A.S. Safiullina, et al.
ThermochimicaActa692(2020)178748
In the present work, FSC was used to study the cyclization of
-
calibration was carried out using standard samples of indium, tin, bi-
phenyl and deionized water. The accuracy of the melting temperature
determination was better than 1 K. Optical images of the samples
were obtained using an Olympus BXFM microscope.
L
leucyl-L-leucine dipeptide in the solid state for the first time. Previously,
the cyclization of this dipeptide was studied by conventional methods
of thermal analysis [30]. In the present study, the kinetic parameters of
the reaction were estimated within the approaches of non-isothermal
kinetics using FSC data. The results obtained were compared with ki-
netic parameters of this reaction determined elsewhere [30]. The study
of kinetics of solid-state reactions of minute amounts allows to develop
effective and economical methods for preparation of biologically active
substances based on oligopeptides.
The Leu-Leu cyclization was studied at heating rates of 300, 700 and
900 K s−1. The higher heating rates led to a substantial broadening of
DSC peaks and an increase in errors.
Since the mass of the dipeptide FSC sample is not available due to
the nanogram sample mass, several approaches have been developed
for an indirect mass determination using the data on specific fusion
enthalpy, the specific heat of the solid or liquid sample, and the heat
capacity change at the glass transition [37]. In this study, we estimated
the sample mass (m) using the specific heat capacities of Leu-Leu and
cyclo(Leu-Leu) obtained from DSC and the heat capacities from FSC
measurements, by the following equation:
2. Experimental
2.1. Materials
Dipeptide L-leucyl-L-leucine (Leu-Leu) was purchased from Bachem
(Lot#: 1054344). Cyclic dipeptide cyclo(leucyl-leucyl) (cyclo(Leu-Leu))
was prepared by heating the Leu-Leu up to 473 K as described in Ref
[30]. For the experiments, Leu-Leu was recrystallized from methanol
and dried in vacuo (P = 7 kPa) to remove the solvent. Methanol (of
grade “for GC” with purity ≥99.9 %) was used without additional
purification.
m = Cp(T)/cp(T)
(1)
where Cp(T) is the heat capacity determined from the FSC experiment
as described below.
The heat capacities of dipeptides were calculated from the heat flow
rates on heating and cooling as described previously [46]. The heat
flow rates of empty sensors were determined before each sample
measurement. Then sample measurements were corrected by sub-
tracting the empty sensor measurement. Further corrections were made
for the heat loss from the sample and the reference to the surroundings.
The measurements were carried out in a temperature range, in which
there is no chemical reaction or phase transition: from 293 K to 423 K in
the case of Leu-Leu and from 293 K to 483 K for cyclo(Leu-Leu). So, the
corrected heat flow rates to the sample (Фh is the corrected heat flow
rate on heating and Фс is that on cooling) may be represented as the
sum of contributions from the heat capacity of the sample (Cp) and the
differential heat loss (Фloss) [37].
2.2. Differential scanning calorimetry
The DSC experiments were performed using the DSC204 F1 Phoenix
differential scanning calorimeter (Netzsch, Germany) in an argon at-
mosphere (flow rate 150 mL min−1) with the heating/cooling rate of
10 K min−1. DSC was calibrated according to the manufacturer's re-
commendations by measuring six standard compounds (Hg, In, Sn, Bi,
Zn, and CsCl) as described previously [31]. The 40 μL aluminum cru-
cibles sealed with a pierced lid having a hole of 0.5 mm hole were used.
Before the experiment, aluminum crucibles were annealed at 473 K for
30 min.
Heating:
h
p
(2)
Cooling:
The specific heat capacities of Leu-Leu and cyclo(Leu-Leu) were
measured as described elsewhere [49]. The measurement procedure
included three steps. Firstly, the baseline for the empty crucibles was
determined. Then using the baseline obtained, a standard sample
(sapphire disc) with a weight of 21.05 mg and a powder of dipeptide
(8−9 mg) were sequentially measured in the same crucible. This pro-
cedure was repeated three times for each sample. The calculation of the
heat capacity was performed using the Netzsch Proteus Thermal Ana-
lysis 6.1.0 according equation:
c
p
(3)
The difference between the heat flow rates measured during heating
and cooling, taking into account, that dT/dth = - dT/dtc, can be written
h (T)
c (T) =
2 ×
Cp (T) ×
dT/dt
(4)
So, heat capacity may be calculated as
(5)
Before the experiments, the dipeptides were heated three times from
293 K to 423 K with the rate of 100 K s−1 to remove residual water and
methanol.
cp = msapphire/mdipeptide × (DSCdipeptide − DSCbaseline)/
(DSCsapphire − DSCbaseline) × cp,sapphire
where cp and cp,sapphire are specific heat capacities of dipeptide and
sapphire [J g−1 K−1], mdipeptide and msapphire are masses of dipeptide
and sapphire [mg], DSCdipeptide, DSCsapphire and DSCbaseline are DSC
signals obtained for sample, standard sample and baseline [μW].
Leu-Leu was previously heated up to 428 K to remove adsorbed
water [50]. The specific heat capacity (accuracy of 2%) was measured
in the range between 313 K and 413 K in case of Leu-Leu and between
313 K and 483 K for cyclo(Leu-Leu). Calculation of heat capacities was
made for a linear region on the DSC heating and cooling curves in the
temperature range from 343 to 411 K (Leu-Leu) and 363–453 K (cyclo
(Leu-Leu)).
2.4. Kinetic analysis of cyclization of Leu-Leu in solid state
Kinetic analysis was performed following the ICTAC recommenda-
tions [52,53] using the NETZSCH Kinetics Neo 2.1.2.2 software
topochemical equation as described in Ref. [29–31,59]. A suitable ki-
proaches: reaction of nth order with autocatalysis by product (CnB) Eq.
(7), reaction of nth order with m-Power autocatalysis by product (Cnm)
Eq. (8), expanded Prout-Tompkins equation (Bna) Eq. (9).
2.3. Fast scanning calorimetry
ln(β/T2) = Const – Ea/RT
(6)
(7)
The FSC experiments were performed using the Flash DSC1 calori-
meter (Mettler-Toledo, Switzerland) with a UFS1 sensor and TC-100
cooler (Huber, Germany) [51] under an atmosphere of nitrogen with a
flow rate of 50 mL min−1. The sensor had been conditioned and cali-
brated before use as described previously [45]. The temperature
)
m
)
(8)
(9)
n
k
cat
)
2