G protein-coupled receptor kinase 5 (GRK5) is thought to associate with membranes in part via N- and C-terminal segments that are typically disordered in available high-resolution crystal structures. Herein we investigate the interactions of these regions with model cell membrane using combined sum frequency generation (SFG) vibrational spectroscopy and attenuated total reflectance-Fourier transform infrared (ATR-FTIR) spectroscopy. It was found that both regions associate with POPC lipid bilayers but adopt different structures when doing so: GRK5 residues 2-31 (GRK5(2-31)) was in random coil whereas GRK5(546-565) was partially helical. When the subphase for the GRK5(2-31) peptide was changed to 40% TFE/60% 10 mM phosphate pH 7.4 buffer, a large change in the SFG amide I signal indicated that GRK5(2-31) became partially helical. By inspecting the membrane behavior of two different segments of GRK5(2-31), namely, GRK5(2-24) and GRK5(25-31), we found that residues 25-31 are responsible for membrane binding, whereas the helical character is imparted by residues 2-24. With SFG, we deduced that the orientation angle of the helical segment of GRK5(2-31) is 46 ± 1° relative to the surface normal in 40% TFE/60% 10 mM phosphate pH = 7.4 buffer but increases to 78 ± 11° with higher ionic strength. We also investigated the effect of PIP2 in the model membrane and concluded that the POPC:PIP2 (9:1) lipid bilayer did not change the behavior of either peptide compared to a pure POPC lipid bilayer. With ATR-FTIR, we also found that Ca(2+)·calmodulin is able to extract both peptides from the POPC lipid bilayer, consistent with the role of this protein in disrupting GRK5 interactions with the plasma membrane in cells.
G protein-coupled receptor kinase 5 (GRK5) is thought to associate with membranes in part via N- and C-terminal segments that are typically disordered in available high-resolution crystal structures. Herein we investigate the interactions of these regions with model cell membrane using combined sum frequency generation (SFG) vibrational spectroscopy and attenuated total reflectance-Fourier transform infrared (ATR-FTIR) spectroscopy. It was found that both regions associate with POPC lipid bilayers but adopt different structures when doing so: GRK5 residues 2-31 (GRK5(2-31)) was in random coil whereas GRK5(546-565) was partially helical. When the subphase for the GRK5(2-31) peptide was changed to 40% TFE/60% 10 mM phosphate pH 7.4 buffer, a large change in the SFG amide I signal indicated that GRK5(2-31) became partially helical. By inspecting the membrane behavior of two different segments of GRK5(2-31), namely, GRK5(2-24) and GRK5(25-31), we found that residues 25-31 are responsible for membrane binding, whereas the helical character is imparted by residues 2-24. With SFG, we deduced that the orientation angle of the helical segment of GRK5(2-31) is 46 ± 1° relative to the surface normal in 40% TFE/60% 10 mM phosphate pH = 7.4 buffer but increases to 78 ± 11° with higher ionic strength. We also investigated the effect of PIP2 in the model membrane and concluded that the POPC:PIP2 (9:1) lipid bilayer did not change the behavior of either peptide compared to a pure POPClipid bilayer. With ATR-FTIR, we also found that Ca(2+)·calmodulin is able to extract both peptides from the POPClipid bilayer, consistent with the role of this protein in disrupting GRK5 interactions with the plasma membrane in cells.
G protein-coupled receptors
(GPCRs) are integral membrane proteins
that transduce extracellular signals such as light, hormones, and
chemoattractants to downstream signal pathways.[1] Activated GPCRs are phosphorylated by a family of serine/threonine
kinases named G protein-coupled receptor kinases (GRKs), a process
that initiates their desensitization. The ability to interact with
membranes in which GPCRs are found is essential for GRK function.[2] The various GRKs have different ways of associating
with lipid bilayers.[3] GRK1 and GRK7 are
post-translationally modified by prenyl groups at their C-termini.
GRK2 and GRK3, on the other hand, bind to membranes by virtue of their
C-terminal pleckstrin homology (PH) domains, which bind to acidic
phospholipids and interact with heterotrimeric Gβγ subunits,
which are prenylated. GRK4, GRK5, and GRK6 constitute a subfamily
of GRKs that have 2–3 membrane-binding motifs. The first is
a basic segment near the N-terminus that is believed to be responsible
for binding phosphatidylinositol-4,5-bisphosphate (PIP2). The second is an amphipathic helix located at the extreme C-terminus
that is believed to interact with anionic lipid bilayers. GRK4 and
GRK6 are in addition palmitoylated on cysteines immediately C-terminal
to this helix. The N-terminal ∼18 amino acids of all GRKs,
however, are highly conserved, predicted to have helical propensity,
and are essential for phosphorylation of activated GPCRs. Proposed
roles for these residues include either direct interaction with activated
receptors[4] or with the phospholipid bilayer,[5,6] either of which is proposed to induce helical character in this
region and promote the formation of an activated form of the kinase
domain.Over the past several years, crystallographic studies
have yielded
new insights into the molecular mechanism for regulation of GRKs by
their interactions with receptors and membranes.[4] However, crystallographic analysis requires the removal
of protein complexes from their native membrane environment and cannot
provide direct information on how these molecules are arranged on
the membrane surface in situ. Sum frequency generation
(SFG) vibrational spectroscopy is a powerful tool to examine peptides
and proteins at biointerfaces[7−14] such as lipid bilayers.[15−21] For example, orientations of peptides with different secondary structures,
such as linear α-helices,[22,23] bent α-helices,[24,25] β-sheets,[26] and 310-helices[27] associated with solid substrate supported lipid
bilayers have been deduced using polarized SFG studies. SFG has also
been applied to investigate the membrane orientations of Gβγ,
the Gβγ–GRK2 complex, and Gαβγ
heterotrimers in situ.[28,29] Recently,
we showed that the use of both SFG and attenuated total reflectance–Fourier
transform infrared (ATR-FTIR) spectroscopy can determine orientations
of complex proteins with greater certainty.[30] In this research, we used SFG and ATR-FTIR to study the membrane
interactions of the N- and C-terminal segments of GRK5 to gain insight
into which regions were most important for membrane binding and what
structure and orientation they adopt while interacting with membranes.GRK5 residues 2–31 (GRK52–31) are highly
conserved in the GRK4 subfamily of GRKs (Figure 1), which includes GRK4, GRK5, and GRK6. In previous research, it
was suggested that residues 22–29, which include basic amino
acids Lys22, Arg23, Lys24, Lys26, Lys28, and Lys29, bind to PIP2.[31] An overlapping region (residues
20–39) has also been implicated in binding to calmodulin·Ca2+ (CaM·Ca2+).[32] The structure of GRK6 (a close homologue of GRK5) determined by
X-ray crystallography suggests that the N-terminal portion of the
peptide (residues 2–23) is disordered when the enzyme is in
an inactive state,[33] but residues 2–18
become ordered when the enzyme assumes a more active, presumably receptor-bound
conformation.[4] However, it is not known
if this region forms a platform for binding to lipid membranes or
activated GPCRs. Therefore, elucidating the ability of different segments
of the GRK5 N-terminus to interact with the membrane is key to understanding
how the membrane influences GRK5 function.
Figure 1
Sequences of the human
GRK5 N-terminal and C-terminal peptides
used in this study. Residues highlighted in gray adopt an α-helical
conformation in the structure of the GRK6·sangivamycin complex.[5]
Sequences of the humanGRK5 N-terminal and C-terminal peptides
used in this study. Residues highlighted in gray adopt an α-helical
conformation in the structure of the GRK6·sangivamycin complex.[5]The C-terminal residues 552–562 of GRK5 are believed
to
be another region that interacts with phospholipids. Deletion of these
residues results in a 100-fold loss in membrane binding affinity.[34] Residues 549–557 are predicted to form
an amphipathic helix when bound to membranes.[35] In the active conformation of the GRK6 crystal structure, residues
548–557 form an amphipathic helix that docks to the core of
the enzyme but is far removed from the predicted membrane surface
and the N-terminal segment believed to bind PIP2.[4] Thus, either this structural element does not
bind to membranes, or it only binds to membranes when GRK6 is in a
more inactive state, or the structure represents a soluble form of
the enzyme, such as when it translocates to the nucleus to phosphorylate
transcription factors.[36]By combining
data from two complementary optical spectroscopic
techniques, SFG and ATR-FTIR, we are seeking to answer the following
questions. First, do peptides representing the N-terminal (GRK52–31) and C-terminal (GRK5546–565)
regions bind to membranes on their own, and, if so, what structure
do they adopt? Second, does PIP2 affect the binding properties
of these two peptides? Finally, is CaM·Ca2+ able to
dissociate these GRK5 peptides from the membrane, as proposed to be
required for nuclear translocation?
Experimental
Section
Materials
Peptides GRK52–31, GRK52–24, and GRK5546–565 (Figure 1) were synthesized by the following procedure. Protected
amino acids and N-methylpyrrolidone (NMP), 1-hydroxybenzotriazole
(HOBt), and O-benzotriazole-N,N,N′,N′-tetramethyluronium
hexafluorophosphate (HBTU) were purchased from Creosalus. Acetonitrile,
HPLC grade water, trifluoroacetic acid (TFA), diethyl ether, and phenol
were from Fisher Scientific. Piperidine, N,N-diisopropylethylamine
(DIPEA), dimethylformamide (DMF), thioanisole, triisopropylsilane
(TIPS), and calmodulin were from Sigma-Aldrich. Solid-phase synthesis
resin NovaPEG Rink Amide Resin (0.5 mmol/g) was purchased from Novabiochem.
Analytical HPLC analysis was done using an Alliance system with 250
× 5 mm C18 3 μm column (Vydac). Mass spectrometry analysis
was done using a 6130 Quadrupole LC/MS (Agilent Technologies). Semipreparative
HPLC purification was performed using a Delta 600 system (Waters)
with 150 × 19 mm XBridge Prep C18 10 μm OBD column (Waters).
HPLC analysis and purification were done using solvent system 0.1%
TFA in water and 0.1% TFA in acetonitrile. Peptides GRK52–24 and GRK52–31 were synthesized using 9-fluorenylmethoxycarbonyl
(FMOC) chemistry. The syntheses of C-terminal sequences up to Ala[15] were carried out on a CS336X automated synthesizer
(C.S. Bio Co.), and the syntheses were then continued on a Discover
SPS single mode manual microwave synthesizer (CEM Corp.) (power =
20 W, 5 min per coupling and power 20 W, 1.5 min per deprotection;
temperature 70–75 °C). The synthesis scale was 0.2 mmol.
The general protocol included double coupling and double deprotection
as well as acetylation of the unreacted amino groups. Coupling cycles
were performed using 4 equiv of incoming amino acid, HOBt/HBTU in
DMF and DIPEA in NMP. Fmoc deprotection was accomplished using 20%
piperidine solution in NMP. Cleavage of the peptide from the resin
and side-chain deprotection was performed using 10 mL of the mixture
DI water:phenol:thioanisole:TIPS:TFA (0.5 mL:0.7 g:0.5 mL:0.25 mL:8.75
mL). The reaction was left running at room temperature for 2 h. After
filtration of the resin, crude peptide was precipitated with cold
ethyl ether. The resulting crude peptides were purified by semipreparative
HPLC, as described above. The purity of the final peptide was analyzed
using HPLC and molecular weight confirmed by MS. Peptide GRK525–31 was synthesized by Peptide 2.0 Inc. by a similar
approach. POPC (1-palmitoyl-2-oleoyl-sn-glycero-3-phosphocholine)
and PIP2 were purchased from Avanti Polar Lipids.
Bilayer
Construction
Supported POPC/POPC lipid bilayers
were constructed on CaF2 prisms by the Langmuir–Blodgett/Langmuir–Schaefer
method, as reported in detail previously.[37,38] The first POPC layer is deposited on one of the square faces of
the right-angle CaF2 prism with A KSV2000 LB system: The
plasma-cleaned prism was first immersed in the LB trough. Then a certain
amount of POPC chloroform solution, typically 5 drops of 10 mg/mL,
was spread on the water surface until the surface tension reaches
∼5 mN/m. Two barrier arms were suppressed so that the surface
tension remained 34 mN/m, while the CaF2 prism was lifted
from the subphase. A layer of POPClipids was deposited on the face
perpendicular to the water surface in this way. After aligning the
laser beams to find the monolayer signal, a 2 mL reservoir filled
with water was placed beneath the prism. POPClipids were added to
the surface of the water in the reservoir so that the surface tension
was around 34 mN/m. The reservoir was elevated so that the the lipid
monolayer on the water surface contacted with the first layer deposited
on the prism to form a lipid bilayer.
SFG Experiments
SFG theory,[39−43] our experimental design, and data analysis method[23,44] have been reported before. The concentration of each of the four
peptides was 3.8 μM, and the peptides were dissolved in 10 mM
potassium phosphate buffer (pH 7.4). Because CaF2 prisms
were used as substrates to prepare the lipid bilayers, small amounts
of Ca2+ may be dissolved in the subphase. 2 mM EDTA was
added to the above buffer solution to minimize any influence of the
Ca2+ released from the CaF2 substrates. For
each of the three N-terminal peptides studied here, we added the peptide
into the subphase in contact with the substrate supported bilayer
and after equilibration recorded the SFG signal in the water O–H
stretching frequency range as well as in the peptide amide I frequency
region. For all peptides we studied, the adsorption time on the POPClipid bilayer in either 10 mM phosphate buffer or PBS buffer was less
than 200 s (see the time-dependent SFG signals detected in the CH
and OH stretching frequency range in the Supporting
Information). For the second step, we substituted the peptide
solution subphase with potassium phosphate buffer (∼6 mL in
total) to wash off loosely associated peptides and recorded the SFG
signal in the water O–H stretching frequency range again. For
the last step, we substituted the phosphate buffer subphase with a
solution of buffer containing 40% TFE and again collected SFG spectra
in the water O–H stretching frequency range and the amide I
frequency range. For the C-terminal peptide, we only performed the
first two steps of the above procedure. PIP2 experiments
were performed in the same way as POPC experiments except that when
making bilayers, lipids with a 9:1 molar ratio of POPC:PIP2 were used. Because peptides were used at the same concentration
in these experiments yet likely have different affinities and because
water signals are also strongly affected by net charge as well as
charge distribution in the peptides (and other effects), we defined
peptides as weakly membrane associated if the water signal recovered
after the buffer wash, as opposed to direct comparison of changes
in the SFG signals from water O–H stretching after addition
of peptide.
ATR-FTIR Spectroscopy
ATR-FTIR experiments
were performed
on a Nicolet Magna 550 FTIR spectrometer. Lipid bilayers were deposited
on a ZnSe crystal (Specac Ltd. RI, U.K.) using the vesicle fusion
method. 1 mL of POPC toluene solution (5 mg/mL) was dried with nitrogen
flow and then in vacuum for 2 h. The POPC power was then dissolved
in 10 mM phosphate D2O buffer pH 7.4, and the mixture was
vortexed for 5 min before addition to the surface of the detachable
ZnSe crystal to form bilayers. After 30 min, the vesicles floating
in the subphase were washed away using excess buffer. GRK5 peptides
were then injected into the subphase (1.6 mL) to achieve a concentration
of 11.4 μM. After the system reached equilibrium, spectra before
and after extensive wash with D2O buffer were recorded.
For GRK5546–565, s- and p-polarized spectra were
taken so that data analysis on the peptide orientation could be performed.
In the CaM·Ca2+ experiments, after peptides were associated
with the lipid bilayers equimolar CaM (11.4 μM) and 50 μM
CaCl2 solution were added to the subphase.
Results
SFG Studies
on N-Terminal Peptides
We first investigated
molecular interactions between the GRK5 N-terminal peptides GRK52–31, GRK52–24, and GRK525–31 and a POPC/POPClipid bilayer. The POPC/POPC bilayer is zwitterionic,
and the electrostatic potential across the bilayer induces the water
dipoles to orient near the bilayer surface.[45,46] The water region (detected between 2700 and 3700 cm–1)[47,48] monitored by SFG spectroscopy can be used
to determine the binding properties of ions[49,50] or peptides.[25] In our experiments, we
observed two broad water O–H stretching peaks centered at ∼3200
and 3400 cm–1 in the SFG spectrum from the lipid
bilayer/potassium phosphate buffer interface (Figure 2a). Peptides were then added into the subphase, and the system
was allowed to reach equilibrium. The water OH stretching signal decreased
upon addition of the GRK52–31 or GRK525–31 peptides to the subphase, consistent with their interaction with
the POPC/POPC bilayers (Figures 2a and 3a). SFG spectra were also collected after extensive
washing, but no substantial changes were observed, suggesting that
both GRK52–31 and GRK525–31 peptides
are strongly associated with the bilayer. However, the SFG water O–H
stretching signal only decreased slightly after the addition of the
GRK52–24 peptide to the subphase, and the SFG water
signal recovered after washing the interface with buffer (Figure 3c), consistent with GRK52–24 only
being weakly associated with the POPC/POPC bilayer. Thus, the highly
charged residues spanning residues 25–31 are primarily responsible
for membrane binding in these peptides.
Figure 2
SFG signals from GRK52–31 indicate strong association
with model membranes and helical character in a more hydrophobic environment.
(a) Spectra in the C–H and O–H stretching frequency
region detected from the interface between the POPC/POPC bilayer and
buffer alone (black), GRK52–31 in 10 mM phosphate
buffer pH 7.4 (red), after washing (blue), and in a mixture of 60%
buffer/40% TFE (dark cyan). (b) SFG spectra of GRK52–31 associated with a POPC/POPC bilayer in contact with peptide solution
in 60% 10 mM phosphate buffer pH 7.4/40% TFE in the amide I frequency
region. (c) SFG spectra of GRK52–31 associated with
a POPC/POPC bilayer in contact with 60% PBS/40% TFE.
Figure 3
SFG ppp signals detected from the GRK525–31 and
GRK52–24 peptides indicate that the latter peptide
only weakly associates with model membranes. (a) SFG spectra in C–H
and O–H stretching frequency region from the interface between
the POPC/POPC bilayer and buffer alone (black), GRK525–31 in 10 mM phosphate buffer pH 7.4 (red), after washing (blue), and
in a mixture of 60% buffer/40% TFE (dark cyan). (b) SFG spectra in
the amide I frequency region from GRK525–31 associated
with a POPC/POPC bilayer in 60% 10 mM phosphate buffer pH 7.4/40%
TFE. (c) SFG spectra in C–H and O–H stretching frequency
region from the interface between the POPC/POPC bilayer and buffer
alone (black), GRK52–24 in 10 mM phosphate buffer
pH 7.4 (red), after washing (blue), and in a mixture of 60% buffer/40%
TFE (dark cyan). (d) SFG spectra in the amide I frequency region from
GRK52–24 associated with a POPC/POPC bilayer in
contact with peptide solution in 60% 10 mM phosphate buffer pH 7.4/40%
TFE.
SFG signals from GRK52–31 indicate strong association
with model membranes and helical character in a more hydrophobic environment.
(a) Spectra in the C–H and O–H stretching frequency
region detected from the interface between the POPC/POPC bilayer and
buffer alone (black), GRK52–31 in 10 mM phosphate
buffer pH 7.4 (red), after washing (blue), and in a mixture of 60%
buffer/40% TFE (dark cyan). (b) SFG spectra of GRK52–31 associated with a POPC/POPC bilayer in contact with peptide solution
in 60% 10 mM phosphate buffer pH 7.4/40% TFE in the amide I frequency
region. (c) SFG spectra of GRK52–31 associated with
a POPC/POPC bilayer in contact with 60% PBS/40% TFE.SFG ppp signals detected from the GRK525–31 and
GRK52–24 peptides indicate that the latter peptide
only weakly associates with model membranes. (a) SFG spectra in C–H
and O–H stretching frequency region from the interface between
the POPC/POPC bilayer and buffer alone (black), GRK525–31 in 10 mM phosphate buffer pH 7.4 (red), after washing (blue), and
in a mixture of 60% buffer/40% TFE (dark cyan). (b) SFG spectra in
the amide I frequency region from GRK525–31 associated
with a POPC/POPC bilayer in 60% 10 mM phosphate buffer pH 7.4/40%
TFE. (c) SFG spectra in C–H and O–H stretching frequency
region from the interface between the POPC/POPC bilayer and buffer
alone (black), GRK52–24 in 10 mM phosphate buffer
pH 7.4 (red), after washing (blue), and in a mixture of 60% buffer/40%
TFE (dark cyan). (d) SFG spectra in the amide I frequency region from
GRK52–24 associated with a POPC/POPC bilayer in
contact with peptide solution in 60% 10 mM phosphate buffer pH 7.4/40%
TFE.For all three GRK5 N-terminal
peptides, no discernible SFG amide
I signal could be detected from the lipid bilayer interfaces after
their addition. This suggests that the membrane associated peptides
form either ordered structures but with random orientations or essentially
random structures. After replacing the subphase with a 40% TFE solution,
a strong SFG amide I signal was detected from the GRK52–31 peptide (Figure 2b), but not from GRK525–31 or GRK52–24 (Figures 3b and 3d), consistent with
only GRK52–31 forming α-helical structure
when the subphase becomes more hydrophobic. This conclusion is also
consistent with spectral features detected in the water O–H
stretching frequency range after the subphase buffer was replaced
by the TFE mixture. Figure 2a shows that only
for GRK52–31, a negative peak at ∼3300 cm –1 appeared, originating from the interference between
the N–H stretching signals of well-ordered α-helices
and the broad water background. This N–H stretch signal can
be attributed to the backbone N–H stretch or/and the side chains
such as LysNH3+.[51] Although the predicted helical propensity of GRK52–24 is the same as that of GRK52–31, no changes in
the spectra upon addition of TFE were detected likely because the
peptide was not strongly associated with the membrane and washed off
in the previous step.
Orientation Analysis of the α-Helical
Segment in GRK52–31
After substituting
the subphase with 40%
TFE, a prominent α-helical signal centered at ∼1655 cm–1 arises from GRK52–31. This could
be interpreted as residues 2–18 adopting an α-helical
conformation, consistent with a prior crystal structure of GRK6[4] and secondary structure predictions. This phenomenon
also highlights that SFG, as a second-order nonlinear spectroscopy,
is much more sensitive to ordered structure (such as α-helices)
than disordered molecules (such as random coils), which is not the
case for linear vibrational spectroscopy such as ATR-FTIR.SFG
spectra collected from amide I modes of peptides and proteins using
different polarization combinations can be used to determine membrane
orientations of peptides and proteins, as shown in a previous publication.[22] Using the measured signal strength ratio of
the α-helical contribution in the ppp and ssp spectra, we deduced
that in 40% TFE, the orientation angle of the helical segment (presumed
to be residues 2–18) of GRK52–31 is ∼46
± 1° relative to the membrane surface normal (with χppp/χssp = 2.08 ± 0.01) if we assume
the peptides adopt a single orientation distribution. Interestingly,
this orientation angle increases to ∼78 ± 11° (with
χppp/χssp = 2.43 ± 0.06) when
the ionic strength of the subphase is increased by use of PBS instead
of phosphate buffer (Figure 2c). Details of
the orientation analysis can be found in the Supporting
Information. This result suggests that the increase in ionic
strength does not change the conformation of the GRK52–31 but rather changes the charge distribution on the peptide surface
and thus facilitates the interaction of helical elements of the peptide
with the lipid head groups.
SFG Studies on the C-Terminal Peptide
The SFG spectrum
of GRK5546–565 (Figure 4)
is similar to that of GRK52–31, in that the two
broad peaks at 3200 and 3400 cm–1 decreased and
remained so even after extensive washing, indicating strong interaction
of GRK5546–565 with the lipid bilayer. However,
two new peaks centered at 2876 and 2940 cm–1 appeared.
These were also observed for GRK52–31 but were not
as significant. These two peaks could be attributed to amino acid
side chains,[51] disruption of the lipid
bilayer,[52] or both. The SFG amide I spectra
of GRK5546–565, however, is very different from
those of the N-terminal peptides. Without changing the subphase into
40% TFE, an amide I signal was readily detected. In the spectra, the
peak at 1655 cm–1 is attributed to α-helical
structure and the shoulder at ∼1600 cm–1 is
likely from amide groups of side chains.[53] The peak at 1720 cm–1 is from carbonyl groups
in the disrupted lipid bilayer. This agrees with the CH stretching
signal change mentioned above, supporting the hypothesis that the
lipid bilayer is disrupted. Because the intensity is not as high as
that of GRK52–31 in 40% TFE with 10 mM phosphate
buffer, no discernible NH peak (∼3300 cm–1) in the water range (3000–4000 cm–1) was
detected. Orientation analysis was not performed here due to the low
signal-to-noise ratio of the SFG spectra and because there are multiple
contributions to the spectra. In summary, the main difference between
GRK5546–565 and GRK52–31 is that
the former is partially α-helical when associated with lipid
bilayers without need for TFE to induce helical structure.
Figure 4
SFG ppp signals
detected from GRK5546–565 indicate
strong binding to model membranes and helical character. (a) SFG spectra
in the C–H and O–H stretching frequency region from
the interface between the POPC/POPC bilayer and buffer alone (black)
and GRK5546–565 associated in 10 mM phosphate buffer
pH 7.4 (red). (b) SFG spectra in the amide I frequency region from
GRK5546–565 associated with a POPC/POPC bilayer
in 10 mM phosphate buffer pH 7.4.
SFG ppp signals
detected from GRK5546–565 indicate
strong binding to model membranes and helical character. (a) SFG spectra
in the C–H and O–H stretching frequency region from
the interface between the POPC/POPC bilayer and buffer alone (black)
and GRK5546–565 associated in 10 mM phosphate buffer
pH 7.4 (red). (b) SFG spectra in the amide I frequency region from
GRK5546–565 associated with a POPC/POPC bilayer
in 10 mM phosphate buffer pH 7.4.
SFG Studies on the Effect of PIP2
PIP2 is known to enhance the GRK5-mediated phosphorylation of
GPCRs.[31] In order to test whether this
enhancement is related to the membrane binding of the peptides we
are studying herein, we constructed (9:1) POPC:PIP2lipid
bilayers and studied its interaction with GRK52–31, GRK52–24, and GRK5546–565.
These results (see Supporting Information Figure S2) were then compared to those obtained when using a pure
POPClipid bilayer. The SFG intensities and signal strength ratios
of the amide I signals detected in the amide I frequency range using
different polarization combinations of the GRK52–31 associated with the two types of bilayers exposed to the solution
with 40% TFE were observed to be similar, indicating that PIP2 did not enhance the adsorption of GRK52–31 to the lipid bilayer. The interactions of GRK52–24 and GRK5546–565 with (9:1) POPC:PIP2 bilayers were also similar to those with the pure POPC system. This
is reminiscent of protein MARCKS: neither the native protein nor a
peptide representing its positive charged cluster requires PIP2 for binding to the membrane. However, PIP2 is
laterally sequestered in the presence of MARCKS and the peptide.[54] How PIP2 can increase the autophosphorylation
of GRK5 and phosphorylation of activated GPCRs calls for further investigation.
However, it should be noted that residues 24–31 are well ordered
in both available crystal structures of GRK6[4,33] and
that formation of a high affinity site for PIP2 may require
the assumption of tertiary structure by this polypeptide, as mandated
by the fold of the enzyme. The study on the effect of PIP2 suggests that the conclusions on peptide affinity drawn from Figure 2–4 do not require the existence of PIP2.
ATR-FTIR Studies
Because SFG is sensitive to ordered
structures, the signals generated from ordered α-helices are
normally much stronger than those detected from random coil. On the
other hand, ATR-FTIR spectroscopy detects amide I (1600–1700
cm–1) signals with similar sensitivities from different
secondary structural motifs, such as α-helices, random coils,
and β-sheets from peptides and proteins.[55−59] We used ATR-FTIR spectra to confirm the peptide adsorption
behavior detected by SFG. For the ATR-FTIR experiments, the concentrations
of all peptides used were 11.4 μM in 10 mM phosphate D2O buffer (pD 7.1). For all the N-terminal peptides, the amide I peak
center is around 1642 cm–1 (Figure 5), indicating that the peptides are most likely random coils.
For GRK52–31 and GRK525–31, the
amide I peak intensities did not change after washing with buffer,
but for GRK52–24 the amide I signal decreased to
about half, again suggesting a weaker interaction between GRK52–24 and the lipid bilayer, as suggested by the SFG
studies. The reason that membrane associated GRK52–24 did not completely disappear after washing, as observed in SFG,
is likely because the peptide concentration is 3 times higher than
that used in SFG measurements.
Figure 5
ATR-FTIR spectra of GRK5 N-terminal peptides
confirm weak binding
of GRK52–24. Spectra of (a) GRK52–31, (b) GRK52–24, and (c) GKR525–31 associated with a POPC/POPC lipid bilayer in the presence of 10
mM phosphate buffer pH 7.4 before (black) and after (red) buffer wash.
ATR-FTIR spectra of GRK5 N-terminal peptides
confirm weak binding
of GRK52–24. Spectra of (a) GRK52–31, (b) GRK52–24, and (c) GKR525–31 associated with a POPC/POPClipid bilayer in the presence of 10
mM phosphate buffer pH 7.4 before (black) and after (red) buffer wash.By taking secondary derivatives
of the ATR-FTIR spectra for GRK5546–565 (Figure 6), we found
two peaks centered at 1646 and 1653 cm–1, respectively.
The average band position in D2O is reported to be ∼1652
cm–1 for α-helix and ∼1645 cm–1 for disordered secondary structure.[57] Therefore, the peak centered at 1646 cm–1 is attributed
by random coil and the other at 1653 cm–1 is attributed
to α-helices, consistent with SFG results indicating that the
GRK5 C-terminal peptide forms an α-helical structure. After
extensive washing, the ATR-FTIR signal remained, suggesting a strong
interaction with the lipid bilayer, also compatible with the SFG data.
Figure 6
ATR-FTIR
spectra of GRK5546–565 associated with
a POPC/POPC lipid bilayer in contact with 10 mM phosphate buffer pH
7.4.
ATR-FTIR
spectra of GRK5546–565 associated with
a POPC/POPClipid bilayer in contact with 10 mM phosphate buffer pH
7.4.
ATR-FTIR Studies of CaM·Ca2+ Interactions with
N-Terminal and C-Terminal Peptides
ATR-FTIR was further used
to investigate the molecular interactions of GRK52–31 with calmodulin. CaM·Ca2+ itself has very weak binding
with the membrane (Supporting Information). As shown in Figure 7a, the addition of
equimolar amounts of CaM·Ca2+ and GRK52–31 to the subphase decreased the ATR-FTIR amide I signal by about 50%.
Further extensive washing with buffer led to a more substantial decline
of the random coil ATR-FTIR signal. This clearly shows that CaM·Ca2+ facilitates the extraction of GRK52–31 from the lipid bilayer. However, CaM·Ca2+ could
not extract GRK525–31 from the membrane (Supporting Information), suggesting that the
helix formed by residues 2–24 is important for high affinity
binding to CaM·Ca2+.[60] CaM·Ca2+ also was able to extract GRK5546–565 from
our model membranes (Figure 7b). The initial
increase in the signal after addition of CaM·Ca2+ to
GRK5546–565 was unexpected. However, this may simply
reflect that when CaM·Ca2+ forms a complex with this
peptide, it remains associated with the membrane to a greater extent
than when in complex with the GRK52–31 peptide.
Notably, in either case, the subsequent buffer wash eliminates binding,
indicating weak binding.
Figure 7
CaM·Ca2+ decreases the association
of GRK5 N and
C-terminal peptides. ATR-FTIR signals detected before and after the
addition of equimolar CaM·Ca2+ to the subphase for
peptides (a) GRK52–31 and (b) GRK5546–565. The spectra correspond to before (black), and after (red) washing,
to the addition of CaM·Ca2+ to the subphase (blue),
and after subsequent washing (dark cyan).
CaM·Ca2+ decreases the association
of GRK5 N and
C-terminal peptides. ATR-FTIR signals detected before and after the
addition of equimolar CaM·Ca2+ to the subphase for
peptides (a) GRK52–31 and (b) GRK5546–565. The spectra correspond to before (black), and after (red) washing,
to the addition of CaM·Ca2+ to the subphase (blue),
and after subsequent washing (dark cyan).
Discussion
Our study is a clear example of how SFG
and ATR-FTIR spectroscopies
complement each other as methods for interrogating the structure of
proteins/peptides at membrane surfaces. Because SFG is a second-order
nonlinear optical technique, under the electric dipole approximation,
it only detects signal where inversion symmetry is broken. Thus, SFG
can minimize the interfering effects of proteins in bulk solution.
For example, in our studies, we measured well-defined amide signals
using SFG from the GRK52–31 peptide associated with
lipid bilayers in contact with solutions with 40% TFE, which generates
a high background signal in ATR-FTIR spectroscopy (Supporting Information). Another advantage of SFG is that
measurements do not require D2O, which is used in ATR-FTIR
to minimize interference by H2O absorption at ∼1650
cm–1. SFG is also more sensitive to ordered secondary
structures than disordered ones. We observed a drastic change of the
amide I signal of GRK52–31 when its subphase was
altered to contain 40% TFE. This change was more subtle in the ATR-FTIR
spectra because random coils and α-helices have peak centers
close to each other (∼1647 and ∼1653 cm–1, respectively) and usually make similar contributions to the spectra.
For large proteins (e.g., GRK5), sometimes the switch from the active
state to the inactive state is accompanied by conformational changes.
The unique ability of SFG to distinguish random coils from α-helices
might shed light on the mechanisms of these processes, which may not
be easily distinguishable using ATR-FTIR spectra. On the other hand,
ATR-FTIR can directly monitor the adsorption of unstructured peptides
and proteins simply by inspecting the amide I signals. Because unstructured
domains (e.g., random coils) cannot be readily detected by SFG spectroscopy,
the adsorption of such molecules cannot be directly assessed using
the SFG amide I signal. However, this goal can be achieved indirectly
by monitoring the ordered water signal change in SFG spectra.Errors represent standard deviations
of four replicates obtained in each of two individual experiments.In this work we combined SFG
and ATR-FTIR spectroscopies to study
the in situ membrane binding potential of two regions
of GRK5 previously implicated in binding to phospholipid bilayers.
The uniform orientation of water molecules near the bilayer surface
was exploited first, as the disappearance of the SFG water signal
suggests their displacement by peptide molecules. Whether or not the
water signal would resume after washing the system with buffer was
used to determine if the peptide molecules are weakly or strongly
adsorbed. It was shown that of the three N-terminal peptides, only
GRK52–24 binds weakly to the lipid bilayer, suggesting
that GRK52–24 alone does not play a significant
role in GRK5 membrane binding and that residues 25–31 of the
GRK52–31 peptide, which are exceptionally basic
and include a tryptophan residue, are primarily responsible for membrane
binding in this region. This conclusion is also supported by monitoring
the changes in the amide I signal from the peptides before and after
washing with buffer using ATR-FTIR. From the amide I SFG signals we
found that the segment containing amino acid residues 2–24
of peptide GRK52–31 undergoes a conformational change
from a random coil into a well-ordered α-helix when the hydrophobicity
of the environment increases (in our experiment by substituting the
buffer subphase with a solution containing 40% TFE). It is possible
that TFE emulates what happens when this region encounters either
an activated GPCR or its own activated kinase domain. Furthermore,
the interaction of this region, or of an adjacent region (i.e., residues
25–31), with membranes is not enough to induce order in this
segment. Our results are consistent with those reported previously
that residues 2–18 play an important role in protein–protein
interactions, such as those with activated GPCRs or with the catalytic
core of the enzyme to stabilize a more active state.[4,2] Polarization-dependent SFG measurements were used to determine the
angle of the helical segment of this peptide to the surface normal.
This angle was found to increase substantially upon an increase in
ionic strength of the surrounding buffer solution. With a similar
approach, both SFG and ATR-FTIR results showed that GRK5546–565 was partially helical on POPC lipid bilayers, even in the absence
of a helix-inducing agent such as TFE. A model summarizing the membrane
interactions of the peptides is shown in Figure 8.
Figure 8
Schematic showing proposed membrane interaction mechanisms of the
GRK5 N-terminal peptide GRK52–31 and the GRK5 C-terminal
peptide GRK5546–565.
Schematic showing proposed membrane interaction mechanisms of the
GRK5 N-terminal peptide GRK52–31 and the GRK5 C-terminal
peptide GRK5546–565.Therefore, both N- and C-terminal peptide segments of GRK5
contribute
to bilayer binding and likely account for the constitutive localization
of GRK5 on cell membranes, even though it lacks the palmitoylation
found in the closely related enzymes GRK4 and GRK6. Both residues
25–31 and 546–565 bind strongly to membranes, as evidenced
by their persistence even after exhaustive washing. However, residues
2–24 at the extreme N-terminus do not represent a strong membrane
binding determinant. Instead, our results are most consistent with
this highly conserved region only becoming ordered when it forms protein–protein
interfaces, such as when in complex with an activated GPCR or when
it interacts with the small lobe of the GRK kinase domain. Unexpectedly,
PIP2 does not affect the binding properties of the peptides
we studied. It is possible that the N-terminal peptide does not fully
recapitulate the binding site for this lipid because the peptide is
unstructured when bound to membranes, as opposed to the analogous
peptide in the context of the full-length enzyme, where its structure
is imposed by the fold of the enzyme. The membrane interaction mechanisms
of the N-terminal and C-terminal peptides are, however, different.
Previous biochemical studies showed that the C-terminal peptide likely
forms an amphipathic helix that enhances GRK5 membrane binding.[35] The analogous C-terminal region has only been
observed in one structure of GRK6 in a relatively active state,[4] wherein it forms the expected amphipathic helix.
However, the hydrophobic residues bind to the catalytic core of the
enzyme, and the helix seems too far from the predicted membrane surface
to directly engage lipids. As phospholipids are not present in this
crystal structure, the C-terminal structure could represent a crystallographic
artifact. Alternatively, because the interactions of the C-terminus
of GRK6 with the core of the enzyme are extensive (buried accessible
surface area of 2400 Å2), the packing of this helix
could represent the situation when GRK6 is in a cytoplasmic and/or
autoinhibited state. Because PIP2 is believed to bind to
the 25–31 region in the N-terminal region and this site is
a structured part of the catalytic core in prior crystal structures,
this interaction may be more important for achieving proper orientation
of the enzyme at the membrane, whereas the C-terminal amphipathic
helix, which is connected to the rest of the enzyme by a 21-amino
acid linker, is merely important for maintaining its association at
the membrane. CaM·Ca2+ is able to dissociate GRK52–31 and GRK5546–565 peptides from
the membrane, consistent with the ability of this protein to drive
GRK5 off the membrane of cells and consequently to the nucleus, where
it is believed to phosphorylate transcription factors controlling
hypertrophic genes.[36]
Table 1
Fitting Results for SFG Spectra Shown
in Figure 2a
subphase
polarization
peak
center (cm–1)
peak
width (cm–1)
χeff
ratio
tilt angle (deg)
60% phosphate buffer/40% TFE
ssp
1657
14.2
14.8
2.09 ± 0.01
46 ± 1
ppp
1657
14.7
51.1
PBS buffer/40% TFE
ssp
1650
11.0
8.8
2.43 ± 0.06
78 ± 11
ppp
1652
14.0
17.6
Errors represent standard deviations
of four replicates obtained in each of two individual experiments.
Authors: Seung-Yong Jung; Soon-Mi Lim; Fernando Albertorio; Gibum Kim; Marc C Gurau; Richard D Yang; Matthew A Holden; Paul S Cremer Journal: J Am Chem Soc Date: 2003-10-22 Impact factor: 15.419
Authors: Andrew P Boughton; Pei Yang; Valerie M Tesmer; Bei Ding; John J G Tesmer; Zhan Chen Journal: Proc Natl Acad Sci U S A Date: 2011-08-29 Impact factor: 11.205
Authors: J A Pitcher; Z L Fredericks; W C Stone; R T Premont; R H Stoffel; W J Koch; R J Lefkowitz Journal: J Biol Chem Date: 1996-10-04 Impact factor: 5.157
Authors: Tobias Weidner; Manish Dubey; Nicholas F Breen; Jason Ash; J E Baio; Cherno Jaye; Daniel A Fischer; Gary P Drobny; David G Castner Journal: J Am Chem Soc Date: 2012-05-18 Impact factor: 15.419
Authors: Bei Ding; Afra Panahi; Jia-Jung Ho; Jennifer E Laaser; Charles L Brooks; Martin T Zanni; Zhan Chen Journal: J Am Chem Soc Date: 2015-08-11 Impact factor: 15.419
Authors: Hiren Patel; Bei Ding; Kelsey Ernst; Lei Shen; Wenmin Yuan; Jie Tang; Lindsey R Drake; Jukyung Kang; Yaoxin Li; Zhan Chen; Anna Schwendeman Journal: Int J Nanomedicine Date: 2019-04-30