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Stepwise mechanism of temperature-dependent coacervation of the elastin-like peptide analog dimer, (C(WPGVG)) 3
2
Daiki Tatsubo, Keitaro Suyama, Masaya Miyazaki, Iori Maeda, and Takeru Nose Biochemistry, Just Accepted Manuscript • DOI: 10.1021/acs.biochem.7b01144 • Publication Date (Web): 01 Feb 2018 Downloaded from http://pubs.acs.org on February 1, 2018
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Biochemistry
1
Stepwise mechanism of temperature-dependent
2
coacervation of the elastin-like peptide analog
3
dimer, (C(WPGVG)3)2
4
Daiki Tatsubo a, Keitaro Suyama b, Masaya Miyazaki c, Iori Maeda d, and Takeru Nose a,b,*
5
a
6
Fukuoka, 812-8581, Japan.
7
b
8
c
9
and Technology (AIST), Tosu, Saga, 841-0052, Japan.
Department of Chemistry, Faculty and Graduate School of Science, Kyushu University,
Faculty of Arts and Science, Kyushu University, Fukuoka, 819-0395, Japan.
Advanced Manufacturing Research Institute, National Institute of Advanced Industrial Science
10
d
11
Fukuoka 820-8502, Japan.
12 13 14 15 16
Manuscript Correspondence: Prof. Takeru Nose Tel and Fax: +81-92-802-6025 e-mail:
[email protected] 17
KEYWORDS
18
Elastin, Elastin-like peptide, Self-assembly, Coacervation, Intrinsic disordered protein,
19
Secondary structure
Department of Bioscience and Bioinformatics, Kyushu Institute of Technology, Iizuka,
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Abstract
2
Elastin-like peptides (ELP) are distinct, repetitive, hydrophobic sequences, such as
3
(VPGVG)n, that exhibit coacervation— the property of reversible, temperature-dependent self-
4
association and dissociation. ELPs can be found in elastin and have been developed as new
5
scaffold biomaterials. However, the detailed relationship between their amino acid sequences
6
and coacervation properties remain obscure because of the structural flexibility of ELPs. In this
7
study, we synthesized a novel, dimeric ELP analog (H-C(WPGVG)3-NH2)2, henceforth
8
abbreviated to (CW3)2, and analyzed its self-assembly properties and structural factors as
9
indicators of coacervation. Turbidity measurements showed that (CW3)2 demonstrated
10
coacervation at a much lower concentration than its monomeric form and another ELP. In
11
addition, the coacervate held water-soluble dye molecules. Thus, potent and distinct coacervation
12
was obtained with a remarkably short sequence of (CW3)2. Furthermore, fluorescence
13
microscopy, dynamic light scattering, and optical microscopy revealed that the coacervation of
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(CW3)2 was a stepwise process. The structural factors of (CW3)2 were analyzed by molecular
15
dynamics simulations and circular dichroism spectroscopy. These measurements indicated that
16
helical structures primarily consisting of proline and glycine became more disordered at high
17
temperatures with concurrent, significant exposure of their hydrophobic surfaces. This extreme
18
change in the hydrophobic surface contributes to the potent coacervation observed for (CW3)2.
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These results provide important insights into more efficient applications of ELPs and their
20
analogs, as well as the coacervation mechanisms of ELP and elastin.
21 22
Introduction
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Biochemistry
1
In addition to elucidating the molecular mechanisms of biomacromolecules, controlling
2
their various functions is a crucial issue in biochemistry. The functions of intrinsically disordered
3
proteins (IDPs) have attracted much recent attention [1, 2]. These proteins serve significant roles in
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cellular and extracellular functions, particularly by participating in molecular recognition and
5
providing mechanical properties [3, 4]. Of these IDPs, elastin, an elastic protein in the extracellular
6
matrix, provides extensibility and condensability to connective tissues in arterial walls, lungs,
7
and skin [5, 6]. Elastin also exhibits temperature-dependent, reversible association and dissociation
8
that results in phase transition characterized by lower critical solution temperature (LCST)
9
behavior
[7]
. This distinct, self-assembly behavior, known as coacervation, is considered
10
important for elastin maturation [8]. Due to this characteristic, elastin-like peptides (ELPs), which
11
contain elastin derived sequence(s), have been recently considered useful in the design of new
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scaffold materials for developing biomedical products related to drug delivery systems and tissue
13
engineering
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many other IDPs, ELPs have also been studied as a model peptide
15
mechanism of elastin coacervation is important for its efficient use in applications and for
16
understanding the behaviors of other complex IDPs.
17
[9, 10]
. Furthermore, as the biophysical properties of ELPs are similar to those of [11]
. Thus, elucidating the
The characteristic, hydrophobic, repetitive sequences of elastin, such as (Val-Pro-Gly[8, 12]
18
Val-Gly)n, abbreviated as (VPGVG)n, are thought to control its coacervation
19
studies have examined various ELPs based on the (VPGVG)n sequence by altering its length or
20
substituting the amino acid residues
21
sequences and the coacervation properties of ELPs. The introduction of residues with greater
22
hydrophobicity (Ile, Leu > Val > Ala), higher numbers of hydrophobic amino acids, and longer
23
chain lengths resulted in more potent coacervation properties [14-18]. In contrast, few studies have
[9, 13]
. Previous
, which revealed the relationships between peptide
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Page 4 of 49
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focused on ELPs that contain aromatic amino acids, though the significant hydrophobicity of
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aromatic amino acids would clearly contribute to coacervation. ELPs are disordered, because
3
their repetitive sequences contain many secondary structure breakers, such as glycine and proline
4
residues
5
[6, 17]
6
relationship between the structure and coacervation properties of ELPs has not been completely
7
elucidated.
[16]
. Coacervation of ELPs was assumed to be related to their disordered conformations
. Due to the difficulties in analyzing flexible and disordered secondary structures, the
8
The coacervation of ELPs is attributed to the temperature-dependent changes in
9
interpeptide hydrophobic interactions. ELPs are hydrated in clathrate-like water molecules, [8, 21, 22]
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which shield the interpeptide hydrophobic interactions at low temperatures
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hypothesized that ELPs assemble via hydrophobic interactions after the collapse of the clathrates
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at high temperatures [8, 23-25]. In addition, the hydrophobic domains of ELPs are presumed to be
13
dominated by recurring β-turns
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important for interpeptide interaction formation
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that the structures of ELPs fluctuate between folded and disordered depending on the
16
temperature
17
not been clarified. Thus, further structural analyses of ELPs in conjunction with self-assembly
18
measurements to detect interpeptide interactions are required for elucidating the general
19
coacervation mechanism of ELPs.
[26, 27]
[26-30]
. It has been
, and it has been suggested that the β-structures are [31, 32]
. However, previous studies have revealed
. The essential structural factors for regulating the coacervation of ELPs have
20
Short ELPs with a strong coacervation properties have been developed to investigate the
21
mechanism of coacervation. Previous studies have indicated that a sufficiently high repetition
22
number (n > 40) is required for coacervation of ELPs such as (VPGVG)n
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investigate the structure of such a long peptide chain—more than 200 amino acid residues—
[33, 34]
. It is difficult to
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Biochemistry
1
without a fixed conformation. Our previous studies have demonstrated that synthetic
2
hydrophobic oligomers of H-(IPGVG)n-NH2, H-(FPGVG)n-NH2 [Fn], and H-(WPGVG)n-NH2 [Wn]
3
[34-36]
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respectively). It was demonstrated that the increased molecular hydrophobicity enhanced ELP
5
coacervation. Furthermore, we recently reported that dimeric analogs of F5, which were
6
synthesized via introduction of disulfide bonds at N-terminal additional Cys residues, showed
7
strong coacervation properties at lower temperatures and concentrations than the monomer
8
Therefore, short ELPs synthesized by disulfide bond-mediated dimerization allows for
9
convenient structural analyses and simultaneous measurements of coacervation compared to long
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ELPs. Thus, the dimeric elastin-derived peptides were assumed to be useful models for
11
elucidating the mechanism of coacervation due to their short length and strong coacervation
12
activity.
exhibit coacervation at significantly lower repetition numbers (n = 7, 5, and 3,
[37]
.
13
In the present study, we synthesized the novel, dimeric elastin-derived peptide analog
14
(H-C(WPGVG)3-NH2)2, abbreviated as (CW3)2, and investigated its self-assembly properties, dye
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uptake ability, and the structural features important for coacervation. It was demonstrated that
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the short, elastin-derived peptide analog did not require specific, ordered secondary structures for
17
its coacervation. Moreover, the increase in exposed hydrophobic surface area associated with the
18
structural shift mediated interpeptide interactions. This study revealed new information on the
19
relationship between the structure and function of short ELPs, and will be useful for further
20
elucidating and controlling the biophysical functions of elastin, ELPs, and other
21
biomacromolecules.
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Materials & Experimental details
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Chemicals
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Fmoc-amino acids and Rink Amide MBHA resin LL (100–200 mesh) were purchased
4
from
Merck
KGaA.
(Darmstadt,
Germany).
2-(1H-benzotriazole-1-yl)-
1,1,3,3-
5
tetramethyluronium hexafluorophosphate (HBTU) and 1-hydroxybenzotriazole (HOBt) were
6
purchased from Kokusan Chemical Co., Ltd. (Tokyo, Japan). 8-Anilino-1-naphthalenesulfonic
7
acid (1,8-ANS) was purchased from Sigma-Aldrich Co. (St. Louis, MO). Water for sample
8
preparation was purified by Milli-Q Integral 3 (Merck Millipore, Billerica, MA). Other reagents
9
for peptide synthesis were purchased from Watanabe Chemical Industries Ltd. (Hiroshima,
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Japan). Solvents for peptide synthesis and other reagents were also obtained from commercial
11
suppliers and used without further purification.
12 13 14
Synthesis of the monomer peptide A building block of the dimer H-C(WPGVG)3-NH2 [CW3] was synthesized by following [37]
15
the synthesis method in our previous study
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433A peptide synthesizer (Applied Biosystems, Foster city, CA) using the 0.1 mmol scale solid-
17
phase method by Fmoc chemistry. Rink Amide MBHA resin LL (100–200 mesh, 285 mg) was
18
used as the solid phase support. After deresination by a reagent cocktail containing
19
trifluoroacetic acid and 1,2-ethanedithiol, the peptide was purified by reversed phase-high
20
performance liquid chromatography (RP-HPLC). The peptide was obtained as a colorless
21
powder (40.5 mg, 25.2 µmol, 25.2%). The purity and molecular weight was confirmed by ultra-
. In brief, the substrate was synthesized by ABI
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Biochemistry
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performance liquid chromatography–mass spectrometry (UPLC–MS). Further detailed synthesis
2
protocols are described in the Supporting Information.
3 4
H-C(WPGVG)3-NH2.
Retention time = 1.907 min. MS (ESI) m/z, calculated for C78H104N20O16S
5
: 805.94 ([M + 2H]2+) , found 805.96.
6 7
Synthesis of the dimeric peptide
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The dimeric peptide (CW3)2 was synthesized by aerobic oxidation of purified CW3.
9
CW3 (6.49 mg, 4.03 µmol) was dissolved in 1 mg/mL ammonium bicarbonate/60% acetonitrile
10
aqueous solution (649 µL) [37]. This solution was stirred overnight at 5 °C by a rotator, ACR-100
11
(AS ONE Co., Osaka, Japan), in shake mode. The resulting mixture was purified by RP-HPLC.
12
The peptide was obtained as a colorless powder (5.88 mg, 1.82 µmol, 90.3%). The purity and
13
molecular weight were confirmed by UPLC–MS, with the method described in Supporting
14
Information. The molecular weight of the dimeric peptide was also strictly determined by matrix-
15
assisted laser desorption ionization (MALDI)–time of flight (TOF)–MS using a mass
16
spectrometer VoyagerTM DE-PRO (PerSeptive Biosystems Inc., Framingham, MA).
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(H-C(WPGVG)3-NH2)2. Retention time = 2.438 min. MS (ESI) m/z, calculated for
18
C156H206N40O32S2 : 1073.59 ([M + 3H]3+), found 1073.46 (Figure S1). MS (MALDI-TOF) m/z,
19
calculated 3218.75 ([M + H]+), found 3218.58 (Figure S2).
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Turbidity measurement
2
The temperature-dependent coacervation of (CW3)2 was evaluated using a JASCO V-
3
660 spectral photometer, (JASCO Co., Tokyo, Japan). Solutions of (CW3)2 were prepared at
4
0.050, 0.50, and 1.0 mg/mL in pure water. Turbidity measurements were collected at 400 nm
5
while increasing or decreasing the temperature by 0.2°C/min (for the 0.50 and 1.0 mg/mL
6
samples) or 0.5°C/min (for the 0.05 mg/mL samples) from 5°C. Each concentration was
7
measured at least three times. Coacervation was determined by the phase transition temperature
8
(Tt), which is temperature at which the turbidity of the solution reaches half the maximum value
9
[37]
10
. Reversibility was defined as the percent decrease in solution turbidity after cooling to 5°C
(which took at least 8 h) to the increase in absorbance after increasing the temperature [38].
11 12
Fluorescence measurement
13
The fluorescence of (CW3)2 was measured using 1,8-ANS and was conducted on a FP-
14
8500 Fluorescence Spectrometer (JASCO Co.). Fluorescence intensity of the peptide solution
15
was measured between 400–700 nm with excitation wavelength of 370 nm. The emission of the
16
peptide solution was measured at various concentration of 0.003–0.5 mg/mL in pure water
17
containing 50 µM 1,8-ANS
18
10 °C from 5 °C to 25 °C. The measurement of each concentration was performed at least three
19
times.
[39]
, and it was measured by increasing temperature at an interval of
20 21
Dynamic light scattering (DLS) analysis
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Biochemistry
1
The distribution of the particle size in (CW3)2 solution was analyzed by DLS
2
measurement using Zetasizer nano ZS (Malvern Instruments Ltd., Worcestershire, UK) in a
3
measurement cell ZEN0112 (Malvern Instruments Ltd.). The peptide sample solution was
4
diluted to a concentration of 1.0 mg/mL in pure water and filtered using the Millex®-LG (Merck
5
Millipore) filter before measurement. DLS analysis was performed by increasing temperature at
6
10 °C intervals from 5 °C to 65 °C. Measurement duration was selected automatically. Protein
7
(dataset: refractive index, 1.450; absorption, 0.001) was used as the material, and water (dataset:
8
refractive index, 1.330; viscosity, 0.8872) was chosen as the dispersant. Attenuation was selected
9
automatically. The measurement of each concentration was performed at least three times.
10 11
Optical microscopy
12
The morphologies of the coacervates of (CW3)2 in the presence and absence of a water-
13
soluble dye, Ponceau S (Sigma-Aldrich Co.) was observed by bright-field microscopy at 180X
14
magnification using a BIOREVO BZ-9000 (KEYENCE Co., Osaka, Japan) equipped with a
15
PlanApo VC 60X oil objective (digital zoom = 3X; Nikon Co., Tokyo, Japan). The peptide
16
solution was diluted to 1 mg/mL in pure water and applied to a glass slide. Sample imaging was
17
performed at 25°C or after heating to 60°C on a hot plate for 30 s.
18
Coacervates containing dye was prepared as follows: 1.0 mg/ml (CW3)2 solution was
19
prepared with 25 mM Ponceau S at 4°C. The mixture was heated to 60°C for 1 h and then
20
centrifuged (14,000 rpm, 2 min). The resulting precipitate was washed with hot water (60°C).
21
Bright-field microscopy was performed at 400X magnification using a Leica DM IL LED (Leica
22
Microsystems CMS GmbH, Wetzlar, Germany) equipped with HI PLAN 40X oil objective
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(Leica Microsystems CMS GmbH) and an HC PLAN 10X eyepiece (Leica Microsystems CMS
2
GmbH).
3 4
Molecular dynamics (MD) simulation
5
Computational experiments were performed using the software package Discovery
6
Studio 4.0 (Accelrys, Inc., San Diego, CA). All calculations were performed using DELL
7
PRECISION™ T3610 Workstation (Dell Inc., Round Rock, TX). MD simulations of (CW3)2
8
and W3 were performed at 278 K, 294 K, 310 K, 326 K, and 343 K. These models were
9
subjected to “Standard Dynamics Cascade” protocol, which implements a series of energy
10
minimization and molecular dynamics steps with the CHARMM force field. The simulation
11
parameters were set as described in a previous study [37]. Further detailed synthesis protocols are
12
described in the Supporting Information.
13 14
Circular dichroism (CD) measurement
15
CD measurement was performed in a 1.0 mm path-length cuvette using a JASCO J-725
16
spectropolarimeter (JASCO Co.). (CW3)2 was dissolved in pure water at 0.1 mg/mL. Spectra of
17
the sample solution were measured from 190 to 260 nm at various cell temperatures between 5
18
°C and 65 °C. All spectra of the peptide solution were obtained by subtracting the solvent spectra
19
obtained under the same conditions and smoothing with Savitzky–Golay smoothing filters. The
20
measurement was performed two times.
21
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Biochemistry
1
Results and Discussion
2
Synthesis of the peptide
3
The monomeric peptide CW3 was successfully synthesized by a conventional solid
4
phase peptide synthesis procedure and then dimerized by aerobic oxidation in 60% acetonitrile
5
aqueous solution with 1 mg/mL ammonium bicarbonate. The dimerization was not successful in
6
pure water owing to the production of insoluble CW3 precipitate. Therefore, acetonitrile aqueous
7
solution was used to dissolve the peptide deposition. The purity and molecular weight of each
8
peptide were confirmed by RP-UPLC-MS and MALDI-TOF-MS (Figures S1 and S2). The
9
synthetic yield of the dimeric peptide was approximately 90%. In summary, we found that the
10
reaction conditions were suitable to obtain a dimeric short elastin-like peptide with a high yield.
11 12
Coacervation of the dimeric peptide
13
The temperature-dependent coacervation of the synthetic peptide, (CW3)2, was
14
evaluated by measuring the turbidity of aqueous peptide solutions at various concentrations. To
15
quantitatively evaluate coacervation, Tt and reversibility were calculated from the change in
16
turbidity [37, 38]. Our previous study showed that at least 30 mg/mL of W3 monomer was required
17
to demonstrate turbidity [36]. In comparison with the W3 monomer, (CW3)2 showed coacervation
18
at significantly lower concentrations of 0.50 and 1.0 mg/mL (Figure 1 and Table 1), which
19
indicated that dimerization significantly enhanced the coacervation of the W3 monomer.
20
Similarly, this trend has been observed in dimeric peptides of F5
21
required a concentration of at least 10 mg/mL and a longer chain length than the W3 dimer to
22
exhibit coacervation. Thus, it was established that (CW3)2 possessed a stronger coacervation
[37]
. However, F5 dimers
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propensity than the F5 dimer. Peptides that exhibit properties at low concentrations and having
2
short chain lengths can be advantageous for analytical experiments and applied research [34-37].
3
Thus, we hypothesized that (CW3)2 could be used to elucidate the mechanism of coacervation.
4
We concluded that dimeric peptides demonstrate distinct characteristics from their linear peptide
5
analogs that have longer peptide chains. Specifically, (CW3)2 showed enhanced coacervation
6
while maintaining high water solubility, whereas the linear 6-mer analog of (WPGVG),
7
C(Cyc)W6, had low water solubility and irreversible self-assembly (Figures S3 and S4). Thus,
8
ELP dimers are an effective method for obtaining peptide analogs that possess strong
9
coacervation abilities and are easy to handle.
10
In this study, (CW3)2 showed hysteresis during coacervation. In the turbidity assay
11
profile, the two turbidity curves of (CW3)2 obtained while heating and cooling the sample did
12
not coincide. This disagreement between the heating and cooling processes could indicate that
13
aggregates formed during heating remained stable while cooling to temperatures below the Tt.
14
However, the turbidity of the dimer solution gradually lowered when the temperature reached
15
below 10°C with some additional time. Finally, almost complete reversibility was observed after
16
maintaining low temperature for a several hours (5°C for at least 8 h). This hysteresis was also
17
observed for the F5 dimer
18
244) that contains repeats of exons 20–24 from the human aortic elastin gene
19
previous studies determined that the aggregation and dissociation rates of the ELPs disagreed
20
with each other. Similar to these reports, the dissociation of (CW3)2 progressed more slowly
21
than the aggregation. These results suggested that hysteresis during coacervation of (CW3)2 was
22
caused by differences in the association and dissociation rates.
23
Figure 1 and Table 1
[37]
and other ELPs, such as (APGVGV)n, (VPAVG)n, and (EP20– [39-41]
. These
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Biochemistry
1 2 3
Existence of invisible initial microcoacervates The self-assembly behavior of (CW3)2 was examined by the use of the fluorescent [42]
4
probe 1,8-ANS
. The fluorescence analysis showed that the fluorescence intensity increased
5
when the concentration of (CW3)2 solution was higher than 0.03 mg/mL (Figure 2A). This
6
increase in the fluorescence intensity at a particular peptide concentration indicated that 1,8-ANS
7
penetrated into the hydrophobic peptide assemblies. These results showed that the peptides
8
required a critical concentration to form assemblies and suggested that the initial
9
microaggregates may be generated above the boundary concentration.
10
The effect of temperature on the critical concentration of (CW3)2 was also investigated.
11
The analysis was only performed at relatively low temperatures (5 °C, 15 °C, and 25 °C),
12
because the fluorescence intensity was significantly decreased at higher temperatures. The
13
critical concentrations were analyzed by the two-line method
14
0.05 mg/mL, 0.032 ± 0.05 mg/mL, and 0.033 ± 0.05 mg/mL at 5 °C, 15 °C, and 25 °C,
15
respectively (Figures 2B and S5). Therefore, a temperature-dependent critical concentration was
16
not observed between 5 °C and 25 °C. However, these observed critical concentrations were
17
significantly lower than the concentrations at which the peptide solution became turbid, which
18
suggested that the formation of initial invisible microaggregates occurred at a low temperature
19
and at a concentration at which coacervation was apparently not observed. Consequently,
20
fluorescence analysis has revealed a novel morphology of (CW3)2 that could not be observed by
21
conventional turbidity measurements.
[42]
and were calculated as 0.031 ±
22
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Figure 2
2 3
Size distribution of the microaggregates
4
The coacervation behavior of (CW3)2 was also analyzed by DLS analysis at various
5
temperatures in the range from 5–65 °C. The observed distribution of the hydrodynamic diameter
6
of the peptide aggregates is shown in Figure 3. In this analysis, (CW3)2 showed a broad peak at
7
approximately 100 nm between 5 °C and 25 °C. Moreover, DLS analysis of the turbidity showed
8
that the submicrometer aggregates did not induce apparent phase transition behavior.
9
Furthermore, the size of the aggregates increased with an increase in temperature (Figure 3).
10
Because light scattering and turbidity are dependent on the particle size, the growth of the
11
aggregates would imply coacervation. Based on the DLS analysis, we suggested that the
12
coacervation of (CW3)2 probably follows a stepwise process in which the generation of
13
microaggregates is followed by coacervate maturation triggered by the increase in temperature.
14 15
Figure 3
16 17
Observation of the coacervate morphology
18
The optical microscopy analysis of (CW3)2 solution was performed to study the
19
morphology of the aggregates at different temperatures. Microscopic images of the peptide
20
solution were captured at 25 °C and after heating to 60 °C (Figure 4). At 25 °C, several dozen
21
distorted and non-spherical microaggregates were observed (Figure 4A). Microaggregates of
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Biochemistry
1
(CW3)2 were formed below the phase transition temperature. Although microaggregates
2
between 0.2 µm and 0.8 µm in diameter were hardly observed in solution, microaggregates
3
between 0.8 µm and 1.0 µm in diameter, which were also observed in the DLS measurement,
4
were commonly observed (Figure S6). After heating, the number of spherical coacervates was
5
significantly increased at 60 °C. Microaggregates between 0.8 µm and 1.0 µm in diameter were
6
also predominantly observed (Figures 4B and S6). Owing to the limited resolution of the optical
7
microscope, smaller microaggregates (approximately 200 nm or less) were hardly observed;
8
therefore, the measurements were not as specific as those obtained in DLS and the size
9
distribution did not necessarily agree with DLS. In this study, the distribution trend changed
10
between 200 nm and 1000 nm; an increase in the distribution of large aggregates in optical
11
microscopy (Figure S6) was similar to that observed in the DLS measurement (Figure 3), but a
12
change in the dominant distribution between two temperatures was not clearly observed in
13
optical microscopy. Consequently, it was suggested that the increment in turbidity during
14
coacervation was derived from the proliferation of the aggregates observed in microscopy and
15
the increase in the distribution of large aggregates, which could be also observed in DLS. The
16
morphological changes in the peptide aggregates affected the coacervation behavior. Because
17
these results were consistent between fluorescence and DLS analyses, the hypothesis of the
18
stepwise coacervation process was strongly supported.
19
Furthermore, the ability to hold water-soluble dye was observed in the coacervate of
20
(CW3)2. As shown in Figure S7, the dye uptake of the (CW3)2 coacervate was observed at 60°C
21
and was also stable during observation at 25°C. The uptake ability of exogenous molecules such
22
as drugs and the stability of the coacervate at low temperatures might be useful while developing
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Page 16 of 49
1
ELP biomaterials possessing temperature-sensing capabilities, such as matrices for drug delivery
2
systems or tissue engineering.
3 4
Figure 4
5 6
Estimation of the structural properties of the dimeric peptide by MD simulation
7
The analysis of the structural properties of the dimeric peptide was valuable to
8
determine the intermolecular events of self-assembly. Thus, the conformational behavior of W3
9
and (CW3)2 in the solution was estimated by MD simulation at various target temperatures. In
10
addition, the structural parameters of these peptides were analyzed from the trajectories of the
11
MD simulation.
12
A proportion of the representative secondary structures in the peptides was calculated
13
from the trajectory. The representative structures of W3 and (CW3)2 at varying temperatures are
14
shown in Figures 5 and S8. The secondary structures were determined by using the method of
15
Kabsch and Sander
16
structures (Table 2). The ratios of each secondary structure on a residue were also estimated. The
17
turn structure frequently appeared in each PGV sequence and was present in the middle of the
18
building block. The sheet structures were formed in VG and WP sequences, which were present
19
at the either sides of the turns (Figure S9). These peptides exhibited a well-folded structure and
20
lower Rg between 278 K and 310 K. As shown in Figure 5, accumulated turn structures were
21
frequently observed in the dimer at 273 K. In addition, the consecutive secondary structure sheet-
[43]
. The peptides primarily showed turns, sheets, and random-coiled
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Biochemistry
1
turn-sheet was frequently observed at 294 K and 310 K. However, the proportion of these
2
secondary structures decreased with increased simulation temperature. A random coiled structure
3
was predominantly observed at 326 K and 343 K. These results suggested that the dimeric
4
peptide possessed a tendency to alter the ordered structure observed at low temperatures to a
5
disordered structure at higher temperatures.
6 7
Figure 5 and Table 2
8 9
The Rg and total solvent-accessible surface area (SASA) value were calculated to
10
describe the manner in which the structural changes of the peptide chain were associated with
11
temperature change (Table 2). These values increased gradually with an increase in temperature.
12
Notably, the changes in the Rg and SASA values of the dimeric peptide were significantly higher
13
than those of the monomer, which suggested that the dimeric peptide experienced a remarkable
14
change in structure with increases in temperature. The SASA value of the side chain on each
15
residue was also calculated in the trajectory at various simulation temperatures (Figure 6).
16
Although the SASA value of each residue tended to increase with an increase in temperature, the
17
change in the dimer was more significant than that in the monomer. In particular, the SASA
18
values of hydrophobic residues, such as valine and tryptophan, were markedly altered in the
19
dimeric peptide. As the SASA value of the monomer did not change drastically, it was plausible
20
that the molecular surface of the monomeric peptide was exposed in both ordered or disordered
21
states. In contrast, it has been suggested that the hydrophobic surface of the dimeric peptide
22
would be embedded when the peptide dissolves in water, which implied that the estimated
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Page 18 of 49
1
molecular structure of the dimeric peptide preserved its water solubility by effectively
2
embedding hydrophobic residues into the interface between single peptide chains. The increase
3
in SASA value with a corresponding increase in temperature indicated that the secondary
4
structures could collapse and the folded structure of the dimeric peptide shifted to an extended
5
structure. Because the extended structure of (CW3)2 was not water dispersible, the molecules of
6
(CW3)2 assembled to form hydrophobic intermolecular interactions via the hydrophobic surfaces
7
of the peptides. This drastic change in the hydrophobic surface may contribute toward the potent
8
coacervation property of (CW3)2. Furthermore, these results may indicate that coacervation
9
occurred primarily as a result of the exposure of the hydrophobic surface of the peptides and not
10
as a result of the formation of a particular structure.
11 12
Figure 6
13 14
The structural transitions of the dimeric peptide are temperature-dependent
15
Since the conformational change of (CW3)2 was temperature-dependent, its structure
16
was further analyzed by circular dichroism spectroscopy. A reversible spectrum shift was
17
observed during heating and cooling (Figure 7). The spectrum showed a minor negative band at
18
225 nm, a positive band at 220 nm, and a prominent negative band at 198 nm. As the
19
temperature increased, the intensity of these bands decreased; this result was similar to the CD
20
spectra of the W3 monomer observed in our previous study
21
exhibited conformational changes similar to the monomer. Conversely, it was considered that the
22
structural features of the peptide were not altered by dimerization. In addition, this spectral
[36]
. Thus, the dimeric peptide
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Biochemistry
1
change was similar to that observed during disordering of collagen helices or polyproline helix II
2
structures
3
based on proline at low temperature and was converted to a disordered structure during heating.
[44-46]
. Thus, it was suggested that the dimeric peptide formed a helix-like structure
4 5
Figure 7
6 7
Plausible mechanism of the stepwise coacervation process of ELP
8
The stepwise coacervation process of the dimeric peptide (CW3)2, with detailed
9
analyses of the morphology after coacervation, is shown in Figure 8. As shown in Figure 2,
10
(CW3)2 exhibited a critical concentration for the generation of initial microaggregates. In
11
addition, these aggregates matured at higher temperatures, showing increased size and
12
proliferation. To the best of our knowledge, we report the first demonstration of these
13
characteristic properties of the ELP analog using the tryptophan residue. Previous studies
14
showed that the hydrophobicity of the residue enhanced the coacervation property of ELP
15
34-35]
16
residue affected the morphology of the coacervates. Hydrophobic amino acids are abundantly
17
contained in tandem repeats of elastin. Therefore, the morphology of elastin could be regulated
18
by an ingenious combination of hydrophobic amino acid residues.
[14-18,
. In addition to these studies, the present study revealed that the hydrophobicity of the
19 20
Figure 8
21
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1
Page 20 of 49
Insights into the coacervation mechanism of the dimeric peptide
2
In this study, we demonstrated novel insight into the relationship between the structure
3
and coacervation property of ELP. The hydrophobicity of (CW3)2 was extremely potent; the
4
peptide formed microaggregates, even at low concentration and temperature. Previous studies
5
have suggested that ELP exhibit coacervation via collapse of the clathrate water
6
Therefore, we considered that the strong hydrophobicity of the dimeric peptide effectively
7
destabilized the hydrating water. Consequently, the potent coacervation property of (CW3)2 that
8
resulted from the hydrophobic interpeptide interaction occurred during the early stages of
9
aggregate formation (Figure 8). Previous studies have suggested that the manner of the structural [30, 47, 48]
[8, 21-25]
.
10
shift of ELP was dependent on the peptide chain length
11
that longer ELP exhibited stronger coacervation property and were likely to show ordered
12
structures at high temperatures [47, 48]. However, the results of this study clearly indicated that the
13
short dimeric elastin-like peptide (CW3)2 possessed a potent coacervation property and that the
14
structure was disordered at high temperatures. Thus, this study showed that the expression of
15
coacervation property did not necessarily require long peptide chain length or specific ordered
16
structure at high temperatures, but required potent hydrophobicity and soluble structures at low
17
temperatures. Therefore, we believe that this study offered new insights into the self-assembly
18
mechanism of ELP, based on the results of hydration, dispersion, and stereostructural analyses of
19
the hydrophobic molecule. Research on IDP, including ELP, has gained momentum in recent
20
years [1-4, 6, 11] and the applications of ELP have been fervently studied [9, 10, 13]. The present study
21
on ELP appears to provide insights with respect to its structure and coacervation properties that
22
would assist the design of more efficient ELP for industrial applications and support future
23
research on IDP.
. Moreover, it was considered
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Biochemistry
1 2
Conclusion
3
In this study, we conducted turbidity measurements, fluorescence microscopy, dynamic
4
light scattering (DLS), molecular dynamics (MD) simulation, and circular dichroism (CD)
5
spectroscopy on the novel, model, elastin-derived, dimeric peptide (H-C(WPGVG)3-NH2)2. The
6
results revealed that the hydrophobicity of the residues regulated the morphology of the
7
aggregates. Moreover, it was shown that the dimeric peptide exhibited strong coacervation and
8
ability to uptake dye, despite its low molecular weight and disordered structure at high
9
temperatures. It was also suggested that its coacervation was dependent on the hydrophobicity
10
and structure solubility at low temperatures rather than the high molecular weight compounds or
11
formation of any specific ordered structures at high temperatures. In conclusion, these findings
12
elucidated the coacervation mechanism of the short-length ELP dimer and demonstrated the
13
potential for the future development of short coacervatable peptide-based biomaterials.
14 15
Supporting Information.
16
The supporting information includes detailed experimental procedures regarding peptide
17
synthesis and molecular dynamics simulations. This section also includes the following
18
supporting figures and a table: identification of (CW3)2 by ultra-performance liquid
19
chromatography (UPLC) (Figure S1), matrix-assisted laser desorption ionization-time of flight
20
spectrometry (MALDI-TOF) (Figure S2), structure of C(Cys)W6 (Figure S3), coacervation of
21
C(Cys)W6 (Figure S4), dynamic light scattering results (Figure S5), optical microscopy (Figure
22
S6 and S7), molecular dynamics simulations results (Figures S8, S9 and Table S1), and
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Page 22 of 49
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identification of C(Cys)W6 by UPLC (Figure S10) and MALDI-TOF (Figure S11). This
2
information is available free of charge via http://pubs.acs.org.
3 4
Corresponding Authors
5
Prof. Takeru Nose
6
e-mail:
[email protected] 7 8
Funding Sources
9 10
This work was supported by JSPS KAKENHI Grant Number JP26550068 and JP17K20066, and research fund by Urakami Foundation.
11 12 13
Notes The authors declare no competing financial interests.
14 15 16 17 18
Acknowledgment We thank Dr. Ayami Matsushima (Associate Professor of Kyushu university) for equipment use and her help in CD spectra measurement.
19 20
Abbreviations
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Biochemistry
1
1,8-ANS, 8-anilino-1-naphthalenesulfonic acid; CD, circular dichroism; CHARMm,
2
chemistry at Harvard macromolecular mechanics; DLS, dynamic light scattering; ELP, elastin
3
derived polypeptides; Fmoc, 9-fluorenylmethyloxycarbonyl; GBSW, generalized born with
4
simple
5
hexafluorophosphate; HOBt, 1-hydroxybenzotriazole; HPLC, high performance liquid
6
chromatography; IDPs, Intrinsic disordered proteins; LCST, lower critical solution temperature;
7
MALDI, matrix-assisted laser desorption/ionization; MD, molecular dynamics; MS, mass
8
spectrometry; Rg, radius of gyration; RP, reverse phase; SASA, solvent-accessible surface area;
9
TOF, time of flight; Tt, phase transition temperature; UPLC, ultra performance liquid
10
switching;
HBTU,
2-(1H-benzotriazole-1-yl)-1,1,3,3-tetramethyluronium
chromatography
11
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Biochemistry
[46] Tamburro, A. M., Lorusso, M., Ibris, N., Pepe, A., Bochicchio, B. (2010) Investigating by circular dichroism some amyloidogenic elastin-derived polypeptides, Chirality 22, E56-66.
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[47] Ghoorchian, A., Holland, N. B. (2011) Molecular architecture influences the thermally
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induced aggregation behavior of elastin-like polypeptides, Biomacromolecules. 12, 4022-
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4029.
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[48] Zhao, B., Li N. K., Yingling, Y. G., Hall, C. K. (2016) LCST Behavior is Manifested in a
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Single Molecule: Elastin-Like polypeptide (VPGVG)n, Biomacromolecules 17, 111-118.
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Figures & Tables
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Figure 1. Turbidity measurement of (CW3)2.
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Turbidity changes associated with heating (solid line) and cooling (dashed line) were shown.
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Figure 2. Fluorescent measurement at various concentration of (CW3)2 with 1,8-ANS. (A) Fluorescence spectra of 50 µM 1,8-ANS were measured at 5 °C and various concentration of peptide. (B) Critical concentration of (CW3)2 was determined from maximum fluorescence intensity of the spectra by the two-line method. Assays were repeated six times and the critical concentration was calculated with the mean SE.
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1 2 3
Figure 3. Particle size distribution of (CW3)2 at various temperature.
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Micro-aggregation of the peptide grew up its size with increasing temperature.
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Biochemistry
1 2 3
Figure 4. Phase-contrast microscopy images of (CW3)2.
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(A) The images were obtained at room temperature (25 °C) and (B) after heating at 65 °C. An aqueous solution of the peptide was prepared at concentration of 1.0 mg/mL.
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1 2 3
Figure 5. Representative structures of (CW3)2 estimated by MD simulation.
4 5 6 7
The structure at (A) 278.0 K, (B) 294.0 K, and (C) 343.0 K were shown. The dimeric peptide shifted disordered structure by increasing temperature. Each secondary structure was indicated as follows, light blue: sheet, green: turn, and white random.
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Biochemistry
Figure 6. SASA of side chain at each residue of (CW3)2. The SASA values of monomer (A) and dimer (B) were obtained from trajectory analyses of the MD simulation.
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1 2 3
Figure 7. CD spectra of (CW3)2 at various temperature.
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The spectra were measured from 5 °C to 65 °C with increasing temperature. Inset shows spectra with decreasing temperature.
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Biochemistry
Figure 8. Images of structural feature and stepwise coacervation model of (CW3)2. The morphology is changed stepwise. The dimeric peptide would be dissolved in water as microaggregation over critical concentration, by taking soluble structure. However, heating would cause destabilization of hydration and maturing of coacervation.
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Table 1. Properties in turbidity measurement of (CW3)2. Concentration
Tt [˚C]
Maximum OD400
Reversibility (%)
1.0 mg/mL
38.5 ± 1.5
0.63 ± 0.03
97.9 ± 1.0
0.50 mg/mL
40.3 ± 1.5
0.41 ± 0.03
99.1 ± 0.8
0.050 mg/mL
N. D.
0.032 ± 0.016
N. D.
Assays at a concentration of 1.0 mg/mL and 0.5 mg/mL were repeated seven times. The assay at concentration of 0.050 mg/mL was repeated three times. Data were shown with the mean ± standard error. N. D., not determined.
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Table 2. Structural properties of (C(WPGVG)3)2 obtained from MD simulation. Temperature Rg (Å) (K) 278.0 9.09 ± 0.02 294.0 9.29 ± 0.07 310.0 10.81 ± 0.15 326.0 14.68 ± 0.18 343.0 15.10 ± 0.16
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Total SASA Random coil (Å2) (%) 2357.3 ± 7.2 75.6 ± 0.5 2392.8 ± 11.9 61.2 ± 0.4 2656.6 ± 21.7 75.6 ± 0.6 3230.2 ± 21.5 85.3 ± 0.7 3274.6 ± 18.2 84.5 ± 0.7
Turn (%) 23.1 ± 0.5 20.7 ± 0.2 19.4 ± 0.4 13.1 ± 0.6 12.5 ± 0.5
Sheet (%) 1.2 ± 0.3 17.9 ± 0.5 4.9 ± 0.5 1.3 ± 0.2 2.9 ± 0.4
The properties were obtained from trajectories of the MD simulation with the mean SE. Contents of secondary structure were calculated as ratios of the residue recognized as each secondary structure by the discovery studio to the number of all residues.
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TOC Graphic (For Table of Contents Use Only)
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Title: Stepwise mechanism of temperature-dependent coacervation of the elastin-like peptide
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analog dimer, (C(WPGVG)3)2
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Authors: Daiki Tatsubo, Keitaro Suyama, Masaya Miyazaki, Iori Maeda, and Takeru Nose
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Biochemistry
Figure 1. Turbidity measurement of (CW3)2. Turbidity changes associated with heating (solid line) and cooling (dashed line) were shown.
51x31mm (300 x 300 DPI)
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Biochemistry 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60
Figure 2. Fluorescent measurement at various concentration of (CW3)2 with 1,8-ANS. (A) Fluorescence spectra of 50 µM 1,8-ANS were measured at 5 °C and various concentration of peptide. (B) Critical concentration of (CW3)2 was determined from maximum fluorescence intensity of the spectra by the two-line method. Assays were repeated six times and the critical concentration was calculated with the mean SE.
51x14mm (300 x 300 DPI)
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Biochemistry
Figure 3. Particle size distribution of (CW3)2 at various temperature. Micro-aggregation of the peptide grew up its size with increasing temperature.
51x31mm (300 x 300 DPI)
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Biochemistry 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60
Figure 4. Phase-contrast microscopy images of (CW3)2. (A) The images were obtained at room temperature (25 °C) and (B) after heating at 65 °C. An aqueous solution of the peptide was prepared at concentration of 1.0 mg/mL.
51x14mm (300 x 300 DPI)
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Biochemistry
Figure 5. Representative structures of (CW3)2 estimated by MD simulation. The structure at (A) 278.0 K, (B) 294.0 K, and (C) 343.0 K were shown. The dimeric peptide shifted disordered structure by increasing temperature. Each secondary structure was indicated as follows, light blue: sheet, green: turn, and white random.
51x14mm (300 x 300 DPI)
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Biochemistry 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60
Figure 6. SASA of side chain at each residue of (CW3)2. The SASA values of monomer (A) and dimer (B) were obtained from trajectory analyses of the MD simulation.
51x14mm (300 x 300 DPI)
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Biochemistry
Figure 7. CD spectra of (CW3)2 at various temperature. The spectra were measured from 5 °C to 65 °C with increasing temperature. Inset shows spectra with decreasing temperature.
51x31mm (300 x 300 DPI)
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Biochemistry 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60
Figure 8. Images of structural feature and stepwise coacervation model of (CW3)2. The morphology is changed stepwise. The dimeric peptide would be dissolved in water as micro-aggregation over critical concentration, by taking soluble structure. However, heating would cause destabilization of hydration and maturing of coacervation. 51x31mm (300 x 300 DPI)
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TOC Graphic (For Table of Contents Use Only) Title: Stepwise mechanism of temperature-dependent coacervation of the elastin-like peptide analog dimer, (C(WPGVG)3)2 Authors: Daiki Tatsubo, Keitaro Suyama, Masaya Miyazaki, Iori Maeda, and Takeru Nose
34x13mm (300 x 300 DPI)
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