An optimized reverse micelle surfactant system has been developed for solution nuclear magnetic resonance studies of encapsulated proteins and nucleic acids dissolved in low viscosity fluids. Comprising the nonionic 1-decanoyl-rac-glycerol and the zwitterionic lauryldimethylamine-N-oxide (10MAG/LDAO), this mixture is shown to efficiently encapsulate a diverse set of proteins and nucleic acids. Chemical shift analyses of these systems show that high structural fidelity is achieved upon encapsulation. The 10MAG/LDAO surfactant system reduces the molecular reorientation time for encapsulated macromolecules larger than ~20 kDa leading to improved overall NMR performance. The 10MAG/LDAO system can also be used for solution NMR studies of lipid-modified proteins. New and efficient strategies for optimization of encapsulation conditions are described. 10MAG/LDAO performs well in both the low viscosity pentane and ultralow viscosity liquid ethane and therefore will serve as a general surfactant system for initiating solution NMR studies of proteins and nucleic acids.
An optimized reverse micelle surfactant system has been developed for solution nuclear magnetic resonance studies of encapsulated proteins and nucleic acids dissolved in low viscosity fluids. Comprising the nonionic 1-decanoyl-rac-glycerol and the zwitterionic lauryldimethylamine-N-oxide (10MAG/LDAO), this mixture is shown to efficiently encapsulate a diverse set of proteins and nucleic acids. Chemical shift analyses of these systems show that high structural fidelity is achieved upon encapsulation. The 10MAG/LDAO surfactant system reduces the molecular reorientation time for encapsulated macromolecules larger than ~20 kDa leading to improved overall NMR performance. The 10MAG/LDAO system can also be used for solution NMR studies of lipid-modified proteins. New and efficient strategies for optimization of encapsulation conditions are described. 10MAG/LDAO performs well in both the low viscosity pentane and ultralow viscosity liquid ethane and therefore will serve as a general surfactant system for initiating solution NMR studies of proteins and nucleic acids.
Solution nuclear magnetic
resonance (NMR) spectroscopy is a powerful
technique for studying the structures of macromolecules under a variety
of conditions and their internal dynamics on a wide range of time
scales.[1] Sample preparation is often a
key factor in being able to obtain high-quality NMR data on complex
macromolecular systems. Methods for encapsulating proteins within
the aqueous core of a reverse micelle, and then dissolving the micelle
in low viscosity fluid, were introduced in the late 1990s to help
overcome the “slow tumbling” problem presented by large,
soluble proteins (Figure 1).[2] Since then, reverse micelles have been used to study integral[3,4] and anchored[5] membrane proteins, as well
as soluble proteins[6] and nucleic acids[7] of marginal stability. Encapsulation has also
enabled studies of various biophysical properties of protein including
cold denaturation,[8,9] hydration[10,11] and internal motion.[12]
Figure 1
10MAG/LDAO reverse micelle
surfactant system for solution NMR studies
of encapsulated proteins and nucleic acids. (a) Chemical structures
of the nonionic/zwitterionic surfactant system 10MAG/LDAO compared
to the currently used ionic surfactants AOT or CTAB. (b) Cut-away
view of a space-filling model of flavodoxin encapsulated in a 10MAG/LDAO
reverse micelle. (c) The direct injection method for sample preparation
is illustrated using flavodoxin bound to its brightly yellow cofactor
flavin mononucleotide. Conditions: 300 μM flavodoxin in 150
mM 10MAG/LDAO surfactant at a molar percent ratio of 65%:35%, 15 mM
hexanol and water loading (W0) of 20.
10MAG/LDAO reverse micelle
surfactant system for solution NMR studies
of encapsulated proteins and nucleic acids. (a) Chemical structures
of the nonionic/zwitterionic surfactant system 10MAG/LDAO compared
to the currently used ionic surfactants AOT or CTAB. (b) Cut-away
view of a space-filling model of flavodoxin encapsulated in a 10MAG/LDAO
reverse micelle. (c) The direct injection method for sample preparation
is illustrated using flavodoxin bound to its brightly yellow cofactor
flavin mononucleotide. Conditions: 300 μM flavodoxin in 150
mM 10MAG/LDAO surfactant at a molar percent ratio of 65%:35%, 15 mM
hexanol and water loading (W0) of 20.A critical issue when using reverse
micelle techniques in NMR studies
is that the surfactants must be able to efficiently encapsulate the
macromolecule with high structural fidelity while also allowing the
use of low viscosity solvents such as liquid pentane, propane or ethane.
Thus, the overall size of the surfactant and the electrostatic characteristics
of the headgroup are critical for maintaining the native structure
while also providing the desired reduction in molecular reorientation
time for the encapsulated macromolecule. Several studies have identified
reverse micelle surfactant systems that meet the strict requirements
of high-resolution reverse micelle NMR,[13,14] but a surfactant
system of general utility has not yet been described. Currently, the
two commonly used surfactants in reverse micelle NMR are the anionic
bis(2-ethylhexyl)-sulfosuccinate (AOT)[2] and the cationic hexadecyltrimethylammonium bromide (CTAB),[15] where the latter uses hexanol as a cosurfactant
(Figure 1). Applications of AOT in this context
are limited because few proteins have been encapsulated with high
structural fidelity, presumably due to the denaturing effect of the
anionic headgroup. CTAB has proven more successful—possibly
due to the help of the nonionic cosurfactant hexanol—and has
been used to encapsulate various proteins with high structural fidelity
and high quality NMR spectra.[15,16] Nevertheless, the search
for optimal encapsulation conditions for a given protein has been
somewhat ad hoc, which has likely limited general
application of this approach. Thus, there is a need for a highly robust
reverse micelle surfactant system that allows for efficient discovery
of encapsulation conditions for a given macromolecule with high structural
fidelity. Here, we describe the development of a novel surfactant
system that can be generally applied to proteins and nucleic acids
thus allowing for high-resolution NMR studies of a wide-range of encapsulated
biological macromolecules. The experimental requirements imposed by
reverse micelle NMR spectroscopy led to identification of a binary
surfactant system consisting of the nonionic 1-decanoyl-rac-glycerol (10MAG) and the zwitterionic lauryldimethylamine-N-oxide
(LDAO). By combining a zwitterionic headgroup with a relatively short
contour length tail, the 10MAG/LDAO surfactant systems provides both
high biocompatibility and fast molecular tumbling for the encapsulated
macromolecule.The performance of 10MAG/LDAO was evaluated by
comparing the NMR
properties of a variety of reverse micelle encapsulated biological
macromolecules with their properties in free aqueous solution. It
is also demonstrated that 10MAG/LDAO reverse micelles provide an excellent
membrane mimetic for studying lipid-modified, membrane associated
proteins by solution NMR. An improved procedure that greatly simplifies
sample preparation by avoiding the high protein concentrations previously
required for preparing reverse micelle samples is also presented.
Experimental Section
Proteins
and tRNA were isotopically labeled and purified as described
in the Supporting Information (SI). All
proteins and tRNA used in this study were expressed without deuteration.
Surfactant
Screening
Mixtures of up to four different
surfactants featuring nonionic, ionic, or zwitterionic head groups
and different types of linear, branched, or cyclic hydrophobic tails
were screened for their ability to form stable reverse micelle solutions
in the absence of protein. The surfactants examined are listed in SI Table S1. Hexanol, which is typically present
as a stabilizing cosurfactant in reverse micelle preparations, was
not included in this initial screen. The total concentration of surfactants
was kept constant at 75 mM. Solutions were prepared in hexane. The
buffer for testing empty reverse micelle formation was 20 mM sodium
phosphate (pH 7.0) with 50 mM NaCl. Bromophenol blue (0.2 mg/mL) was
added to the buffer as a visual aid to detect reverse micelle formation.
The molar ratio of water to surfactant, also known as the water loading
or W0, was typically tested from 10 to 30. Positive surfactant
combinations were defined as those showing a single clear blue phase
and the absence of any precipitate with a W0 of at least
20. Further details may be found in the SI.
Preparation of Encapsulated Proteins and tRNA
The 10MAG/LDAO
surfactants were used in a molar percent ratio of 65%:35% and at a
total surfactant concentration of 75–150 mM as noted. The concentration
of the cosurfactant hexanol depended on the total 10MAG/LDAO surfactant
concentration and on the type of bulk alkane solvent used (pentane
or ethane). Pentane samples were prepared with 10–20 mM hexanol
at 75 mM surfactant and 20–30 mM hexanol at 150 mM surfactant.
Ethane samples were typically prepared with 30–50 mM hexanol
at 75 mM surfactant and 60–70 mM hexanol at 150 mM surfactant.
Further details may be found in the SI.Reverse micelle samples in liquid ethane were prepared using specialized
apparatus from Daedalus Innovations, LLC (Aston, PA). LDAO, 10MAG,
and hexanol were dissolved in 300 μL of d12-pentane
and transferred to the mixing chamber (1.65 mL nominal volume) of
a Daedalus Innovations RM Synthesizer unit. A volume of concentrated
protein solution yielding the desired final W0 was added
and the mixing chamber was sealed. Pressurized liquid ethane was pumped
into the mixing chamber with an Isco 65D (Lincoln, NE) syringe pump
while the sample was being stirred. The sample pressure was increased
until a distinct phase transition from a cloudy suspension to a clear
solution was observed. This generally occurred in the range of 275–450
bar though higher pressures were sometimes required for macromolecules
of larger size and/or at higher concentrations. After completion of
mixing, the sample pressure was adjusted to 14–20 bar above
the observed encapsulation (transition) pressure. The sample was then
transferred[17] to a high-pressure 3.6 mm
i.d. NMR cell rated to 1 kbar (Daedalus Innovations, LLC, Aston, PA)
for further analysis by NMR. The final sample contained 80% (v/v)
ethane and 20% (v/v) pentane.For samples prepared by the injection–evaporation
method,
water, alkane solvent, and to some degree volatile surfactants such
as hexanol are removed under a gentle stream of N2 gas.
The pentane solvent and volatile components other than water are replenished,
as indicated by 1H NMR spectra, to rebalance the surfactant
mixture. Another round of injection can then take place. Each round
takes ∼5 min. By repeating these steps the amount of encapsulated
macromolecule accumulates in the sample. See Supporting Information for further details.
NMR Spectroscopy
NMR spectra were obtained using Bruker
Avance III NMR spectrometers equipped with 5 mm cryogenically cooled
triple resonance probes. Samples were locked on the deuterated alkane
solvent. All data were collected at 25 °C. Standard two- and
three-dimensional heteronuclear NMR pulse sequences were used to assess
spectral perturbations.[1] Effective molecular
reorientation correlation times (τ̃) were estimated using the 15N-TROSY-based (TRACT)
relaxation experiment.[18] To determine τ̃, multiple portions of the amide (or imino)
region were integrated and that which gave the highest measured τ̃ is reported. Error was estimated from the
variance in integrated area for duplicate relaxation delay points.
This error was far smaller than that imposed by the rigid body approximation
assumed in the TRACT analysis. In order to more rigorously compare
the tumbling of encapsulated MBP to that in aqueous solution, 15N T1, T2 and heteronuclear NOE experiments[19] were collected at 750 and 600 MHz. For comparison of 15N T2 values, T2 relaxation of aqueous MBP was collected at 750 MHz using a TROSY-based
pulse sequence.[20]T1 and T2 experiments were collected
using six delay times with two collected in duplicate for error analysis.
Rotational correlation times were determined by fit to an isotropic
tumbling model using in-house software.[21] Spectra were processed using Felix (Accelrys, San Deigo, CA) or
in-house NMR processing software (AL NMR).[22] The SPARKY software package was used for spectral analysis and plotting
(Goddard, T.D. and Kneller, D.G. SPARKY 3, University of California,
San Francisco).
Results and Discussion
Identification and Optimization
of the 10MAG/LDAO Surfactant
System
A systematic screen was undertaken to identify promising
surfactant mixtures for reverse micelle NMR, where various mixtures
were tested for their ability to form stable “empty”
reverse micelles, as described in Materials and Methods and the SI. The screen consisted of mixtures of up to
four different commercially available surfactants featuring nonionic,
ionic, or zwitterionic headgroups and different types of linear, branched,
or cyclic hydrophobic tails (SI Table S1).
This screen identified a binary surfactant mixture of 1-decanoyl-rac-glycerol and lauryldimethylamine-N-oxide (10MAG/LDAO)
as having highly desirable properties for encapsulation of proteins
(SI Figure S1 and Table S2).The
chemical structures of 10MAG and LDAO are given in Figure 1a. The nonionic monoacylglycerol head groups of
10MAG were expected to suppress denaturing ionic interactions between
the surfactant shell and the surface of an encapsulated macromolecule
(Figure 1b). The zwitterionic character of
LDAO was also anticipated to be similarly gentle. These properties
suggested that 10MAG/LDAO should faithfully encapsulate target macromolecules
independent of their net surface charge. In addition, the relatively
short linear hydrophobic tails of 10MAG and LDAO (10 and 12 carbons,
respectively) were anticipated to favor fast molecular reorientation
of the reverse micelle particle and thus to enhance their performance
in NMR spectroscopy.In a secondary screen we fine-tuned the
molar ratio of the components
of the 10MAG/LDAO reverse micelle system for optimal NMR performance.
The molar ratio of water to surfactant is particularly important because
larger proteins require larger encapsulation volumes to form a stable
reverse micelle. Nevertheless, the total amount of water should be
limited to minimize the size and achieve the fastest reorientation
of the reverse micelle particle. Optimization of both the 10MAG/LDAO
molar ratio and the amount of hexanol was required to achieve the
desired range of water loading (W0) (Supplementary Figure 2). The hexanol cosurfactant acts as
a stabilizer of reverse micelle preparations.[15] A molar ratio of 65%:35% of 10MAG:LDAO at a total surfactant concentration
of 75 – 150 mM accommodated water loadings from 5 to 40, which
is sufficient to fully hydrate proteins up to ∼100 kDa. The
required hexanol concentration ranged from 0 to 100 mM depending on
W0 and the alkane solvent employed. These globally optimized
conditions were then used for all subsequent encapsulation studies.
Diverse proteins retain structural integrity when encapsulated
in 10MAG/LDAO
A total of seven globular, water-soluble proteins
were tested to determine the general utility of the 10MAG/LDAO surfactant
system for reverse micelle NMR. All seven of these proteins were successfully
encapsulated in 10MAG/LDAO mixtures in pentane with minimal optimization
required. W0 and the total surfactant and hexanol concentrations
were optimized to maximize encapsulation efficiency (highest encapsulated
protein concentration). The seven tested proteins range from 8.5 to
81 kDa and have isoelectric points between 4.5 and 11. Five of these
proteins, ubiquitin (Ub, 8.5 kDa, pI ≈ 6.8), cytochrome c (Cyt c, 11.7 kDa, pI ≈ 11), flavodoxin (Flv, 18.8 kDa,
pI ≈ 4.5), maltose binding protein (MBP, 40.8 kDa, pI ≈
5.2), and malate synthase G from E. coli (MSG, 81.4 kDa, pI ≈ 5.9) have been previously encapsulated
using the ionic surfactants AOT or CTAB, or a triple surfactant mixture
also containing tetraethylene glycerol monododecyl ether (C12E4).[2,13,15,16] In addition, two proteins were examined that are large by routine
solution NMR standards and have not previously been studied by reverse
micelle NMR: arginine kinase from the horseshoe crab L. polyphemus (AK, 40.2 kDa, pI ≈ 6.3) and
human aldo-keto reductase 1C2 (AKR, also known as type III 3α-hydroxysteroid
dehydrogenase, 36.7 kDa, pI ≈ 7.1).Reverse micelle samples
were prepared by the direct injection method,[26] where a specific volume of concentrated aqueous
solution of protein is directly pipettd to an alkane solution of surfactants
and mixed by vortexing (Figure 1c). Ub, Cyt c, and Flv were used to examine how the charge of the protein
affects the efficiency of encapsulation. The pH of the reverse micelle
water core was adjusted so that the net charge of the encapsulated
protein was negative for Flv and positive for Ub and Cyt c. Setting the pH of the aqueous core of reverse micelles is critically
important for achieving optimal encapsulation. The pH of the water
core is dominated by the surfactants and only marginally influenced
by the buffer employed since there are a hundred or more zwitterionic
head groups and only a handful of buffer molecules per reverse micelle.
Methods for adjusting the effective pH inside the water core of a
reverse micelle sample have been described elsewhere.[27] All three proteins were encapsulated in pentane at final
concentrations of 200 μM with W0 = 10 (Ub, Cyt c) and W0 = 12 (Flv). All reverse micelle solutions were clear, showed no
visible precipitate, and gave excellent 15N HSQC spectra
(SI Figure S3). These samples were stable
at room temperature for at least 2 months.Comparison of the
backbone chemical shifts for the protein in aqueous
solution and encapsulated in the reverse micelle was used as a quantitative
measure of structural integrity. For flavodoxin there are negligible
differences between the amide 1H and 15N chemical
shifts in aqueous solution and encapsulated in 10MAG/LDAO (histogram
in Figure 2a). A more extensive backbone chemical
shift analysis (1HN, 13Cα, 13Cβ, 13C′, 15N) showed
that reduced cytochrome c is encapsulated in 10MAG/LDAO
with little apparent structural perturbation (Figure 2b). Three proteins—AKR bound to NADP+, MBP
bound to maltose, and apo-AK—were used to assess the ability
of 10MAG/LDAO to encapsulate larger proteins. Comparison of the resolved
cross peaks of the 15N HSQC spectra obtained in pentane
and in aqueous solution indicates that the three proteins were encapsulated
in their native state (SI Figure S4). AK
was more extensively examined using triple resonance spectroscopy
of a sample prepared in ethane, which afforded better relaxation properties
and narrower lines. An excellent chemical shift correspondence was
found, demonstrating the high structural fidelity of the encapsulated
protein (Figure 2c). Finally, MSG (81 kDa)
was used with minimal optimization required to demonstrate the application
of the 10MAG/LDAO mixture to even larger proteins. The successful
encapsulation of seven globular proteins of diverse physical characteristics
with only minimal specific optimization demonstrates that 10MAG/LDAO
represents a major step forward in the general applicability of the
reverse micelle encapsulation methodology.
Figure 2
Encapsulation of diverse
proteins with high-structural fidelity
in the 10MAG/LDAO surfactant system. Proteins of distinctly different
net surface charges and molecular weights retain their bulk solution
structure as evidenced by minimal chemical shift (δ) perturbations
upon encapsulation. (a) 15N HSQC spectrum (left) of encapsulated 15N-flavodoxin (18.8 kDa, pI ≈ 4.5) in pentane acquired
at 500 MHz (1H). Histogram of gyromagnetic ratio weighted 1H and 15N chemical shift differences relative to
flavodoxin in free aqueous solution[23] (right).
(b) 15N HSQC spectrum (left) of encapsulated horse 13C,15N-cytochrome c (12 kDa, pI
≈ 11) in pentane acquired at 600 MHz (1H). Histograms
of weighted 1H and 15N (middle) and 13Cα, 13Cβ, and 13C′ (right)
chemical shift differences relative to the protein in free aqueous
solution.[24,25] (c) 15N HSQC spectrum (left)
of encapsulated 13C,15N-arginine kinase (AK)
(40.2 kDa, pI ≈ 6.3) in ethane acquired at 750 MHz (1H). Correlation of amide 1H and 15N and carbonyl 13C′ chemical shifts for AK. Encapsulated Cyt c and Flv were dissolved in pentane, and AK was dissolved
in ethane at 380 bar. All spectra were recorded at 25 °C.
Encapsulation of diverse
proteins with high-structural fidelity
in the 10MAG/LDAO surfactant system. Proteins of distinctly different
net surface charges and molecular weights retain their bulk solution
structure as evidenced by minimal chemical shift (δ) perturbations
upon encapsulation. (a) 15N HSQC spectrum (left) of encapsulated 15N-flavodoxin (18.8 kDa, pI ≈ 4.5) in pentane acquired
at 500 MHz (1H). Histogram of gyromagnetic ratio weighted 1H and 15N chemical shift differences relative to
flavodoxin in free aqueous solution[23] (right).
(b) 15N HSQC spectrum (left) of encapsulated horse13C,15N-cytochrome c (12 kDa, pI
≈ 11) in pentane acquired at 600 MHz (1H). Histograms
of weighted 1H and 15N (middle) and 13Cα, 13Cβ, and 13C′ (right)
chemical shift differences relative to the protein in free aqueous
solution.[24,25] (c) 15N HSQC spectrum (left)
of encapsulated 13C,15N-arginine kinase (AK)
(40.2 kDa, pI ≈ 6.3) in ethane acquired at 750 MHz (1H). Correlation of amide 1H and 15N and carbonyl 13C′ chemical shifts for AK. Encapsulated Cyt c and Flv were dissolved in pentane, and AK was dissolved
in ethane at 380 bar. All spectra were recorded at 25 °C.
Lowering the Molecular
Reorientation Time
A central
advantage of the reverse micelle encapsulation strategy is the ability
to manipulate the NMR relaxation properties of the macromolecule by
actively decreasing the molecular reorientation time (τm) through the use of low viscosity solvents. Though n-pentane is often initially employed to explore sample
conditions for encapsulation, the “volume penalty” imposed
by the reverse micelle particle (water core plus surfactant shell)
often outweighs gains in tumbling. Lower viscosity liquid alkanes
require preparation under pressure. Reverse micelle solutions prepared
with liquid butane or propane are often sufficient to overcome this
“volume penalty,” thereby providing shorter molecular
reorientation times for large proteins.[2] However, the minimum molecular reorientation time is achieved using
liquid ethane.[28] Although only moderate
pressure is required to liquefy ethane at room temperature (47 bar),
considerably higher pressures are needed to support homogeneous and
stable NMR samples of encapsulated proteins in condensed gases (typically
250–500 bar).[28−34] A specialized mixing apparatus is therefore employed.[17] The “volume penalty” is evident
for small proteins even when encapsulated in the ultralow viscosity
ethane, as shown by the higher τ̃ values for encapsulated ubiquitin, cytochrome c, and flavodoxin
shown in Figure 3.
Figure 3
15N-TRACT
estimates of effective molecular reorientation
times (τ̃) of six proteins
and tRNAval encapsulated in 10MAG/LDAO reverse micelles
in liquid ethane (■) or free in aqueous solution (○).
The rec[+myr] point is interpreted as a dimer. All data were recorded
at 25 °C. Error bars, as propagated from the quality of the relaxation
fits, are smaller than the size of the symbols shown. As addressed
in the text, the primary source of error in the TRACT analysis is
the inherent assumption of no internal motion.
15N-TRACT
estimates of effective molecular reorientation
times (τ̃) of six proteins
and tRNAval encapsulated in 10MAG/LDAO reverse micelles
in liquid ethane (■) or free in aqueous solution (○).
The rec[+myr] point is interpreted as a dimer. All data were recorded
at 25 °C. Error bars, as propagated from the quality of the relaxation
fits, are smaller than the size of the symbols shown. As addressed
in the text, the primary source of error in the TRACT analysis is
the inherent assumption of no internal motion.The optimal sample conditions obtained in pentane were generally
transferable to ethane although higher concentrations of the cosurfactant
hexanol were often required (see SI for
detailed sample conditions). Hexanol significantly lowers the pressure
required for forming stable reverse micelle samples, and the resulting
reduced pressure lowers the viscosity and therefore reduces the molecular
reorientation time.[34] After the sample
is fully formed inside the mixing chamber it is transferred to a specialized
NMR cell.[17] Six of the seven soluble proteins
were stably encapsulated in ethane. 15N HSQC spectra of
these proteins show excellent agreement with aqueous samples (Figures 2c, 4a, 5a, and SI Figure S1). The encapsulation
pressures required for preparation in ethane ranged from 275 to 480
bar, which are well below that typically required to significantly
perturb the structure and dynamics of folded proteins.[35] Long-term stability of the ethane samples at
room temperature ranged from more than 4 months for Flv, to 6 weeks
for MSG, MBP, Cyt c, Ub, and 1 week for AK. The samples
of AKR in ethane were not stable for more than a day. Determination
of optimal encapsulation conditions in ethane required optimization
of hexanol concentration, W0, and encapsulation
pressure for each of the proteins tested. In general, optimal conditions
were identified after only a few (∼5 or less) tests. Once optimal
conditions were identified, these proved to be highly reproducible
(τ̃ ± 2 ns). AKR proved
unstable in liquid ethane despite numerous tests for optimal conditions.
Subsequent to these tests, several other soluble, globular proteins
have been tested for encapsulation in 10MAG/LDAO mixtures. To date,
only one has been identified that does not encapsulate in 10MAG/LDAO.
Encapsulation of integral membrane proteins in 10MAG/LDAO mixtures
has not yet been examined.
Figure 4
(a) 15N HSQC spectra are shown of
MBP in aqueous solution
and encapsulated in 10MAG/LDAO reverse micelles dissolved in liquid
ethane. Spectra were collected to have comparably high signal-to-noise
for direct comparison of line widths. (b) One-dimensional normalized 15N cross sections (aqueous: dashed lines, RM: solid lines)
of three cross peaks (red arrows in a) are shown to illustrate the
narrowed line widths as a result of improved tumbling upon encapsulation.
(c) 15N T2 values were measured
for 278 and 291 sites in the encapsulated (black bars) and aqueous
(white bars) MBP samples, respectively, at 750 MHz. A histogram illustrates
the overall improvement in relaxation behavior of the encapsulated
protein as a result of improved tumbling. The difference in average T2 values (35 and 46 ms for aqueous and encapsulated
protein, respectively) corresponds to a 31% improvement and correlates
well the ∼32% decrease in rotational correlation time.
Figure 5
(a) 15N-TROSY spectra are shown of
MSG in aqueous solution
and encapsulated in 10MAG/LDAO reverse micelles in liquid ethane.
These spectra were collected with the same total acquisition time
and show comparable signal-to-noise despite the reverse micelle sample
containing approximately one-third of the protein as that of the aqueous
sample. (b) 1H cross sections of exemplary (red arrows
in a) cross peaks are shown for aqueous (red) and encapsulated (black)
MSG.
(a) 15N HSQC spectra are shown of
MBP in aqueous solution
and encapsulated in 10MAG/LDAO reverse micelles dissolved in liquid
ethane. Spectra were collected to have comparably high signal-to-noise
for direct comparison of line widths. (b) One-dimensional normalized 15N cross sections (aqueous: dashed lines, RM: solid lines)
of three cross peaks (red arrows in a) are shown to illustrate the
narrowed line widths as a result of improved tumbling upon encapsulation.
(c) 15N T2 values were measured
for 278 and 291 sites in the encapsulated (black bars) and aqueous
(white bars) MBP samples, respectively, at 750 MHz. A histogram illustrates
the overall improvement in relaxation behavior of the encapsulated
protein as a result of improved tumbling. The difference in average T2 values (35 and 46 ms for aqueous and encapsulated
protein, respectively) corresponds to a 31% improvement and correlates
well the ∼32% decrease in rotational correlation time.(a) 15N-TROSY spectra are shown of
MSG in aqueous solution
and encapsulated in 10MAG/LDAO reverse micelles in liquid ethane.
These spectra were collected with the same total acquisition time
and show comparable signal-to-noise despite the reverse micelle sample
containing approximately one-third of the protein as that of the aqueous
sample. (b) 1H cross sections of exemplary (red arrows
in a) cross peaks are shown for aqueous (red) and encapsulated (black)
MSG.The 15N-TRACT experiment,[18] which measures the relaxation rates of the α
and β spin
states of the amide 15N, was used to estimate the protein’s
effective molecular reorientation time (τ̃m). Although this method systematically underestimates the true molecular
reorientation time (τm), it provides a rapid method
for comparing the tumbling of proteins in reverse micelle and aqueous
solutions. The error that results from the rigid body assumption inherent
in the TRACT analysis is far greater than the error resulting from
the fits to the relaxation profiles. In general, the errors resulting
from the quality of the relaxation fits are on the order of the sizes
of the symbols shown in Figure 3. Comparing
the τ̃m values shows that macromolecules larger
than ∼20 kDa can be made to tumble faster than in aqueous solution
when encapsulated and prepared in liquid ethane (Figure 3). For example, encapsulated MBP and MSG showed approximately
50% reduction in τ̃. However,
it is important to note that, because the TRACT experiment underestimates
the true rotational correlation time, the actual advantage may be
more modest. To examine this, the rotational correlation time of MBP
encapsulated in 75 mM 10MAG/LDAO was determined with a full suite
of 15N-relaxation experiments to be 15.5 ns.[19] This corresponds to a markedly slower tumbling
behavior than indicated by the TRACT analysis (8.9 ns), but a similar
discrepancy was noted previously for the TRACT estimation of tumbling
for aqueous MBP.[16]Based on this
more rigorous measurement of encapsulated MBP tumbling
in ethane, the true improvement in rotational correlation time (15.5
ns for RM versus 23 ns for aqueous solution[36]) is ∼32%.It should also be noted that some trade-off
exists between optimal
encapsulation efficiency (i.e., concentration of protein in the final
sample) and molecular tumbling. In general, increasing the amount
of surfactant in the reverse micelle system permits encapsulation
of higher concentrations of protein, but the tumbling improvement
at high surfactant concentrations is slightly reduced and there is
the potential for partial alignment of reverse micelle systems at
high surfactant concentrations.[37]As an example, the optimal sample conditions for MBP in ethane
were determined to be at 75 mM total surfactant with 100 mM hexanol.
Because AK is more difficult to concentrate in aqueous solution, higher
surfactant concentrations (100–150 mM) and higher water loading
(W0 = 20 versus 12 for MBP) were required
for this protein in order to achieve appropriate encapsulated concentrations
(80–100 μM) for efficient collection of NMR data. As
shown in Figure 3, the tumbling of MBP in ethane
is better than that of AK due to this difference in surfactant conditions.
The spectral improvements in tumbling are demonstrated in Figure 4 for MBP encapsulated in ethane as compared to the
aqueous protein. The 15N HSQC spectrum of encapsulated
MBP shows improved resolution due to narrowing of the resonance lines.
This narrowing can more clearly be seen in the one-dimensional spectra
given. In addition, the distribution of 15N T2 values is shifted markedly toward longer relaxation
times for the encapsulated protein, demonstrating a general improvement
in the relaxation properties of the encapsulated protein. This T2 advantage not only translates to improved
line widths but also provides substantial gains in coherence transfer
efficiencies in multidimensional NMR experiments.[1]It is also important to consider that the sensitivity
of a modern
cryoprobe with RM samples is markedly better than that with aqueous
solutions due to the low conductivity of the reverse micelle solution.[38] This results in improved signal-to-noise per
unit of protein in the encapsulated sample. In combination with the
improved tumbling and resultant line narrowing and improved coherence
transfer, encapsulation can produce substantially improved signal-to-noise.
This is particularly true for larger proteins. For example, the spectra
shown in Figure 5 demonstrate that comparable
signal-to-noise is obtained for encapsulated MSG as compared to the
aqueous condition using the same amount of signal averaging (i.e.,
identical collection time) but less than half the protein concentration
of the aqueous sample. In summary, the successful encapsulation of
a diverse set of globular proteins up to 81 kDa in ultralow viscosity
ethane shows that 10MAG/LDAO is a general surfactant system for comprehensive
reverse micelle NMR.
Concentration by Injection–Evaporation
Method
The direct injection method (Figure 1c) is
the simplest approach for preparing homogeneous solutions of encapsulated
macromolecules. Such solutions are usually prepared under water-limited
conditions to obtain the desired water loading (W0) and fast molecular tumbling. Thus, the concentration
of protein in the injected solution defines the final concentration
of encapsulated protein. If the protein cannot be sufficiently concentrated,
the direct injection method will fail to provide a sufficiently high
concentration of encapsulated protein to allow facile multidimensional
NMR spectroscopy. For example, using a 1 mM protein stock solution
would result in a final concentration of encapsulated protein of only
18 μM with W0 of 10 and 100 mM surfactant.To address this limitation, a method was developed that allows
fewer soluble macromolecules to be encapsulated by employing successive
rounds of injection of a dilute solution followed by evaporation of
excess water. We call this procedure the injection–evaporation method. The injection–evaporation method is illustrated using
a solution of 500 μM flavodoxin and performing seven rounds
of protein injection and water evaporation (Figure 6).
Figure 6
The injection–evaporation method of encapsulation eliminates
the requirement for millimolar protein concentrations. (a) Reference 15N HSQC spectrum of 500 μM Flv in aqueous solution.
(b) 15N HSQC spectrum of 200 μM encapsulated Flv
dissolved in pentane prepared by direct injection using 6.3 mM Flv
(bottom) and prepared by seven rounds of injection–evaporation
using a 500 μM Flv stock solution (top). (c) The effective tumbling
rate of Flv can be greatly increased by subsequent solvent exchange
to ethane. All data were recorded at 25 °C and at 500 MHz (1H) and processed identically.
The injection–evaporation method of encapsulation eliminates
the requirement for millimolar protein concentrations. (a) Reference 15N HSQC spectrum of 500 μM Flv in aqueous solution.
(b) 15N HSQC spectrum of 200 μM encapsulated Flv
dissolved in pentane prepared by direct injection using 6.3 mM Flv
(bottom) and prepared by seven rounds of injection–evaporation
using a 500 μM Flv stock solution (top). (c) The effective tumbling
rate of Flv can be greatly increased by subsequent solvent exchange
to ethane. All data were recorded at 25 °C and at 500 MHz (1H) and processed identically.The first round of protein injection yielded an encapsulated
flavodoxin
concentration of ∼30 μM. After the seventh round the
concentration was 200 μM. In this example, this allows for a
12-fold reduction in the starting protein concentration (6.3 mM).
The 15N HSQC spectra of encapsulated flavodoxin prepared
by injection–evaporation or direct injection were identical
(Figure 6b). Furthermore, the flavodoxin sample
prepared by the injection–evaporation method could be redissolved
in liquid ethane after partial evaporation of the pentane solvent
(Figure 6). Thus, the advantages of the injection–evaporation
method can be combined with the improved molecular tumbling offered
by ultralow viscosity ethane.
10MAG/LDAO as a Membrane
Mimetic for Lipid-Modified Proteins
Post-translational lipid
modification of proteins, such as attachment
of myristate or isoprene groups, is responsible for a variety of specialized
functions including localization at membranes or hydrophobic molecular
switch-like behavior.[39] Exposure of the
hydrophobic lipid to water can lead to poor solution behavior that
severely compromises structural studies. Consequently, high-resolution
structures of lipid-modified proteins in the putative membrane-anchored
state obtained using standard NMR spectroscopy or crystallography
are surprisingly rare. It was recently shown that myristoylated recoverin
and myristoylated HIV matrix protein could be stably encapsulated
in CTAB/hexanol reverse micelles in the lipid-extruded state.[5] However, CTAB is cationic and has electrostatic
properties different from those of natural lipid bilayers, and this
mismatch may become limiting. In contrast, the 10MAG/LDAO surfactant
system more closely resembles the lipids of biological membranes.
The zwitterionic LDAO headgroup mimics the phosphatidylcholine headgroup,
and 10MAG is a glycerol group esterified to a fatty acid.The
23 kDa myristoylated humanrecoverin (Rec[+myr]), which acts as a
Ca2+ sensor in the visual system,[40] was used to test if 10MAG/LDAO could support lipid-anchored proteins.
The myristoyl group is extruded upon calcium binding.[40] Calcium-loaded Rec[+myr] was efficiently encapsulated at
100 μM in 10MAG/LDAO in both pentane and ethane at a water loading
of 12. The 15N HSQC spectra of encapsulated Rec[+myr] were
very similar to spectra of natively folded, Ca2+-bound,
myristoyl-extruded protein (see refs (5 and 40) and Figure 7). The 15N-TRACT measurements
showed much faster molecular tumbling in ethane than in pentane (τ̃m = 11.7 and 18.8 ns, respectively). Interestingly, the τ̃m values suggested that two Rec[+myr] molecules were encapsulated
in occupied reverse micelles. A similar observation was made in the
previous study of Rec[+myr] encapsulated in CTAB/hexanol,[5] suggesting that the protein in the lipid-extruded
state is a dimer. The physiological significance of this apparent
homodimerization remains to be established.[41]
Figure 7
10MAG/LDAO
provides a membrane mimetic environment for NMR spectroscopy
of membrane-anchored proteins. 15N HSQC 600 MHz spectrum
of encapsulated calcium-saturated myristoylated recoverin. The dashed
line box highlights two cross peaks that are assigned to two Gly residues
involved in stabilizing the Ca2+-bound, myristoyl-extruded
protein conformation.[5,40] Sample prepared in ethane at
100 μM Rec[+myr] and W0 = 12 in
100 mM 10MAG/LDAO at 450 bar.
10MAG/LDAO
provides a membrane mimetic environment for NMR spectroscopy
of membrane-anchored proteins. 15N HSQC 600 MHz spectrum
of encapsulated calcium-saturated myristoylated recoverin. The dashed
line box highlights two cross peaks that are assigned to two Gly residues
involved in stabilizing the Ca2+-bound, myristoyl-extruded
protein conformation.[5,40] Sample prepared in ethane at
100 μM Rec[+myr] and W0 = 12 in
100 mM 10MAG/LDAO at 450 bar.
Encapsulation of RNA
DNAs and RNAs represent a significant
challenge to solution NMR spectroscopy because they are built from
only four different nucleotides and the proton and carbon resonances
are highly overlapped due to their narrow chemical shift ranges.[42−45]The 27 kDa natively modified valine tRNA (tRNAval) from E. coli(46) was employed here to evaluate the 10MAG/LDAO surfactant
system for NMR studies of nucleic acids. The structure and dynamics
of tRNAval have been extensively studied,[47] and it therefore serves as a model system for medium-sized
RNAs. 15N-labeled tRNAval was encapsulated at
100 μM in 10MAG/LDAO reverse micelles in both pentane and ethane
using the procedures developed above for proteins. The imino region
of the 15N HSQC spectrum of encapsulated tRNAval is indicative of a natively folded macromolecule using a buffer
that included 5 mM Mg2+ (Figure 8).
Figure 8
High-fidelity encapsulation of tRNAval. 15N HSQC spectra of the imino region of tRNAval acquired
at 500 MHz (1H) (a) aqueous solution at 200 μM with
16 scans per FID and (b) encapsulated in 150 mM 10MAG/LDAO and dissolved
in ethane at 450 bar at W0 = 9 at 100
μM with 32 scans per FID. The dashed line boxes highlight amino
cross peaks, folded in the 15N chemical shift dimension,
showing somewhat improved signal-to-noise for the encapsulated RNA
compared to RNA tumbling free in aqueous solution. The tRNA was prepared
in 10 mM sodium phosphate (pH 6.8), 80 mM NaCl, 5 mM MgCl2, 0.1 mM EDTA. Recorded at 25 °C.
Interestingly, amino resonances were sharper and consequently
better
resolved for the tRNA encapsulated in ethane (at relatively low water
loading W0 = 9) than in free solution
(boxes in Figure 8). This is partially related
to the reduced effective molecular reorientation time (τ̃m = 7.0 and 9.0 ns, for the encapsulated and aqueous tRNAs,
respectively). In addition, many A, C, and G amino protons are in
the intermediate exchange regime in aqueous solution due to either
rotation about the C–N bond, which has partial double bond
character, or through the effects of hydrogen exchange with water.
Hydrogen exchange chemistry is slowed in the reverse micelle,[10,11,48,49] and the corresponding reduction in hydrogen exchange rates will
tend to sharpen the amino hydrogen resonances. Furthermore, the relatively
high effective viscosity of the water core of reverse micelles[48−50] would also tend to slow conformational exchange processes toward
the slow exchange time regime. Conversely, the imino protons are in
the slow exchange regime in bulk solution, and their resonances are
largely unaffected by the slowed hydrogen exchange chemistry or the
increased viscosity of the reverse micelle water core.[51]High-fidelity encapsulation of tRNAval. 15N HSQC spectra of the imino region of tRNAval acquired
at 500 MHz (1H) (a) aqueous solution at 200 μM with
16 scans per FID and (b) encapsulated in 150 mM 10MAG/LDAO and dissolved
in ethane at 450 bar at W0 = 9 at 100
μM with 32 scans per FID. The dashed line boxes highlight amino
cross peaks, folded in the 15N chemical shift dimension,
showing somewhat improved signal-to-noise for the encapsulated RNA
compared to RNA tumbling free in aqueous solution. The tRNA was prepared
in 10 mM sodium phosphate (pH 6.8), 80 mM NaCl, 5 mM MgCl2, 0.1 mM EDTA. Recorded at 25 °C.The effect of slowed hydrogen exchange chemistry on the line
shape
of exchangeable hydrogens has been observed for encapsulated proteins
before, particularly in the ability to resolve NOE cross peaks to
hydroxyl hydrogens of serine and threonine residues.[11,52] These hydroxyl hydrogens exchange far too rapidly in bulk solution
for such signals to be observed, but they are visible upon encapsulation.
At water loadings less than ∼20, the water dynamics and hydrogen
exchange rates are considerably slower than in bulk water.[10,11,48,49] Many RNAs require divalent ions for proper folding and function,
with Mg2+ generally being the physiologically relevant
ion.[53] The zwitterionic character of the
10MAG/LDAO surfactant system means that neither the RNA nor the metal
ions required for correct folding/function of the macromolecule are
likely to interact to any significant extent with the surfactant.
Furthermore, since nucleic acids all carry a large number of negative
charges, they will have similar overall electrostatic surface charges,
and encapsulation conditions that work for one nucleic acid, such
as tRNAval studied here, should be readily applicable to
other nucleic acids.
Conclusions
A new binary surfactant
system for high-resolution solution NMR
studies of encapsulated biological macromolecules dissolved in low
viscosity fluids has been developed. The performance of 10MAG/LDAO
in reverse micelle NMR has been validated with respect to encapsulation
efficiency (yield), fidelity, and molecular tumbling behavior using
a set of seven proteins and a tRNA. 10MAG/LDAO therefore represents
a single surfactant system that can encapsulate with high structural
fidelity a broad range of different target macromolecules with molecular
weights at least up to 81 kDa. This simplifies the process of preparing
reverse micelle NMR samples, which is often plagued by trial and error
searches for optimal encapsulation conditions. It has been found that
10MAG/LDAO may be employed with minimal a priori assumptions
about the properties of a given target protein or RNA to obtain significant
reductions in molecular reorientation times at ambient temperature.
This is a significant advantage. Results presented here indicate that
proteins in the 40 kDa range are rendered completely accessible to
the full battery of triple resonance spectroscopy without the limitations
imposed by extensive deuteration or use of the TROSY effect. It should
also be noted that the dielectric properties of reverse micelle solutions
are more optimal for cryogenic probe technology than standard aqueous
samples and can provide a 50–100% gain in sensitivity.[38]The ability of 10MAG/LDAO to faithfully
encapsulate a range of
protein sizes and charge states clearly originates from the favorable
physicochemical properties of the two surfactant headgroups—a nonionic monoacylated glycerol group in 10MAG and a zwitterionic amine-N-oxide group in LDAO.
The nonionic surfactant content (65 mol % 10MAG) combined with the
zwitterionic character of LDAO mixture reduces charge–charge
interactions in much the same spirit as the triple surfactant system
derived from mixtures of anionic, cationic, and neutral polyether
surfactants.[13] Here, however, the relatively
short contour length of the LDAO and 10MAG minimizes the size of the
resulting particle and thereby maximizes the effective tumbling time
of the encapsulated macromolecule. The surfactant combination of 10MAG
and LDAO also provides a very favorable environment for encapsulating
proteins of poor solution properties, such as lipid-modified proteins.
It also faithfully encapsulates tRNA. Because all nucleic acids have
an overall negative electrostatic surface, it is likely that encapsulation
by the 10MAG/LDAO surfactant system will generally not be sensitive
to the precise sequence of the RNA (or DNA). Finally, the injection–evaporation
method allows for the preparation of reverse micelle samples using
relatively dilute protein solutions and represents a significant advantage
as it avoids the need for concentrated aqueous solutions of the target
macromolecule. In conclusion, 10MAG/LDAO provides many aspects of
an optimal surfactant system for solution NMR of encapsulated proteins
dissolved in low viscosity fluids. It relieves the experimental problems
that exist with the currently employed surfactants AOT, CTAB, and
triple surfactant mixtures. We anticipate that the 10MAG/LDAO surfactant
system will find broad utility in structural and biophysical studies
of encapsulated proteins by high-resolution reverse micelle NMR.
Authors: Nathaniel V Nucci; Bryan S Marques; Sabrina Bédard; Jakob Dogan; John M Gledhill; Veronica R Moorman; Ronald W Peterson; Kathleen G Valentine; Alison L Wand; A Joshua Wand Journal: J Biomol NMR Date: 2011-07-12 Impact factor: 2.835
Authors: William K Myers; Xianzhong Xu; Congmin Li; Jens O Lagerstedt; Madhu S Budamagunta; John C Voss; R David Britt; James B Ames Journal: Biochemistry Date: 2013-08-16 Impact factor: 3.162
Authors: Kathleen G Valentine; Ronald W Peterson; Jamil S Saad; Michael F Summers; Xianzhong Xu; James B Ames; A Joshua Wand Journal: Structure Date: 2010-01-13 Impact factor: 5.006
Authors: N A Farrow; R Muhandiram; A U Singer; S M Pascal; C M Kay; G Gish; S E Shoelson; T Pawson; J D Forman-Kay; L E Kay Journal: Biochemistry Date: 1994-05-17 Impact factor: 3.162
Authors: Nathaniel V Nucci; Brian Fuglestad; Evangelia A Athanasoula; A Joshua Wand Journal: Proc Natl Acad Sci U S A Date: 2014-09-08 Impact factor: 11.205
Authors: Brian Fuglestad; Bryan S Marques; Christine Jorge; Nicole E Kerstetter; Kathleen G Valentine; A Joshua Wand Journal: Methods Enzymol Date: 2018-12-10 Impact factor: 1.600
Authors: Bryan S Marques; Nathaniel V Nucci; Igor Dodevski; Kristina W C Wang; Evangelia A Athanasoula; Christine Jorge; A Joshua Wand Journal: J Phys Chem B Date: 2014-02-19 Impact factor: 2.991
Authors: Kathleen G Valentine; Guinevere Mathies; Sabrina Bédard; Nathaniel V Nucci; Igor Dodevski; Matthew A Stetz; Thach V Can; Robert G Griffin; A Joshua Wand Journal: J Am Chem Soc Date: 2014-02-05 Impact factor: 15.419