Centre for Bioprocess Technology, Department of Biochemistry and
Molecular Biology, Monash University, Victoria 3800, Australia
In this paper, a general procedure is described to
determine thermodynamic parameters associated with the interaction of
thrombin receptor antagonistic peptides (TRAPs) with immobilized
nonpolar ligands. The results show that these interactions were
associated with nonlinear van't Hoff dependencies over a wide
temperature range. Moreover, changes in relevant thermodynamic
parameters, namely the changes in Gibbs free energy of interaction,
G
, enthalpy of interaction,
H
, entropy of interaction,
S
, and heat capacity,
C
, have been related to the structural properties of these TRAP analogs. The implications of these
investigations for the design of thrombin receptor agonists/antagonists
with structures stabilized by intramolecular hydrophobic interactions are discussed.
 |
LIST OF SYMBOLS |
| b(0), b(1), b(2),
b(3) ... |
Coefficients for the polynomial dependency of ln
k' versus 1/T |
| c1 |
Mole fraction of displacing solvent |
Aapolar |
Apolar accessible surface area |
Apolar |
Polar accessible surface area |
Atotal |
Total accessible surface area |
C |
Change in the heat capacity for the association of the polypeptide
Pi with the nonpolar ligands |
G |
Change in Gibbs free energy due to the association of the polypeptide
Pi with the nonpolar ligands |
H |
Change in the enthalpy due to the association of the polypeptide
Pi with the nonpolar ligands |
S |
Change in the entropy due to the association of the polypeptide
Pi with the nonpolar ligands |
 |
Volume fraction of organic solvent in binary water-solvent mixture |
 |
Phase ratio of the chromatographic system (=
VS/VM) |
| Kassoc |
Equilibrium binding constant |
| k' |
Capacity factor, k' = (te t0)/t0 = (nS/nM) × (VS/VM) = Kassoc ×  |
| ln k' |
Logarithm of the capacity factor, k' |
| ln k0 |
Value of ln k' when ci 0, or 0 |
| nS |
Number of moles of the peptide in the bound states |
| nM |
Number of moles of the peptide in the free states |
| Nres |
Number of amino acid residues in a polypeptide |
| r2 |
Correlation coefficient |
| R |
Gas constant |
| t0 |
Retention time of noninteracting solute |
| te |
Retention time of a polypeptide Pi |
| T |
Temperature in degrees Kelvin |
| TH |
Temperature at which H 0 |
| TS |
Temperature at which T S 0 |
| VM |
Volume of the solvent in the system |
| VS |
Volume of the immobilized ligands plus support matrix in the system |
 |
INTRODUCTION |
Protease-activated receptors (PARs) play an important role in
platelet function. In particular, various serine proteases, including
thrombin, are known to activate PARs by cleaving their amino-terminal
extracellular domains to reveal a new amino terminus that can then
function as a tethered ligand. By binding intramolecularly to the
receptor, the tethered ligand causes transmembrane signaling (Vu et
al., 1991
). In human platelets, a dual receptor system for the
activation of PARs has been found to occur (Kahn et al., 1998
). From an
experimental perspective, the existence of this second
receptor-mediated pathway adds a further level of complexity in the
cell biology of PAR activation. However, it also has the potential to
provide exquisite levels of regulation for a diverse range of
physiological functions, including a safeguard against irreversible
activation or inhibition of a single class of PAR receptor by potent
agonists/antagonists.
The thrombin receptor (PAR-1) is a transmembrane G-protein-coupled
structure that is activated by serine protease cleavage of its
extracellular N-terminus to expose an agonist peptide ligand that is
tethered to the receptor itself. Synthetic peptides that contain the
agonist motif of human PAR-1, such as H-Ser-Phe-Leu-Leu-Arg-Asn-Pro-OH (TRAP-1) (Mari et al., 1994
), are capable of receptor activation in the
absence of thrombin. TRAP-1 has been used as a pharmacological tool to
probe the function of the PAR-1 receptor in various cell types (Mari et
al., 1994
; Seiler et al., 1996
). Replacement of Phe2 with
Ala in TRAP-1, with elimination of the
-phenyl side chain group,
results in complete receptor inactivation (Nose et al., 1998a
). Other
results indicated that the electrostatic interaction of the
guanidino-group of Arg5 is important for TRAP-1 to interact
with its receptor (Nose et al., 1998b
). On the basis of introduced
conformational perturbations, structure-function relationships of
various bioactive thrombin receptor-activating peptide analogs (TRAPs),
prepared by solid phase peptide synthesis procedures, have been
explored in vitro with cultured human glomerular messiangial cells
(Troyer et al., 1992
), naturally thrombin-responsive CCL-29 cells and
Jurkat T cells (Mari et al., 1994
) and in vivo in rabbit models (M. Cunningham, K. Tipping, S. Holdsworth, R. I. Boysen, and M. T. W. Hearn, unpublished results). Based on these latter and other
studies (Ceruso et al., 1999
), it has been proposed that an extended
structure of the agonist peptide is responsible for receptor
recognition, with a hydrophobic contact occurring between the side
chains of Phe2 and Leu4.
To gain further insight into the conformational and interactive
behavior of TRAP analogs, the interaction of TRAP-1 and a complete set
of Ala-replacement analogs (Table 1) with
immobilized n-octyl ligands has been investigated. The use
of immobilized n-alkyl or phospholipid ligands to illuminate
the biophysical basis of the structure-function behavior of bioactive
peptides has attracted increasing attention during the past several
years (Houston et al., 1998
; Kondejewski et al., 1999
; Beyermann et al., 1996
; Hearn, 2001b
). In particular, these procedures permit the
thermodynamics of peptide-ligand interaction to be studied. Insight
can thus be gained into the role of intramolecular hydrophobic stabilization or the consequences of solvation/desolvation effects, permitting correlations to be established with membrane-associated receptor binding events and the respective changes in the Gibbs free
energy,
G
, enthalpy,
H
, entropy,
S
, and heat capacity,
C
, for peptide-ligand interactions
determined. In the present studies, changes in thermodynamic parameters
associated with TRAP-peptide-n-octyl ligand interactions
have been evaluated in terms of the molecular structure and the
associated linear free energy relationships of these peptides. Based on
these results, guidelines can be proposed to facilitate the design of
TRAP-1 analogs with enhanced stability in nonpolar environments.
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|
TABLE 1
Peptide code, sequence, molecular weight (MW), accessible
surface areas, Atot (Å2) for
the unfolded and folded forms of the peptide analogs, relative
hydrophobicity, and RP-HPLC elution order of the TRAP peptide analogs
|
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 |
EXPERIMENTAL PROCEDURES |
Chemicals and reagents
Acetonitrile (HPLC grade) was obtained from Biolab Scientific
Pty. Ltd. (Sydney, Australia); all other solvents were of analytical grade. Water was distilled and deionized in a Milli-Q system
(Millipore, Bedford, MA). Trifluoroacetic acid (TFA),
N,N-dimethylformamide (DMF), piperidine,
1-hydroxybenzotriazole (HOBt),
O-benzotriazole-N,N,N',N'-tetramethyluronium-hexafluorophosphate (HBTU), Boc-L-Pro-PAM-resin and all of the
L-
-Boc-protected and L-
-Fmoc-protected
amino acids were obtained from Auspep Pty. Ltd. (Melbourne, Australia).
Thioanisole, acetic anhydride, 1,3-dilsopropylethylamine (DIEA), and
trifluoromethanesulphonic acid (TMFSA) were obtained from
Aldrich Chemical Co. (Milwaukee, WI).
Solid phase peptide synthesis
The thrombin receptor antagonistic peptides, TRAP-1
(H-Ser-Phe-Leu-Leu-Arg-Asn-Pro-OH), and the alanine-scan analogs,
TRAP-2 (H-Ser- Ala-Leu-Leu-Arg-Asn-Pro-OH), TRAP-3
(H-Ser-Phe-Ala-Leu-Arg-Asn-Pro-OH), TRAP-4
(H-Ser-Phe-Leu-Ala-Arg-Asn-Pro-OH), TRAP-5
(H-Ser-Phe-Leu-Leu-Ala-Asn-Pro-OH), and TRAP-6
(H-Ser-Phe-Leu-Leu-Arg-Ala-Pro-OH) respectively, were synthesized by
9-fluorenylmethyloxycarbonyl (Fmoc)/Boc solid phase peptide
synthesis procedures (Fields and Noble, 1990
; Keah et al., 1998
; Boysen
and Hearn, 2000
). The synthesis of TRAP was performed using the
Boc-L-Pro-PAM-resin (0.88 mmole/g) at a 0.5-mmol scale using a combined
Fmoc/Boc strategy. Typically, the appropriate Boc- or Fmoc-amino acids
(3 eq), HOBt (3 eq) and HBTU (3 eq) dissolved in DMF (5 ml) with 0.25 ml DIEA were used. During the synthesis, the presence of free amino
groups was monitored by the ninhydrin test (Kaiser et al., 1970
). The
synthesis was started using Boc-chemistry (TFA deprotection of Pro)
with the following two Boc-protected amino acids double-coupled. This
double-coupling strategy was predicated on the fact that the extent of
deprotection of the first residue, Pro (being a secondary amino acid),
cannot be tested with the ninhydrin reagent, whereas the ninhydrin test
gives ambiguous results following deprotection of Asn (and Ser)
(Fontenot et al., 1991
). After each deprotection with TFA,
neutralization was performed with 10% (v/v) DIEA in DMF. Following
incorporation of the Asn residue, the synthesis was then based on
Fmoc-chemistry with deprotection of the next and subsequent residues
achieved with 20% (v/v) piperidine in DMF. Earlier utilization of
Fmoc-chemistry in the SPPS inevitably lead to the release of the AsnPro
dipeptide from the resin as the cyclic dipeptide diketopiperazine
(Fields and Noble, 1990
; Bornstein and Balian, 1977
).
The synthesis of the Ala-scan TRAP analogs was performed using similar
methods, with the exception that a split resin strategy was used,
whereby after each coupling the resin was dried and
of the
resin was placed in a separate vessel, prior to coupling the Boc- or
Fmoc-Ala residue. The syntheses then proceeded in parallel in an
analogous manner to that used for the parent peptide, with the
respective peptide-resin repeatedly dried and subdivided until all
peptide sequences had been synthesized.
The cleavage of the crude peptide products was performed with TFMSA by
incubating 500 mg peptide-resin with 0.25 ml ethane-1,2-dithiol and 0.5 ml thioanisole for 10 min on ice. TFA (5 ml) was added and the mixture
incubated for further 10 min on ice. Finally 0.5 ml TFMSA (0.5 ml) was
added dropwise and the resulting solution stirred at room temperature
for 2 h. After completion of the TFMSA cleavage of the crude
peptide products from the resin, the crude peptide was precipitated by
the addition of 40 ml cold diethyl ether, the solution stirred for 1 min and then filtered. The precipitate was extracted with 25 ml TFA
through the glass sintered filter directly into a round bottom flask.
The volume of filtrate was reduced in vacuo with a rotary evaporator
(Buchi, Labortechnik AG, Flawil, Switzerland) and again
precipitated by adding ice-cold diethylether. The precipitate,
containing the crude peptide, was recovered by filtration and the ether
disregarded. The precipitate was dissolved in 50% (v/v)
acetonitrile/water, lyophilized and the crude peptide stored at 353 K
(
20°C).
Peptide purification
The six crude synthetic peptides were each purified by gradient
elution reversed-phase high-performance liquid chromatography (RP-HPLC)
using a Waters 600/486 HPLC system with a TSK-ODS-120 T column
(300 × 21.5 mm inside diameter, Tosoh Corp. Yamaguchi, Japan)
packed with 10 µm, 300 Å pore-sized octadecyl silica. The eluents
used were: A, 0.1% TFA in water, and B, 0.09% TFA in 60% (v/v)
acetonitrile-water, with a linear gradient of 25-75% B over 90 min.
Ultraviolet (UV) detection was used at 254 nm except for TRAP-2 (in
which Ala replaces Phe2) where detection at 214 nm was
used. The flow rate was 7.5 ml/min. Because TRAP-1 precipitates in
eluent A at high concentrations, this peptide was dissolved in 0.09%
TFA, 25% acetonitrile (v/v) in water, and 50-150 mg aliquots were
injected. Recovered fractions were analyzed using the Waters 600/486
HPLC system by analytical RP-HPLC and a TSK-ODS-120 T column (150 × 4.6 mm inside diameter, Tosoh Corp.), packed with 5 µm, 300 Å average pore size octadecyl silica. The eluents used were the same as
above for the semi-preparative separation, with a linear gradient of
0-100% B over 60 min, UV detection at 214 nm, and a flowrate of 1 ml/min. The molecular masses of the purified peptides were confirmed by
electrospray ionization mass spectrometry (ESI-MS) using a Micromass
platform (II) quadrupole MS with an electrospray source with Masslynx
NT Ver. 3.2 software (Micromass, Cheshire, UK). The synthetic peptides in 50:50 (v/v) ACN/water, with 3% (v/v) formic acid were infused into
the instrument at a speed of 10 µl per minute. The ESI-MS spectra of
the TRAP peptides were acquired at 343 K at 55V/50V over the
mass/charge (m/z) range of 200-2000.
Molecular modeling
Molecular modeling and energy minimization were performed using
the CS Chem3D Pro 4.0 software (CambridgeSoft, Corp., Cambridge, MA).
Standard molecular dynamics was performed in 10,000 steps by heating
the molecule to 600 K at a rate of 1.000 kcal/atom/ps. Energy-minimized
structures of each peptide were acquired using the molecular mechanics
subroutine MM2 (Allinger, 1977
; Allinger et al., 1988
; Torrens, 2000
)
with 2-fs intervals, with average backbone and side-chain conformations
determined from the overlap of five acquired structures. The molecular
surface area,
Amol, solvent accessible
surface area,
Asolv, and hydrophobic surface area,
Ahydr, of the TRAP peptides (Table 1)
in their folded (globular) conformations, and the corresponding surface
areas for the TRAP-related peptides in their unfolded conformations, were calculate according to established procedures (Makhatadze and
Privalov, 1995
; Spassov et al., 1997
). The relative hydrophobicities of
the TRAP peptide analogs in the presence of immobilized
n-octyl ligands were calculated according well documented
approaches (Wilce et al., 1995
).
Instrumental methods
Analytical chromatographic measurements were performed on a
Hewlett Packard HP1090 chromatograph and a HP Chemstation (Hewlett Packard, Waldbronn, Germany). All peak profiles were monitored at 215 nm. Temperature was controlled by immersing the analytical columns in a
thermostated column coolant-jacket (Alltech Associates, Deerfield, IL)
coupled to a recirculating cooler (Colora Messtechnik GmbH, Lorchwutt,
Germany). All chromatographic experiments were performed on 150 × 4.6 mm inside diameter Zorbax 300SB-C8 columns (Rockland Technologies,
Inc., Littlefalls, DE).
Determination of capacity factor, k', dependencies
Bulk solvents were filtered and degassed by sparging with
helium. Capacity factor measurements (Purcell et al., 1999
) were performed using water containing 0.09% (v/v) TFA with acetonitrile contents of 14, 15, 16, 17, 18, 19, and 20%, respectively with Zorbax
300SB-C8 columns operated at a flow rate of 1 ml/min and at
temperatures of 278-338 K in 5-K increments. Solutions of TRAP-1, -2, -3, -4, -5, and -6 peptides were prepared by dissolving the peptide at
a concentration of 1 mg/ml in 0.09% (v/v) TFA in water. The injection
size varied between 2.5 and 3.5 µg. Under these concentration and
mass loading conditions, the TRAP-1 to TRAP-6 peptides exist as
monomeric species. All data points were derived from at least duplicate
measurements with retention times between replicates varying typically
by less than 1%. The column dead volume was measured as the retention
time of the noninteractive solute, sodium nitrate. Various
thermodynamic and extra-thermodynamic parameters were calculated using
the Eudoxos and Hephaestus software developed in
this laboratory, coupled to the Excel version 5.0 program (Microsoft),
whereas the statistical analysis involved the Sigmaplot 4.01 program
(Jandel Scientific) linear and nonlinear regression analysis. The
relative standard deviations of the replicates for the k'
measurements were
±0.6%, i.e., the standard deviation of the
k' values were smaller than the size of the data points shown in Figs. 1, 2, 4, and 5, respectively. Similarly, the precision in the temperature measurements was
±0.5 K over the studied
temperature range.
 |
RESULTS AND DISCUSSION |
General considerations
The extent of binding of a peptide to an immobilized nonpolar
ligand as a function of experimental conditions can be evaluated for a
reversible, equilibrium interaction from the ratio of the bound-to-free
peptide concentration (Hearn, 1998
, 2000
). When measured with a
solid/liquid two-phase system, such as occurs in membrane-based
environments or chromatographic adsorption formats, this concentration
dependency can be expressed in terms of the unitless term
k', also known as the capacity factor, which is the ratio of
the peptide mass bound to the immobilized ligand(s) to the peptide mass
in free solution. For convenience, k' is usually expressed
as a concentration ratio such that
|
(1)
|
where nS and nM are
the number of moles of the peptide in the bound and free states
respectively, Kassoc is the equilibrium binding
constant and
the phase ratio of the system, defined as the ratio
VS/VM, where
VS and VM are,
respectively, the volume of the immobilized ligands/support matrix and
the volume of the solvent in the system. Similarly, the dependency of
k' on temperature can be evaluated in terms of the
respective enthalpic and entropic thermodynamic parameters, such that
|
(2)
|
where
H
and
S
are the apparent changes in
enthalpy and entropy associated with the interaction, R is
the universal gas constant, and T is the absolute
temperature in degrees Kelvin. The equilibrium binding behavior of a
large number of ligands for G-protein coupled receptors and
ligand-gated ion channel receptors have recently been analyzed in
considerable detail based on these relationships (Borea et al., 2000
),
revealing that the discrimination of various agonists/antagonists mechanistically appears to be a consequence of the thermodynamic reorganization of solvent molecules that occur during the binding. Analogous situations occur when peptide agonists/antagonists interact with immobilized nonpolar n-alkyl or phospholipid ligand(s).
When this interaction is an isothermic and isobaric (constant pressure) process, linear van't Hoff plots are anticipated, with the change in
heat capacity,
C
, equalling zero
(Boysen et al., 1999
; Hearn et al., 1999
). However, when the
interaction follows a homothermic or heterothermic process, curvilinear
van't Hoff plots are anticipated whereby
C
0 and is a function of
T (Boysen et al., 1999
; Hearn et al., 1999
). Although
fitting of experimental data to the linear form of the van't Hoff
dependency has often been used in studies related to the thermal
stability of proteins in bulk solution, differential scanning and
isothermal titration microcalorimetric studies with proteins bound to
chemical defined surfaces or undergoing ligand-binding events have
shown that the temperature dependence of
C
is often associated with dome-shaped
(or inverted dome-shaped) dependencies of the logarithmic equilibrium
association constant, ln Kassoc (or
G
) on temperature (Klotz, 1999
).
Similarly, nonlinear van't Hoff behavior has been observed for
peptides and proteins in both reversed-phase and hydrophobic interaction chromatographic systems. Such behavior can be approximated (Melander et al., 1984
; Vailaya and Horvath, 1996
; Haidacher et al.,
1996
; Hearn, 2001a
) as a quadratic relationship linking k' and the temperature, T,
|
(3)
|
Hence, from Eqs. 1 and 2, the change in enthalpy,
H
, can be expressed as
|
(4)
|
whereas the change in entropy,
S
, is given by
|
(5)
|
and the change in heat capacity,
C
, is given by
|
(6)
|
where b(0), b(1), and
b(2) are steri-electronic parameters specific for the
structure of the peptide (or protein). In the present investigation,
the interactive behavior of a series of TRAP-related peptide analogs
with immobilized n-octyl ligands has been evaluated
according to Eqs. 1-6 from the corresponding ln k' versus
1/T plots measured under reversible, equilibrium-binding conditions at fixed solvent composition(s). This analysis permits the
respective thermodynamic parameters associated with the interaction to
be derived and quantified, and the related extra-thermodynamic dependencies to be evaluated in terms of corresponding structural relationships.
Figure 1 shows the plot of the
logarithmic capacity factor, ln k', of TRAP-1 versus the
volume fraction of acetonitrile,
, for water-acetonitrile mixtures
of different acetonitrile contents over the temperature range 278-338
K. The experimental data obtained were fitted to first and second order
dependencies of ln k' on
, with regression coefficients
falling within the range of r2 = 0.9902-0.9992 for the first-order fit and
r2 = 0.9983-0.9999 for the second order
fit. The higher correlation coefficients observed when the TRAP-1 data
were fitted to quadratic dependencies of ln k' on
are consistent with the well-known parabolic binding relationship
for polypeptides and proteins on adsorption to immobilized
n-alkyl ligands from aquo-organic solvent mixtures (Hearn et
al., 1999
, 2001a
) Similarly, the corresponding plots at 298 K for the
TRAP 1-6 peptides where, in all cases, the ln k' versus
plots were curvilinear (Fig. 2).

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FIGURE 1
Plots of logarithmic capacity factor, ln k',
versus the volume fraction of organic solvent, , for the TRAP-1 at
different temperatures from 278 to 338 K (5-65°C).
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FIGURE 2
Plots of the logarithmic capacity factor, ln
k', versus the volume fraction of organic solvent, , for
the alanine-scan TRAP peptides, TRAP-2-6 at 298 K.
|
|
For the TRAP-1 peptide, and for the Ala-scan analogs, the
expected hydrophobic interaction mechanism for the peptide-nonpolar ligand interaction was observed, with decreases in ln k'
values as the
value was increased. The relative trend for the
binding of the TRAP-1 analogs was in agreement with the effect
anticipated for amino acid substitution, i.e., the substitution of a
more hydrophobic residue by a less hydrophobic residue in TRAP-2,
TRAP-3, and TRAP-4 leads to smaller k' values, whereas the
replacement of a charged or polar residue in TRAP-5 and TRAP-6 by the
alanine residue results in an increase in the k' value as
compared to the naturally occurring TRAP-1 (cf. Table 1).
The results from the molecular modeling and associated energy
minimization studies indicated that all TRAP analogs have globular shape, assuming that a local minimum not an absolute minimum was found.
These investigations show that TRAP-1 has a hydrophobic face consisting
of Phe2, Leu3, and Pro7. In Fig.
3 A is shown an overlay
presentation of five randomly selected energy-minimized conformational
structures for TRAP-1, having energy minima between 63.1 and 73.8 kcal/mol. As evident from Fig. 3 A, the
N-termini can be overlayed very well, with the
Phe2 side chain of the peptide with the lowest energy
minimum closest to the core, whereas the C-termini with the
Pro7 are more flexible. In Fig. 3 B is shown
the overlay presentation for energy-minimized conformational structures
for TRAP-1, TRAP3, TRAP-4, and TRAP 5, where the Phe2 and
Pro7 side chains are in close proximity. Although the
N-termini and the residues at position 1, 2, and 4 are in good
alignment for these peptides, the location of the C-termini varies
according to the position of the Ala substitution. The corresponding
overlay presentation for the simulated energy-minimized conformational structures for TRAP-2 and TRAP-6, where the Pro7 side chain
is distal to the Phe2 side chain, is shown in Fig.
3 C. Here, the Ala substitution of the Phe residue has
virtually no impact on the rest of the molecule. However, as will be
discussed later, the thermodynamic data for both peptides revel that
they behave differently in response to increasing temperature.

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FIGURE 3
(A) Overlay presentation for five simulated
energy-minimized conformer structures for TRAP-1. (B)
Overlay presentation of TRAP and TRAP-related analogs TRAP-3, TRAP-4,
and TRAP-5 with Phe2 and Pro7 side chains in
close proximity. (C) Overlay presentation of TRAP-2 and
TRAP-6 with the side chain of Pro7 distal to the side chain
of Phe2.
|
|
The strength of binding of TRAP-1 and the Ala-scan analogs to the
immobilized n-octyl ligands, expressed in terms of the
relative Kassoc or ln k' values, is
largely in agreement with the relative hydrophobicity values calculated
for these peptides according to the procedures of Wilce et al. (Wilce
et al., 1995
) (cf. Table 1). TRAP-3 and TRAP-4 have identical amino
acid compositions but different amino acid sequences with respect to
positions 3 and 4 and nominally have the same relative hydrophobicity.
However, as apparent from the ln k' versus
plots (Fig. 1
and 2) these peptides differ in terms of their equilibrium binding
constants with the immobilised n-octyl ligands. The reason
for this difference becomes apparent when their possible structures,
derived by molecular modeling methods, are examined. According to the
molecular modeling results, TRAP-4 is the far more compact molecule,
with Pro2, Leu3 and Phe2
collectively generating a hydrophobic patch, only part of which can be
accessed by the immobilized n-octyl ligands. In contrast, TRAP-3 has the more open structure with Leu4 and
Pro7 in distal positions with the hydrophobic patch
associated with the Phe2 residue also more accessible to
the immobilized n-octyl ligands. This structure-interaction
correlation is in agreement with the observed changes in heat capacity
of these peptides (as discussed later).
van't Hoff measurements
The van't Hoff plots for TRAP-1 determined at different
-values with water-acetonitrile mixtures containing 0.09% TFA are shown in Fig. 4. In all cases, for an
individual TRAP peptide examined in different solvent compositions or
with different TRAP peptides using the same solvent composition, the
correlation coefficients for the second-order fit of the experimental
data to the dependency of ln k' on 1/T were
significantly higher than for a first-order fit (cf. Tables
2 and
3) at both the 95% and 99%
confidence intervals. Thus, the van't Hoff data for TRAP-1 in
different solvent compositions followed a quadratic relationship as
given by Eq. 3, e.g., when
= 0.17, the correlation coefficient
was r2 = 0.9995 at a 95% confidence level,
with significantly lower correlation coefficients determined when the
ln k' versus 1/T data for TRAP-1 was fitted to a
first-order approximation for a defined
-value over the same
temperature ranges. Consequently, the van't Hoff dependencies of
TRAP-1 can be described in terms of heterothermic processes (Boysen et
al., 1999
; Hearn and Zhao, 1999
; Hearn 2001a
) with
H
,
S
and
C
all dependent on T. As evident from Fig.
5, analogous nonlinear van't Hoff
behavior was also evident in all cases for the Ala-scan TRAP analogs at
a defined value of
, for example at
= 0.14.

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FIGURE 4
Plots of the logarithmic capacity factor, ln
k', versus 1/T for TRAP-1 at different values
with the experimental data fitted to a second-order polynomial function
(solid lines) with the 95% confidence intervals depicted as
dotted lines. The correlation coefficients for these second-order fit
and the corresponding first-order fit of the experimental ln
k' versus 1/T data are listed in Table 2.
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TABLE 2
The correlation coefficients for a linear and quadratic
fit of the corresponding experimental data to the dependency of ln
k' versus 1/T for TRAP-1 at different values as shown in Figure 4
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TABLE 3
The correlation coefficients and 95% confidence intervals
for a linear and quadratic fit of the experimental ln k'
versus 1/T data for TRAP-1 and its Alanine-scan peptide
analogs at = 0.14 corresponding to the data shown in Fig. 5
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FIGURE 5
Plots of the logarithmic capacity factor, ln
k', versus 1/T for TRAP-1 and its alanine-scan
peptide analogs at = 0.14 with the experimental data fitted to
a second-order polynomial function (solid lines) with the
95% confidence intervals depicted as dotted lines. The correlation
coefficients for these second-order fit and the corresponding
first-order fit of the experimental ln k' versus
1/T data are listed in Table 3.
|
|
Changes in the entropy and enthalpy of association for the
TRAP-peptide-nonpolar ligand interaction
The respective values of
H
and
S
for TRAP and the Ala-scan analogs
as a function of T and
were calculated according to Eqs.
3-5 and the results are shown in Fig. 6,
7, and Table
4. Thus, at 318 K and
= 0.17, the values of
H
and
S
for TRAP-1 were
13.31 ± 0.03 kJ· mol
1 and
32.86 ± 0.10 Jmol
1·K
1, respectively, with the results
obtained for TRAP-1 (and the other peptides) under the different
temperature and solvent conditions similarly exhibiting narrow
confidence intervals. As evident from Figs. 6 A and
7 A, the TRAP-1 peptide-ligand interaction was
enthalpically-driven over the temperature range of 278-358 K, with
H
progressively becoming more
negative as T was increased. Moreover, the
H
values for the interaction of the
TRAP peptides with the immobilized n-octyl ligands were more negative for solvent mixtures of higher water content (Fig.
6 A). The heat required for (partial) dehydration of the
TRAP peptides prior to or during adsorption to the immobilized
n-octyl ligands differs for the different peptides (Fig.
7 A), i.e., the heat required under low temperature
conditions (278 K) to dehydrate the most hydrophilic peptide (TRAP-2)
was ~10-15 kJmol
1 higher than that required to
dehydrate the other more hydrophobic TRAP peptides. Both
H
and
S
were temperature dependent with
the TRAP peptides exhibiting characteristic compensation temperatures
given by TH (where
H
= 0) and
TS (where
S
= 0). When the
H
values for the
TRAP peptides obtained from these van't Hoff plots are compared to
related studies (Lin et al., 2001
), based on isothermal titration
microcalorimetric procedures, for the determination of the adsorption
enthalpy of peptides and proteins when bound to immobilized
n-alkyl ligands, similar dependencies of
H
, and hence
C
, on T are evident at
comparable solute concentrations. Compared to large polypeptides or
small proteins where
H
differences of between 100 and 200 kJmol
1 have been
observed under similar adsorption conditions over the same temperature
range of 278-338 K, the changes in
H
values for a specific TRAP
peptide were relatively small, i.e., 
H
15-30
kJmol
1 over this temperature range, values that are
consistent with the small molecular size, composition and solvational
potential of these peptides.

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FIGURE 6
Plots of (A) the change in enthalpy
H versus T;
(B) the change in entropy
S versus T;
(C) the change heat capacity
C versus T; and
(D) the change in Gibbs free energy
G versus T for the
TRAP-1 peptide at different values.
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FIGURE 7
Plots of (A) the change in enthalpy
H versus T;
(B) the change in entropy
S versus T;
(C) the change heat capacity
C versus T; and
(D) the change in Gibbs free energy
G versus T for the
TRAP-1 and its Alanine-scan peptide analogs at = 0.14.
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TABLE 4
The slopes and 95% confidence intervals of the dependence
of the enthalpy of interaction,
H , entropy of
interaction, S ,
heat capacity, C ,
and Gibbs free energy of interaction,
G , on
temperature for TRAP-1 and its alanine scan peptide analogs at = 0.14, based on a first- and second-order fit of the experimental ln
k' versus 1/T data shown in Fig. 5
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As evident from Fig. 8, the interaction
of TRAP-1 with the n-octyl ligands involves an
entropy-enthalpy compensation phenomenon at different solvent
compositions. Entropy-enthalpy compensation was also observed for the
TRAP Ala-scan analogs. Such behavior is consistent with these
peptide-ligand systems involving participation of multiple, weak,
intermolecular forces (Dunitz, 1995
). The results indicate that the
binding of TRAP 1-6 peptides within this interactive molecular system
(including solvent) was generally exothermic (i.e., involved a negative
H
under most conditions) but was
compensated by a decrease in
S
that
results from the reduced molecular flexibility of the peptide on
binding to the immobilized n-octyl ligands. As the
temperature was increased, the TRAP-related peptides and the
n-octyl ligands are progressively solvated to a greater
extent, resulting in smaller contact areas, and thus reduced
association between the peptides with the nonpolar environment of the
n-octyl ligands.

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FIGURE 8
Plot of the change in entropy
S versus the change in enthalpy
H for the TRAP-1 peptide at
different values.
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Changes in the heat capacity of association for the TRAP
peptide-nonpolar ligand interaction
Another thermodynamic parameter important for characterizing the
TRAP-n-octyl ligand interaction is the change in heat
capacity,
C
, with an increase in the
extent of burial of hydrophobic surfaces in a nonpolar environment
yielding a more negative value of
C
(Ross and Rekharsky, 1996
). It is widely accepted that
C
is proportional to the accessible
surface area of a peptide or protein, which can be partitioned into an
apolar surface (with the energetics related to the hydrophobic effect)
or into a polar surface (where the energetics are predominantly related
to hydrogen-bonding effects) (Murphy and Gill, 1991
; Murphy, 1999
). To
assess the nature of the dependence of
C
on temperature for these TRAP
peptides, the experimental data used for the generation of the ln
k' versus 1/T plots for TRAP-1 at different
solvent compositions and for TRAP-1-Trap-6 at
= 0.14 were
fitted to the relevant equations with and without
C
having a temperature dependence,
i.e., ln k' fitted as a first-order or second-order
dependence on 1/T. These results are found in Table
3-6.
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TABLE 5
The correlation coefficients and 95% confidence intervals
for a linear and quadratic fit of the experimental ln k'
versus 1/T data for TRAP-1 at different values,
corresponding to the data shown in Fig. 4
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TABLE 6
The slopes and 95% confidence intervals of the dependence
of the enthalpy of interaction,
H , entropy of
interaction, S ,
heat capacity, C ,
and Gibbs free energy of interaction,
G , on
temperature for TRAP-1 peptide at different values, based on a
first- and second-order fit of the experimental ln k'
versus 1/T data shown in Fig. 6
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Figure 6 C shows that the change in
C
for TRAP-1-n-octyl ligand
interaction was negative under all solvent conditions as expected for a
hydrophobic interaction process. Thus, at 318 K and
= 0.17, the value of
C
for TRAP-1 was
0.192 ± 0.002 kJmol
1·K
1.
Moreover, the corresponding
C
values for TRAP-1 obtained under the other temperature and solvent conditions or the related analogs obtained at
= 0.14 similarly exhibiting negative values with small standard deviations at the 95% and 99%
confidence intervals for second-order fit of the experimental data
(Table 4 and 6) for the ln k' dependency on 1/T
according to Eq. 3. In all cases, the
C
values followed the important criterion of being
0 and <0 under the
experimental conditions investigated with the
C
values (Figs. 6 C and
7 C) becoming more positive at higher temperatures, indicating a decrease in the hydrophobic contact area associated with
the peptide-nonpolar ligand interaction. This behavior was also
paralleled by changes in the Gibbs free energy,
G
, as the temperature was increased
(Figs. 6 D and 7 D). Thus, the plots of
G
versus T for these
TRAP-related peptides confirm that their interaction with the
n-octyl ligands was spontaneous at all temperatures, but
their interactions became less favorable at more elevated temperatures.
These findings indicate a small but nevertheless significant dependence
of
C
values (e.g., 
0.13
kJmol
1K
1 ± 0.01
C
0.27
kJmol
1K
1 ± 0.01) on the temperature
over the range of 278-338 K for TRAP-1 and its Ala-scan analogs and
are consistent with the small molecular size and lack of well-developed
secondary structure of these peptides under these experimental
conditions. These
C
values are
comparable in value to
C
for the highly
stabilized equine cytochrome c (
C
0.9 kJmol
1K
1) (R. I. Boysen, A. J. O. Jong and M. T. W. Hearn, in preparation) but are
significantly smaller than found for the interaction of multimeric
coiled-coil polypeptides, such as the transcription factors
c-Jun or c-Fos, with nonpolar ligands, i.e.,
C
43.8
kJmol
1K
1 for the interactions of this
coiled-coil polypeptide with n-octyl ligands under similar
experimental conditions (Boysen et al., 2002
). In this latter case with
the homo- or hetero- c-Jun or c-Fos dimers, the
experimental findings have documented that a two-state unfolding
process occurs with the coiled coil c-Jun/c-Fos polypeptide
dimers first uncoiling and the individual
-helical coils then
transitioning toward random coil structures with large incremental
changes in
C
arising as the temperature
was increased. Beside the overall trends in the
C
values of the TRAP analogs as
depicted in Fig. 7 C with respect to temperature, the
incremental changes in
C
with regard to
temperature or residue number, namely

C
and

C
, over the
temperature range of 278-338 K are highly diagnostic. Thus, the larger
the 
C
value, the more sensitive is
the peptide to heat, which translates into less structural rigidity of
the peptide as it interacts with the nonpolar ligand. The observed
variations in the
C
and

C
values follow the order expected for the reduction in hydrophobic stabilization of the various TRAP
peptides as their structures are kinetically destabilized at higher
temperatures. Thus, in a solvent composition whereby
= 0.14, the 
C
value for the more open TRAP-3 was the lowest at 2.1 Jmol
1K
2 with
the more compact TRAP-4 exhibiting a

C
value of 2.7 Jmol
1K
2, whereas, for the most compact
structure, TRAP-2, the 
C
value was
3.5 Jmol
1K
2. It is well known that
polypeptide or protein denaturation or the transfer of nonpolar
compounds to more aqueous environments is accompanied by a heat
capacity increase and associated enthalpy change (Makhatadze and
Privalov, 1990
; Graziano et al., 1998
). Changes in the partial molar
heat capacity of small peptides, such as Gly-Xaa-Gly, in aqueous
solutions over a temperature range of 353 K, as determined by
differential scanning microcalorimetry, have been reported to be
~0.2-0.3 kJmol
1K
1 (Hackel et al.,
1998
, 1999
) with corresponding changes in the enthalpy of
10 to
20
kJmol
1. As apparent from Figs. 6 and 7, variations in the
C
or
H
values for all of the TRAP
peptides in association with the n-octyl ligands have
similar magnitudes as the temperature was increased.
In Fig. 9 C are shown the
plots of 
C
versus
Atotal for the TRAP-related peptides in their
folded (globular) conformations (Table 2) over a defined temperature range of 273-338 K and
= 0.14, where the trend was apparent for larger 
C
values to follow an
increase in the molecular surface-area properties of these peptides.
These data reveal two notable effects. First, for TRAP-2, which has the
highest 
C
value, it can be concluded that this is the most heat-sensitive TRAP peptide, although TRAP-2 is
not the most compact analog, as assessed from the molecular modeling
and energy minimization data (see Fig. 3 C). A possible explanation for the larger 
C
value
of TRAP-2 is that the stabilizing effect of the
-n
interaction of the Phe2 with Pro7 is missing.
The change in the thermodynamic properties of TRAP-2 with the
Phe2 replaced by Ala mirrors the effect of elimination of
the
-phenyl side-chain group in biological assays, which is
associated with the complete loss of receptor activation (Nose et al.,
1998a
), i.e., TRAP-2 acts as an antagonist.

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FIGURE 9
Plot of the (A) change in enthalpy
 H versus
Atotal; (B) change in entropy
 S versus
Atotal; (C) change in heat
capacity  C versus
Atotal; and (D) change in Gibbs
free energy  G versus
Atotal for the TRAP-1 and its Alanine-scan
peptide analogs at = 0.14.
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The other effect evident from the experimental data related to the
change in heat capacity versus the molecular surface area is associated
with TRAP-3. This TRAP analog was the least heat sensitive of the
TRAP-related peptides with the data consistent with the conclusion that
TRAP-3 is the least compact peptide. When compared with TRAP-4, which
has identical amino acid c