68
H. Perrotin-Brunel et al. / Journal of Molecular Structure 987 (2011) 67–73
The first section of this paper presents experimental work to
on Total Energies, corrected for Zero Point Energy contributions
(ZPE-contributions).
determine the best reaction conditions (i.e. temperature and time)
for decarboxylation and its kinetics. Molecular modeling is then
used to support or justify proposed mechanism and kinetics
parameters for this solid state reaction in accordance with avail-
able literature and experimental data herein.
3. Results and discussion
3.1. Experimental results
Decarboxylation is a rather common chemical reaction in which
a carboxyl group splits off from a compound as carbon dioxide. The
2. Experimental
reaction for
by light or heat during e.g. storage or smoking. This reaction trans-
forms the acidic cannabinoids to their psychoactive forms
9-THC.
D
9-THCA shown schematically in Fig. 1, can be induced
2.1. Materials
D
Methanol was HPLC grade and was purchased from J.T. Baker
(Deventer, The Netherlands). Medical grade cannabis plant mate-
rial (female flower-tops) was obtained from Bureau Medicinale
Cannabis (The Hague, The Netherlands). It had a
of about 18%, and virtually no free
9-THC. The water content was
ꢂ3.6%. The standards of
9-THC (4.2 mg mLꢀ1 in methanol – ref
number 130-151205x) and
9-THCA (1.0 mg mLꢀ1 – ref number
In this article, only thermal decarboxylation will be considered. As
described above, the decarboxylation reaction has been studied in
the range of 90–140 °C. Under the experimental conditions, the
D
9-THCA content
highest yield to
D
9-THC was obtained at 110 °C and 110 min. Anal-
D
ysis of the data leads to the conclusion that this solid state reaction
surprisingly obeys a first order rate law. Raw kinetic data are pre-
sented in Fig. 2. Related k values are reported in Table 1. The cor-
responding ln k versus 1/T plots are shown in Fig. 3. This is a
straight line, described by the formula:
D
D
380-250407), with purity higher than 98%, were kindly donated
by PRISNA B.V.
E
ln k ¼ ln k0 ꢀ
RT
2.2. Method
from which E and k0 are determined to be 84.8 kJ molꢀ1 and
A sample of around 400 mg cannabis was blended in a mixer,
and heated at different temperatures in vacuum conditions for a
certain time. The temperature range studied was from 90 to
140 °C. To follow the reaction rate, a sample was taken every
5 min for the first hour and then every half an hour until the con-
3.7 ꢁ 108 sꢀ1 respectively.
3.2. Literature results
version of
D D
9-THCA to 9-THC was complete. Each solid sample
In the literature, only a few liquid phase thermal decarboxyl-
ation reactions of carboxylic acids, both aromatic as well as non-
aromatic, can be found [10–13]. Li and Brill reported experimental
activation energies for the first order decarboxylation of a series of
OH substituted benzoic acids under acidic conditions, ranging from
82 to 97 kJ molꢀ1 for 2,4,6-trihydroxybenzoic acid and 2,3-dihy-
droxybenzoic acid. Their k0-values range from 3.61 ꢁ 1010 sꢀ1 to
3.58 ꢁ 108 sꢀ1, the latter being similar to the one observed by us
[13].
was extracted with 50 mL methanol and sonicated for 15 min be-
fore being analysed with HPLC. In a series of extraction experi-
ments it was determined that the extraction process was
essentially complete. Calibration lines were determined for both
D
9-THCA and 9-THC. By this method the solid samples were
D
inherently corrected for weight loss (up to ꢂ30% at 140 °C) during
thermal treatment. Balances during the experiments, based on the
molalities of
D D
9-THCA and 9-THC, are >95%, indicating that the
In addition, by applying computational chemistry techniques
(B3LYP/6-31Gꢃ), Li and Brill found that intra-molecular decarbox-
ylation of the acids via a four membered ring transition state
yielded a very high activation barrier, thus suggesting that a real
first order process is very unlikely. The calculated activation barri-
ers for four-membered transition state for a series of caboxylic
acids ranged from 213 kJ molꢀ1 for 2,4-dihydroxybenzoic acid, to
225 kJ molꢀ1 for 2-hydroxybenzoic acid, and with a constant value
of 260 kJ molꢀ1 for 3-hydroxybenzoic acid, 3,5-dihydroxybenzoic
acid, and benzoic acid itself.
Li and Brill also found that the addition of one molecule of water
in the mechanism transformed the preferred transition state from
a four membered ring to a six membered ring with concomitant
reduction in the activation barrier to 130 kJ molꢀl, a value much
closer to the experimental values. However, these values are still
far too high, especially if it is realized that these barriers are based
on the ꢂ28 kJ molꢀl energetically unfavorable anti-conformer of
the acid [10–13] which acts as a highly reactive intermediate.
Recently, Chuchev and BelBruno [14] published a study on the
mechanism of the decarboxylation of ortho-substituted benzoic
acids, wherein they supported the work of Li and Brill that a single
water molecule is a potential model for an aqueous environment.
In addition, they concluded that the presence of a water molecule
forces the reaction through a keto-intermediate in the case of 2-
hydroxybenzoic-acid. The keto-intermediate then intramolecularly
decarboxylates to yield phenol and CO2. The overall process is illus-
trated in Fig. 4. However, their calculated activation barrier for the
decarboxylation of salicylic acid is ꢂ150 kJ molꢀ1, which is still
decarboxylation process itself proceeds with ꢂ100% selectivity.
Some skeletal rearrangements however cannot be excluded.
2.3. HPLC analyses
The HPLC profiles were acquired on a Chromapack HPLC system
consisting of an Isos pump, an injection valve and a UV–VIS detec-
tor (model 340 – Varian). The system is controlled by Galaxie
Chromatography software. The profiles were recorded at 228 nm,
as absorption by the solute is at its maximum at this wavelength.
The analytical column was a Vydac (Hesperia, CA) C18, type
218MS54 (4.6 ꢁ 250 mm2, 5
lm). The mobile phase consisted of
a mixture of methanol–water in a concentration gradient contain-
ing 25 mM of formic acid (pH 3). The methanol/water concentra-
tion ratio was linearly increased from 65% to 100% over 25 min,
and then kept constant for 3 min. Then the column was re-equili-
brated under initial conditions for 4 min, so the total running time
was 32 min. The flow rate was 1.5 mL minꢀ1 [8].
2.4. Molecular modeling
The Spartan ’06 package [9] was used for all calculations. All
structures were optimized using DFT B3LYP, level (6- 31Gꢃꢃ), start-
ing from PM3 optimized geometries. Transition states were identi-
fied and characterised using its unique imaginary vibrational
frequency or Internal Reaction Coordinate. Thermodynamical cor-
rections were applied; however activation energies were based