stock solutions of PS and GC lipids in chloroform were mixed in the desired weight ratio. The chloroform was evaporated under Argon gas, and the lipids were resolubilized in HBS buffer. The MSP1D1 and MSP1E3D1 were reconstituted in HBS buffer with 15 mm Na cholate and mixed with the lipids in the desired molar ratios. After 1-h incubation at 37°C, the Na cholate was removed by adding 1 g of Bio-Beads SM-2 per milliliter of mixture. After 4-h incubation at room temperature, the Bio-Beads were removed by centrifugation and ND were separated by SEC through a Superdex 200 HR 10/30-gel filtration column equilibrated in HBS buffer. Elution fractions of 0.5 ml were collected at 1-min intervals. The fractions corresponding to the ND peak were combined and concentrated. The final ND concentration was determined by the MSP absorption at 280 nm (extinction/280 nm 21,000 m−1 cm−1 for MSP1D1 and 29,400 m−1 cm−1 for MSP1E3D1, Sigma-Aldrich protocols: sigmaaldrich.com/etc/medialib/docs/) with a NanoDrop UV-VIS spectrophotometer (Thermo Scientific, Wilmington, DE, USA), as previously described [7]. The size of the ND was estimated from the SEC elution profiles by comparing to the elution profiles of standard proteins with known Stokes diameters: albumin (BSA) – 7.1 nm, aldolase – 9.6 nm, ferritin – 12.2 nm, and thyroglobulin – 17 nm.
2.3 Dynamic light scattering (DLS)
All DLS measurements were carried out with a Zetasizer μV particle analyzer (Malvern Instruments Ltd., Malvern, Worcestershire, UK) at a light-scattering detection angle of 90° with a 2-μl volume quartz cuvette at 21°C, as previously described [7]. All calculations were done with the Zetasizer Software [18].
2.4 Small-angle X-ray scattering (SAXS)
SAXS data were collected using a Rigaku BioSAXS-1000 camera with a FR-E++ X-ray source (Rigaku Americas, The Woodlands, TX, USA). For each measurement, 30 μl of ND sample at 1 mg/ml concentration was manually pipetted into a quartz capillary cell, sealed, placed under vacuum, and aligned in the camera. A series of 30-min exposures were collected and averaged in SAXLab to produce separate sample and buffer curves of 6–9-h exposure. Buffer subtraction, absorption correction, and molecular weight (MW) calibration were performed using the SAXNS-ES server (http://xray.utmb.edu/SAXNS). Data analysis was performed with the Primus software. The distance distribution function – P(r) – was calculated with the GNOM software, both from the ATSAS suite [18].
2.5 Electron microscopy (EM)
The negatively stained and cryogenic EM experiments were conducted, as previously described in Refs. [7], [19]. Shortly, the ND samples were diluted to 0.005 mg/ml in HBS or HBS-Ca buffer and 5 μl deposited on a freshly carbon coated plasma-treated hexagonal copper EM grid (300 mesh, Ted Pella Inc., Redding, CA, USA). The sample was stained with 1% Uranyl acetate for 2 min. Digital electron micrographs were collected with a 200-kV JEM2100-LaB6 electron microscope (JEOL USA Inc., Peabody, MD, USA) equipped with a 4k Ultrascan CCD camera (Gatan Inc., USA) at low electron doses (<16 e− Å−2 s−1) and a final magnification of 56,400× (2.9 Å/pixel). The size of the ND was evaluated with the Digital Micrograph (DM) software (Gatan Inc., Pleasanton, CA, USA).
2.6 ND stacking experiments
ND stacks were obtained from ND assembled with MSP1E3D1 at MSP-to-lipid ratios of 1:80 and 1:150 in the presence of 5 mm CaCl2. The number and length of ND stacks were followed at seven different Ca2+ concentrations ranging from 10 μm to 15 mm Ca2+. The ND were first incubated with the CaCl2 solutions for 10, 30, and 60 min; diluted to 0.005 mg/ml and negatively stained as previously described in Refs. [7], [19]. EDTA was added in two times the excess of the CaCl2 concentration to reverse the stacking and incubated for 10 min before negative staining. Digital electron micrographs were collected as described for the single ND, and the length and frequency of the ND stacks were evaluated with the DM software (Gatan, Inc., USA).
2.7 Cryo-electron microscopy (EM)
For the cryo-EM experiments, the ND stacks were formed at 10 mm CaCl2 from ND assembled at MSP1E3D1-to-lipids ratio of 1:150 after 60-min incubations. The cryo-EM grids were prepared similarly to the negative stain samples, except for replacing the carbon-coated grids with holey grids (Ted Pella Inc., USA) and the negative staining with flash-freezing with a Vitrobot Mark IV (FEI Inc., USA), as described previously [13], [19]. Digital cryo-EM images were recorded at low electron doses (<16 e− Å−2 s−1) and close to liquid nitrogen temperature (−174°C) with the same electron microscope and at the same EM conditions as the negatively stained samples.
3 Results
3.1 Size distribution of ND assembled with different MSP and MSP-to-lipid ratio
All ND were assembled from a two-component lipid mixture of 80% PS and 20% GC that has been previously optimized for structural studies of clotting proteins by cryo-EM [7], [13], [15], [16]. The type of PS and PC was defined in our early studies of binding FVIII to LNT with different lipid composition [20], [21]. We further repeated this experiments with vesicles and ND assembled with MSP1D1 at MSP-to-lipids ratio of 1:47 [7], [14], [19] and confirmed that the 80% PS and 20% GC lipid composition is optimal for structural studies of membrane-bound FVIII in vitro [15], [16]. The ND assembled at a MSP1D1-to-lipids ratio of 1:40 showed a similar SEC elution profile to the one previously assembled at a MSP1D1-to-lipids ratio of 1:47 [7] (Figure 1). The theoretical area calculated for the circular arrangement of two MSP1E3D1 surrounding the ND bilayer is twice the size of the area calculated for circular arrangement of two MSP1D1 [2], [3], [10]. Therefore, for the assembly of ND with MSP1E3D1, we started with an initial MSP-to-lipids ratio of 1:80. The SEC elution profiles of the ND assembled at a MSP1D1-to-lipids ratio of 1:40 and at a MSP1E3D1-to-lipids ratio of 1:80 were quite similar, presenting a predominant elution peak of ND with a Stokes’ diameter centered around 10 nm (Figure 1, Table 1). To obtain ND with a larger diameter, we gradually decreased the MSP1E3D1-to-lipid ratio to 1:150. A shift to larger diameters was observed for the main eluted ND fraction at a MSP1E3D1-to-lipids ratio of 1:125 showing a broad elution peak spanning from 10- to 12-nm Stokes’ diameter. Further decreasing the MSP1E3D1-to-lipids ratio to 1:150 resulted in a well-defined elution peak of ND with a Stokes’ diameter centered around 11 nm (Figure 1, Table 1). As SEC is not always accurate for size determination of discoid (non-globular) particles, the size and morphology of the ND particles collected from the fractions indicated on Figure 1 (with dashed lines) were further evaluated by conventional EM, dynamic light scattering (DLS), and SAXS [7] (Table 1). The SEC elution profiles also showed that the ND population is quite polydisperse for the GC-PS lipid mixtures, type of MSP, and MSP-to-lipids ratio employed in this study (Figure 1). The correlation of SEC, DLS, SAXS, and EM methods presented in this work shows the potential of these techniques for the characterization of heterogeneous ND population in the context of ND optimization for structural studies of membrane-bound clotting factors by cryo-EM (Table 1).

SEC of ND with 80% PS and 20% GC lipid composition assembled from either MSP1D1 or MSP1E3D1 at different MSP-to-lipid ratios. The grey areas indicate the fractions, which were collected for further characterization. The elution time of standard proteins with known Stokes’ diameters is shown: albumin (BSA) – 7.1 nm, aldolase – 9.6 nm, ferritin – 12.2 nm, and thyroglobulin – 17 nm.
Comparison between the size of nanodiscs (ND) with 80% PS and 20% GC lipid composition, assembled from two types of MSP and at three MSP to lipids ratios, as evaluated by four different methods.
| ND size groups | |||||
|---|---|---|---|---|---|
| ND diameter±SD (nm) | 8±2 | 12±2 | 16±2 | >18 | |
| Measurement method | MSP1D1:Li=1:40 | ||||
| EM | Weight (%) | 6 | 85 | 7 | 2 |
| Diameter±SD (nm) | 9.4±0.4 | 11.9±1.0 | 15.0±0.6 | 17.5±0.9 | |
| SEC | Diametera±SD (nm) | 11.2±1.9 | |||
| DLS | Diameterb±SD (nm) | 10.0±1.0 | |||
| SAXS | Rg±SD (nm) | 5.20±0.04 | |||
| MSP1E3D1:Li=1:80 | |||||
| EM | Weight (%) | 2 | 78 | 17 | 2 |
| Diameter±SD (nm) | 9.6±0.3 | 11.9±0.9 | 15.1±0.8 | 19.2±1.0 | |
| SEC | Diametera±SD (nm) | 10.0 ±1.0 | |||
| DLS | Diameterb±SD (nm) | 11.2±1.9 | |||
| SAXS | Rg±SD (nm) | 5.18±0.03 | |||
| MSP1E3D1:Li=1:150 | |||||
| EM | Weight (%) | 2 | 36 | 45 | 17 |
| Diameter±SD (nm) | 9.4±0.4 | 12.3±1.1 | 15.8±1.1 | 19.9±1.5 | |
| SEC | Diametera±SD (nm) | 11.0±1.0 | |||
| DLS | Diameterb±SD (nm) | 14.1±3.2 | |||
| SAXS | – | – | |||
EM, transmission electron microscopy of negatively stained ND absorbed on amorphous carbon films. The diameter is directly measured form the EM micrographs. SEC, size exclusion chromatography. aThe diameter is evaluated from the hydrodynamic radius of the particles. SAXS – small angle X-ray scattering. Rg is the radius of gyration. SD is the statistical deviation in nm. bThe diameter is evaluated from the Stokes’ diameter of standard proteins as shown on Figure 1. DLS – dynamic light scattering.
For the EM experiments, the ND particles were negatively stained as absorbed on amorphous carbon, and the particles’ size and shape were evaluated from ~15 EM micrographs. Only micrographs showing homogenously distributed and evenly stained ND particles were selected for the statistics shown on Figure 2B. Less than 5% of the ND particles showed an oval shape due to incomplete or unsuccessful assembly. Less than 10% of the ND particles showed “side-on” views when absorbed on the amorphous carbon film (Figure 2A). Therefore, the diameter of each particle was determined by measuring the longest dimension of the ND directly from the digital micrographs, when the particles are adsorbed “face on” the carbon (Figure 2A). More than 500 representative ND particles were selected from 15 micrographs and for each MSP-to-lipid ratio. The ND particles were separated into four ND size groups with a bandwidth of 4 nm: 8±2 nm, 12±2 nm, 16±2 nm, and >18 nm (Table 1). The number of particles in each ND group was plotted as percentage of the total amount of measured particles (Figure 2B, Table 1). Direct visualization by negatively staining EM showed that the main population (~80%) of the ND assembled at a MSP1D1-to-lipids ratio of 1:40 and at a MSP1E3D1-to-lipids ratio of 1:80 has a diameter of ~12 nm (Figure 2B, Table 1). The ND assembled at a MSP1E3D1-to-lipids ratio of 1:150 showed nearly equal distribution of ND with diameter of ~12-nm diameter (36%) and ~16 nm (45%). A significantly larger population of ND (~17%) showed a diameter >18 nm (Figure 2B, Table 1). The ND assembled with MSP1E3D1-to-lipids ratio of 1:125 eluted with a broad peak after SEC at the same conditions as the ND assembled at the MSP1E3D1-to-lipids ratio of 1:80 and 1:150 (Figure 1). Our attempt to obtain more homogenous populations with ND assembled at a MSP1E3D1-to-lipids ratio lower than 150 was unsuccessful and not suitable for further characterization by the methods employed in this study.

Negative staining electron microscopy (EM) of ND with 80% PS and 20% GC lipid composition assembled from either MSP1D1 or MSP1E3D1 at different MSP-to-lipid ratio. (A) EM micrographs of negatively stained ND absorbed on amorphous carbon film. Scale bar: 50 nm. (B) Size distribution graphs as measured directly from the EM micrographs.
The DLS and SAXS experiments showed similar values for the size of the ND assembled at a MSP1D1-to-lipid ratio of 1:40 and at a MSP1E3D1-to-lipid ratio of 1:80. These values correspond well to the ones measured by SEC and EM for the predominant ND population (Table 1). As the ND population is quite heterogeneous in size, the ND diameters calculated from the DLS values for the hydrodynamic radius of the ND particles in the Z direction are quite similar to the ND diameters measured from the EM micrographs for the main ND fractions (Figure 2B, Table 1). The SAXS scattering curves presented a characteristic shape for discoidal particles consisting of a sharp minimum and a broad maximum with identical radii of gyration (Rg)~5.2 nm and Dmax of ~9.6 nm (Figure 3, Table 1) [2]. While the SAXS weighted averages for the radius of gyration (Rg) values are determined at high accuracy, they are well within the error of the DLS data and show an average for the ND diameter of 10.4 nm, which is slightly smaller than the one calculated from the DLS data of 11.2 nm (Table 1). Although the SAXS scattering curves for both ND populations (assembled with MSP1D1 or MSP1E3D1 at MSP-to-lipids ratio of 1:40 and 1:80, respectively) are very similar, they are not identical and display systematic variations with a Chi-squared metric of 2.9 up to q of 3 nm−1 (Figure S1). The nearly identical distance distribution function – P(r) curves – suggests that these variations reflect changes in the organization of the MSP that circumscribe the lipids (Figure 3).

Small-angle X-ray scattering (SAXS) of ND with 80% PS and 20% GC lipid composition assembled at MSP1D1-to-lipids ratio of 1:40 and at MSP1E3D1-to-lipids ratio of 1:80. (A) SAXS curves in reciprocal (Fourier) space and GNOM fits for the MSP1D1 (
,
) and MSP1E3D1 (
,
) ND. I(q) is radially symmetric, where I is the intensity of the scattered beam and q=2π/d is the scattering vector. 1/d is the reciprocal distance in Å−1. The curves are offset for clarity. (B) Corresponding pair-wise distance distribution function – P(r) curves for MSP1D1 (
) and MSP1E3D1 (
) in real space. (r) is the inter-atomic distance in Å, and Dmax is the maximum dimension of the particles.
3.2 Stacking of ND in the presence of CaCl2
As the blood clotting proteins require 5 mm Ca2+ for function in vitro [7], [14], we undertook to investigate the effect of CaCl2 on the ND stacking and aggregation. It is well known that introducing milimolar concentrations of Ca2+ to a solution of PS-rich liposomes induces strong aggregation of the vesicles [22], [23]. Therefore, we did expect changes in the monodispersity of the ND at millimolar Ca2+ concentration. What we observed, however, was not large aggregates but the formation of well-ordered ND stacks. We followed the ND stacking induced by the presence of 5 mm CaCl2 for ND assembled at a MSP1E3D1-to-lipids ratios of 1:80 and 1:150, as representatives for the predominant ND size groups of ~12-nm and ~16-nm diameter, respectively (Figure 2). The ND were absorbed on amorphous carbon film and negatively stained after 10-min incubation with 5 mm CaCl2 at room temperature (Figure 4). The length and average diameter of the ND stacks for each MSP1E3D1-to-lipids ratio were measured directly from ~15 EM micrographs. Increasing the incubation time to 30 and 60 min did not significantly affect the appearance and length of the ND stacks at the MSP1E3D1-to-lipid ratio of 1:80. A substantial increase in the length (~180 nm) and number of stacks per micrograph was observed for the ND assembled at a MSP1E3D1-to-lipids ratio of 1:150 after 60-min incubation with 5 mm CaCl2 (Figure 4). The ND stacks were formed predominantly from the ND with a larger diameter (~16 nm) for both MSP1E3D1-to-lipids ratios (1:80 and 1:150). No stacks were observed for the ND with ~12-nm diameter assembled at a MSP1E3D1-to-lipids ratio of 1:150, and only short stacks (~25 nm in length) were observed for the MSP1E3D1-to-lipids ratio of 1:80 (Figure 5). For larger ND with diameter >18 nm, only a few short ND stacks were observed at a MSP1E3D1-to-lipids ratio of 1:80, whereas at a MSP1E3D1-to-lipids ratio of 1:150, a sizable population of ND stacks was formed. These stacks did not exceed 100 nm in length even after 60-min incubation (Figure 5).

Negative staining EM of ND stacks formed from ND assembled at a MSP1E3D1-to-lipids ratio of 1:80 (row A) and a MSP1E3D1-to-lipids ratio of 1:150 (row B) after 10, 30, and 60 min of incubation with 5 mm CaCl2. Scale bar: 80 nm. The insets show magnified views of the ND stacks from the respective micrographs, denoted with white dashed squares.

Distribution of the ND stacks by length and diameter formed from ND assembled at MSP1E3D1-to-lipids ratios of 1:80 (A) and 1:150 (B) after incubation with 5 mm CaCl2 for 10, 30, and 60 min.
3.3 Effect of the Ca2+ concentration on the ND stacks formation
To evaluate the effect of Ca2+ concentration on the ND stacking, we followed the length of the ND stacks from ND assembled at MSP1E3D1-to-lipids ratio of 1:150 after 60-min incubation with CaCl2 at concentrations ranging from 0.1 to 15 mm. The ND stacks were assessed by several parameters: number of stacks per EM micrograph, average length of the stack, and diameter of the ND in the stack. The average ND stacks’ length at low CaCl2 concentrations (<2.5 mm) corresponds to two-disc stacks (~14 nm). The average length of the ND stacks increases to ~19 nm at 2.5 mm CaCl2 concentration, corresponding to three-disc stacks (Table 2, Figure 6A). A five-fold increase of the number of ND stacks per EM micrograph was observed at 5 mm CaCl2 concentration (Table 2, Figure S2). Increasing the CaCl2 concentration above 5 mm resulted in a pronounced increase in the length of the ND stacks with simultaneous decrease of the number of stacks per micrograph. Above 10 mm Ca2+, Y-branching and side-to-side bundling of the ND stacks were observed (Figure 6A) leading to the formation of large aggregates of ND stacks above 15 mm CaCl2 concentrations that are not suitable for further EM characterization. Adding millimolar concentrations of EDTA to the ND stacks resulted in the reversing of the ND stacking after 10-min incubation (Figure S3). An increased number (~30%) of ND absorbed “side-on” on the amorphous carbon field was observed after adding EDTA, which can be useful for single particle reconstruction from 2D projections [7] (Figure S3). Cryo-EM of the ND stacks formed after a 60-min incubation with 10 mm CaCl2 showed that the stacks could reach microns in length if suspended in vitreous water (Figure 6B). The ND stacks showed the same morphology and diameter when either negatively stained or frozen-hydrated, confirming that the negative staining procedure employed in our work is free of the artifact observed in other studies using slightly different staining procedures (Figure 6).
Ca2+ dependence of the length of the ND stacks formed from ND assembled with MSP1E3D1 to lipids ratio of 1:150 after 60 min incubation.
| CaCl2 (mm) | Number of stacks (per micrograph) | Stack length (nm) | SD (nm) | SD (%) |
|---|---|---|---|---|
| 0 | 6 | 14 | 1.2 | 8.8 |
| 0.1 | 7 | 14 | 1.2 | 8.8 |
| 1.0 | 5 | 16 | 3.8 | 24.1 |
| 2.5 | 6 | 19 | 8.3 | 44.4 |
| 5.0 | 29 | 52 | 38.3 | 74.0 |
| 7.5 | 20 | 91 | 80.0 | 88.4 |
| 10.0 | 10 | 136 | 111.1 | 81.9 |
| 15.0 | 6 | 182 | 152.8 | 84.0 |
The average length of the ND stacks was calculated from 30 individual stacks and the number of stacks per micrograph was averaged from five EM micrographs. The statistical deviation (SD) is given in nm and %. See also Figure S2.

Negative staining and cryo-EM micrographs of ND stacks formed from ND assembled at a MSP1E3D1-to-lipids ratio of 1:150 in the presence of 10 mm CaCl2 after a 60-min incubation. Scale bar: 50 nm. (A) EM micrographs of negatively stained Y-branched and side-bundled ND stacks. Scale bar: 10 nm. (B) Cryo-EM micrographs of frozen-hydrated ND stacks suspended in amorphous ice (vitreous water) over the holes of a lacey carbon film coating an EM grid. Scale bar: 50 nm.
Free ND (not involved in stacks) for the ND assembled at a MSP1E3D1-to-lipids ratio of 1:150 at different CaCl2 concentrations were observed even for high CaCl2 concentrations (>10 mm) and long incubation time (>60 min) (Figure S4). The number and diameter of the free ND (not included in the stacks) per EM micrograph after 60-min incubation at different Ca2+ concentrations were also assessed (Figure S4). At low Ca2+ concentrations, the size distribution of the free ND corresponded roughly to the control population without CaCl2. The number of free ND with diameter of 16±2-nm discs steadily declined as the CaCl2 concentration exceeded 7.5 mm until fully disappearing at 15 mm CaCl2 (Figure S4). These results support the observed increase in the length of the ND stacks with increasing CaCl2 concentration (Table 2). The significant decrease in the number of free ND with a diameter of ~16±2 nm at greater than 5 mm CaCl2 concentration confirms our observations that at 5 mm CaCl2, the ND stacks are predominantly formed by ND with diameters >16 nm (Figure 2).
4 Discussion
It is well known that at a given lipid composition, the type of MSP and MSP-to-lipids stoichiometry is critical for the ND assembly [2], [4]. A correct MSP and MSP-to-lipids ratio secures a more homogenous distribution of self-assembled ND. If this ratio is off, the excess lipids and MSP will form aggregate and elute before the main ND peak as seen in Figure 1 [10]. It is important to take into account that this heterogeneity is assessed differently by different techniques. EM is a direct qualitative approach, which at its low end (conventional EM) can give an accurate estimate of the size and shape of a macromolecular solution absorbed on amorphous carbon and at its high end (cryo-EM) can give direct structure information at the subnanometer and near atomic resolution. SEC, DLS, and partially SAXS are more amenable for characterizing the heterogeneity of nanoparticles in solution and at a larger set of conditions. They lack, however, the sensitivity to characterize the size outside of the predominant nanoparticle population and assess directly the heterogeneity in the context of structure (Table 1). Furthermore, structure determination by SAXS requires highly homogenous particle solutions [24], which is not as stringent for single particle cryo-EM, where the particles can be selected individually and separated in homogenous subsets by reference-free 2D averaging algorithms as demonstrated in EMAN2 [25]. An additional inconvenience is that the Rg value measured by SAXS is based on scattering from the electron density variation, which is positive for the protein and negative for the lipid bilayer [24], thus producing an incomplete 3D reconstruction of the ND, including only the MSP part (Figure 7A). Therefore, combination of both SAXS and EM as structural approaches can be complimentary and useful to fully characterize a ND system in solution, as shown in Figure 7B.
![Figure 7: Three-dimensional (3D) ND reconstructions. (A) SAXS reconstruction of the ND assembled with MSP1D1 at MSP-to-lipid ratio of 1:47, as described in Ref. [7]. The volume of the MSP is shown as a “bead” model. The Human Apo AI crystal structure (2AO1.PDB) shown as “rainbow” colored ribbons aligned within the DAMMIF bead model (blue-grey surface) using SUPCOMB. The diameter has been estimated at ~10.4 nm. (B) 3D reconstruction of the same ND by single particle electron microscopy from electron micrographs of negatively stained ND in solution, as described in Ref. [7]. The 3D-EM density of the ND is shown as a surface (blue mesh) and density (solid blue color) representation. The ND “bead” model from the SAXS data (solid yellow color) was fitted in the 3D-EM structure with the “fit volume” option of the UCSF-Chimera software [26].](/document/doi/10.1515/ntrev-2016-0073/asset/graphic/j_ntrev-2016-0073_fig_007.jpg)
Three-dimensional (3D) ND reconstructions. (A) SAXS reconstruction of the ND assembled with MSP1D1 at MSP-to-lipid ratio of 1:47, as described in Ref. [7]. The volume of the MSP is shown as a “bead” model. The Human Apo AI crystal structure (2AO1.PDB) shown as “rainbow” colored ribbons aligned within the DAMMIF bead model (blue-grey surface) using SUPCOMB. The diameter has been estimated at ~10.4 nm. (B) 3D reconstruction of the same ND by single particle electron microscopy from electron micrographs of negatively stained ND in solution, as described in Ref. [7]. The 3D-EM density of the ND is shown as a surface (blue mesh) and density (solid blue color) representation. The ND “bead” model from the SAXS data (solid yellow color) was fitted in the 3D-EM structure with the “fit volume” option of the UCSF-Chimera software [26].
The blending of SEC, DLS, SAXS, and EM methodologies reported in this work showed that the predominant ND population obtained at the selected binary lipid composition of 80% PS and 20% GC and at both MSP1D1-to-lipids ratio of 1:40 and MSP1E3D1-to-lipids ratio of 1:80 has a diameter of ~12 nm. The SEC eluted ND fractions were also more heterogeneous than the one obtained for pure lipid mixtures at the same MSP1D1 and MSP1E3D1-to-lipids ratio, suggesting that more MSP types should be tested to improve the assembled ND for structural studies of clotting proteins. A gradual increase in size was not observed for the ND assembled in this study, in contrast to the previously reported ND assembled from pure PL mixtures with the same type of MSP and at similar MSP-to-lipids ratio [2], [4], [10]. One explanation may be that the presence of GC even at 20% weight ratio can lead to more rigid membrane patches that can stretch or shrink the MSP with different lengths, as their predominant alpha-helical structure makes them spring-like [27]. The superposition of the SAXS and single-particle EM 3D reconstructions for ND assembled at MSP1D1-to-lipids ratio of 1:47 shown on Figure 7 further supports that. The presence of 5 mm Ca2+ ions, 80% PS lipids, and low MSP1E3D1-to-lipid ratio of 1:150 drives the formation of micron long-ordered ND stacks formed predominantly from larger ND of ~16 nm in diameter. The role of the ND size for the stacks formation suggests that a critical size/area might be required for the formation of stable membrane-membrane interactions between the ND at the chosen lipid composition of 20% GC and 80% PS. The formation of long- and well-ordered ND stacks is directly proportional to the proportion of the ND fraction with diameter of ~16 nm (Figures 2 and 4). The fact that smaller ND, with a diameter of ≤12 nm, do not form stacks even after 60-min incubation in the presence of 15 mm Ca2+ (Figure S4) can be employed to selectively recruit larger ND from heterogeneous ND populations.
Adding millimolar concentrations of EDTA easily reverses the interactions between the ND in the stacks, pointing to the critical role of Ca2+ concentrations for stabilizing the ND stacks. The cryo-EM micrographs of the ND stacks suspended in vitreous water further support this conclusion by showing significantly longer ND stacks than the ones observed by negative-staining EM, suggesting that absorption on amorphous carbon may fragment the stacks.
The ND stacks formed in the presence of Ca2+ are nanostructures with periodic features. Therefore, obtaining well-ordered and stable ND stacks will allow high-resolution structure determination of the MSP and MSP-lipid bilayer interactions by cryo-EM, which has not been possible for isolated ND due to the ND’s intrinsic flexibility. Recently, ND stacks obtained through DNA spacers were reported [28]. The ND stacks presented here may offer an alternative, employing negatively charged lipid mixture and metal cations instead of macromolecular spacers and linkers.
In conclusion, the presented results are a first step in the characterization and optimization of ND assembly at a desired lipid composition, size, and organization for the direct structure determination of membrane-associated protein and complexes by cryo-EM at close to physiological membrane and solution conditions. Our study offers cryo-EM images of “naked” ND with sufficient quality for further high-resolution structure analyses. The lipid composition and MSP-to-lipids ratio of the assembled ND in combination with the proposed conditions for reversible stacking, as discussed in this study, can be further optimized for the characterization of specific protein systems in a membrane-bound state.
Acknowledgments
We wish to thank the Sealy Center for Structural Biology at UTMB and its Director, Dr. BM Pettitt, for continuous support on this project. SSM acknowledges the American Heart Association National Scientist Development Grant, 10SDG3500034, and the Provost’s office and the Department of Neuroscience and Cell biology at UTMB for start up and bridging funds. The authors declare no conflict of interest.
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Articles in the same Issue
- Frontmatter
- In this issue
- Editorial
- Lipid nanotechnologies for macromolecular structure determination
- Reviews
- Nanodisc characterization by analytical ultracentrifugation
- Membrane mimetics for solution NMR studies of membrane proteins
- Membrane protein reconstitution in nanodiscs for luminescence spectroscopy studies
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- Research highlight
- Façade detergents as bicelle rim-forming agents for solution NMR spectroscopy
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- Lipid nanotechnologies for structural studies of membrane-associated clotting proteins by cryo-electron microscopy
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