The molecular mechanisms by which different proteins assemble into highly ordered fibrillar deposits and cause disease remain topics of debate. Human amylin (also known as islet amyloid polypeptide/hIAPP) is found in vivo as amyloid deposits in the pancreatic islets of sufferers of type II diabetes mellitus, and its self-aggregation is thought to be a pathogenic factor in disease and to contribute to the failure of islet transplants. Here, electrospray ionization-ion mobility spectrometry-mass spectrometry (ESI-IMS-MS) has been used to monitor oligomer formation from IAPP. The detection, identification and characterization of oligomers from both human and rat amylin (rIAPP) are described. Oligomers up to and including hexamers have been detected for both peptides. From ESI-IMS-MS derived collision cross sections (CCS), these species are shown to be elongated in conformation. Collision-induced dissociation (CID-MS/MS) revealed differences in the gas-phase stability of the oligomers formed from hIAPP and rIAPP, which may contribute to their differences in amyloid propensity. Using ESI-IMS-MS, the mode of inhibition of amyloid formation from hIAPP using small molecules or co-incubation with rIAPP was also investigated. We show that the polyphenolic compounds epigallocatechin gallate (EGCG) and silibinin bind to specific conformers within a dynamic ensemble of hIAPP monomers, altering the progress of oligomerization and fibril assembly. Hetero-oligomer formation also occurs with rIAPP but leads only to inefficient inhibition. The results indicate that although different small molecules can be effective inhibitors of hIAPP self-assembly, their modes of action are distinct and can be distinguished using ESI-IMS-MS.
The molecular mechanisms by which different proteins assemble into highly ordered fibrillar deposits and cause disease remain topics of debate. Humanamylin (also known as islet amyloid polypeptide/hIAPP) is found in vivo as amyloid deposits in the pancreatic islets of sufferers of type II diabetes mellitus, and its self-aggregation is thought to be a pathogenic factor in disease and to contribute to the failure of islet transplants. Here, electrospray ionization-ion mobility spectrometry-mass spectrometry (ESI-IMS-MS) has been used to monitor oligomer formation from IAPP. The detection, identification and characterization of oligomers from both human and ratamylin (rIAPP) are described. Oligomers up to and including hexamers have been detected for both peptides. From ESI-IMS-MS derived collision cross sections (CCS), these species are shown to be elongated in conformation. Collision-induced dissociation (CID-MS/MS) revealed differences in the gas-phase stability of the oligomers formed from hIAPP and rIAPP, which may contribute to their differences in amyloid propensity. Using ESI-IMS-MS, the mode of inhibition of amyloid formation from hIAPP using small molecules or co-incubation with rIAPP was also investigated. We show that the polyphenolic compoundsepigallocatechin gallate (EGCG) and silibinin bind to specific conformers within a dynamic ensemble of hIAPP monomers, altering the progress of oligomerization and fibril assembly. Hetero-oligomer formation also occurs with rIAPP but leads only to inefficient inhibition. The results indicate that although different small molecules can be effective inhibitors of hIAPP self-assembly, their modes of action are distinct and can be distinguished using ESI-IMS-MS.
Amyloid
disorders are characterized by the aberrant aggregation
of proteins or peptides into amyloid fibrils.[1] In each case, normally soluble proteins or peptides that may be
folded, partially folded, or intrinsically disordered embark on alternative
aggregation energy landscapes[2] leading
to the formation of β-sheet-rich fibrillar assemblies that can
be characterized by the binding of dyes such as Congo red or thioflavin
T (ThT).[3,4] The identity of the toxic species associated
with amyloid diseases is widely debated as a result of the difficulty
of separating, identifying, and individually characterizing these
heterogeneous and transient intermediates of the assembly process.Human islet amyloid polypeptide (hIAPP), also known as amylin,
is a highly amyloidogenic 37-residue peptide hormone produced by the
β-cells of the pancreas. It is produced, stored, and co-secreted
with insulin and plays a role in the control of gastric emptying,
glucose homeostasis, and suppression of glucagon release.[5,6] In its monomeric state, hIAPP is a soluble, intrinsically disordered
polypeptide but forms islet amyloid in cases of type-2 diabetes mellitus
(T2DM).[5,7] Islet amyloid formation leads to β-cell
dysfunction, death, and reduction in β-cell mass[8,9] and contributes to the failure of islet cell transplantation.[5] Amyloid formation by IAPP is highly sequence-specific.[10] hIAPP forms amyloid readily at neutral pH, while
ratIAPP (rIAPP) does not, despite differing in sequence at only six
out of 37 amino acid positions (Figure 1a).
Significantly, five of these amino acid substitutions are located
within residues 20–29, three of which are Pro residues in rIAPP,
leading to supposed disruption of secondary structure formation.[11] Despite numerous studies on the conformational
properties, membrane binding, and aggregation of IAPP,[5,10,12] important challenges remain in
revealing the mechanism of amyloid formation of hIAPP, particularly
in the characterization of oligomeric intermediates, which would enable
detailed studies of the mechanisms of assembly and the effects of
known inhibitors on the aggregation process.[13,14]
Figure 1
hIAPP
forms an array of oligomeric species during fibril formation.
(a) Comparison of hIAPP and rIAPP sequences. Both peptides have a
disulfide bridge between Cys-2 and Cys-7 and have an amidated C-terminus.
Residues that differ from those of the human peptide are colored pink
in the rat sequence. (b) ESI-IMS-MS driftscope plot of the hIAPP oligomers
present 2 min after diluting the monomer to a final peptide concentration
of 50 μM in 20 mM ammonium acetate, pH 6.8, 37 °C, 600
rpm. ESI-IMS-MS driftscope plots show IMS drift time versus m/z versus intensity (z = square root scale), and the corresponding mass spectrum is shown
on the left-hand side. Numbers adjacent to peaks denote oligomer order,
with the positive charge state of each oligomer ions in superscript.
The ESI mass spectrum shows the 2+ and 3+ charge state ions of hIAPP
monomer (labeled 1) and minor amounts of dimer and trimer (labeled
2 and 3, respectively).
hIAPP
forms an array of oligomeric species during fibril formation.
(a) Comparison of hIAPP and rIAPP sequences. Both peptides have a
disulfide bridge between Cys-2 and Cys-7 and have an amidated C-terminus.
Residues that differ from those of the humanpeptide are colored pink
in the rat sequence. (b) ESI-IMS-MS driftscope plot of the hIAPP oligomers
present 2 min after diluting the monomer to a final peptide concentration
of 50 μM in 20 mM ammonium acetate, pH 6.8, 37 °C, 600
rpm. ESI-IMS-MS driftscope plots show IMS drift time versus m/z versus intensity (z = square root scale), and the corresponding mass spectrum is shown
on the left-hand side. Numbers adjacent to peaks denote oligomer order,
with the positive charge state of each oligomer ions in superscript.
The ESI mass spectrum shows the 2+ and 3+ charge state ions of hIAPP
monomer (labeled 1) and minor amounts of dimer and trimer (labeled
2 and 3, respectively).Most conventional biophysical techniques used in the study
of amyloid
systems, including CD, FTIR spectroscopy, and fluorescence-based assays,
are limited to providing data relating to a global average of species
within heterogeneous mixtures. Previous analytical ultracentrifugation
studies,[15] conducted at pH 4.9 where aggregation
is very slow, and 19F NMR studies[16] have failed to detect low order oligomeric species for hIAPP, possibly
due to the low population, or heterogeneous and/or transient nature
of such species. By contrast, photoinduced cross-linking has identified
oligomeric states, including monomer through hexamer.[17] Ion mobility spectrometry-mass spectrometry (IMS-MS) has
the unique advantage of being capable of resolving complex mixtures
of species present in solution, including transiently populated states
and even isobaric species without requiring their prior separation.[18−21] IMS-MS has been utilized previously to provide insights into the
oligomerization pathways of other intrinsically unstructured amyloid-related
peptides and proteins including amyloid-β (Aβ) peptide[20,22] and α-synuclein,[21,23] which are associated
with Alzheimer’s disease and Parkinson’s disease, respectively.
In the case of Aβ40 and Aβ42, oligomeric
species up to and including 16-mer and 12-mer, respectively, have
been identified, and their rotationally averaged collision cross-sectional
areas (CCS) were measured using either positive or negative ion IMS-MS.[20,22] For α-synuclein, the conformeric states of monomers were determined
and the pH dependence of dimer formation was demonstrated.[23] IMS-MS has also provided structural insights
into the hIAPP monomer[24] and dimer,[25] as well as the self-assembly of a series of
short synthetic peptides derived from an amyloidogenic sequence (20–29)
of hIAPP.[26] Using IMS-MS and replica-exchange
molecular dynamics (REMD) simulations, Dupuis et al. proposed that
full-length monomeric hIAPP occupies both a helix–coil conformation
and an extended β-hairpin conformation that has a significantly
(18%) larger collision cross-section (CCS).[24] These extended hairpin structures were not observed for rIAPP, leading
to the conclusion that this conformer is an amyloidogenic precursor.
Dupuis et al. also investigated dimeric structures of hIAPP, using
IMS-MS, reporting that the dimers observed are significantly more
extended than those formed by rIAPP, suggestive of a higher percentage
of β-sheet content that is formed from extended β-hairpin-containing
monomers.[25] An early conformational transition
to β-sheet-rich conformers was proposed, therefore, as a first
step in hIAPP self-assembly, by contrast with other reports that have
suggested a transition to amyloid via helix-rich oligomers.[27−29] None of these studies, however, reported the detection or identification
of higher order species.A wealth of studies has assessed the
ability of small molecules
to interfere with the progress of fibril formation from many amyloid-prone
peptides and proteins in vitro.[29−31] Despite these analyses, the precise
mechanisms of inhibition remain elusive. Currently, there are no clinically
approved inhibitors of hIAPP assembly. In addition, the mode of action
of small molecule inhibitors of hIAPP aggregation is not well understood.
Electrospray ionization (ESI)-IMS-MS has been utilized previously
to identify inhibitors of β-2-microglobulin (β2m) amyloid formation.[32] Using a similar
approach, we aimed here to detect, identify, and characterize oligomeric
intermediates of hIAPP aassembly and, thereby, to determine the mode
of action of two known small molecule inhibitors of hIAPP amyloid
formation, epigallocatechin gallate (EGCG)[33] and silibinin.[34] In addition, we used
ESI-IMS-MS to investigate the moderately effective inhibition caused
by mixing hIAPP and rIAPP.[11] EGCG is one
of the most effective amyloid inhibitors known[35] and has generated considerable attention given its ability
to inhibit or modulate amyloid formation from a diverse range of polypeptides.
Despite the plethora of these studies[33,35−40] and the interest they have generated, the mode of action of EGCG
is not well understood. It is thought to direct some, but not all,
amyloidogenic proteins into off-pathway aggregates.[33,35]Here, using ESI-IMS-MS, we demonstrate the presence of high
order
oligomers formed by both hIAPP and rIAPP and use this technique to
determine the populations, shapes, and gas-phase stabilities of these
co-populated, transient species. The results reveal significant differences
in the stability of otherwise similarly organized oligomers of these
peptides. In addition, the binding of the small molecule inhibitors,
EGCG and silibinin, to specific conformers within the dynamic ensemble
of hIAPP species has also been ascertained, and the progress of oligomer
formation and fibril assembly and disassembly was monitored. The results
indicate that ligand binding either arrests oligomerization (silibinin)
or diverts hIAPP onto new assembly routes resulting in the formation
of amorphous aggregates without a buildup of oligomeric species (EGCG).
The results presented provide evidence for the mode of action of these
two effective small molecule inhibitors of hIAPP amyloid formation
and reveal why rIAPP is such a poor inhibitor of hIAPP assembly.
Experimental Section
Sample Preparation for
MS
hIAPP and rIAPP were synthesized
and purified as described previously.[41] Lyophilized peptide samples were dissolved in dimethyl sulfoxide
(DMSO) at a final concentration of peptide of 5 mM. After 24 h of
incubation at 25 °C, stock solutions were diluted 100-fold into
20 mM ammonium acetate, pH 6.8, to a final peptide concentration of
50 μM for MS analysis. The final concentration of DMSO was 1%
(v/v). All samples were incubated at 37 °C in 96-well plates
with or without agitation (600 rpm). Experiments were repeated at
a range of IAPP concentrations, from 10 μM to 100 μM.
As expected, there is a concentration-dependence of the rate of fibril
formation and oligomer consumption as measured using ESI-IMS-MS. However,
the oligomers formed are of the same mass and CCS under each condition.
ESI-(IMS)-MS Analysis
A Synapt HDMS quadrupole time-of-flight
mass spectrometer (Micromass UK Ltd., Waters Corpn., Manchester, U.K.),
equipped with a Triversa (Advion Biosciences, Ithaca, NY, U.S.) automated
nano-ESI interface, was used for these analyses. Positive ion mode
was chosen because IAPP has a pI of >9 and therefore should be
predominantly
positively charged at near-neutral pH. The instrument has a traveling-wave
IMS device situated in-between the quadrupole and the time-of-flight
analyzers and has been described in detail elsewhere.[42] Samples were analyzed by positive ionization nanoESI (nESI)
with a capillary voltage of 1.7 kV and a nitrogen nebulizing gas pressure
of 0.8 psi. The following instrumental parameters were used: cone
voltage 30–100 V; source temperature 60 °C; backing pressure
4.0 mBar; ramped traveling wave height 7–20 V; traveling wave
speed 400 m/s; IMS nitrogen gas flow 20 mL/min; IMS cell pressure
0.55 mBar. The cone voltage was optimized to transmit the higher order
peptide oligomers; the CCS of the oligomers did not alter over the
range 30–100 V. Data were processed by use of MassLynx v4.1
and Driftscope software supplied with the mass spectrometer. The m/z scale was calibrated with aq CsI cluster
ions. CCSs were estimated by use of an IMS-MS calibration.[43] Calibration of the drift time cross-section
function was achieved by analysis of the denatured proteins equinecytochrome c and horse heart myoglobin (10 μM
in 50:40:10, v/v/v, acetonitrile/water/acetic acid[44]), whose CCS values had been predetermined elsewhere by
use of conventional ion mobility measurements.[44]The collision cross-sectional areas (Ω) of
the analytes were then obtained after calibration from their corrected
drift times according to eq 1:[43]This step also includes an
adjustment for the mass and charge of the protein ions, where Ω
is the calibrated collision cross-section, A is the
calibration determined constant, tD′
is the absolute drift time (corrected), z is the
charge state of the ion, mion is the mass
of the ion, and mgas is the mass of the
target gas used in the IMS cell. The exponential factor B is determined
experimentally.[43]Collision induced
dissociation (CID) MS/MS experiments were performed
using the quadrupole analyzer to select isobaric m/z ions representing the dimer and tetramer, separating
these ions in the IMS device and performing CID in the transfer collision
cell prior to the time-of-flight analyzer (the pressure in the collision
cell was kept constant). Increasing collision energy was applied to
the transfer collision cell in 10 V increments from 10 to 100 V until
the oligomers ions were completely dissociated into monomer ions.
CID energies are displayed as center of mass energy (eV) by use of
the eq 2:where z is the charge state
of the ion, EMS is the collision energy
used (eV), Margon is the mass of argon
the collision gas, and Mion is the mass
of the analyte of interest. Note that the equation is missing a multiplication
factor of e, elementary charge (1.602 × 10–19 C). This has been omitted as conversion of the zeVMS from Joules to electron volts is facilitated
by division of e.
Fibril Depolymerization
A mixed sample containing a
1:1 molar ratio of hIAPP:rIAPP was prepared by diluting 5 mM stock
solutions of each peptide in DMSO 100-fold into 20 mM ammonium acetate,
pH 6.8, to a final concentration of each peptide of 50 μM in
1% (v/v) DMSO for MS analysis. After 5 days of incubation at 37 °C
and 600 rpm, mixed samples were centrifuged in a Beckman ultracentrifuge
at 300,000g for 45 min. Fibrillar samples in the
pellet were depolymerized by incubation in 100% (v/v) HFIP for 24
h. Samples were air-dried and then redissolved in 50:40:10 (v/v/v)
acetonitrile/water/acetic acid, and fibril constituent peptides were
identified by ESI-MS.
Analysis of Ligand Binding to Monomeric hIAPP
hIAPP
(50 μM) was dissolved in 20 mM ammonium acetate (pH 6.8) containing
5, 50, or 500 μM EGCG or silibinin in 1% (v/v) DMSO. For analysis
of these samples by nESI-MS, a sampling cone voltage of 30 V was used
to preserve protein–ligand interactions, and a backing pressure
of 3.0 mbar was applied. Data were acquired over the range m/z 400–8,000. For IMS-MS experiments,
the wave height was ramped from 7 to 20 V at a speed of 300 m/s.
Thioflavin T Fluorescence Assays
Samples were prepared
in a 96-well plate (Corning Costar 3915, Corning Life Sciences, Amsterdam,
The Netherlands) sealed with clear sealing film and were incubated
in a FLUOstar OPTIMA plate reader (BMG Labtech, Aylesbury, Bucks,
U.K.) for 5 days at 37 °C with or without agitation (600 rpm).
Samples had a volume of 100 μL containing 100 μM ThT and
50 μM peptide in 20 mM ammonium acetate, pH 6.8 and a 1% (v/v)
final concentration of DMSO. Fluorescence was excited at 440 nm, and
emission intensity was measured at 485 nm. Turbidity measurements
were performed by monitoring the apparent absorbance at 635 nm using
a NEPHALOstar Galaxy reader (BMG Labtech, Aylesbury, Bucks, UK) and
96-well clear plates sealed with clear sealing film. For these experiments,
the samples were prepared as described above, except that ThT was
not included. In each experiment readings were taken every 5 min,
from 2 min to 50 h. In parallel, samples were analyzed at different
time points (but in the absence of ThT) using ESI-IMS-MS. Each experiment
under each condition was repeated a minimum of three times with at
least triplicate measurements for each condition, and representative
traces are shown.
Transmission Electron Microscopy (TEM)
The TEM images
of each 50 μM peptide solution were acquired after 5 days of
incubation at 37 °C on a CM10 microscope (Phillips, Electron
Optics, Amsterdam, The Netherlands). Carbon grids were prepared by
irradiating under UV light for 30 min and stained with 4% (w/v) uranyl
acetate solution as described previously.[45]
Results
hIAPP Forms an Array of Oligomers Early in
Amyloid Assembly
To understand the aggregation process of
amyloid-prone peptides
and proteins, oligomeric intermediates need to be identified and characterized
in detail. Here, by exploiting the separative and investigative powers
of MS coupled with IMS and CID-MS/MS, we describe higher order oligomeric
states populated by hIAPP and rIAPP and elucidate their CCS, growth
mechanism, and relative gas-phase stability. The rat and human peptides
were each dissolved in 100% DMSO to remove any preformed aggregates[46] and diluted 100-fold into 20 mM ammonium acetate,
pH 6.8, and the distribution of oligomeric species was analyzed immediately
and at various time points after dilution, using ESI-IMS-MS. The data
obtained (Figure 1b) showed that oligomers
up to and including hexamers are formed within 2 min of dilution of
hIAPP into buffer. ESI-IMS-MS allows co-populated oligomeric ions
with the same m/z to be separated
and identified individually (e.g., dimer3+ and tetramer6+) (Figure 1b). Multiple charge states,
predominantly doubly and triply charged, and different conformers,
both compact and expanded for species of the same mass, are observed
for the hIAPP monomer at this pH. For example, the monomer 2+ ions
occupy two distinct peaks in the IMS-MS spectrum (Figure 1b) with drift times of 7.6 and 10.6 ms. These represent
two conformations of this charge state, which have CCSs that differ
by a significant ∼15%. Although less well-resolved, the monomer
3+ ions also exhibit two distinct conformations, having drift times
of 6.0 and 8.0 ms, a ∼14% difference in their CCS (Figure 1b). Oligomers of hIAPP also populate a range of
charge states and conformations, for each of which the CCS was determined
(Supporting Information, Table 1).Previous studies have shown that increased ionic strength increases
the rate of aggregation of many proteins and peptides, including hIAPP.[47] To investigate whether the presence of oligomers
of hIAPP correlates with the ability of the peptide to assemble into
amyloid fibrils, the ionic-strength dependency of the oligomers of
hIAPP observed using ESI-IMS-MS was investigated and compared with
the rate of fibril formation, measured using ThT fluorescence. Under
the conditions employed, an enhanced rate of amyloid formation is
observed as the ionic strength is increased from 20 to 500 mM, consistent
with previous studies[47] (Figure 2a). Gross fibril morphology was unchanged with the
buffer conditions employed (a representative TEM image is shown (Figure 2b)). A more rapid decrease in oligomer signal intensity
over time was also detected with increasing ionic strength (using
ESI-IMS-MS, Figure 2c), consistent with the
oligomers observed being involved in assembly into amyloid.
Figure 2
Dependence
of hIAPP oligomer and fibril formation on ionic strength.
(a) ThT fluorescence intensity of hIAPP (50 μM peptide, 37 °C,
600 rpm) in 20 mM (squares/purple), 100 mM (triangles/orange), or
500 mM (circles/green) ammonium acetate buffer, pH 6.8. (b) Representative
negative stain TEM image of hIAPP fibrils after 5 days in 100 mM buffer
(37 °C, 600 rpm) (scale bar = 100 nm). (c) ESI-IMS-MS driftscope
plots of hIAPP oligomers present at t = 2 min (left-hand
side) and t = 5 h (right-hand side) at different
ionic strengths (20, 100, and 500 mM). (d) CCSs of hIAPP oligomers
measured using ESI-IMS-MS plotted versus oligomer order showing that
oligomers have the same CCS regardless of ionic strength: 20 mM (squares),
100 mM (triangles), and 500 mM (circles). The orange dashed line represents
a globular fit based on the average density of a protein (0.44 Da/Å3),[49] the purple dashed line represents
a linear growth model,[48] and the green
dashed line represents an isotropic growth model.[48]
Dependence
of hIAPP oligomer and fibril formation on ionic strength.
(a) ThT fluorescence intensity of hIAPP (50 μM peptide, 37 °C,
600 rpm) in 20 mM (squares/purple), 100 mM (triangles/orange), or
500 mM (circles/green) ammonium acetate buffer, pH 6.8. (b) Representative
negative stain TEM image of hIAPP fibrils after 5 days in 100 mM buffer
(37 °C, 600 rpm) (scale bar = 100 nm). (c) ESI-IMS-MS driftscope
plots of hIAPP oligomers present at t = 2 min (left-hand
side) and t = 5 h (right-hand side) at different
ionic strengths (20, 100, and 500 mM). (d) CCSs of hIAPP oligomers
measured using ESI-IMS-MS plotted versus oligomer order showing that
oligomers have the same CCS regardless of ionic strength: 20 mM (squares),
100 mM (triangles), and 500 mM (circles). The orange dashed line represents
a globular fit based on the average density of a protein (0.44 Da/Å3),[49] the purple dashed line represents
a linear growth model,[48] and the green
dashed line represents an isotropic growth model.[48]To probe the properties of the
oligomers formed from hIAPP in more
detail, their CCSs were estimated from the ESI-IMS-MS arrival time
distributions and compared with CCSs estimated for theoretical models
including a fit assuming isotropic growth,[48] a globular fit based on the average density of a protein under similar
conditions (0.44 Da/Å3),[49,50] and a model that assumes growth in a single dimension[48] (note that more detailed molecular models cannot
be generated for the underlying structures of the oligomers detected,
given the lack of information about the type, location, or extent
of secondary structure in these species). CCS determination (Experimental Section) suggests that hIAPP oligomers
≥4-mer in size adopt an extended conformation and that the
CCS of the different oligomers observed are independent of ionic strength
(Figure 2d). However, the relative population
of compact vs expanded monomeric and dimeric conformers is altered
with increasing ionic strength (discussed below).
CID Reveals
Differences in Gas-Phase Stability between hIAPP
and rIAPP Oligomers and Monomers
For rIAPP, which does not
form ordered amyloid fibrils when incubated at near neutral pH,[5] a surprisingly similar array of oligomers was
observed using ESI-IMS-MS compared with that detected for hIAPP (Figure 3a, Supporting Information Figures S1a and S2). Akin to the results observed for hIAPP, multiple
conformers are observed for rIAPP monomer and oligomers, albeit at
different relative intensities compared with those observed for hIAPP.
Accordingly, hIAPP consistently occupies a greater proportion of more
expanded conformers than rIAPP (Supporting Information Figure S1b). To investigate the relative stabilities of the different
monomeric conformers of hIAPP and rIAPP, the dependence of the ion
arrival time distribution versus increasing the trap energy (used
to effect CID) was examined (Supporting Information, Figure S1c). The results of these experiments showed that hIAPP
monomer 3+ ions unfold at lower trap collision energies than those
required for the rIAPP monomer, with hIAPP more readily converting
to expanded conformers at lower trap voltages (Supporting Information Figure S1c).
Figure 3
Oligomers formed from
rIAPP resemble those of hIAPP. (a) ESI-IMS-MS
driftscope plot of rIAPP oligomers present at 2 min after dilution
into 20 mM ammonium acetate buffer, pH 6.8 to a final peptide concentration
of 50 μM. The number adjacent to each peak denotes oligomer
order with charge state of the oligomer in superscript. (b) Aggregation
of rIAPP (diamonds) and hIAPP (circles) monitored using turbidity
at 635 nm. In both cases, 50 μM peptide was incubated in 20
mM ammonium acetate buffer, pH 6.8 (37 °C, 600 rpm). (c) Negative
stain TEM image of rIAPP aggregates after 5 days of incubation (37
°C, 600 rpm); scale bar = 100 nm. (d) ThT fluorescence intensity
of rIAPP (50 μM peptide, 37 °C, pH 6.8, 600 rpm). The data
are normalized to the signal intensity of a hIAPP fibril formation
end point at the same peptide concentration.
Oligomers formed from
rIAPP resemble those of hIAPP. (a) ESI-IMS-MS
driftscope plot of rIAPP oligomers present at 2 min after dilution
into 20 mM ammonium acetate buffer, pH 6.8 to a final peptide concentration
of 50 μM. The number adjacent to each peak denotes oligomer
order with charge state of the oligomer in superscript. (b) Aggregation
of rIAPP (diamonds) and hIAPP (circles) monitored using turbidity
at 635 nm. In both cases, 50 μM peptide was incubated in 20
mM ammonium acetate buffer, pH 6.8 (37 °C, 600 rpm). (c) Negative
stain TEM image of rIAPP aggregates after 5 days of incubation (37
°C, 600 rpm); scale bar = 100 nm. (d) ThT fluorescence intensity
of rIAPP (50 μM peptide, 37 °C, pH 6.8, 600 rpm). The data
are normalized to the signal intensity of a hIAPP fibril formation
end point at the same peptide concentration.Although rIAPP has been reported previously not to form amyloid
fibrils,[5] turbidity measurements (Figure 3b) and TEM images (Figure 3c) showed that under the conditions employed here (20 mM ammonium
acetate, pH 6.8, 1% DMSO (v/v)), rIAPP forms small globular aggregates
that scatter light but do not bind ThT (Figure 3d). The rIAPP oligomers observed are similar in CCS, as well as order
and mass, to those of hIAPP (Supporting Information Table S1 and Figures S1a and S3). These results indicate, therefore,
that the presence of oligomers of similar numbers of subunits and
CCS cannot account for the very different amyloidogenic properties
of the two sequences.Next, the gas-phase stabilities of oligomers
of hIAPP and rIAPP
were probed to investigate whether their gas-phase dissociation can
be related to the differences in the ability of these sequences to
form amyloid. These oligomers are not amenable to solution-phase stability
assays, since they are so lowly populated and co-populated with each
other and the monomeric species. Accordingly, CID-MS/MS was utilized
to provide a side-by-side comparison of the gas-phase stabilities
of the two peptides in different oligomeric forms. In this experiment,
ions of specific m/z were selected
by the quadrupole analyzer, followed by IMS separation of the different
oligomers contributing to this m/z and then sequential fragmentation of the oligomer ions in the transfer
collision cell immediately prior to the time-of-flight analyzer. The
data revealed that hIAPP dimers are significantly less stable than
rIAPP dimers in the gas phase. hIAPP dimers were found to dissociate
into monomer at an energy (0.4 eV) that is lower than that required
for the equivalent rIAPP dimers, which only began to dissociate at
0.7 eV (Figure 4a). Oligomeric species, including
tetramer ions with six charges, also showed subtle differences in
stability for the two sequences. The hIAPP tetramer6+ ions
begin to dissociate at 0.3 eV, whereas rat tetramer6+ ions
remain fully associated until an energy of 0.5 eV is applied (Supporting Information Figure S4a,b). The significant
difference in the gas-phase stability of the dimer ions of hIAPP and
rIAPP could be related to the capability of hIAPP to access amyloidogenic
conformations more easily than its rIAPP counterpart. Consistent with
this view, the expanded conformers of the hIAPP monomer and dimer
ions became increased in population, and the dimer 3+ ions become
less stable in the gas phase as the ionic strength of the buffer used
is increased (Figure 4b). This supports the
hypothesis that peptide gas-phase stability is inversely correlated
with the amyloid competence of IAPP, given that both the hIAPP monomer
and its oligomers are less stable than their counterparts for the
rat sequence and that high ionic strength destabilizes oligomers and
increases the rate of amyloid fibril formation for hIAPP.
Figure 4
Differences
between rIAPP and hIAPP dimer and monomer stabilities
in the gas phase measured using collision induced dissociation (CID).
(a) CID MS/MS of rIAPP (blue) and hIAPP (red) dimers (50 μM
peptide, 20 mM ammonium acetate buffer, pH 6.8). Relative intensity
of the 3+ dimer ions (squares) of each peptide is plotted versus increasing
ion-accelerating voltage into the transfer T-wave collision cell (CID).
Monomer ion intensity (diamonds) increases as dimers (squares) dissociate.
Bar chart (inset) showing the appearance of hIAPP (red) and rIAPP
(blue) monomer from dissociation of dimer ions with increasing CID
voltage. (b) Arrival time distributions (ATDs) of 3+ hIAPP monomer
ions 2 min after dissolving into 50 mM (purple), 100 mM (orange),
or 500 mM (green) ammonium acetate, pH 6.8. Bar chart (inset) showing
relative intensity of monomer ions with increasing ion-accelerating
voltage at different ionic strengths: 50 mM (green), 100 mM (orange),
and 500 mM (purple) (25 μM peptide, 50/100/500 mM ammonium acetate
buffer, pH 6.8).
Differences
between rIAPP and hIAPP dimer and monomer stabilities
in the gas phase measured using collision induced dissociation (CID).
(a) CID MS/MS of rIAPP (blue) and hIAPP (red) dimers (50 μM
peptide, 20 mM ammonium acetate buffer, pH 6.8). Relative intensity
of the 3+ dimer ions (squares) of each peptide is plotted versus increasing
ion-accelerating voltage into the transfer T-wave collision cell (CID).
Monomer ion intensity (diamonds) increases as dimers (squares) dissociate.
Bar chart (inset) showing the appearance of hIAPP (red) and rIAPP
(blue) monomer from dissociation of dimer ions with increasing CID
voltage. (b) Arrival time distributions (ATDs) of 3+ hIAPP monomer
ions 2 min after dissolving into 50 mM (purple), 100 mM (orange),
or 500 mM (green) ammonium acetate, pH 6.8. Bar chart (inset) showing
relative intensity of monomer ions with increasing ion-accelerating
voltage at different ionic strengths: 50 mM (green), 100 mM (orange),
and 500 mM (purple) (25 μM peptide, 50/100/500 mM ammonium acetate
buffer, pH 6.8).
Probing the Mechanism of
Inhibition of hIAPP Fibril Formation
with Small Molecules
Having identified the prefibrillar species
populated by hIAPP, the mode of action of two known small molecule
inhibitors of hIAPP fibril formation was investigated using ESI-IMS-MS.
In these experiments, hIAPP (50 μM) was incubated at 37 °C
in 20 mM ammonium acetate buffer, pH 6.8, in the presence of EGCG[33,35] or silibinin[34] at molar ratios of small
molecule:hIAPP of 0.1:1, 1:1, or 10:1. The oligomer populations were
characterized subsequently using ESI-IMS-MS. To complement the gas-phase
analyses, fibril formation was monitored by ThT fluorescence, and
peptide aggregates were characterized using negative stain EM. The
primary objectives here were to determine how the presence (or binding)
of each small molecule affects the distribution of monomeric conformers
and populations of oligomers and whether such changes can be correlated
with the inhibition of hIAPP amyloid formation.
Action
of EGCG on Fibril Formation of hIAPP
Probed by ESI-IMS-MS
EGCG, a polyphenol flavanol found in
green tea, has shown promise as a generic anti-amyloid agent as this
small molecule has been found to redirect aggregating proteins onto
alternative pathways[35] or to maintain them
in a native-like state.[37] It has also been
shown to promote remodeling of mature amyloid fibrils,[33] with recent work of Kelly et al. demonstrating
that hydrophobic binding to the amyloid fibril by EGCG is a significant
step in this process.[40] Despite being proposed
as a potent inhibitor of amyloid formation for several proteins and
peptides including hIAPP,[36] α-synuclein,
and Aβ42,[35] the mode of
action of EGCG remains elusive. To identify the effects of EGCG on
hIAPP aggregation, the binding capabilities of individual monomeric
conformers of hIAPP for EGCG were investigated. The results revealed
that EGCG binds to monomeric hIAPP (∼10% monomer remains bound
in the gas phase) (Figure 5a) (note that estimating Kd values of binding events by MS was not feasible
in this instance, given the difficulty of maintaining quantitative
amounts of bound ligand in the gas phase). The presence of the small
molecule also alters the equilibrium of monomer charge states present.
The monomer 3+ ions are more highly populated in samples incubated
with EGCG (compare Figures 1b and 5a), with a change in ratio of 3+:2+ monomer charge
states in the spectra changing from ∼1:2 to ∼1:1.2 in
the presence of the ligand. It is possible that the changes in monomer
charge state distribution observed may arise from direct binding of
EGCG to the monomer that causes conformational changes and hence alters
the profile of the charge state distribution, despite the ligand dissociating
in the gas phase. Alternatively, changes in the charge state distribution
may arise from gas-phase dissociation of ligand-bound higher order
oligomeric species. In addition to its effects on the monomeric conformers
of hIAPP, EGCG binding inhibits assembly of the peptide into higher
order oligomers and fibrils (Figure 5b–d).
Both of the observed charge states (2+ and 3+) of the hIAPP monomer
(Figure 5a) and indeed each monomeric conformer
(both the expanded and the compact form of each charge state) (Supporting Information Figure S5) are bound by
EGCG, with one or two molecules binding to one doubly charged monomer
and up to three EGCG molecules binding to the triply charged monomer
when EGCG is added in an 10-fold molar excess over hIAPP (Figure 5a). Binding of EGCG to both the 2+ and 3+ monomer
ions was also observed at a stoichiometry of 1:1 hIAPP:EGCG, albeit
at a lower intensity (data not shown). The low levels of binding observed,
despite complete inhibition of fibrillation, are consistent with hydrophobic
interactions playing a role in the binding interface[36] and may help toward explaining the ability of EGCG to inhibit
a wide range of natively unfolded polypeptides, including IAPP mutants.[37,38]
Figure 5
Inhibition
of hIAPP fibril formation by EGCG. (a) Positive ion
ESI mass spectrum showing binding of EGCG (added at 500 μM to
50 μM peptide) to both the 2+ (orange) and 3+ (purple) charge
state ions of hIAPP monomer. Stoichiometry of binding is shown by
color: 1:1 inhibitor molecule bound to an IAPP monomer is highlighted
in green, 2:1 in pink, and 3:1 in blue. EGCG is shown as an inset.
(b) ThT fluorescence intensity of hIAPP (black) (50 μM peptide,
20 mM ammonium acetate buffer, pH 6.8, 37 °C, 600 rpm) with increasing
EGCG:hIAPP molar ratios: 0.1:1 (pink), 1:1 (orange), and 10:1 (blue).
(c) ESI-IMS-MS driftscope plots of hIAPP oligomers formed in the presence
of (i) 0.1:1, (ii) 1:1, and (iii) 10:1 molar ratios of EGCG:peptide
monomer at t = 5 h. The number of EGCG molecules
bound to each species is shown as a colored dot. (d) Negative stain
TEM images of hIAPP incubated with (i) 0.1:1, (ii) 1:1, and (iii)
10:1 molar ratios of EGCG for 5 days (37 °C, 600 rpm). (iv) hIAPP
fibrils alone and aggregates formed when a 10-fold molar excess of
EGCG:hIAPP is added to preformed hIAPP fibrils after 5 h (v) and 24
h (vi). Scale bar is 100 nm.
Inhibition
of hIAPP fibril formation by EGCG. (a) Positive ion
ESI mass spectrum showing binding of EGCG (added at 500 μM to
50 μM peptide) to both the 2+ (orange) and 3+ (purple) charge
state ions of hIAPP monomer. Stoichiometry of binding is shown by
color: 1:1 inhibitor molecule bound to an IAPP monomer is highlighted
in green, 2:1 in pink, and 3:1 in blue. EGCG is shown as an inset.
(b) ThT fluorescence intensity of hIAPP (black) (50 μM peptide,
20 mM ammonium acetate buffer, pH 6.8, 37 °C, 600 rpm) with increasing
EGCG:hIAPP molar ratios: 0.1:1 (pink), 1:1 (orange), and 10:1 (blue).
(c) ESI-IMS-MS driftscope plots of hIAPP oligomers formed in the presence
of (i) 0.1:1, (ii) 1:1, and (iii) 10:1 molar ratios of EGCG:peptide
monomer at t = 5 h. The number of EGCG molecules
bound to each species is shown as a colored dot. (d) Negative stain
TEM images of hIAPP incubated with (i) 0.1:1, (ii) 1:1, and (iii)
10:1 molar ratios of EGCG for 5 days (37 °C, 600 rpm). (iv) hIAPP
fibrils alone and aggregates formed when a 10-fold molar excess of
EGCG:hIAPP is added to preformed hIAPP fibrils after 5 h (v) and 24
h (vi). Scale bar is 100 nm.ESI-IMS-MS data (Figure 5c) reveal
that
incubation with increasing molar ratios of EGCG:hIAPP prevents the
appearance of higher order oligomers in a dose-dependent manner. At
0.1:1 and 1:1 molar ratios of EGCG:hIAPP, monomer through tetramer
species of hIAPP are observed (Figure 5c),
but no pentamer or hexamer (which were observed in the absence of
the small molecule (Figure 1b)). At a 10:1
molar ratio of EGCG:hIAPP, no oligomers are observed (Figure 5c). Under the latter conditions, there is no increase
in ThT fluorescence (Figure 5b), and TEM images
(Figure 5d, panel iii) do not show any aggregated
material, indicating complete inhibition of amorphous aggregate and
amyloid formation. These results suggest that EGCG may trap amyloidogenic
oligomers as low order species and differentially stabilize distinct
monomeric charge states of hIAPP with the result that amyloid fibrils
cannot form. Alternatively, EGCG may divert low order oligomers of
hIAPP onto other aggregation pathways that result in the formation
of aggregates that are incapable of forming amyloid. In the latter
scenario, the oligomers that form must be of low abundance, low ionization
propensity, or too heterogeneous to be detected by ESI-IMS-MS.
Remodeling of Mature IAPP Fibrils by EGCG
In addition
to its ability to remodel oligomers,[35] EGCG
has been shown previously to remodel amyloid fibrils formed by a range
of polypeptides, including hIAPP.[35,36] Having determined
the effect of EGCG on the aggregation reaction of hIAPP, the effect
of this small molecule on fibril depolymerization was studied also,
using TEM to monitor fibril loss and ESI-IMS-MS to investigate how
fibril remodeling by EGCG influences oligomer populations. Fibril
samples formed by incubation of hIAPP at pH 6.8 for 5 days were mixed
with a 10-fold molar excess of EGCG, and the subsequent loss of fibrils
was monitored by TEM and ESI-IMS-MS at various time points after addition
of the small molecule. The results of these experiments are shown
in Figure 5d (panels iv–vi) and in Supplementary Figure S6a. Under the conditions
employed, clumping of hIAPP fibrils followed by remodeling into amorphous
aggregates over a 24 h period was observed (Figure 5d, panels iv–vi). This is accompanied by a subtle increase
in intensity of the signal arising from monomer ions, measured using
ESI-IMS-MS, compared with the same sample prior to addition of EGCG
(Supporting Information Figure S6a). There
is, however, an absence of higher order oligomers indicating that
fibril remodeling by EGCG does not result in the reformation of higher
order oligomeric species.
Action of Silibinin on Fibril
Formation of hIAPP
Probed by ESI-IMS-MS
Silibinin, a flavonol extracted from
seeds of the herb milk thistle, has been proposed as a potential therapeutic
for amyloidosis associated with T2DM.[34] The interaction of this inhibitor with hIAPP was also probed using
ESI-IMS-MS. The resulting data (Figure 6a)
revealed that silibinin binds to the 3+ charge state ions of monomeric
hIAPP (∼20% remaining bound in the gas phase), with no detectable
binding to the 2+ charge state ions of the monomer. This may be due
to selectivity of the small molecule or the low abundance of the 2+
charge state in the presence of the small molecule. In the latter
case, the intensity of ligand-bound ions may fall below the levels
of detection. Like EGCG, but more obviously, the presence of excess
silibinin alters the equilibrium of the two different charge states
of monomeric hIAPP, favoring the population of the triply charged
monomer ions, changing the ratio of 3+:2+ monomer charge state ions
in the spectra from ∼1:2 without silibinin to ∼3:1 in
the presence of the small molecule. In addition, analysis using ESI-IMS-MS
indicates that the presence of substoichiometric ratios of silibinin:hIAPP
prevents hIAPP oligomer formation (Figure 6b). More specifically, binding of silibinin is observed only to the
expanded conformer of the 3+ monomer ions (Figure 6c). This conformer (CCS = ∼790 Å2),
adopted by the hIAPP monomer, but not the rIAPP monomer (Supporting Information Figure S1b,ii), has been
proposed previously as the on-pathway, amyloid-competent conformation,
the formation of which precedes the generation of extended dimers
and β-sheet-rich oligomers.[24,25] There is no
detectable binding of silbinin to the rIAPP monomer when incubated
under identical conditions (Supporting Information Figure S7). Specific binding to the expanded monomer conformation
of hIAPP is thus consistent with the ability of silibinin to inhibit
amyloid formation. ThT data (Figure 6d) showed
that aggregation of hIAPP decreases significantly as the concentration
of silibinin is increased, although in a 10-fold molar excess of silibinin
a weak positive ThT signal is still observed (Figure 6d), likely due to the presence of aggregates not visible by
ESI-IMS-MS. TEM images indicated that incubation of monomeric hIAPP
with silibinin for 5 days leads to few aggregates, with none visible
by TEM when a 10-fold molar excess of silibinin:hIAPP is used (Figure 6e, panels i–iii).
Figure 6
Inhibition of hIAPP fibril
formation by silibinin. (a) Positive
ion ESI mass spectra showing binding of silibinin molecules (added
at 500 μM to 50 μM peptide) to the 3+ monomer ions (purple)
and absence of binding to the 2+ monomer ions (orange) at a molar
ratio of silibinin:hIAPP of 10:1. The structure of silibinin is inset.
(b) ESI-IMS-MS driftscope plots showing the lack of hIAPP oligomers
in the presence of 0.1:1, 1:1, and 10:1 molar ratios of silibinin:hIAPP
at t = 5 h. (c) Arrival time distribution of 3+ monomer
ions shows two conformers are present (tD = 6 and 8 ms). Silibinin binds to the extended conformer of the
3+ monomer ions (pink) but does not bind to the compact conformer
(blue). (d) ThT fluorescence intensity of hIAPP (black) (50 μM
peptide, 20 mM ammonium acetate buffer, pH 6.8, 37 °C, 600 rpm)
with increasing silibinin:hIAPP molar ratios: 0.1:1 (pink), 1:1 (orange),
and 10:1 (blue). (e) Negative stain TEM images of hIAPP incubated
with (i) 0.1:1, (ii) 1:1, and (iii) 10:1 molar ratios of silibinin:hIAPP
for 5 days (37 °C, 600 rpm). Lower panels show hIAPP fibrils
alone (iv) and aggregates formed when a 10-fold molar excess of silibinin:hIAPP
is added to preformed hIAPP fibrils after 5 h (v) and 24 h (vi). Scale
bar is 100 nm.
Inhibition of hIAPP fibril
formation by silibinin. (a) Positive
ion ESI mass spectra showing binding of silibinin molecules (added
at 500 μM to 50 μM peptide) to the 3+ monomer ions (purple)
and absence of binding to the 2+ monomer ions (orange) at a molar
ratio of silibinin:hIAPP of 10:1. The structure of silibinin is inset.
(b) ESI-IMS-MS driftscope plots showing the lack of hIAPP oligomers
in the presence of 0.1:1, 1:1, and 10:1 molar ratios of silibinin:hIAPP
at t = 5 h. (c) Arrival time distribution of 3+ monomer
ions shows two conformers are present (tD = 6 and 8 ms). Silibinin binds to the extended conformer of the
3+ monomer ions (pink) but does not bind to the compact conformer
(blue). (d) ThT fluorescence intensity of hIAPP (black) (50 μM
peptide, 20 mM ammonium acetate buffer, pH 6.8, 37 °C, 600 rpm)
with increasing silibinin:hIAPP molar ratios: 0.1:1 (pink), 1:1 (orange),
and 10:1 (blue). (e) Negative stain TEM images of hIAPP incubated
with (i) 0.1:1, (ii) 1:1, and (iii) 10:1 molar ratios of silibinin:hIAPP
for 5 days (37 °C, 600 rpm). Lower panels show hIAPP fibrils
alone (iv) and aggregates formed when a 10-fold molar excess of silibinin:hIAPP
is added to preformed hIAPP fibrils after 5 h (v) and 24 h (vi). Scale
bar is 100 nm.
Remodeling of Mature IAPP
Fibrils by Silibinin
Although
silibinin has been shown previously to inhibit fibril formation by
hIAPP,[34] the interaction of this small
molecule with preformed fibrils had not been reported. Preformed hIAPP
fibrils were incubated, therefore, with a 10-fold molar excess of
silibinin, and the effect of addition of the small molecule was measured
using TEM and ESI-IMS-MS. The results showed that addition of silbinin
causes depolymerization of preformed fibrils over a 24 h time period
during which time fibrils decrease in length (Figure 6e, panels iv–vi). During fibril depolymerization, ESI-IMS-MS
revealed a simultaneous increase in low-order oligomeric species (Supporting Information Figure S6b), suggesting
that depolymerization may occur via oligomer release. Alternatively,
monomer release may occur and initiate rapid reformation of oligomers
in solution. Oligomers reformed upon fibril depolymerization are comparable
in CCS to those formed during amyloid formation (data not shown).
Formation of Hetero-oligomers and Heterofibrils of hIAPP and
rIAPP
A range of peptide inhibitors has been developed against
hIAPP.[51−54] However, the lack of structural information available on the intermediates
of aggregation has made it difficult to rationalize why some are more
effective than others. Despite rIAPP having been used previously as
the basis for design of an FDA approved therapy to treat T2DM,[55] this peptide is only moderately effective in
inhibiting hIAPP aggregation when added at equimolar concentrations.[11] A two-dimensional infrared spectroscopy study
revealed that rIAPP can become amyloid-competent in the presence of
hIAPP, converting from a natively disordered rIAPP monomer into an
ordered β-sheet-rich complex with hIAPP.[56] To determine why the rIAPPpeptide is an ineffective inhibitor
of hIAPP assembly and to identify how the hIAPP-rIAPP complex forms,
ESI-IMS-MS was used to study the oligomeric structures present in
a mixture (1:1 molar ratio) of the two peptides.By contrast
with the decrease in oligomer populations of hIAPP observed in the
presence of the two small molecule inhibitors studied here, oligomers
up to and including hexamer were formed upon incubation of the hIAPP
and rIAPP (Figure 7a), consistent with results
observed when each peptide was incubated in isolation. The presence
of rIAPP did not prevent fibril formation of hIAPP under the conditions
of these experiments (Figure 7b), consistent
with previous reports suggesting that the ratpeptide must be present
in an ∼10-fold molar excess to inhibit hIAPP amyloid formation
noticeably.[11,56] The fibrils formed from the mixed
sample were of similar morphology to those of hIAPP incubated alone
(Figure 7c). Mixed oligomers were observed
using ESI-IMS-MS with m/z values
corresponding to all-hIAPP, all-rIAPP, and oligomers containing a
mixture of hIAPP and rIAPP monomer subunits. The triply charged dimer
ions (Figure 7a, inset), for example, have
an m/z of 2608, corresponding to
one hIAPP monomer (3904 Da) and one rIAPP monomer (3921 Da), carrying
three positive charges. Mixed trimers and higher order oligomers were
observed also, as well as homo-oligomers of both peptides. The ability
to form mixed oligomers rationalizes why rIAPP is inefficient at inhibiting
hIAPP amyloid formation. After 5 days, the fibrils formed were ultracentrifuged
and depolymerized by incubation in 100% HFIP for 24 h with agitation.
Samples were then air-dried and resuspended in denaturing solvent
(50:40:10 acetonitrile/water/acetic acid (v/v/v)). The resulting mass
spectra (Figure 7d, panel i) showed the presence
of both hIAPP and rIAPP monomer subunits in the aggregate pellet,
confirming the presence of both peptides in the fibrillar state, with
approximately twice as many hIAPP monomer units being incorporated
into the fibrils compared with rIAPP monomers under the conditions
employed. Both monomers were also found in the supernatant of the
original mixed sample, with rIAPP monomers being in excess here (Figure 7d, panel ii). The CID-MS/MS method of interrogation
of oligomer stability was used to probe the stability of the mixed
oligomers formed from hIAPP and rIAPP by subjecting the heterodimer
and heterotetramer ions to increasing transfer collision cell voltages
to promote gas-phase dissociation. Interestingly, the hetero-oligomers
exhibited gas-phase stabilities between those of homo-oligomers of
hIAPP and rIAPP of the same mass, being less stable than rIAPP oligomers
but more stable than hIAPP oligomers (Supporting
Information Figure S8).
Figure 7
Lack of hIAPP inhibition by rIAPP. (a)
ESI-IMS-MS driftscope plot
of oligomers present at t = 2 min in a mixed sample
of hIAPP and rIAPP at a 1:1 molar ratio (50 μM final peptide
concentration, 20 mM ammonium acetate buffer, pH 6.8, 25 °C).
Extracted driftscope peak shows masses corresponding to a mixed dimer
of one hIAPP monomer plus one rIAPP monomer (inset). (b) ThT fluorescence
intensity during agitation of hIAPP:rIAPP 1:1 (50 μM final peptide
concentration, 20 mM ammonium acetate buffer, pH 6.8, 37 °C,
600 rpm). Data for three replicates are shown. (c) Negative stain
TEM image of 1:1 hIAPP: rIAPP fibrils after 5 days. Scale bar = 100
nm. (d) ESI mass spectra of depolymerized fibrils showing the presence
of both hIAPP and rIAPP monomer constituents in the pellet (i) and
supernatant (ii) following ultracentrifugation.
Lack of hIAPP inhibition by rIAPP. (a)
ESI-IMS-MS driftscope plot
of oligomers present at t = 2 min in a mixed sample
of hIAPP and rIAPP at a 1:1 molar ratio (50 μM final peptide
concentration, 20 mM ammonium acetate buffer, pH 6.8, 25 °C).
Extracted driftscope peak shows masses corresponding to a mixed dimer
of one hIAPP monomer plus one rIAPP monomer (inset). (b) ThT fluorescence
intensity during agitation of hIAPP:rIAPP 1:1 (50 μM final peptide
concentration, 20 mM ammonium acetate buffer, pH 6.8, 37 °C,
600 rpm). Data for three replicates are shown. (c) Negative stain
TEM image of 1:1 hIAPP: rIAPP fibrils after 5 days. Scale bar = 100
nm. (d) ESI mass spectra of depolymerized fibrils showing the presence
of both hIAPP and rIAPP monomer constituents in the pellet (i) and
supernatant (ii) following ultracentrifugation.Taken together, therefore, the ESI-IMS-MS and CID-MS/MS data
suggest
that differences in gas-phase stability of monomer and low order oligomers
between hIAPP and rIAPP sequences could be related to their differences
in amyloid propensity. In addition, small molecule binding to hIAPP
prevents fibril formation by disfavoring oligomer formation via binding
to monomers. As a result, the aggregation pathway is diverted to alternative
routes that result in the formation of monomers and/or amorphous aggregates.
Discussion
Identifying and characterizing the structures
and dynamics of prefibrillar
oligomers is vital for understanding the mechanisms of protein aggregation
in amyloid disease, identifying the specific culprits of toxicity,
and designing therapeutics to prevent aggregation. Here, using ESI-IMS-MS,
the high order oligomers of hIAPP and rIAPP have been characterized
for the first time, and their structural organization and relative
gas-phase stabilities were compared. Additionally, the binding and
mode of action of two small molecule inhibitors of hIAPP have been
determined, and the relative ineffective inhibition of hIAPP by rIAPP
has been investigated. Previous IMS-MS studies into the structure
of hIAPP monomer and dimer have suggested that a conformational transition
to an extended structure is likely as an early step in amyloid formation.[24,25] In the study presented here, the population of monomer through hexamer
has been revealed for both peptides. These oligomers likely assemble
via monomer addition (since every species from monomer to hexamer
is observed). In the case of hIAPP, further monomer association into
higher order oligomers is not observed, suggesting that fibril formation
occurs without measurable population of larger oligomeric intermediates
or that higher order species are too lowly populated, too transient,
or too heterogeneous to be detected by ESI-IMS-MS. The oligomeric
states observed may be “on-pathway” to fibril formation
or alternatively may be off-pathway. In the latter case, conformational
changes occurring due to the oligomers’ relative lack of structural
stability may facilitate amyloid assembly compared with their counterparts
in rIAPP.CCS estimations on hIAPP species indicate that the
early oligomers
formed are elongated rather than globulamers, akin to the oligomers
observed during β2m assembly into amyloid.[50] Of interest, early oligomers of rIAPP, which
are similar in size and CCS to those of hIAPP, are formed when the
peptide is incubated under conditions identical to those used to analyze
hIAPP but are significantly more stable in the gas phase as judged
by CID experiments. Although solution-phase stability cannot be directly
inferred from gas-phase stability,[57,58] the difference
in stability observed may rationalize the difference in aggregation
propensity of the two peptides, assuming that a conformational change
is necessary for fibril formation that is impeded for the more stable
ratpeptide. The ability of the two peptides to form mixed oligomeric
species on pathway to heterofibrils in vitro has been revealed using
ESI-IMS-MS and has provided an explanation as to the inefficient inhibition
of hIAPP amyloid formation by rIAPP. The study highlights the pitfalls
associated with designing peptide inhibitors based on amino acid sequence,
given that rIAPP in principle would be expected to be a good inhibitor
of hIAPP since it combines a recognition motif with a β-sheet
breaker unit.[11]Having characterized
the oligomeric species of hIAPP, the binding
of two potent hIAPP amyloid inhibitors, EGCG and silibinin, were studied
using ESI-IMS-MS. Negative controls were performed using molecules
that do not have an inhibitory effect on hIAPP amyloid formation (e.g.,
rifampicin[59] and benzimidazole); these
do not to bind hIAPP or inhibit oligomerization (data not shown).
We show that both EGCG and silibinin are able to block oligomer and
fibril formation from hIAPP when added prior to amyloid assembly,
despite showing different binding characteristics and having different
effects on the equilibrium of species present. By contrast with the
observations made at high ionic strength, in which oligomers are formed
and then lost from the ensemble rapidly as they elongate into fibrils,
the presence of these small molecules inhibits formation of oligomeric
species from monomer subunits. In both scenarios, the observation
is the same (lack of persistence of signal arising from oligomeric
ions). However, the interpretation of the molecular events that lead
to the observed absence of oligomeric species is fundamentally different.
EGCG was found to bind to both observed charge states of the hIAPP
monomer, inhibiting early oligomer formation in a dose-dependent manner
and preventing fibril formation. By contrast, silibinin was detected
to bind only to the most expanded conformer of the monomer 3+ ions
within the dynamic ensemble of intrinsically disordered monomeric
conformations, blocking oligomerization and fibrillation. The latter
result supports the notion of the role of the extended state of the
monomer 3+ species in the fibril assembly mechanism of hIAPP because
the hIAPP conformer bound by silibinin is absent in rIAPP. Binding
to monomer may inhibit assembly directly or may create a structure
that associates with other monomers to generate non-amyloidogenic
aggregates. The fact that both EGCG and silibinin were found to be
effective as amyloid inhibitors at substoichiometric concentrations
suggests that the small molecules may bind to oligomers, as well as
the monomer. Due to the low intensity of oligomers in the presence
of small molecules, however, binding of small molecules to these species
could not be observed by ESI-IMS.Both EGCG and silibinin alter
the equilibrium of the monomeric
charge states of hIAPP present, with the addition of each small molecule
leading to increased population of the triply charged monomer ions.
We propose that binding to these extended species prevents their self-assembly
into amyloid. Previous studies have shown that altering the equilibration
between different monomeric conformers can divert β2m to alternative assembly pathways,[32] leading
to formation of spherical aggregates rather than highly ordered β-sheet
rich fibrillar assemblies. For hIAPP, these alternative aggregation
pathways are presumably kinetically or thermodynamically unfavorable
in the absence of EGCG and silibinin but made feasible upon ligand
binding to unfolded hIAPP monomers. The fact that both of these small
molecules are capable of disaggregating hIAPP amyloid fibrils in distinguishable
manners is also of interest. EGCG remodels fibrils into amorphous
aggregates without reformation of low order oligomers, while silibinin
depolymerizes fibrils and re-establishes the prefibrillar array of
monomer plus early oligomeric species observed by ESI-IMS-MS.It is widely accepted that early oligomeric states are key to protein
self-assembly and subsequent amyloid disease, and determination of
which species are on-pathway to amyloid assembly is vital. Here we
have used ESI-IMS-MS to show that specific, lowly populated hIAPP
monomeric conformers are capable of binding small molecule ligands.
In addition we have used this technique to identify a range of extended
oligomeric assemblies. We have assessed the effect of ligand binding
on each individual species within a heterogeneous mixture of peptide
monomers and their conformers populated prior to fibril formation.
Our experimental results provide support for a route to hIAPP amyloid
fibrils via formation of elongated oligomers. We propose that reduced
stability (relative to nonamyloidogenic rIAPP) is related to the ability
of hIAPP to form extended monomer and oligomeric conformations that
have increased amyloid propensity compared with their more stable
counterparts. Binding to and stabilizing monomers, thereby preventing
their polymerization, could be key to the mechanism of inhibition
of amyloid by EGCG and silibinin.
Conclusions
The
data presented herein, and previously by Bowers and co-workers,[24,25] demonstrate that formation of extended structures is likely key
in early amylin amyloid formation. Small molecule binding to these
extended structures, which results in alteration of the distribution
of conformers present, leads to inhibition of oligomerization and
fibrillation by hIAPP. We hypothesize that stability plays a role
in the sequence specificity of IAPP amyloid formation, given that
oligomers of rIAPP (that differs at only six amino acid positions
compared with hIAPP) are similar in size and shape to those of hIAPP
but are significantly more stable in the gas phase. In order for amyloid
systems to be fully understood, all species on the energy landscape,
both “on-pathway” and “off-pathway”, must
be identified. We cannot determine unequivocally whether the oligomers
detected here using MS are on- or off-pathway. Whichever scenario
is correct, our data are consistent with a lower stability corresponding
to an enhanced rate and/or ability to form amyloid fibrils. Oligomers
either may be on-pathway to fibril formation and require conformational
changes to progress assembly or alternatively may undergo conformational
changes allowing off-pathway species to enter the aggregation pathway
to amyloid. Additionally, we demonstrate that the mixing of the hIAPP
and rIAPP sequences leads to copolymerization into amyloid, hence
explaining the lack of inhibition of hIAPP fibril formation by rIAPP.
Authors: Summer L Bernstein; Nicholas F Dupuis; Noel D Lazo; Thomas Wyttenbach; Margaret M Condron; Gal Bitan; David B Teplow; Joan-Emma Shea; Brandon T Ruotolo; Carol V Robinson; Michael T Bowers Journal: Nat Chem Date: 2009-07 Impact factor: 24.427
Authors: Lucy A Woods; Geoffrey W Platt; Andrew L Hellewell; Eric W Hewitt; Steve W Homans; Alison E Ashcroft; Sheena E Radford Journal: Nat Chem Biol Date: 2011-08-28 Impact factor: 15.040
Authors: Chris T Middleton; Peter Marek; Ping Cao; Chi-cheng Chiu; Sadanand Singh; Ann Marie Woys; Juan J de Pablo; Daniel P Raleigh; Martin T Zanni Journal: Nat Chem Date: 2012-03-11 Impact factor: 24.427
Authors: Yunxiang Sun; Aleksandr Kakinen; Yanting Xing; Emily H Pilkington; Thomas P Davis; Pu Chun Ke; Feng Ding Journal: Biochim Biophys Acta Mol Basis Dis Date: 2018-11-28 Impact factor: 5.187
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Authors: M Ankarcrona; B Winblad; C Monteiro; C Fearns; E T Powers; J Johansson; G T Westermark; J Presto; B-G Ericzon; J W Kelly Journal: J Intern Med Date: 2016-05-10 Impact factor: 8.989
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