[2012] physicochemical characterization and decomposition kinetics of trandolapril
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Thermochimica Acta 539 (2012) 92–99
Contents lists available at SciVerse ScienceDirect
Thermochimica Acta
journal homepage: www.elsevier .com/ locate / tca
Physicochemical characterization and decomposition kinetics of trandolapril
E. Roumelia, A. Tsiapranta b, K. Kachrimanis b, D. Bikiaris c, K. Chrissafis a,∗
a Solid State Physics Section, Physics Dept., Aristotle University of Thessaloniki, Thessaloniki, Greeceb School of Pharmacy, Aristotle University of Thessaloniki, Thessaloniki, Greecec Laboratoryof Organic Chemical Technology, Dept. of Chemistry, Aristotle University of Thessaloniki, Thessaloniki, Greece
a r t i c l e i n f o
Article history:
Received 24 January 2012
Received in revised form 29 March 2012Accepted 6 April 2012
Available online 15 April 2012
Keywords:
Trandolapril drug
Thermal stability
Decomposition mechanism
Thermal destruction
a b s t r a c t
The purpose of this work was to study the physicochemical properties of trandolapril, to perform a
detailed kinetic study of its decomposition and also to evaluate its thermal stability in order to provide
the essential tools to design a thermal destruction method for expired trandolapril-based drugs. Tran-
dolapril was characterized with FTIR, XRPD and SEM and its thermal behaviour was studied with DSC and
TGA in dry air and nitrogen flows. The decomposition process was also followed by Py-GC–MS, the activa-
tion energy was calculated with isoconversional methods and the reaction model was determined with
model-fitting method. Trandolapril is stable until the onset of its melting (110 ◦C) in both nitrogen and
dry air environments. Thermal degradation of trandolapril can be described by two consecutive mech-
anisms of n-th order with activation energies 97.4 and 180.0 kJ/mol respectively. Trandolapril reaches
zero residual at 510 and 560 ◦C in nitrogen and dry air flow respectively. The detailed analysis of decom-
position mechanism allows the industry to design integrated thermal destruction processes for expired
trandolapril-based drugs. The results of Py-GC–MS agree with the theoretical calculations of thermal
analysis techniques, which highlights that the different techniques used in this work are complementary
and equally important.
© 2012 Elsevier B.V. All rights reserved.
1. Introduction
Trandolapril is the ethyl ester prodrug of a non-
sulfhydryl angiotensin converting enzyme (ACE) inhibitor,
trandolaprilat. Trandolapril is chemically described as
(2S,3aR,7aS)-1-[(S)-N-[(S)-1-carboxy-3-phenylpropyl]alanyl]
hexahydro-2-indolinecarboxylic acid, 1-ethyl ester [1]. It is used
for the treatment of hypertension and its blood pressure lower-
ing effect can be further enhanced by the addition of a diuretic
medication, such as hydrochlorothiazide.
An area that has been gaining more and more attentionrecently
by both the pharmaceutical industry and academic research is drug
disposal and destruction. Concern for the environment, both in
terms of limiting the use of finite resources and the need to man-
age waste disposal, has led to increasing pressure to safely dispose,
destruct or recycle materials at the end of their useful life [2]. Even
though waste management is nowa high priority in every country,
we hardly ever talk about pharmaceutical pollution and therefore,
little, if any, literature is dedicated to studies of pharmaceuticals
∗ Corresponding author at: Solid State Physics Section, Physics Dept., Aristotle
University of Thessaloniki, Thessaloniki, Greece. Tel.: +30 2310 998188;
fax: +30 2310 998188.
E-mail address: [email protected] (K. Chrissafis).
destruction processes. The ultimate challenge nowadays is to pre-
vent medications from being released into the environment.
People nowadays takemore prescription drugs thanever before.
With thousands of pills being washed down the drain or land-
filled, it’s no surprise that pharmaceuticals have been detected in
surface, ground and drinking water in many countries [3]. Cur-
rently there are no concrete guidelines concerning drug disposal
and most people continue to dispose of their medications in the
household garbage or by flushing down the sink or toilet. This is
becoming a global issue and therefore, many countries are evalu-
ating their drug disposal programs [4–6] which also aimto educate
and raise awareness [7]. Because the effects of many pharmaceu-
tical compounds on the environment are not fully understood,
many environmentalists consider sewage-mediated disposal to be
the least desirable means of disposal [8–10]. It is widely believed
that high-temperature incineration is the most environmentally
friendly method for disposal and destruction of unused or expired
pharmaceutical products [11,12]. In certain countries take back
programs have been funded providing the legal framework and
logistics resources to allow people and health care facilities to
return unused or expired drugs so that they can either be reused or
safely incinerated in appropriate facilities [13,14].
In this work trandolapril has been extensively studied with var-
ious techniques and much attention has been paid to its thermal
decomposition, in order to collect essential information needed to
design a possible expired-drug destruction process, which can only
0040-6031/$ – seefrontmatter © 2012 Elsevier B.V. All rights reserved.
http://dx.doi.org/10.1016/j.tca.2012.04.009
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E. Roumeli et al./ Thermochimica Acta 539 (2012) 92–99 93
be designed when all the components forming the drug (active,
excipients, etc.) are well studied. It is also important to mention
that no prior thermal stability studies of trandolapril have been
reported in the literature.
2. Materials andmethods
2.1. Materials
Trandolapril crystalline powder with molecular formula
C24H34N2O5 and molecular weight 430.54g/mol was kindly pro-
vided from Chunghwa Chemicals Synthesis and Biotech Co Ltd
(Taipei Hsien, Taiwan).
2.2. Fourier transform infrared spectroscopy (FTIR)
In order to proceed to the optical characterization of tran-
dolapril, FTIR spectroscopy in transmittance mode was used. KBr
pellets with 1w t% of the powdered material were produced.
The spectra were obtained with a Spectrum 1000 PERKIN-ELMER
spectrometer in the spectral range 4000–400cm−1, with 2 cm−1
resolution and 32 scans.
2.3. X-ray powder diffraction (XRPD)
X-ray powder diffraction patterns were recorded by a water-
cooled Rigaku Ultima+ diffractometer using CuKa radiation, a step
size of 0.02◦ and a step time of 3 s, operating at 40kV and 30mA.
2.4. Hot stage polarized optical microscopy (HSPM)
A polarizing optical microscope (Nikon, Optiphot-2 (Tokyo,
Japan)) equipped with a Linkam THMS 600 (Surrey, UK) heating
stage with a TP 91 control unit was used for HSM observations.
2.5. Scanning electron microscopy (SEM)
The morphology of the prepared samples was examined in a
SEM system (JEOL JSM 840A-Oxford ISIS 300microscope). The sam-
ples were carbon coated in order to provide good conductivity of
the electron beam. Operating conditions were: acceleratingvoltage
20kV, probe current 45nA, and counting time 60s.
2.6. Thermogravimetric analysis (TGA)
Thermal stability of trandolapril was evaluated by TGA using
a SETARAM SETSYS TG-DTA 16/18. Samples (6.0±0.2mg) were
placed in alumina crucibles. An empty alumina crucible was usedas reference. The samples were heated from ambient temperature
to 600 ◦C in a 50ml/min flow of nitrogen or dry air, at heating rates
of 5, 10, 15 and 20 ◦C/min. Continuous recordings of sample tem-
perature, sample weight, its first derivative and heat flow were
performed.
2.7. Differential scanning calorimetry (DSC)
Differential scanning calorimetry curves were obtained with
DSC 141, SETARAM instrument. 6.0±0.2mg of each sample was
placed in crimped aluminium crucibles, while an empty one was
used as reference.Samples were heated from ambient temperature
to 180 ◦C ina 50ml/min flowof N2
with a heating rate of 5 ◦C/min.
2.8. Pyrolysis-gas chromatography–mass spectroscopy
(Py-GC–MS)
For Py-GC–MS analysis the drug is “dropped” initially into the
“Double-Shot” Pyrolyzer. The furnace temperature is programmed
from100to 700 ◦C. Thesample was retained at 100 ◦Cfor2min and
heated with a rate 20◦C/min to its decomposition. As the sample is
heated, vapors evolve. Pyrolysis products are flushed through the
split/splitlessinjection portby the carrier gas (nitrogen 50 ml/min).
The sample is split, and a fraction (e.g. 1/50) of the gases passes
through the EGA capillary tube which is kept at 300 ◦C to prevent
condensation. The pyrolyzates are separated using temperature
programmed, capillary column GC and analyzed by the mass spec-
trometer (MS) GCMS-QP 2010. Optimal pyrolysis temperatures can
be determined with the thermogram (EGA chromatogram) as fol-
lows, peak end point of degradation step +50 ◦C.
3. Results and discussion
3.1. XRPD and FTIR characterization
The XRPD pattern of trandolapril is presentedin Fig. 1. Fromthe
study of the XRPD pattern of trandolapril, its high crystallinity can
be seen andthe peaks with higher intensity are observed at 16.95◦,
18.63◦, 21.47◦, 7.25◦, 14.53◦, 22.07◦ and 21◦. These peaks corre-
spond to the W crystalline polymorph of trandolapril, as described
in the literature [15].
The FTIR spectrum of trandolapril is presented in Fig. 2 and
is rather complex, with many sharp peaks, characteristic of each
bond. The carbonyl group appears in 3 instances in trandolapril: in
carboxylic acid, ester group and tertiary amide and therefore, the
peaks in the area of 1600–1800 cm−1 canbe assigned to it. Namely,
the peaks at 1736cm−1, 1706cm−1 and 1654cm−1 are attributed
to C O stretching vibrations of ester, carboxylic acid and amide
groups respectively [16]. The peak at around 1500cm−1, can be
attributed to C N vibrations of the tertiary amide, while the peaks
at 1103–1180 cm−1 and 700–750 cm−1, to C N stretch and N H
wag vibrations of the secondary amine group. Finally, the peakat 3280cm−1 can be assigned to N H stretching vibrations of the
amine. Due to stretching vibrations of C H of aromatic rings some
small peaks appear in the spectral regions of 3000–3100cm−1.
3.2. HSPM investigation
The HSM images that were recorded during heating from 25
to 128 ◦C, cooling from 128 to 90 ◦C, subsequent heating up to
160 ◦C and final cooling to 50◦C are presented in Fig. 3. Crystalline
Fig. 1. XRPD pattern of (a) trandolapril and (b)trandolapril after heating at 180◦
C.
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94 E. Roumeli et al. / Thermochimica Acta 539 (2012) 92–99
Fig. 2. FTIR spectrum of (a)trandolapril and(b) trandolaprilafterheating at 180◦C.
polymorph W of trandolapril was completely melted at 128◦C and
then upon cooling it started to crystallize again. From 120 ◦C the
newly formed crystal began to grow and the process was com-
plete at 90 ◦C. The subsequent heating showed that trandolaprilcould not melt at the same temperature anymore. After its first
melting, trandolapril was found to have a much higher melting
point, at 160◦C. Upon thesecond cooling it wasdiscovered that the
morphology, shape and size of trandolapril crystallites was rather
different; round-shaped spherulites had been formed, instead of
the narrow-shaped ones that were observed after the first heating.
3.3. SEM investigation
SEM micrographs (Fig. 4) reveal that trandolapril crystals are of
columnar crystal habit, long and slender with a great variation in
their length. This is also in accordance with literature where it has
been reported that crystals of trandolapril areneedle-like andhave
columnar shape [17].
3.4. Thermal analysis in nitrogen and dry air environments
Physicochemical stability of the active pharmaceutical ingredi-
ent(API)at elevated temperatures is an essential parameter for the
production of a solid dosage formulation. In order to investigate
the thermal stability of trandolapril, DSC and TGA measurements
were carried out in both nitrogen and dry air environments with
a heating rate of 5 ◦C/min. TG/DTG curves of trandolapril heated
under nitrogenenvironment arepresentedin Fig.5a andtheyreveal
that the API remains stable up to 110 ◦C. The first degradation step
occurs between 110 and 178 ◦C and corresponds to a 4.25% mass
Fig. 4. (a and b) SEM microphotographs of trandolapril.
loss. The second degradation step, which results in no residual,beginsat200 ◦Candiscompletedat510 ◦C.TheDSCheatflowcurve,
shown in Fig. 5b, reveals two overlapping endothermic events that
correspond to the melting and the beginning of mass loss of tran-
dolapril, respectively. The melting point of trandolapril, that can
clearly be seen from the heat flow curve in Fig. 5b has an onset at
110 ◦C and peak temperature at 128 ◦C and is in agreement with
literature reported values [17]. The shoulder at 138◦C corresponds
to the beginning of mass loss of trandolapril.
The same measurements were carried out under dry air envi-
ronment and the resulting TG/DTG curves are presented in Fig. 6.
In thiscase, which is rather interesting as the industrial deconstruc-
tion processes of expired drugs usually operate under air flowing
Fig. 3. HSPM images of phase transition during heating process.
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E. Roumeli et al./ Thermochimica Acta 539 (2012) 92–99 95
Fig. 5. (a) (i) TG, (ii) DTG and (b) DSC curvesof trandolapril heated in N2 environment with rate 5 ◦C/min.
conditions, there are three degradation steps. The first is ranging
between 110and 172◦C and results in a 4.2%massloss. The second
is completed at 412 ◦C resulting in 71% mass loss and the third one
leading to zero residual is completed at 560 ◦C.
Three differences between heating trandolapril under nitrogen
and dry air environments were observed from our results. One
major difference is the number of degradations steps, which is two
in nitrogen and three in dry air environment, implying that theAPI decomposes by different mechanisms in these conditions. This
however, does not apply for the first degradation step, whichis the
same for both of the studied cases. Indeed, the mass loss and heat
flow curves in Figs. 5 and 6, reveal that the first step is the same for
both cases. The second difference is that the second degradation
step begins at lower temperatures and is more rapid under dry air
flow. From these figures it is also clear that degradation under dry
airreaches itsmaximum rate at 320 ◦C,whichis 30◦C lower thanin
nitrogen. Finally, the temperature at which zero residual is reached
is 510 and 560 ◦C for nitrogen and dry air respectively. At 510 ◦C
there is no residue in nitrogen while in dry air there is a residue
of about 7%. Consequently, in order to reach absolutely no residual
in a thermal destruction process, temperatures as high as 510 and
560
◦
C should be reached for nitrogen and dry air environmentsrespectively.
3.5. Investigation of the first degradation step of trandolapril
In order to thoroughly examine the first small mass loss
step of trandolapril, which almost coincides with its melting
and is completed before 180◦C in every case, trandolapril was
heated up to that temperature and then cooled down to room
Fig. 6. (i)TG and(ii) DTGcurvesof trandolapril heated in dryair environmentwith
rate 5◦
C/min.
temperature. Afterwards, thethermally treated sample wasstudied
with DSC, FTIR and XRPD in order to investigate with all com-
plementary methods the reactions taking place during the first
degradation step of trandolapril.
From the obtained heat flow curves (Fig. 7) it is clear that tran-
dolapril undergoes a transformation when heatedup to 180 ◦C that
results in a product with a completely different melting point.
Indeed, from Fig. 7 it can be seen that trandolapril after the firstdegradation step results in a substance with melting point approx-
imately at 160 ◦C, which is 32 ◦C higher than the starting active
substance. That proves that some major changes have happened to
the molecule of trandolapril during its first degradation step.
In Figs. 1 and 2, the XRPD pattern and FTIR spectrum of tran-
dolapril after being heated at 180◦C confirmthat many differences
occurred during its thermal treatment.
From the XRPD pattern (Fig. 1) after the thermal treatment, it
is clear that new peaks appear, while some of the original peaks
of trandolapril are absent. The main peaks in the XRPD patterns
of the heated trandolapril were recorded at 8.14◦, 16.38◦, 22.08◦,
15.44◦, 12.48◦ and12.2◦. This confirms that the APIafter its heating
at 180 ◦C results in a quite different crystal structure.
IntheFTIRspectrum(Fig.2) manypeaks havebeen shifted, somehave been overlapped and some new have appeared. The most
important differences between the spectra of trandolapril pre and
post heating, are located in the 1600–1800cm−1 and 3300cm−1
spectral regions. The peak at 3280cm−1 that is due to vibrations of
the N H bond of the secondary amine is absent from the spectrum
of the heated trandolapril. Therefore by the absence of that char-
acteristic peak, it is revealed that this particular bond is no longer
present in heated trandolapril indicating that no secondary amine
groups remain in the molecule after its heating until 180 ◦C.
Fig. 7. DSCcurves oftrandolapril heated(1) forthe first and(2) forthe secondtime,
both in nitrogen environment, with rate 5◦
C/min.
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By focusing on the region 1600–1800cm−1, which corresponds
to carbonyl group vibrations, we notice that the peak at 1736 cm−1
is slightly shifted to higher wavenumbers (1740cm−1), indicating
that the chemical environment of the ester carbonyl group has
changed (Supplementary material). Ascan beseenfromthemolec-
ular structure of trandolapril, this group can form intermolecular
hydrogen bond with the N H group. Therefore, the shifting of the
1736cm−1 peak to higher wavenumbers indicates that this possi-
bility does not exist anymore. Additionally, the absence of weakand broad peak at 1705c m−1, due to the vibrations of the car-
boxylic acid C O, confirms its deformation. Studying further the
area of carboxymethyl vibrations, a new peak at 1670 cm−1 can be
observed whilethe peak at 1654 cm−1 remains. This suggests that a
newamide group wascreatedduringthe thermaltreatment of tran-
dolapril. The difference between the peaks at 1670 and 1654 cm−1,
which can both be attributed to tertiary amide vibrations, can be
assigned to the different chemical environment of the carbonyl
group. So, the differences in the surrounding bonds and chemical
groups seem to induce a shifting to the peaks that are attributed to
amide groups.
Based on the molecular structure changes and weight loss of
trandolapril during melting (4.25% and 4.2%for nitrogenand dry air
environments respectively) and considering the molecular struc-
ture of trandolapril it is reasonable to assume that a reaction
occurred between the secondary amine and the OH of the car-
boxyl group, producing a water molecule, following a cyclization
procedure via nucleophilic attack, as illustrated in Fig. 8. The theo-
retically expected mass loss in such a case would be 4.2%, which is
practically the same with the recorded value.
In details, the methyl group near the carbonyl of the amide, can
be rotated and the secondary amine can easily attack via nucle-
ophilic reaction the carbonyl group of the acid. The new stable
six-member ring is formed, containing a new imide group, while
a water molecule is eliminated as a byproduct of the nucleophilic
attack (cyclization reaction). The chemical description of the new
product is ethyl 2-(3-methyl-1,4-dioxodecahydropyrazino[1,2-
a]indol-2(1H)-yl)-4-phenylbutanoate. It can be described as a
dipiperazine, its molecular formula is C24H32N2O4 and it has amolecular weight of 412.52amu. This compound’s XRPD pattern
and FTIR spectrum are presented in Figs. 1 and 2. The fact that after
heatingtrandolaprilat 180◦C we obtaineda dipiperazine thatcould
possibly be used to design a new formulation with a completely
different pharmaceutical use was happily welcome. Furthermore,
it might lead to the design of an excellent recycling process that
would recover a useful substance from an expired drug. Towards
thisperspective,many other studies including biological evaluation
of the product need to be carried out. This opportunity should not
be overlooked since pharmaceuticals recycling is a much needed
prospective nowadays.
The differences of the crystallites of trandolapril and the new
dipiperazine formed after heating trandolapril at 180◦C can alsobe
Fig. 9. Decomposition mechanism of cyclizised trandolapril.
seenby comparing the correspondingHSPM images fromFig. 3. The
transformation takes place almost simultaneously during melting
and the new spherulites with completely different shape and size
are formed. The melting point of the newly formed dipiperazine, is
close to 160 ◦C as revealed by both DSC thermograms (Fig. 7) and
HSPM images (Fig. 3).
3.6. Py-GC–MS
For the study of decomposition mechanism with Py-GC–MS,
trandolapril is maintained for 2min at 100 ◦C in the pyrolyser
and heated with 20◦C/min till its full decomposition. The exper-
iment was conducted under nitrogen flow. The thermogram shape
(Supplementarymaterial) is similar totheDTGcurve(Fig.5), where
two decomposition peaks were also recorded. A small event is
recorded around 135◦C and the second degradation step around
280 ◦C. Thefirst mass loss step corresponds to gasses with ionmass
18 and is attributed to elimination of water that takes place dur-
ing cyclization of a trandolapril drug and the formation of imide
derivative (Fig. 8). This analysis is in good agreement with the data
already recorded withFTIR spectroscopy. Trandolapril has a molec-
ular weight 430.54g/mol and as can be seen after water removal,
the remaining ion mass is 412 and corresponds to the mass of
cyclizised trandolapril. The second degradation step, which results
in no residual, begins at 180 ◦C and is completed at 450 ◦C.
As can be seen from the mass spectra the weakest part of
cyclizised trandolapril that decomposes first is the ethoxy group
withion mass 45and after this thecarbonyl groupsis removed with
ion mass 28 (Fig. 9). The remaining ion mass after these elimina-
tions is 339.The decompositionafter thisstage is morecomplicated
since a more stablestructure is left. From thegas analysisof decom-
position products it seems that imide ring with the carbonylgroups
and themethylene groups connectedwith benzene ring are broken
Fig. 8. Theproposedreactionof secondary amine with thehydroxyl group of carboxylic acid (cyclizationvia nucleophilic attack).
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E. Roumeli et al./ Thermochimica Acta 539 (2012) 92–99 97
Fig. 10. (a) TG and (b) DTG curvesof trandolapril for heating rates (1) 5 ◦C/min, (2)
10 ◦C/min, (3)15 ◦C/min and (4) 20 ◦C/min.
and removed. The second remaining imide group is more stable
and thus the connected carbonyl group and the methylene groupswith ion mass 55 are next removed. The most stable molecules
andless volatile arethese of benzene andcyclohexane rings,which
both have ion masses 160 and as can be seen from ion spectra, are
decomposing at the final stage.
3.7. Thermal degradation kinetics of trandolapril
In order to analyze more thoroughly the degradation mecha-
nism of trandolapril W, the kinetic parameters (activation energy E
and pre-exponentialfactor A) andthe conversion function f (˛) need
to be evaluated. In this particular work we focused on the second
degradation step (179–510◦C) as it results in no residue and corre-
sponds to a 96% loss of the initial mass. The relationship between
kinetic parameters andextent of conversion (˛) canbe determinedusingthe mass loss curves. Thedegradation forthisAPI was studied
through non-isothermal measurements at multiple heating rates,
according to the recommendations of the International Confedera-
tion for Thermal Analysis and Calorimetry [18]. In Fig. 10 the mass
lossatdifferentheatingrates,5,10,15and20◦C/min, arepresented.
For the determination of activation energy it is preferable to use
isoconversional methods [19]. Since every isoconversional method
has different error, the use of more than one method can give a
range of values for the activation energy at every particular value
of the degree of degree of conversion, ˛.
The Ozawa–Flynn–Wall (OFW) method is the first one used
[20,21] which involves the measurement of temperature T , cor-
responding to a fixed value of the extent of conversion ˛, from
experiments carried out at different heating rates (ˇ). The OFWmethod is based on the equation:
ln ˇ = −1.052 E
RT + const
The plotof lnˇ vs. 1/T gives the slope−1.0516 E /R by which the
activation energy is calculated.
If the determined activation energy is the same for the various
values of ̨ , theexistence of a single-step reactioncan be concluded
with certainty. On the contrary, a variation of E with degree of
conversion is an indication of a complex reaction mechanism that
invalidates the separationof variables involvedin the OFW analysis
[22]. These complications are significant, especially in the case that
the total reaction involves competitive mechanisms.
Fig. 11. Dependence of activation energy (E ) o n t he e xte nt of con ve rs ion (˛) as
calculatedwith Friedman and OFW methods.
The second isoconversional method applied in this work was
suggested by Friedman [23] and it is a differential method based
on the equation:
ln
ˇd˛
dT
= ln A+ ln f (˛)−
E
RT
Where A is the pre-exponential factor and f (˛) the conversion
function (reaction model). For a constant ˛, the plot of ln(ˇd˛/dT )
vs. (1/T ) obtained from curves recorded at several heating rates,
should be a straight line whose slope gives the value of E . Itis obvi-
ous from this equation that if the function f (˛) is constant for a
particular value of ˛, thenthe sum ln f (˛) +ln A/ˇ, is also constant.
In Fig. 11 the dependence of the activation energy on the dif-
ferent mass conversion values is presented for both methods. The
differences in the values of E calculated by the OFW and Friedman
methods can be explained by a systematic error due to improper
integration. The method of Friedman employs instantaneous rate
values and is therefore, very sensitive to experimental noise. WithOFWmethod, the equation used is derived assuming constant acti-
vation energy, introducing a systematic error in the estimation of
E , in the case E varies with ˛. That error can be estimated by com-
parison with the Friedman analysis results [24].
Both of the used methods present more or less the same trend.
For conversion values up to 0.4, activation energy increases almost
linearly with˛. For higher ˛ values, the activation energy remains
almost stable. This variation indicates that probably a two-step
mechanism will describe the degradation of trandolapril more
accurately. That is in good agreement with the findings of Py-
GC–MS that suggested one relatively easier decomposition process
followed by a more difficult one.
The determination of the reaction model for multiple heating
rates is based on the “model fitting method”. Different kineticmodels were used for the fitting and the conversion range was
0 <˛< 1. Model-fitting methods involve fitting different models to
˛-temperature curves and simultaneously determining the acti-
vation energy E and the pre-exponential factor A. It has recently
been demonstrated that the complementary use of the model-free
method withisoconversionalmethodsfor one stepreactions is very
useful in order to understand the solid-state reaction kinetics [25].
In order to determinethe natureof the mechanisms through the
comparison of the experimental and theoretical data, initially it is
considered that the degradation of the APIcan be described only by
a single mechanism thatcorrespondsto themain massloss, without
presuming the exact mechanism. If the result of the fitting cannot
be considered as acceptable, then the fitting of the experimental
data with a combination of two mechanisms should follow [26].
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98 E. Roumeli et al. / Thermochimica Acta 539 (2012) 92–99
Fig. 12. Mass loss curves for different heating rates and the corresponding fit-
ting curves with Fn–Fn consecutive mechanisms for heating rates (1) 5 ◦C/min, (2)
10 ◦C/min, (3) 15 ◦C/min and (4) 20◦C/min.
Sixteen different models were tested and the n-th order (Fn)
and n-th order with autocatalysis (Cn) gave the best fit, but in bothcases,divergences appear in the early andthe final stages of degra-
dation, especially in the lower heating rates. The quality of the
fitting, especially in the initial and final degradation stages cannot
be considered as acceptable and taking into account that the ther-
mal degradation of organics is usually very complex, more than
one reaction mechanisms should be considered. That was also sug-
gested by the dependence of the activation energy on the fraction
of mass conversion (Fig. 11).
For the determination of the degradation parameters, two con-
secutivemechanisms wereassumedwhichcorrespond to theinitial
and the main mass loss steps respectively. The Fn mechanism that
was proposed by our preliminary study corresponds to the main
mass loss step while an unknown mechanism corresponds to the
initial mass loss step. In the process of identification by two differ-
entmechanisms, at least six unknown factors are involved, making
the mathematical problem of identification quite complex, with
several possible solutions. For this reason, at this stage of identi-
fication, it is important to limit the scope of the search among all
possible combinations of the widely used models. So, the models
that were used and theircombinations were only those whichhave
already given satisfactory results from the identification through a
singlestep mechanism, such as the reactionmodels Fn,Cn andBna.
The results of the best fitting are presented in Fig. 12 and the
calculated parameters in Table 1. The fit of the experimental data
is rather good for the whole area of mass loss for the studied sam-
ples for the combination of Fn–Fn models. As it can be seen, the
improvement in the quality of the fitting when using two mecha-
nisms instead of one, is profound.
Taking into account the above, the simplest combination of models can be chosen. Thus, Fn–Fn models are the combination
that describes best the degradation of the trandolapril. The acti-
vation energy of each step was calculated 97.4 and 180.0kJ/mol
respectively and the regression coefficient for the selected com-
bination of consecutive steps was 0.999940. This finding is also
in agreement with Py-GC–MS results that were presented above
Table 1
Calculated values of activation energy, pre-exponential factor and exponent n, f or
trandolapril samples.
Model Mechanism E (kJ/mol) log A (s−1) n R
Fn First 97.4 6.33 1.420.999940
Fn Second 180.0 12.37 0.73
and suggested the existence of one relatively easier decomposition
process followed by a more difficult one.
The fact that we were able to combine the actual findings of Py-
GC–MS with the theoretical kinetic studies is very important and
supports the complementary use of such techniques towards the
study of thermal behaviour of pharmaceuticals.
4. Conclusion
The thermal properties of trandolapril were studied in order to
investigate the conditions needed for its safe thermal destruction.
It was found that trandolapril is stable until the onset of melt-
ing (110◦C). In nitrogen and dry air environments it was found
that zero residual is reached at 510 and 550 ◦C respectively. DSC,
HSM, XRPD and FTIR studies confirmed that trandolapril during
heatingjust above its melting point undergoes cyclization via inter-
molecular nucleophilic attack, to form the substituted molecules
of a dipiperazine. From the decomposition mechanism evaluated
with Py-GC–MS it was found that unstable moieties like ethoxy
groups arefirst degradedwhile themost stable likethe benzeneand
cyclohexane groups are at the end. Finally, the activation energy
of the second degradation step was calculated using Friedman’s
and Ozawa, Flynn andWall’s isoconversionalmethods andthe TGA
curves were found to be described best by two consecutive mech-
anisms of n-th order (Fn–Fn). This study is one of the rare cases in
which findings of Py-GC–MS and theoretical calculations of kinetic
parameters of thermal decomposition actually agree, as they both
suggest theparticipation of twosteps in thedecomposition process.
Appendix A. Supplementary data
Supplementary data associated with this article canbe found, in
the online version, at http://dx.doi.org/10.1016/j.tca.2012.04.009.
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