From the Department of Chemistry, University of
Cambridge, Lensfield Road, Cambridge CB2 1EW, United Kingdom and
¶ Max Planck Institute für Molekular Genetik, AG Ribosomen,
Ihestraße 73, 14195 Berlin, Germany
Received for publication, September 3, 2002, and in revised form, October 18, 2002
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ABSTRACT |
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We used mass spectrometry to identify proteins
that are released in the gas phase from Escherichia coli
ribosomes in response to a range of different solution conditions and
cofactor binding. From solution at neutral pH the spectra are dominated
by just 4 of the 54 ribosomal proteins (L7/L12, L11, and L10). Lowering the pH of the solution leads to the gas phase dissociation of four
additional proteins as well as the 5 S RNA. Replacement of Mg2+ by Li+ ions in solutions of ribosomes
induced the dissociation of 17 ribosomal proteins. Correlation of these
results with available structural information for ribosomes
revealed that a relatively high interaction surface area of the protein
with RNA was the major force in preventing dissociation. By using the
proteins that dissociate to probe their interactions with RNA, we
examined different complexes of the ribosome formed with the elongation factor G and inhibited by fusidic acid or thiostrepton. Mass spectra recorded for the fusidic acid-inhibited complex reveal subtle changes
in peak intensity of the proteins that dissociate. By contrast gas
phase dissociation from the thiostrepton-inhibited complex is markedly
different and demonstrates the presence of L5 and L18, two proteins
that interact exclusively with the 5 S RNA. These results allow us to
propose that the ribosome elongation factor-G complex inhibited by
thiostrepton, but not fusidic acid, involves destabilization of 5 S
RNA-protein interactions.
The ribosome, the machinery responsible for the translation of RNA
into proteins (1), is composed of two unequal subunits the 30 S and
50 S that together constitute the intact 70 S. This macromolecular
assembly which in Escherichia coli consists of 54 proteins
and 3 RNA molecules has a molecular mass of 2.3 MDa. We have
shown previously by using MS1
that it is possible to maintain the non-covalent associations of
E. coli ribosomes in the gas phase (2, 3). These studies revealed the intact 30 S, 50 S, and 70 S particles (3) and complexes
containing up to six proteins, assigned to the five proteins from the
stalk region (four copies of L7/L12 and one of L10) and protein L11
immediately proximal to the stalk. Unlike the stalk proteins, the
majority of ribosomal proteins has been shown by x-ray crystallography
to be largely globular with highly basic polypeptide tails, 26% of the
amino acid composition being either arginine or lysine, and having
little or no secondary structure. These tails insert into crevices
between RNA helices in the ribosomal subunits and act to maintain the
structure of the ribosome (4). Previously, we observed that the
proteins that are released in the mass spectrometer (3) are among the
most acidic of the ribosomal proteins (5) implying that dissociation of
proteins from ribosomes in the gas phase is in part dependent on
reducing the positive charge of the protein, thereby weakening
interactions with negatively charged RNA.
In addition to detailed structural information, considerable insight
into the mechanistic details of protein synthesis has also arisen from
atomic resolution images of the ribosome. The original picture of a
multistep process requiring a number of protein factors that hydrolyze
GTP (6) is emerging with atomic detail (7). The elongation phase of
protein synthesis begins with the insertion of an aminoacyl-tRNA into
the aminoacyl site by elongation factor EF-Tu. Subsequent binding of
the elongation factor G (EF-G) to the ribosome triggers the movement of
tRNA from the aminoacyl to the peptidyltransferase site in a process known as translocation. EF-G binding to the ribosome is labile but can
be trapped using antibiotics. Fusidic acid allows translocation and GTP
cleavage but prevents the release of EF-G from the ribosome and traps
the ribosome in the post-translocational state (post-state) (8, 9). By
contrast thiostrepton does not bind directly to EF-G or affect factor
binding and GTP hydrolysis, rather it is reported to bind directly to
RNA in a region close the L11-binding site (10) and traps the ribosome
in a pre-translocational state (pre-state). Thiostrepton has been shown
to block translocation even in the absence of EF-G (11) and recently
under certain conditions to prevent complex formation (12). This is in
contrast to a report where inhibition of phosphate ion and EF-G release from the ribosome was inferred (13). Biochemical studies have also
revealed changes of conformation of the ribosome upon interaction with
elongation factors, in particular protein L12 and its acetylated counterpart L7 (14, 15). The results were substantiated by cryo-electron microscopy studies that demonstrate large scale movements
in response to binding EF-G (16, 17).
The primary aim of this study is to investigate the factors that govern
the loss of proteins from ribosomes in the mass spectrometer. A
secondary aim is to apply the information that can be gained from such
experiments to probe conformational changes in complexes of the
ribosome. The recent x-ray analyses of 50 S ribosomes from Haloarcula marismortui (18) and the 30 S
subunit from Thermus thermophilus (19) allows examination of
the precise protein-RNA interactions and solvent accessibility for a
number of ribosomal proteins and enables us to relate this information
to ribosomes from E. coli. To investigate gas phase
dissociation, we have manipulated samples of E. coli
ribosomes, specifically the pH and metal ion content of the solution,
and recorded spectra under identical MS conditions. By using the
molecular weight calculated from known amino acid sequences to identify
the individual ribosomal protein, we examined the relationship between
pI of the protein and its interaction with other proteins and with
different RNA molecules. These experiments demonstrate, through
distinctive protein dissociation patterns, the sensitivity of the
approach to changes in RNA structure. By having established a
relationship between the surface area of interaction and the propensity
for gas phase dissociation, we examined the release of proteins from
ribosomes in complexes with the cofactor EF-G in the presence of two
inhibitors of elongation: fusidic acid and thiostrepton freezing the
ribosome in complexes analogous to post- and pre-translocation states,
respectively. The results show that the two EF-G ribosome complexes are
significantly different and are indicative of conformational changes in
the mobile stalk region and, in the case of the thiostrepton-inhibited complex, of the 5 S RNA molecule itself.
Materials--
Ribosomes were harvested from E. coli
strain MRE600 in the log phase of the growth cycle by using standard
protocols and were stored in Tico buffer (20 mM HEPES-KOH,
pH 7.6, 6 mM magnesium acetate, 30 mM ammonium
acetate, 4 mM EF-G Preparation--
XL1 cells were transformed with the vector
pQE70fusA, which carries the EF-G gene under the pLac promoter. The
cells were grown at 37 °C at 300 rpm with aeration, in Luria Broth
(LB) containing 100 mg/ml ampicillin. The 6 liters of culture was
induced with isopropylthiogalactopyranoside at a final concentration of
1 mM, when cell growth reached a logarithmic phase. The
absorbance was 0.45 at 560 nm. The incubation was continued for 4 h after induction. Cells were harvested by centrifugation at 5000 × g for 20 min at 4 °C and then washed twice in 1 liter
of buffer A, pH 7.5, containing 50 mM KHPO4, 10 mM NH4OAc, 1 mM dithiothreitol, and 100 mM NaCl. The final cell pellet was resuspended in 5 ml
of buffer A/g of cell pellet. Lysozyme, DNase, and phenylmethylsulfonyl fluoride were added to a final concentration of 0.5 and 0.1 g/liter and
0.1 mM, respectively. The mixture was sonicated, and the
lysate was centrifuged at 30,000 × g for 30 min at
4 °C. The supernatant was centrifuged at 10,000 × g
for 45 min at 4 °C. EF-G was purified from the cell extract using a
BioCAD system (Applied Biosystems). The supernatant from the last
centrifugation process was loaded onto a nickel column equilibrated in
buffer A with 10 mM imidazole. The fractions containing
EF-G were pooled and dialyzed five times against 30 volumes of buffer
A. The final yield of EF-G was 28 mg/g of cell pellet. The EF-G
produced by this process has N- and C-terminal extensions of ML and
RSHHHHHH, respectively, and two sequence changes I575V and E357A
resulting in an increase in mass of 1237 over the calculated mass for
the sequence of EF-G from the Swiss Protein Data Bank (code
P02996).
Sample Preparation--
Solutions were kept at 4 °C
throughout buffer exchange and immediately before electrospray
analysis. The precise solution pH was measured as 4.7, 7.0, and 10.8 after addition of the pH 4.5, 7.0, and 11.0 buffered solutions. For the
LiCl treatment ribosomes were exchanged into 300 µM LiCl
solution and incubated for 30 min. Immediately prior to analysis by MS,
samples were buffer-exchanged at 4 °C into 10 mM
ammonium acetate solution at pH 6.5 and analyzed as described below.
EDTA in ethanol was added to 20-µl aliquots of a 1 µM
solution of ribosomes equilibrated with 10 mM ammonium
acetate, to give final EDTA concentrations of 50 and 300 µM and 50 mM. Each solution was incubated for
1 h at 4 °C. The EDTA was removed immediately before analysis
using a Bio-Spin 6 column pre-equilibrated with 10 mM
ammonium acetate, and samples were analyzed as described below.
Preparation of Ribosome EF-G Complexes--
The
ribosome-EF-G complex was prepared by using 50 µl of a stock
solution of 70 S ribosomes at a concentration of 1.5 µM
in 10 mM ammonium acetate, pH 7.0. 40 µl of EF-G from a
stock solution at a concentration of 60 µM and 19 µl
GTP at a concentration of 3 mM were added to give a final
volume of 119 µl. Stock solutions of fusidic acid and thiostrepton
were prepared at a concentration of 1 mM in 10 mM ammonium acetate, pH 7.0. For the thiostrepton stock
solution it was necessary to add 2% v/v of Me2SO to ensure complete dissolution of the antibiotic. 1 µl of the antibiotic solution, either fusidic acid or thiostrepton, was added to the solution containing ribosomes, EF-G, and GTP after incubation on ice
for 1 min. The resulting solution was kept at 4 °C. The molar ratio
of 70 S/EF-G/GTP/antibiotic was 1:32:760:13, closely similar to that
employed in cryo-EM studies of these complexes (22). Excess antibiotic
was removed before analysis by filtering the reaction mixture through a
Bio-Spin 6 column equilibrated with 10 mM ammonium acetate,
pH 7.0. To examine the effect of trace amounts of
Me2SO on gas phase dissociation from the ribosome, mass spectra were recorded for ribosomes in 10 mM ammonium
acetate containing 0.2% (v/v) Me2SO (the maximum amount of
Me2SO that could be present in the solution of the complex
after 10-fold dilution and after Bio-Spin chromatography). The spectra
recorded were identical to those recorded in the absence of
Me2SO confirming that at these low concentrations
Me2SO does not affect the pattern of gas phase dissociation
from ribosomes.
Further control experiments were carried out in which a single
component from the reaction was omitted, and the solutions were
prepared and incubated as described above. In the absence of the
antibiotics fusidic acid and thiostrepton, but with identical solvent
composition to the inhibited EF-G ribosome complexes, the spectra
showed similar patterns of peaks observed routinely for naked
ribosomes. In the absence of GTP, EF-G was observed in mass spectra but
showed no hydrolysis of GTP. For EF-G in the absence of ribosomes no
appreciable hydrolysis of GTP to GDP could be detected.
Mass Spectrometry--
All samples were analyzed by nanoflow
electrospray using capillaries prepared as described previously (23).
The high viscosity of the ribosomal samples necessitated the use of
needles with large tip orifices and a backing pressure of 10-20
pounds/square inch. 2-µl aliquots of sample were loaded into
capillaries, and spectra were recorded on a modified Micromass QToF2
mass spectrometer (Micromass, Manchester, UK). This modified mass
spectrometer has been described in detail elsewhere (24) and consists
of a nanoflow electrospray interface, a low frequency extended mass
range quadrupole, capable of isolating ions up to
m/z 32,000, followed by a hexapole collision
cell, and a time-of-flight (ToF) mass analyzer. The capillary and cone
voltages were maintained at 1800 and 80 V, respectively, throughout
this investigation. Pressure conditions were maintained at 9 × 10
For the comparison between the EF-G complexes and naked ribosome
sample, the same batch of ribosomes was used throughout, and the mass
spectra were recorded on the same day to ensure that conditions were
entirely reproducible. In addition the use of the same batch of
ribosomes ensures that the tRNA content is identical in each of the
complexes formed. Control experiments with re-associated ribosomes, in
which tRNA is absent, have shown that the dissociation pattern is the
same as that observed for naked ribosomes used in this study.
Data Analysis--
The calculated masses of ribosomal proteins
from E. coli were calculated from the known amino acid
sequences in the Swiss-Prot data base. For the spectra recorded from
solutions at different pH values results were calculated from three
replicate experiments. The spectra recorded from LiCl solutions were
repeated twice, whereas those for complexes were repeated at least in
triplicate. The intensities of three charge states from each series
were summed, and the average intensity of the peaks assigned to each
protein from the replicate experiments was calculated. These values
were expressed as a percentage of total intensity assigned to protein peaks in the spectra. It was not possible to deconvolute the peaks assigned to L7/L12 because of extensive metal ion binding under neutral
pH solution conditions. However, because low pH conditions confirm
their equal population on the ribosome, the intensity of the peaks
assigned to L7/L12 was divided by two, and only the intensity
calculated for L12 is displayed.
Calculation of Surface Areas of Interaction--
Because only
three small subunit proteins (S1, S8, and S10) are released in mass
spectra from the different solution conditions, it was difficult to
draw conclusions about the extent of protein dissociation from 16 S
RNA. This study therefore focuses on interactions in the large subunit.
For the large subunit 16 proteins were released from the 23 S and 5 S
RNA molecules. To calculate the extent of protein-protein and
protein-rRNA interactions, the solvent-accessible surface areas of the
protein, buried in the respective contact, was calculated ( Solutions of E. coli ribosomes were prepared over a
range of pH values to examine the influence of pH on the dissociation of proteins (see "Experimental Procedures"). An example of a
typical spectrum recorded for a solution of E. coli
ribosomes at pH 7.0 is shown (Fig.
1A). Assignment of the peaks
together with the known masses of the ribosomal proteins shows that
spectra are dominated by L10, L11, and L7/L12. Under these MS and
solution conditions, no intact stalk complex was observed, in contrast to our previous experiments, as in this case the mass spectrometer was
optimized for dissociation of proteins (2, 3). Observation of these
individual proteins from solution at neutral pH is attributed to their
preferential gas phase dissociation from the intact ribosome. These
proteins are located in the 50 S stalk region together with the
protein L11, located immediately at the base of the stalk complex. The
intensity of the peaks assigned to the proteins L10 and L11 is much
lower than those of L7/L12. Intensity in a mass spectrum is governed by
the interplay of many different factors, and in this case can be
attributed at least in part to the fact that four copies of L7 or L12
are present on ribosomes. However, the peaks assigned to L7/L12 are a
factor of ~10 greater than those of both L11 and L10, and this
relatively high intensity is therefore consistent with their more
favorable release from ribosomes. Close examination of the peaks
assigned to L7/L12 in the spectrum recorded for E. coli
ribosomes from pH 7.0 shows multiple peaks each separated by 22 Da
(Fig. 1C). This mass difference could be attributed either
to sodium ion binding, in which a monovalent sodium ion replaces a
single proton, or divalent magnesium ion binding in which two protons
are replaced. To distinguish these two possibilities, EDTA was added in
increasing amounts to chelate the divalent cation and spectra recorded.
The resulting spectra showed a substantial reduction in the intensity
of the multiplet with increasing concentrations of EDTA. Removal of the
multiple peaks under these conditions identifies the ion binding as
magnesium.
INTRODUCTION
TOP
ABSTRACT
INTRODUCTION
EXPERIMENTAL PROCEDURES
RESULTS AND DISCUSSION
CONCLUSION
REFERENCES
EXPERIMENTAL PROCEDURES
TOP
ABSTRACT
INTRODUCTION
EXPERIMENTAL PROCEDURES
RESULTS AND DISCUSSION
CONCLUSION
REFERENCES
-mercaptoethanol) (20). Stock solutions
were prepared immediately prior to analysis by buffer-exchange at
4 °C to give a final concentration of 1 µM ribosome in
10 mM ammonium acetate (pH 7.0) using Bio-Spin 6 chromatography columns (Bio-Rad) equilibrated previously with 10 mM ammonium acetate at pH 7.0 unless stated otherwise.
Although some separation of 70 S particles into 30 S and 50 S
subunits is observed in the mass spectrometer as the Mg2+
ion concentration is reduced, we have shown previously (21) that the
majority of particles (>90%) remains associated as the 70 S.
Moreover, the fact that MS conditions could be found whereby no
individual proteins are observed strongly implies that protein-RNA interactions are not perturbed by this treatment (3). GTP, thiostrepton, and fusidic acid were purchased from Sigma.
3 mbar in the hexapole ion guide. For the MS/MS
experiments of the 5 S RNA, the peak centered at
m/z 3570 was isolated with a window of ±30
m/z units. A voltage of 40 V was applied to the collision cell at an argon pressure of 3.0 × 10
2 mbar.
SASA).
These values were calculated using a modified version of the program
NACCESS (25), which implements the algorithm of Lee and Richards (26).
Default atomic radii (27) and a standard probe radius of 1.4 Å were
used. The buried surface area
SASA was computed for protein-rRNA and
protein-protein interactions in the 50 S subunit. The results showed
the same trends for
SASA when both protein backbone and side chain
atoms are computed as when only backbone atoms are considered. Because
only a limited data set is available for the three-dimensional
structure of protein backbone and side chains (12 proteins from the
50 S as opposed to 21 for which only backbone coordinates have been
deposited, Protein Data Bank accession code 1KQS), the larger data set was used to enable trends to be established. Both protein-RNA and
protein-protein interactions in the 50 S subunit were calculated. However, given that L12 is associated solely through protein-protein interactions and is readily observed in mass spectra, such interactions are clearly not the driving force for maintaining the gas phase ribosome. Moreover with the exception of L7, L3, and L14, all other
proteins interact exclusively with rRNA and no other proteins. Therefore, to examine the correlation between the extent of protein dissociation in the mass spectrometer and protein-rRNA interactions, protein-protein interactions were not included. Considering only protein-rRNA interactions the values calculated for L7, L3, and L14 are
reduced by 65, 2.6, and 45%, respectively, from the values calculated
for protein-protein and protein-rRNA interactions. Protein interaction
surface area calculated in this way will depend at least in part on the
size of the protein. In order to reduce this dependence, the
SASA
was divided by the molecular mass of the protein. This value is then
plotted against the extent of protein dissociation calculated from the
mass spectra from the different solution conditions.
RESULTS AND DISCUSSION
TOP
ABSTRACT
INTRODUCTION
EXPERIMENTAL PROCEDURES
RESULTS AND DISCUSSION
CONCLUSION
REFERENCES
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Fig. 1.
Mass spectra of E. coli ribosomes
recorded from solution at pH 7.0 (A) and pH 4.5 (B). The peaks are labeled with the protein, and the charge
states are given in parentheses. From solution at pH 7.0, four proteins located in the mobile stalk region of the ribosome
dominate the spectra. From solution at pH 4.5 eight proteins are
identified. Inset, MS/MS spectrum of the peak labeled *.
Acceleration in the collision cell yields a mass consistent with that
calculated for the 5 S RNA. Individual charge states of the L7/L12
proteins reveal their metal binding properties and post-translational
modifications. From solution at pH 7.0 (C) the +6 charge
state shows multiple peaks each separated by 22 Da corresponding to the
binding of Mg2+. From solution at pH 4.5 Mg2+
binding is removed revealing the extent of methylation and acetylation
of L7 and L12 (D). The 50 S subunit structure was produced
using the program RASMOL (41) with coordinates from T. thermophilus at 5.5-Å resolution, Protein Data Bank code 1GIY
(31). The 100-residue fragment of L10 was taken from the crystal
structure of the large ribosomal subunit at 2.4-Å resolution from
H. marismortui (Protein Data Bank code 1KQS) and
inserted in the ribosome structure (42). The 23 S RNA is show in
yellow with 5 S RNA in red, and proteins that
are released from pH 4.5 solution conditions are in color,
whereas those that are not observed are shown in
white.
We also examined solutions of E. coli ribosomes at unit pH values from 7 to 11 to investigate further the effect of charging proteins and rRNA on the propensity for release. Although little is known of the solution structure of ribosomes at these high pH values, the proteins that were observed (L7/L12, L10, and L11) are the same subset as those released under neutral pH conditions. These results suggest therefore that reducing the positive charge of the proteins at high pH does not alter their dissociation pattern from that observed at pH 7.0. By contrast at low pH (4.5), the spectra reveal a number of additional proteins not seen at neutral pH that correspond in mass to the proteins L1, L6, L9, and S8 (Fig. 1B). Unlike L7/L12, L10, and L11 stalk proteins that dissociate at neutral pH, the proteins released from ribosomes at pH 4.5 are known from x-ray crystallography to have no mutual interactions, see structure in Fig. 1. Moreover the peaks assigned to L7/L12 are of comparable intensity to those of other ribosomal proteins implying that at pH 4.5 additional proteins dissociate from the ribosome as readily as L7/L12. The multiplets assigned to L7/L12 recorded from low pH solutions, Fig. 1D, give rise to fewer peaks than were seen at neutral pH. Their m/z values are consistent with their identity as L12 and its acetylated counterpart L7. The similarity in their intensity under these solution conditions confirms their equal population on the ribosome. Removal of the multiple peaks due to Mg2+ binding also allows an examination of the post-translational modifications of the proteins and reveals the extent of methylation of both proteins as <10%.
Also apparent in the spectra recorded from pH 4.5 solution conditions are signals at m/z 3,600-4,400 (data not shown). It is difficult to assign a mass to this series due to the broad nature of the peaks (100 m/z units at half-height for the peak at m/z ~3500). In order to obtain a precise mass measurement of these peaks, a single charge state was isolated in the quadrupole of the Q ToF mass spectrometer (see "Experimental Procedures") and subjected to increased acceleration in the collision cell. Under these conditions the width of the peaks decreases (40 m/z units at half-height for the +11 charge state) enabling the mass to be measured as 39,038 ± 24 Da (Fig. 1B and Table I). This value is in reasonable agreement to that calculated from the sequence of the 5 S RNA of 38,731 Da. The broad appearance of the peaks and increased molecular mass over that calculated from the sequence are consistent with multiple metal ions adducting to negatively charged RNA. Acceleration within the mass spectrometer and multiple collisions are sufficient to remove small molecule binding strongly suggesting the identity of the species as 5 S RNA.
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Solution based methods for removing subsets of proteins from ribosomes
have been devised to investigate proteins required to establish
ribosomal function. These experiments have recognized that it is
possible to dissociate proteins from the ribosome in solution by
addition of LiCl to leave a stable structural nucleus (28). To compare
the dissociation of proteins in the mass spectrometer with those
destabilized by LiCl treatment in solution, a similar protocol was
employed, although excess Li+ was removed before mass
spectra were recorded (see "Experimental Procedures"). After this
treatment a large number of additional proteins were released (Fig.
2). 13 large subunit proteins are known
to remain tightly bound to the 50 S subunit after addition of 2 M LiCl in solution (L2, L3, L4, L13, L14, L17, L19, L21, L22, L23, L24, L29, and L30) (28). From similar treatment and analysis
by MS, only three of the tightly binding proteins were observed in mass
spectra (L21, L24, and L29). Four and twelve proteins, identified
previously as partially and fully released, respectively, by treatment
with LiCl, were all observed in mass spectra with the exception of L15,
L16, and L26 (Table I). In summary, 10 of the 13 proteins known to
remain bound to RNA after LiCl treatment do not dissociate in the gas
phase, whereas 16 of the 19 proteins released by this protocol are
identified in mass spectra. Thus the majority of proteins removed from
ribosomes in LiCl solutions are substantially destabilized by this
treatment and consequently readily observed by mass spectrometry.
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Examination of the intensity of the peaks in the spectra recorded after LiCl treatment shows that the proteins L7/L12 are no longer dominant; L11, L10, and L29 are released as readily under these conditions. It is also apparent from this spectrum that the multiplets assigned to L7/L12 appear less well resolved than those observed in spectra recorded when Mg2+ is the predominant cation (Fig. 2B). This is explained by the fact that the molecular masses of both L7 and L12 recorded after LiCl treatment are consistently higher (7-10 Da see Table I) than those recorded from the solution containing Mg2+ or from the low pH solution conditions. This increased mass is consistent with binding of a single Li+ to these proteins. Under these solution conditions L7/L12 are only observed in the Li+-bound form. Consequently, the mass difference between the peaks corresponding to L7/L12-Li and L7/L12-Mg is reduced compared with the corresponding mass difference observed for the L7/L12 and L7/L12-Mg when Mg2+ is the predominant cation. From the spectra recorded under these solution conditions, we can conclude that Mg2+ ions are replaced partially by Li+ and that as a result of this cation exchange only a subset of proteins remains firmly attached to the RNA scaffold in the gas phase. It is well established that Mg2+ is crucial for the structural integrity of RNA interacting either by diffuse binding in which fully hydrated Mg2+ binds to RNA via nonspecific long range electrostatic interactions or by site-specific interactions with anionic ligands facilitated by the RNA fold (29). The binding of Mg2+ to the acidic stalk proteins observed in the present study is presumably nonspecific, because multiple adducts are observed, and demonstrates the presence of the diffuse Mg2+ cloud surrounding rRNA. It is also established that monovalent cations such as Li+ can compete for Mg2+-binding sites (30). This was also observed in this study because both Li+- and Mg2+-bound L7 and L12 were observed indicating the presence of both cations in the diffuse cloud.
To establish the factors that govern protein dissociation from the ribosome in the gas phase, we first examined the relationship between the pI of the protein and its intensity in mass spectra. The fact that proteins L7, L12, and L10 are readily observed in spectra recorded from neutral pH solution conditions and have pI values of 4.8, 4.0, and 7.5, respectively (Table I), suggests a correlation in which reduced electrostatic interactions between RNA and proteins with a greater extent of negatively charged residues lead to their preferential release. However, from neutral solution conditions dissociation of L11 with a pI of 9.7, a value greater than 8 of the ribosomal proteins listed in Table I that are not observed, is not explained by this correlation. Moreover, the proteins that are observed in spectra recorded at low pH have pI values that range from 4.0 to 12.2 (Table I). An explanation based solely on the loss of electrostatic interactions does not therefore explain the observed dissociation behavior from solutions at different pH values.
The high resolution atomic structures of ribosomes of 50 S subunit
from H. marismortui (18) as well as those reported
from the 70 S of T. thermophilus (31) enable us to examine
protein-RNA interactions and, because of the widely accepted
conservation of structure across bacterial ribosomes (4), to draw
conclusions about those from E. coli. The interactions
between individual large subunit proteins and RNA were examined using a
modified version of the program NACCESS (see "Experimental
Procedures"). A plot of the SASA against the extent of gas phase
dissociation measured from the spectra under different solution
conditions is shown in Fig. 3. From these
data we have used an arbitrary classification of proteins, based on the
rate of change of the extent of
SASA as high (>0.030
Å2/Da), intermediate <0.030 Å2/Da,
>0.015 Å2/Da), and low (<0.015 Å2/Da). By
using this classification, it can be seen that proteins with a high
SASA do not dissociate from ribosomes under the different solution
conditions employed in this study. Similarly proteins with a relatively
low
SASA undergo gas phase dissociation from either neutral or low
pH solutions of ribosomes or after cation exchange with
Li+. There are only two exceptions to these
generalizations, L15 and L19. L15 falls within the category of having
low
SASA but is not observed in mass spectra recorded from any
solution conditions described in this study. Given the fact that
SASA of L15 is smaller per unit mass than that calculated for six
proteins that are released from 23 S RNA, this result is surprising.
However, examination of the pI of this protein (5) reveals that it has
an anomalously high value (>12.0). This is the highest pI value of all
the proteins that fall in the low surface area of the interaction
category (Table I) implying that high positive charge in this case may prevent its release from 23 S RNA.
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Between these extremes of proteins with high and low surface area of interactions are those with intermediate interaction surface areas, and L19 borders this group. Examination of this subset of proteins in conjunction with the x-ray structure reveals that those that are released (L1, L11, and L24) interact with only one of the six folding domains in the 23 S RNA (31). By contrast L2, L19, and L23 interact with 4, 4, and 2 domains, respectively. Thus for those proteins with intermediate surface area of interaction the number of contacts with different domains and the extent of interaction appear to play a role in maintaining protein-RNA interactions in the gas phase. Proteins with higher surface areas of interaction than L24 are not released under any of the solution conditions examined here. It was not possible to calculate interaction surface areas for L10, L21, L27, L28, L32, and L33 because x-ray structure data are not available for these proteins. Given the fact that proteins with a high interaction surface area are not released by this treatment and that L10, L21, L27, L28, L32, and L33 are readily observed strongly implies that these proteins have either intermediate or low interaction surface areas with the 23 S RNA.
Because it is well established that the Li+-bound RNA structure is often destabilized relative to its Mg2+-bound counterpart (30), it is also of interest to examine the proteins that are released by LiCl treatment and their interactions with the six folding domains of the 23 S RNA (18). In this respect it is interesting to note that two proteins (L29 and L24) are released in appreciable amounts by LiCl treatment but not by changing the pH, despite having relatively high interaction surface areas with RNA. Analysis of the x-ray structure reveals that these are the only two proteins that involve a significant interaction with domain I of the 23 S RNA (31). This would imply that Li+ may have displaced Mg2+ from a specific binding site critical for the stability of domain I of the 23 S rRNA. This observation highlights the sensitivity of this MS approach to changes in the tertiary RNA structure in individual folding domains.
To investigate further the sensitivity of gas phase dissociation to
protein-RNA interactions and hence to changes in the conformation of
ribosomes, we have investigated the effects of complex formation on
proteins that are released. By using cryo-EM, it has been established that complexes formed between ribosomes and EF-G can undergo major conformational changes depending on the particular translocation stage
that is inhibited by a given antibiotic (32, 33). These complexes
therefore provide excellent model systems to test our hypothesis that
gas phase dissociation is a sensitive probe of protein-RNA
interactions. Ribosome EF-G complexes were prepared as described under
"Experimental Procedures" and inhibited with either fusidic acid or
thiostrepton. The spectra recorded for the fusidic acid-inhibited
complex, Fig. 4, display additional peaks
at high m/z. The doublets that appear at
m/z 3,800-4,400 correspond in mass to EF-G and
the high m/z component of the doublet to EF-G GDP
in which the majority of the nucleotide has undergone hydrolysis of GTP
to GDP and remained associated to the elongation factor. Under the
conditions used here EF-G is present in excess, and it is therefore not
clear whether the peaks observed in the mass spectra and assigned to
EF-G are due to the protein factor that is bound to ribosomes or free
in solution. Control experiments, in which GTP is added to EFG in the
absence of ribosomes, however, show no appreciable hydrolysis of GTP
under these conditions. This implies that under the conditions used
here EF-G is in complex with ribosomes, at least transiently, during
GTP hydrolysis.
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In the mass spectrum of the fusidic acid-inhibited complex, peaks can also be assigned to the largest ribosomal protein S1 and to the stalk pentamer ([L7/L12]4 L10), despite the fact that the conditions within the mass spectrometer were optimized to promote dissociation. This observation suggests that, in the ribosome EF-G complex, interactions between these stalk proteins are enhanced. Changes in the interactions of the stalk complex and in the release of S1 are in fact the only significant differences between the spectra recorded for fusidic acid-inhibited complex and those recorded for the 70 S particle alone. This indicates that this ribosome EF-G complex is in a conformation that is largely indistinguishable from naked ribosomes save the changes that persist in both the stalk region and in the binding of protein S1. The high m/z region of the spectrum obtained for the thiostrepton-inhibited complex was closely similar to that obtained with fusidic acid demonstrating the same GTP hydrolysis product associated to EF-G as well as the presence of S1 and the pentameric complex of the stalk proteins.
At the low m/z region of the spectra recorded for
the two complexes there are marked differences (Fig.
5). For the spectrum recorded for the
fusidic acid-inhibited complex the dissociation products are primarily
those from the mobile stalk region and are of comparable intensity to
those observed for solutions of ribosomes at neutral pH (cf.
Fig. 1). Minor increases in the intensity of L11 relative to those of
L7/L12 and L10 are consistent with the enhanced interactions of
L7/L12/L10 in the pentameric stalk complex reducing the extent of
dissociation to individual proteins. By contrast the low
m/z region of the spectrum recorded in the presence of thiostrepton (Fig. 5B) shows that the proteins
L7/L12 that dominate spectra obtained in fusidic acid and naked
ribosomes are virtually absent under these conditions. Moreover, a
number of additional peaks are observed and identified as the proteins L1, L5, L6, and L18.
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Of the additional proteins that are released, the loss of L1 may be accounted for under these conditions because it has an intermediate interaction surface area with rRNA (Fig. 3), extends significantly beyond the RNA envelope, and interacts with only one RNA domain (18). The combination of these effects would suggest that it is likely to be sensitive to perturbations in protein-RNA interactions. Similarly, the binding site of L6 is established in close proximity to the factor binding site (34) (Fig. 5). Its release can be interpreted in terms of a conformational change to the RNA induced by binding of EF-G. It is interesting to note, however, that both L1 and L6 do not appear to be destabilized by binding of EF-G in the presence of fusidic acid providing evidence for a difference in the protein-RNA interactions in the two complexes.
The proteins L5 and L18, which are also released from the thiostrepton-inhibited ribosome EF-G complex, have the largest surface area of interaction with the 5 S RNA (Fig. 3). Their dissociation is therefore consistent with conformational changes, specifically to the 5 S RNA, reducing the surface area of interaction between the RNA and both L5 and L18. Interestingly, L25 which also interacts with 5 S RNA, although with a significantly reduced surface area of interaction compared with those of L5 and L18, is not released from this complex. This implies destabilization of protein 5 S RNA interactions in the region of the binding sites of L5 and L18 (Fig. 5) rather than at the base of the central protuberance where the binding site of L25 is located. In summary the four additional proteins that are released from the thiostrepton-inhibited complex are located either on the periphery of the particle (L1), at the factor binding site (L6), or interact exclusively with the 5 S RNA (L5 and L18).
As the observation of additional proteins can be interpreted in terms of changes to protein-RNA interactions, so too can the presence of non-covalent associations of proteins. For example the observation of the pentameric stalk complex ([L7/L12]4 L10) in the presence of EF-G is consistent with enhanced interactions between these proteins. Examination of the x-ray structure of the ([L7/L12]4 L10) stalk complex reveals that L7/L12 consists of distinct N- and C-terminal domains separated by a hinge region (35). The N-terminal domains are responsible for binding to L10, whereas the highly mobile C-terminal domains are implicated in the translation process, interacting with EF-G and visiting multiple sites on the ribosome (36). Moreover, cryo-EM analysis has established that the stalk proteins become elongated in the presence of EF-G (16, 37). The fact that the pentameric stalk complex is observed in mass spectra in the presence of EF-G in both complexes is therefore in accord with the observation of elongated forms of the stalk region observed by cryo-EM (17, 37).
It is also of interest to note the virtual absence of individual proteins in the mass spectra recorded for the thiostrepton-inhibited EF-G ribosome complex. The L7/L12 proteins that typically dominate all mass spectra often forming the base peak under neutral pH conditions examined here and in previous investigations (2, 3) are barely detectable in the mass spectra of this complex. This strongly implies that the highly mobile C-terminal domains of L7/L12 are anchored to the ribosome in some way. This observation is consistent with a previous finding of a covalent cross-link between L7/L12 and the protein L5 (38). This cross-link has been established both in the presence and absence of EF-G. For L7/L12 to bind at this location at least one dimer of the L7/L12 tetramer would have to be in an extended conformation, lying across the body of the 50 S subunit (39). By contrast the presence of individual proteins in the fusidic acid-inhibited complex indicates that a significant population of the stalk proteins is less constrained and therefore free to dissociate into individual monomers.
In summary the observation of both L5 and L18, two proteins that
interact exclusively with 5 S RNA, together with the absence of L7/L12
proteins in mass spectra of the thiostrepton-inhibited complex is
consistent with binding of the C-terminal domains of L7/L12 to the 5 S
rRNA scaffold itself in the vicinity of the L5/L18-binding site. These
results therefore suggest that in the ribosome EF-G
thiostrepton-inhibited complex, L7/L12 is capable of destabilizing L5
and L18 5 S RNA interactions, which in turn lead to a markedly
different gas phase dissociation pattern. We propose therefore that in
the thiostrepton-inhibited complex, contacts between the elongated form
of the L7/L12 stalk promote dissociation of L5 and L18 through long
range interactions with the 5 S RNA.
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CONCLUSION |
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![]() ![]() ![]() ![]() ![]() ![]() ![]() |
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The dissociation of proteins in the gas phase of the mass
spectrometer in response to solution conditions has been investigated. The results show that increasing pH values from pH 7 to 11 does not
change the dissociation pattern. By contrast for ribosomes analyzed
from low pH solutions, many more proteins are observed in the mass
spectra. Similarly replacement of Mg2+ ions by
Li+ brought about significant changes in gas phase
dissociation. The dependence of protein dissociation on the magnitude
of protein-RNA interactions allows us to investigate solution
conditions where the precise contacts are not well defined. The results
recorded for ribosome EF-G complexes inhibited by thiostrepton and
fusidic acid reveal markedly different dissociation patterns allowing us to demonstrate interactions between mobile regions of the ribosome with the RNA architecture which result in the dissociation of additional proteins. More generally these results highlight a novel
application of MS to probe protein-RNA interactions, an area likely to
be of increasing importance not only with the growing interest in
ribozymes (40), but also for macromolecular complexes for which the
precise protein-nucleic acid interactions have yet to be defined.
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ACKNOWLEDGEMENTS |
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We thank Helena Hernández, Chris Dobson, and the CVR MS research group for helpful discussions and Hannes Ponstingl for performing interaction surface area calculations. C. L. H. is grateful for helpful discussions with Klaus Schneider.
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FOOTNOTES |
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* This work was supported in part by the Biotechnology and Biological Sciences Research Council.The costs of publication of this article were defrayed in part by the payment of page charges. The article must therefore be hereby marked "advertisement" in accordance with 18 U.S.C. Section 1734 solely to indicate this fact.
§ Supported by GlaxoSmithKline.
Supported by the Royal Society. To whom correspondence should
be addressed. Tel.: 44-1223-763846; Fax: 44-1223-763418; E-mail: cvr24@ cam.ac.uk.
Published, JBC Papers in Press, October 29, 2002, DOI 10.1074/jbc.M208966200
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ABBREVIATIONS |
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The abbreviations used are:
MS, mass
spectrometry;
EF-G, elongation factor G;
ToF, time of flight;
SASA, solvent-accessible surface area buried in the respective contact.
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