We describe a new labeling method that allows for full protonation at the backbone Hα position, maintaining protein side chains with a high level of deuteration. We refer to the method as alpha proton exchange by transamination (α-PET) since it relies on transaminase activity demonstrated here using Escherichia coli expression. We show that α-PET labeling is particularly useful in improving structural characterization of solid proteins by introduction of an additional proton reporter, while eliminating many strong dipolar couplings. The approach benefits from the high sensitivity associated with 1.3 mm samples, more abundant information including Hα resonances, and the narrow proton linewidths encountered for highly deuterated proteins. The labeling strategy solves amide proton exchange problems commonly encountered for membrane proteins when using perdeuteration and backexchange protocols, allowing access to alpha and all amide protons including those in exchange-protected regions. The incorporation of Hα protons provides new insights, as the close Hα-Hα and Hα-HN contacts present in β-sheets become accessible, improving the chance to determine the protein structure as compared with HN-HN contacts alone. Protonation of the Hα position higher than 90% is achieved for Ile, Leu, Phe, Tyr, Met, Val, Ala, Gln, Asn, Thr, Ser, Glu, Asp even though LAAO is only active at this degree for Ile, Leu, Phe, Tyr, Trp, Met. Additionally, the glycine methylene carbon is labeled preferentially with a single deuteron, allowing stereospecific assignment of glycine alpha protons. In solution, we show that the high deuteration level dramatically reduces R2 relaxation rates, which is beneficial for the study of large proteins and protein dynamics. We demonstrate the method using two model systems, as well as a 32 kDa membrane protein, hVDAC1, showing the applicability of the method to study membrane proteins.
We describe a new labeling method that allows for full protonation at the backbone Hα position, maintaining protein side chains with a high level of deuteration. We refer to the method as alpha proton exchange by transamination (α-PET) since it relies on transaminase activity demonstrated here using Escherichia coli expression. We show that α-PET labeling is particularly useful in improving structural characterization of solid proteins by introduction of an additional proton reporter, while eliminating many strong dipolar couplings. The approach benefits from the high sensitivity associated with 1.3 mm samples, more abundant information including Hα resonances, and the narrow proton linewidths encountered for highly deuterated proteins. The labeling strategy solves amide proton exchange problems commonly encountered for membrane proteins when using perdeuteration and backexchange protocols, allowing access to alpha and all amide protons including those in exchange-protected regions. The incorporation of Hα protons provides new insights, as the close Hα-Hα and Hα-HN contacts present in β-sheets become accessible, improving the chance to determine the protein structure as compared with HN-HN contacts alone. Protonation of the Hα position higher than 90% is achieved for Ile, Leu, Phe, Tyr, Met, Val, Ala, Gln, Asn, Thr, Ser, Glu, Asp even though LAAO is only active at this degree for Ile, Leu, Phe, Tyr, Trp, Met. Additionally, the glycine methylene carbon is labeled preferentially with a single deuteron, allowing stereospecific assignment of glycine alpha protons. In solution, we show that the high deuteration level dramatically reduces R2 relaxation rates, which is beneficial for the study of large proteins and protein dynamics. We demonstrate the method using two model systems, as well as a 32 kDa membrane protein, hVDAC1, showing the applicability of the method to study membrane proteins.
The study of proteins by nuclear magnetic resonance (NMR) has been
continuously evolving to improve sensitivity in order to resolve signals in
multidimensional spectra, which serve as the basis for studies of structure and
dynamics. For large proteins that tumble slowly in solution, as well as for proteins
in the solid state, a high level of deuteration with introduction of selective
protons is used to improve proton relaxation, and therefore narrow lines, by
elimination of strong proton–proton dipolar couplings.Proton detected magic-angle spinning (MAS) NMR studies have employed
different combinations of spinning frequency and deuteration to optimize sensitivity
and resolution (Andreas et al. 2015;
Zhang et al. 2015; Wang and Ladizhansky
2014; Brown 2012; Chevelkov et al. 2006; Zhou et al. 2007; Lewandowski et al. 2011; Akbey et al. 2010). Currently, many applications of proton detected MAS NMR
are applied at about 60 kHz with 1.3 mm rotors, a spinning frequency that for fully
protonated samples is not enough to average the strong network of1H–1H dipolar couplings.
This results in proton line broadening and about 200–300 Hz proton linewidths
(Andreas et al. 2015). The advantage of
this spinning frequency is that narrow lines are observed at high sensitivity when
selected sites are labeled to 100% incorporation of protons, while others are
deuterated.In the most straightforward approach, Escherichia coli expression in D2O is
followed by exchange with H2O/D2O to
produce a protein with a specific protonation level at amides, and perdeuteration at
non-exchangeable sites (Chevelkov et al. 2006; Akbey et al. 2010; Lemaster 1990). A protonation level of 100% at amide positions results in high
resolution when using 40–60 kHz MAS in microcrystalline samples, (Lewandowski et al.
2011) enabling structure
determination based on backbone resonances (Zhou et al. 2007).Accessing aliphatic protons is still an area of active development.
Sidechain protons can be selectively introduced using metabolic precursors, which
has the advantage that a single isotopomer is typically present and deuterium
isotope shifts do not result in broadening, even at 100% protonation of the selected
sites. In various ways, methyl groups of I, L, V, T, A can be incorporated
(Tugarinov et al. 2003; Isaacson et al.
2007; Velyvis et al. 2012). Exquisite control of labeling can be
afforded using a synthetic approach known as SAIL labeling, with the only downside
being the high cost, which has typically restricted applications to labeling only
selected amino acid types in cell free expression systems (Kainosho et al.
2006). For fully protonated
samples, high magnetic fields and very fast MAS ~ 100 kHz are required to
sufficiently narrow proton resonances. At lower spinning frequencies, deuteration is
still required, and approaches to resolve aliphatic protons involve using mixtures
of H2O and D2O during protein
expression, along with combinations of protonated or deuterated carbon sources such
as glycerol or glucose (Lemaster 1990;
Asami et al. 2010). While utilizing the
residual protons in perdeuterated samples results in exquisite spectra (Agarwal and
Reif 2008), the low labeling level
severely limits the ability to measure proton–proton distances. At higher proton
concentrations, the carbon resonances are broadened due to deuterium isotope shifts
(Asami et al. 2012). Although this is a
small effect for Hα, since only one proton is directly attached, it would still be
desirable to limit the protons introduced in the sidechains, since such protons
broaden the alpha resonance, and are a magnetization sink during proton–proton
transfer.We therefore sought a strategy that would allow labeling of alpha
protons in E. coli at a cost that allows
widespread adoption of the approach for structure determination and dynamics
investigations. Previously, an approach for Hα labeling was introduced, where the
proton was chemically exchanged in a deuterated amino acid mixture, producing a D/L
mixture of amino acids, the L portion of which can be utilized directly by bacteria
(Yamazaki et al. 1997). Although this
previous method was successful, the alpha proton incorporation level was a problem
for several amino acids, and serine and threonine were lost during the acetylation
and deacetylation reaction. d-amino acids may
also inhibit bacterial growth at high concentrations (Hishinuma et al. 1969; Bardaweel 2014). It was also noted that during growth on deuterated amino
acid media (O’Brien et al. 2018; Fiaux
et al. 2004), exchange of amide
moieties occurs, but results in only 10–50% incorporation of alpha protons for
hydrophobic residues (Löhr et al. 2003).We show an alternative approach that results in up to 100% Hα
incorporation by supplying keto acids. The keto acids are converted by E. coli transaminases to the respective amino acids,
while adding a proton at the alpha position from the water pool. This avoids any
problems due to racemic amino acid mixtures, since the correct l-amino acids are generated enzymatically. The major
pathways of amino acid synthesis from glucose and glycerolcarbon sources are
depicted in Fig. 1a for E. coli. Keto acids are often the direct precursor to
an amino acid, indicating that provided a source of keto acids, protons can be
introduced via transaminase activity (Fig. 1b), a method hereafter referred to as ‘alpha proton exchange by
transamination’ (α-PET). This method, as with any where the growth medium is based
on H2O, results in protonation of the amide position during
protein expression, such that both the alpha and amide positions of the protein are
protonated.
Fig. 1
Amino acid metabolic pathways and the different enzymatic
stages of the α-PET labeling method. The metabolic pathways of the
TCA cycle are shown in a. Inb, the transamination reaction
is shown, which is the main route for Hα incorporation. In c, the generation of α-keto acids from
amino acids by the enzyme LAAO is shown. d Shows the main biosynthesis pathways of glycine
with the observed stereospecific labeling
Amino acid metabolic pathways and the different enzymatic
stages of the α-PET labeling method. The metabolic pathways of the
TCA cycle are shown in a. Inb, the transamination reaction
is shown, which is the main route for Hα incorporation. In c, the generation of α-keto acids from
amino acids by the enzyme LAAO is shown. d Shows the main biosynthesis pathways of glycine
with the observed stereospecific labelingSome transaminases are amino acid-specific, like the glutamate–pyruvate
aminotransferase that transfers the NH3 from glutamate to
pyruvate forming alanine and α-ketoglutarate (Kim et al. 2010). Others are less specific for their
substrate, such as branched-chain-amino-acid transaminase (BCAT) involved in
leucine, isoleucine and valine anabolism (Rudman and Meister 1953). E.
coli has a high diversity of such transaminase enzymes, resulting in
effective labeling for the majority of residue types.We generated keto acids by l-amino acid oxidase (LAAO) treatment of a commercial growth medium that
is primarily comprised of 2H,13C, 15N-amino acids. LAAO
enzymes are found in many organisms (Hossain et al. 2014), with different specificity for the substrate amino acids
(Nuutinen et al. 2012; Sun et al.
2010). We chose as the enzyme
source a crude snake venom containing LAAO, which can be applied directly to the
commercial growth medium (Fig. 1c).
Additional metabolic pathways might also be important, for example, we observed
stereospecific labeling of glycine, which can occur through transaminase, but also
by conversion of serine and threonine (Fig. 1d).Here we show successful introduction of alpha protons for 13 amino
acids, with a high deuteration level that improves transverse relaxation rates in
both solid and liquid samples.
Methods
L-amino acid oxidase stock
10 mg of LAAO powder (crude extract from the snake venom ofCortalus admanteus, Sigma Aldrich) were
dissolved in 1 ml of 100 mM sodium phosphate, 100 mM KCl at pH 7.4. The solution
can be kept at 4 °C for several weeks.
Preparation of keto acid mix
The amino acid mix (SILEX rich growth media as powder) from
Silantes was used as starting material. To obtain keto acids, 1 g of powder was
dissolved in 150 ml of H2O. To this mixture, 10 µl of
bovine liver catalase solution was added at 0 and 12 h (Sigma, fivefold water
dilution from crystalline suspension, 10,000–40,000 units/mg). In total, 3–4 mg
of l-amino acid oxidase (LAAO, Sigma) was
used per gram powder media, added in equal amounts at 0, 3, 6, 9 and 12 h. The
solution was kept shaking at 37 °C for 1 day, then lyophilized.
Protein expression
All proteins were expressed inE. coli BL21(DE3). Two NMR model proteins
were used, ubiquitin in solution, and microcrystalline chicken alpha-spectrin
SH3 (SH3). In addition, the 32 kDa voltage dependent anion channel (VDAC), a
beta barrel membrane protein was prepared in lipid bilayers.For α-PET ubiquitin, a change of medium was used prior to
expression. E. coli cells were grown in 1 L
of M9 using 1 g/L of 15N ammonium chloride and 4 g/L
of 13C glucose until the
OD600nm reached 0.6–0.8. Then cells were spun down at
7000 g at 4 °C for 20 min. The cells were re-suspended in 1L of M9 salts with
4 g of Silantes media either as received, or treated with LAAO. The cells were
adapted to the new media for 30 min before induction at
OD600nm = 0.8 with 1 mM of isopropyl
β-D-1-thiogalactopyranoside (IPTG). Ubiquitin samples, including a13C, 15N-ubiquitin
reference sample were purified as previously described (Lazar et al.
1997).Using this media exchange protocol, four different samples of
ubiquitin were produced, two using 2H Silantes powder
treated with LAAO or as received and two others using2H, 13C,15N Silantes powder again LAAO treated or as
received.Two samples of α-PET SH3 were produced, a media-exchanged sample
(as for ubiquitin), and a second α-PET SH3 grown in the presence of glucose.
Specifically, the growth was started with a low concentration of 1.25 g/L12C-glucose in 800 ml of M9 media. Cells were
grown until OD600nm reached 0.6–0.8. Then 4 g/L of
treated Silantes media solubilized in 200 ml of H2O were
added. The culture was switched to 30 °C for about 30 min until
OD600nm = 0.7–0.8, and protein expression was induced
using 1 mM IPTG. A reference sample (13C,15N-SH3) was expressed and all samples purified
as previously described (Pauli et al. 2000). In brief, the protein was purified by anion exchange
chromatography (Q-TRAP, GE Healthcare) followed by gel filtration on a
Superdex-75 column (GE Healthcare). The purified protein sample was extensively
dialyzed against H2O–HCl pH 3.5 for 2 days (exchanging
the dialysis solution every 12 h). The protein was then concentrated (Amicon,
3.5 kDa cut-off) to 20 mg/ml before lyophilization. The samples were resuspended
in H2O–HCl pH 3.5 or D2O-HCl pH
3.5 at 15–20 mg/ml. Microcrystals were obtained using a pH shift protocol as
previously described (Chevelkov et al. 2007).α-PET VDAC was expressed at 37 °C in dilute glucose media (as for
SH3) and purified and reconstituted in 2D crystalline arrays as previously
described (Eddy et al. 2012; Dolder
et al. 1999). The E73V, C127A,
C232S variant of human VDAC was used.
NMR measurements
Solution NMR data were recorded in a 400 MHz Bruker spectrometer at
298 K. We recorded a set of spectra to characterize the labeling pattern:15N-HSQC, 13C-HSQC in
D2O,1H–15N TOCSY-HSQC, and
1D proton spectra. Quantification of Hα was done from a13C-HSQC spectrum at 950 MHz at 310 K. Transverse
relaxation rates (R2) were measured at 277 K using a 600 MHz Bruker spectrometer
equipped with a 5 mm cryoprobe.The black spectrum of Fig. 6a was recorded at 105 kHz MAS on a 950 MHz Bruker
spectrometer using a 0.7 mm HCND probe. All other solid state NMR data were
recorded on an 800 MHz Bruker spectrometer using a 1.3 mm narrow bore HCN probe
and spinning at 55 kHz MAS. We recorded cross-polarization based (H)NH, (H)CH,
and (H)CANH, (H)NCAHA for resonance assignment of VDAC and SH3. We measured
contacts in H(H)CH, H(H)NH spectra (SH3) and (H)C(HH)CH (VDAC) using RFDR for
the proton–proton mixing. The spectra were apodized with a squared cosine
function (details in Table S6). The data analysis was performed using CcpNMR and
Sparky.
Fig. 6
Identification of a cross beta strand contact
(F99–I114 Hα) in the beta barrel membrane protein VDAC in lipid
bilayers. a Shows, the
comparison of the (H)CH spectrum at 105 kHz on a 950 MHz
spectrometer (black) and at 55 kHz on an 800 MHz spectrometer
(red). b Shows a13C–15N
projection of a (H)NCAHA spectrum. F99 Hα is assigned from the
strip comparing (H)NCAHA (green) and (H)N(CO)CAHA (brown). Inc and e, the contact is shown on the X-ray structure
of mouse VDAC (pdb: 2jk4). d
Shows the F99–I114 cross-peak in the carbon–carbon 2D plane of
the (H)C(HH)CH spectrum at the proton frequency of F99,
4.72 ppm
Results and discussion
Characterization of the labeling pattern
To measure labeling patterns on an amino acid specific basis, we
recorded a 13C HSQC spectrum and integrated isolated
peaks in the alpha region (Fig. 2). The
level of Hα incorporation was determined assuming ideal incorporation of
hydrophobic residues, based on complete reaction with LAAO. The uncorrected and
T2 corrected determinations are shown in Tables S2
and S3, respectively. A 15N-TOCSY (Fig. 3) was recorded using a medium-range mixing time
(75 ms) to assess suppression of sidechain protons. This spectrum cannot be used
in a quantitative manner due to the potential for several isotopomers,
differential relaxation, and relayed transfer. However, since the beta protons
are relatively isolated from these effects, we could show effective suppression
for most amino acid types. Figure 2
shows selected strips for each of the amino acid types of ubiquitin; the1H–15N TOCSY-HSQC of
α-PET Ubiquitin (red) is compared to the 15N,13C-labeled reference sample (black). The TOCSY
was implemented with MLEV-17 mixing (Bax and Davis 1985). The Hα proton was detectable for 13
of the 16 (non-proline) amino acid types present in the ubiquitin sequence. Only
lysine, arginine and histidine remained deuterated at Hα. This can be explained
for lysine because Cortalus admanteus LAAO is
not able to use it as substrate (Fig S1), and the deuterated amino acids are
taken up in E. coli, while endogenous
synthesis is suppressed (Zhou et al. 1998). Although LAAO showed some activity for arginine and
histidine, these two amino acids are clearly relatively poor substrates of LAAO
as reported in previous studies (Arbor 1967) and also herein (Figs. S1 and S4), and therefore it
appears that the resulting keto acid could not be utilized by E. coli, while the remaining amino acid was
effectively incorporated in the protein.
Fig. 2
Effective incorporation of Hα protons in a ubiquitin
sample, while suppressing many side-chain signals. The solution13C-HSQC of uniformly labelled
ubiquitin (blue) is compared with α-PET ubiquitin (red).
Selected slices show the intensity at backbone and sidechain
sites. Intensities are not corrected for differences in
T2
Fig. 3
Residue-specific characterization of labeling from1H–15N
TOCSY-HSQC spectra of 1 mM ubiquitin using 75 ms MLEV-17 mixing.
α-PET ubiquitin (red) is compared with15N,13C-ubiquitin
(black)
Effective incorporation of Hα protons in a ubiquitin
sample, while suppressing many side-chain signals. The solution13C-HSQC of uniformly labelled
ubiquitin (blue) is compared with α-PET ubiquitin (red).
Selected slices show the intensity at backbone and sidechain
sites. Intensities are not corrected for differences in
T2Residue-specific characterization of labeling from1H–15N
TOCSY-HSQC spectra of 1 mM ubiquitin using 75 ms MLEV-17 mixing.
α-PET ubiquitin (red) is compared with15N,13C-ubiquitin
(black)Of the 13 successful amino acid types, tyrosine, phenylalanine,
isoleucine, valine, alanine, threonine and aspartic acid residues show only Hα
signals in the 1H–15N
TOCSY-HSQC spectrum. The anabolic pathway of these residues ends with an
aminotransferase reaction, with the exception of threonine, which explains the
labeling. Effective aspartic acid labeling was unexpected since it enters and
exits the TCA cycle, but is explained by the very high starting
concentration.The amino acid mix from Silantes (Table S1) is obtained from
bacterial proteins by an HCl proteolysis and consequently glutamine, asparagine,
tryptophan, and cystein are not present in the media. Therefore, glutamine and
asparagine require conversion from the respective acids, which explains
protonation of beta and gamma protons for these residues (Fig. 1). Glutamic acid efficiently enters and exits
the TCA cycle, which may explain the incomplete suppression of beta and gamma
protons.Leucine side-chain protons were not expected, but appear to some
extent due to LAAO treatment (Fig. S2). If the LAAO treatment is not performed,
this sidechain labeling is not observed (Fig. S7), thus it is the crude snake
venom extract that introduces leucine Hγ protons. Details of this side reaction
were not investigated further, however we did follow the reaction of LAAO to
test efficiency in different buffer conditions for a variety of amino acids
(Figs. S1–S5).For most amino acids, the reaction proceeded as expected, and the
snake venom LAAO was particularly efficient for hydrophobic amino acids such as
phenylalanine and isoleucine (Crotalus and Allen 2013; Arbor 1967). The degree of conversion to keto acids was also tested for
all 20 amino acids directly in the Silantes medium. To distinguish the signal
from the individual amino acid without significantly changing the composition,
we used deuterated Silantes media, and added only 100 µM of each protonated
amino acid. In this way, we rule out potential issues such as competitive
binding to the enzyme and determine the approximate starting concentration of
all amino- and keto- acids in the medium (Table 1).
Table 1
LAAO activity in deuterated Silantes media, as
determined by solution NMR. Each amino acid was added in
protonated form at a concentration of 100 µM and LAAO was added
exactly as described in the methods section for expression. The
remaining alpha signal intensity was used to determine the
degree of conversion to keto acid
Keto acid conversion (%)
Residue
Measured Hα incorporation (%)
Residue*
90–100
Ile, Leu, Phe, Tyr, Trp, Met
90–100
Ile, Leu, Phe, Tyr, Met, Val, Ala, Gln, Asn,
Thr, Ser, Glu, Asp
*Of 16 amino acids that could be quantified (see
SI)
LAAO activity in deuterated Silantes media, as
determined by solution NMR. Each amino acid was added in
protonated form at a concentration of 100 µM and LAAO was added
exactly as described in the methods section for expression. The
remaining alpha signal intensity was used to determine the
degree of conversion to keto acid*Of 16 amino acids that could be quantified (see
SI)Quantification of the labeling for each residue type is tabulated
in Tables S2 and S3 based on intensities extracted from13C-HSQC spectra. The intensities were corrected
for the measured proton transverse relaxation rates (Fig. S11) and normalized
based on the assumption of complete incorporation of isoleucine, phenylalanine,
and leucine residues, which were cleaved completely and are known to effectively
incorporate in E.
coli (Tugarinov et al. 2003).We also found that efficient transamination occurs when E. coli is grown primarily on amino acids. Some
exchange still occurs at amide positions even without LAAO treatment (Figs. S6,
S7), consistent with a previous report showing significant Hα labeling for TCA
cycle amino acids, but only 10–50% Hα labeling for hydrophobic residues (Löhr et
al. 2003).
Glycine is labeled stereospecifically
The Hα labeling of glycine attracts particular attention, since one
of the two Hα protons is labeled predominantly, resulting in stereospecific
glycine labeling (Figs. 2, 4). For glycine 28, the intensity ratio between
the two alpha protons for microcrystalline 13C,15N SH3 (Fig. 4, black) is 1–0.93 while the ratio is 1–0.30 for α-PET SH3
(Fig. 4, red). This effect was
observed for glycine in all the samples tested, based on signal intensity in
HSQC and CP-HSQC spectra. We also observed a considerable reduction in line
width, by more than a factor of three.
Fig. 4
Cross-polarization based carbon-proton correlation
spectra, hCH, of microcrystalline SH3 either uniformly α-PET
labeled (red) and 13C,15N-labled (black) crystalized
from a protonated buffer. Spectra were recorded at a magnetic
field of 800 MHz and 30 °C, 55 kHz MAS. 1D slices from the
spectrum indicate the improvement in linewidths for G28 (top
left) and A55 (bottom right). The glycine peak intensities show
stereospecific labeling with preference for R (α3 protonated)
over S (α2) configuration. At the bottom right, the backbone and
side-chain protons are indicated on the solution NMR structure
(pdb: 1aey) for α-PET SH3 (red ribbon) and13C,15N SH3 (black
ribbon)
Cross-polarization based carbon-proton correlation
spectra, hCH, of microcrystalline SH3 either uniformly α-PET
labeled (red) and 13C,15N-labled (black) crystalized
from a protonated buffer. Spectra were recorded at a magnetic
field of 800 MHz and 30 °C, 55 kHz MAS. 1D slices from the
spectrum indicate the improvement in linewidths for G28 (top
left) and A55 (bottom right). The glycine peak intensities show
stereospecific labeling with preference for R (α3 protonated)
over S (α2) configuration. At the bottom right, the backbone and
side-chain protons are indicated on the solution NMR structure
(pdb: 1aey) for α-PET SH3 (red ribbon) and13C,15N SH3 (black
ribbon)Glycine can be produced from serine by hydroxymethyltransferase,
from threonine by l-allo-threonine
aldolase, or through serine–glyoxylate or alanine–glyoxylate transaminases.
Information in E. coli is limited, but
analysis of other organisms using tritiated water indicates that the stereo
specificity depends on the pathways involved (Yoshimura et al. 1996; Dunathan et al. 1968; Wellner 1970). If serine transhydroxymethylase acts in tritiated
water, the resulting glycine will predominantly be the S configuration, but if
liver transaminase acts then R will be the predominant configuration. Note that
in our case, each enzyme will produce the reverse stereoisomer because the
starting amino acid is deuterated, and the enzymatic reaction occurs in
protonated water. By examination of NOE spectra of ubiquitin we observed a cross
peak between the glycine 47 Hα and isoleucine 45 HN,
which according to the known structure, indicates that glycine was predominantly
the R configuration. This is consistent with the stereospecific labelling
approach reported previously using cell free extracts (Loscha and Otting
2013), but results in the
opposite labeling, since we expressed in H2O rather than
D2O. We can therefore rule out deuterated glycine
from the medium as the main source of stereospecific glyine found in the
expressed protein.
Resolution and structural data under MAS conditions
To demonstrate that the α-PET labeling scheme results in improved
resolution, we prepared a microcrystalline sample of α-spectrin SH3 according to
established crystallization protocols (Pauli et al. 2000). The Hα line width is significantly
reduced for α-PET SH3 and the effect is particularly improved for certain
residues, by a factor of two and above (Fig. 4). The proton resolution is also superior to labeling with
deuterated glucose in otherwise protonated media (Medeiros-Silva et al.
2016) (Fig. S8). To
characterize the narrowing of the homogeneous part of the lines, the bulk
T2´ relaxation times at 55 kHz was measured for Hα,
Cα, and CO from 1D (HCAN)H, (HCON)H and (HCA)HA spectra by integrating the full
signal. The Hα T2´ of 3–4 ms for α-PET SH3 is a dramatic
improvement compared to 1 ms for the fully protonated sample (Fig S9).The Hα T2´ of α-PET SH3 crystallized in 100%
D2O buffer ranged from 7 to 15 ms, an improvement
over the amide protonated sample large enough that we can directly observe an
increase in resolution in the 1D spectrum (Fig S9). The improvement is further
characterized for select residues in Figure S12. The
HN signals were almost completely removed in the
D2O buffer.Sequential resonance assignment in Fig. 4 were made using a (H)NCAHA spectrum, and are consistent
with those previously reported (Xue et al. 2017). SH3 has 62 residues, of which, two are prolines and
the N-terminal seven residues and residues 46–48 are flexible and are therefore
not observed using cross-polarization based transfer experiments. Thus 50 Hα
peaks are expected for13C,15N SH3. For α-PET
SH3 lysine, arginine and histidine are not expected. Thus only 41 Hα peaks are
expected and indeed 41 peaks were readily identified in (H)NCAHA spectra.Figure 5 shows a comparison
between α-PET SH3 in fully protonated buffer (red) and α-PET SH3 in fully
deuterated buffer (blue) in which long-range structural restraints were
measured. To characterize the benefit of the restraints present with α-PET
labeling, we manually selected peaks in the H(H)CH and H(H)NH spectra, and used
automated shift matching (0.05, 0.5 and 0.5 ppm tolerance, in1H, 13C and15N, respectively) to identify contacts. Of 114
automatically assigned peaks from the 3D H(H)NH of α-PET SH3 in protonated
buffer, two unambiguous contacts were identified, of which one is a long-range
HN–HN contact. For the
3D H(H)CH, 132 peaks were selected, and seven unambiguous contacts were
identified, five of which are long-range restraints. However, for the H(H)CH
spectrum in deuterated buffer we found 150 contacts, of which eight are
unambiguous restraints, seven of which were long range corresponding to either
HN–Hα or Hα–Hα. One of the additional contacts
identified in fully deuterated buffer is highlighted in Fig. 5b. This method clearly improves the number of
structural restraints available at 55 kHz MAS, and in particular, the
unambiguous restraints, a metric that is crucial for the convergence of commonly
used structure calculation methods. A concern with Hα detection is the presence
of water and other solvent signals in this spectral region. Therefore good water
suppression is needed, but as demonstrated here for samples in both
H2O and D2O, control of the
water is possible even without gradient methods.
Fig. 5
Long-range distance information is highlighted in a 3D
H(H)CH spectrum of α-PET SH3 (pdb: 1aey) in
D2O (blue) and in
H2O (red). a Shows a contact between L33 Hα and V44 Hα. Inb, the contact between T32
Hα and L8 Hα is readily observed in D2O
(in blue) while it is much weaker in the presence of additional
protons in H2O (in red). Recorded in a
800 MHz Bruker spectrometer at 30 °C and 55 kHz MAS
Long-range distance information is highlighted in a 3D
H(H)CH spectrum of α-PET SH3 (pdb: 1aey) in
D2O (blue) and in
H2O (red). a Shows a contact between L33 Hα and V44 Hα. Inb, the contact between T32
Hα and L8 Hα is readily observed in D2O
(in blue) while it is much weaker in the presence of additional
protons in H2O (in red). Recorded in a
800 MHz Bruker spectrometer at 30 °C and 55 kHz MASFor resonance assignment, the α-PET labeling approach benefits from
the implementation of new proton detected NMR pulse sequences focused on Hα
detection that were recently developed for > 100 kHz MAS (Stanek et al.
2016). So far, proton detected
MAS NMR structures were mostly based on HN detected
experiments or more recently on fully protonated samples that are best
investigated using >100 kHz MAS. (Cala-De Paepe et al. 2017) New possibilities are opened with the
α-PET approach, allowing effective structural measurements with the inherently
more sensitive equipment for ~ 60 kHz spinning.The method was also successful for a more challenging system, the
human voltage-dependant anion channel (VDAC). The lipid bilayer structure of
this protein has been investigated through MAS NMR spectra of VDAC in liposomes
(Schneider et al. 2010) and in 2D
crystalline arrays (Eddy et al. 2015), and narrow proton resonances were reported for a
perdeuterated sample.(Eddy et al. 2015a, b) With
α-PET labeling, we also observed narrow amide proton linewidths of 150 Hz in
H2O, while ~ 100 Hz lines were observed using
D2O buffer, which is slightly better than the
~ 120 Hz linewidths observed for perdeuterated and HN
back-exchanged protein. This indicates that the non-exchangeable protons are
slightly narrower, and that Hα labeling does not significantly impact the
spectral quality. In this D2O-exchanged buffer, less
improvement in Hα T2´ (Fig. S9) was observed as compared
with the SH3 domain, which is not unexpected, since approximately half the amide
protons were protected from exchange (Fig. S9B).To further characterize the potential spectral resolution, α-PET
VDAC was measured at 105 kHz MAS at a 950 MHz spectrometer (black in
Fig. 6a). Surprisingly, the same
line width was obtained at 110 kHz MAS at 950 MHz (~ 110 Hz) and at 55 kHz MAS
at 800 MHz (~ 95 Hz), showing that the inhomogeneous contributions are
dominating the linewidth at 55 kHz. This shows that even for a highly
homogeneous preparation of a membrane protein, α-PET labeling efficiently
reduces the proton dipolar broadening at 55 kHz.Identification of a cross beta strand contact
(F99–I114 Hα) in the beta barrel membrane protein VDAC in lipid
bilayers. a Shows, the
comparison of the (H)CH spectrum at 105 kHz on a 950 MHz
spectrometer (black) and at 55 kHz on an 800 MHz spectrometer
(red). b Shows a13C–15N
projection of a (H)NCAHA spectrum. F99 Hα is assigned from the
strip comparing (H)NCAHA (green) and (H)N(CO)CAHA (brown). Inc and e, the contact is shown on the X-ray structure
of mouse VDAC (pdb: 2jk4). d
Shows the F99–I114 cross-peak in the carbon–carbon 2D plane of
the (H)C(HH)CH spectrum at the proton frequency of F99,
4.72 ppmThe protection from solvent exchange observed for VDAC highlights
an issue with perdeuteration for proteins that lack refolding protocols.
Perdeuteration of membrane proteins (Medeiros-Silva et al. 2016; Ward et al. 2011) and large complexes (Andreas et al.
2016) in E. coli often results in deuterated amides that cannot be
exchanged with protons from water. Such exchange protected regions of the
protein become inaccessible in the perdeuteration and back-exchange approach,
limiting the analysis to solvent accessible regions (Andreas et al. 2015; Chevelkov et al. 2006; Fricke et al. 2017; Zhou et al. 2007a, b; Ward et al. 2015), although such limited exchange phenomena can also be
used to obtain functional information (Ward et al. 2011; Böckmann and Guittet 1997; Agarwal et al. 2010). Using α-PET labeling, we are now able
to detect both exchangeable as well as non-exchangeable amide protons in highly
deuterated samples as shown previously for amino acid based media (Löhr et al.
2003).Due to the size of the protein, unambiguous assignment of important
cross-strand contacts was not possible in a 3D H(H)CH spectrum of VDAC. We
therefore applied the better resolved 3D (H)C(HH)CH spectrum to measure
cross-strand contacts (Fig. 6). VDAC
assembles as a beta barrel, a topology that places cross-strand Hα pairs in
close proximity (~ 2.3 Å), and much closer than sequential Hα spins, which are
separated by about 4.5 Å. 28 Hα–Hα contacts were detected from this spectrum, of
which we show the cross strand contact between residue phenylalanine 99 and
isoleucine 114, which was assigned based on the existing13C and 15N
assignments of this protein (Eddy et al. 2015a, b) and
(H)NCAHA and (H)N(CO)CAHA spectra. The current published assignments (32% of 283
residues) of VDAC do not allow a characterization of all 28 peaks. However,
resolving 28 peaks is significant, considering that only ~ 4 amide–amide or
alpha–alpha contacts are available in each transmembrane beta sheet interface,
of which VDAC has 19. Further analysis of the expected contacts in VDAC is show
in in Fig. S10 This demonstrates a successful implementation of α-PET labelling
for structure determination in a challenging 32 kDa membrane protein embedded in
lipid bilayers, where structural restraints are particularly difficult to
identify (Eddy et al. 2015).
α-PET labeling for solution NMR
The α-PET labeling approach is also beneficial for the study of
proteins in solution, when deuteration is needed to reduce transverse relaxation
rates (LeMaster and Richards 1988;
Torchia et al. 1988).
Figure 7 and Tables S4–S5 show the
reduction in R2 relaxation rates due to the high level of
deuteration in α-PET labeled Ubiquitin. Such improvement in relaxation rates is
important for the study of protein dynamics. For example in detection of Hα
relaxation dispersion, fractional deuteration was used to improve
R2 (Lundström et al. 2009; Vallurupalli et al. 2009). The current labeling incorporates the alpha positions
at 100% for most residues, with a high overall deuteration level, which improves
sensitivity as compared with random fractional deuteration.
Fig. 7
Selected residues showing the reduction in proton (Hα)
R2 relaxation rates with α-PET
labeling (red) as compared with full protonation (black). The
correlation plot (right) shows a reduction for all residues. The
data is from ubiquitin samples exchanged in 100%
D2O at 277 K and measured at a
600 MHz spectrometer
Selected residues showing the reduction in proton (Hα)
R2 relaxation rates with α-PET
labeling (red) as compared with full protonation (black). The
correlation plot (right) shows a reduction for all residues. The
data is from ubiquitin samples exchanged in 100%
D2O at 277 K and measured at a
600 MHz spectrometer
Conclusions
Here, we introduced a new method to label Hα protons in a protein
without significant isotopic scrambling, and demonstrated how this new sensitive
magnetic probe in the backbone of the protein adds new structural information even
at below 60 kHz MAS. The α-PET labeling approach has several advantages, (i)
adaptation of the cells to D2O is not required, (ii) it gives
similar yields as deuterated expression in M9 media, and (iii) costs are similar to
production of deuterated proteins. It is expected to be particularly useful for
deuteration of proteins that lack refolding protocols, such as membrane
proteins.In this demonstration, we used a commercially available crude snake
venom extract to generate keto acids. This approach results in the designed
incorporation of alpha protons for Tyr, Phe, Leu, Ile, Gly, Gln, Asn, Asp, Glu and
Met. In the future, further optimization of the method might entail other LAAOs with
different substrate specificity, perhaps in combination with auxotrophic strains to
limit unwanted reaction pathways. In addition, other amino acid mixtures or
expression systems could be investigated. This might allow labeling of lysine,
arginine, and histidine, which were currently left deuterated.
Supporting Information
Quantification of labeling patterns, LAAO activity, measurement of
relaxation times under 55 kHz MAS, Hα R2 in solution and
spectral acquisition parameters.Below is the link to the electronic supplementary material.Supplementary material 1 (PDF 3597 KB)
Authors: Evgeny Nimerovsky; Eszter E Najbauer; Kumar Tekwani Movellan; Kai Xue; Stefan Becker; Loren B Andreas Journal: J Phys Chem Lett Date: 2022-02-08 Impact factor: 6.475
Authors: Eszter E Najbauer; Kumar Tekwani Movellan; Karin Giller; Roland Benz; Stefan Becker; Christian Griesinger; Loren B Andreas Journal: J Am Chem Soc Date: 2022-02-14 Impact factor: 15.419
Authors: Evgeny Nimerovsky; Kumar Tekwani Movellan; Xizhou Cecily Zhang; Marcel C Forster; Eszter Najbauer; Kai Xue; Rıza Dervişoǧlu; Karin Giller; Christian Griesinger; Stefan Becker; Loren B Andreas Journal: Biomolecules Date: 2021-05-18
Authors: Kai Xue; Evgeny Nimerovsky; Kumar A Tekwani Movellan; Stefan Becker; Loren B Andreas Journal: J Phys Chem Lett Date: 2021-12-27 Impact factor: 6.475
Authors: Morgane Callon; Alexander A Malär; Sara Pfister; Václav Římal; Marco E Weber; Thomas Wiegand; Johannes Zehnder; Matías Chávez; Riccardo Cadalbert; Rajdeep Deb; Alexander Däpp; Marie-Laure Fogeron; Andreas Hunkeler; Lauriane Lecoq; Anahit Torosyan; Dawid Zyla; Rudolf Glockshuber; Stefanie Jonas; Michael Nassal; Matthias Ernst; Anja Böckmann; Beat H Meier Journal: J Biomol NMR Date: 2021-06-25 Impact factor: 2.835