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v/v). The gradient employed started with 10% B, then increasing
linearly to 100% B at 30 min. Flow rate was 0.6 mL minꢀ1 and
oven temperature was 40 ꢃC. All samples were ltered with
0.45 mm GHP syringe lters (Acrodisc).
Experimental
Chemicals
`
Cyanidin chloride was purchased from Extrasynthese (Genay,
France), 2,4,6-trihydroxybenzaldehyde was purchased from
Aldrich, 2,4,6-trihydroxybenzoic acid and 3,4-dihydroxybenzoic
acid were purchased from Fluka.
Results and discussion
All aqueous solutions were prepared with type I water.
Methanol and ethanol were of HPLC grade. A universal buffer of
Theorell Stenhagen was made by dissolving 2.25 mL of phos-
phoric acid (85% w/w), 7.00 g of monohydrated citric acid, 3.54
g of boric acid and 343 mL of 1 M NaOH solution in water,
completed until 1 L.9
Fig. 1 shows the absorption spectra taken 20 ms aer a direct
pH jump followed by stopped ow. The spectral variations are
compatible with an acid base equilibrium between AH+ and A.
Representation of the absorbance as a function of pH (inset of
Fig. 1) gives a pKa ¼ 4.8.
The spectra shown in Fig. 1 evolve according to Fig. 2A. The
AH+/A species disappear to give other species absorbing pref-
erentially in the UV. Representation of the rate constant of this
process as a function of pH is a bell shaped curve as shown in
Fig. 2B.
Instrumentation and procedures
A stock solution of cyanidin chloride 1.50 ꢂ 10ꢀ4 M was prepared
by dissolving the appropriate amount of cyanidin in EtOH acid-
ied with 1% concentrated HCl. The use of an ethanolic instead
of an aqueous solution conferred an increased stability to the
stock solution and avoided precipitation during the experiments.
All pH measurements were made in a Crison BASIC 20+ pH-
meter tted with a Crison electrode. The calibration was made
with standard buffers at pH 4.00, 7.00 and 9.00 purchased from
CRISON.
The data shown in Fig. 2B would suggest a behaviour of
cyanidin similar to compounds lacking cis–trans isomerization
barrier, like many synthetic avylium compounds and also
some natural.6 However, a deeper analysis of the system proves
that it is not the case. The question is that in eqn (5) and (6) the
complete reversibility of the system is a requirement, which is
followed in the systems already reported.6 The data shown in
Fig. 3 clearly shows that this system is not reversible: aer a
direct pH jump and upon a certain delay, if a reverse pH jump is
applied back to pH ¼ 1 the absorption of the avylium is not
completely recovered, and increasing the delay decreases the
extent of absorption recovery.
The UV-vis measurements were made in a CARY 5000 spec-
trophotometer (VARIAN) using quartz cuvettes (1 cm path)
at 20 ꢃC, in the 220–800 nm range and at a scan rate of
1010 nm minꢀ1
.
The stopped ow experiments were conducted in an Applied
Photophysics SX20 stopped ow spectrometer provided with a
PDA.1/UV photodiode array detector with a minimum scan time
of 0.65 ms and a wavelength range of 200–700 nm.
All thermodynamic and kinetic constants of the cyanidin
chloride solution were determined by a spectrophotometric
method, as described elsewhere.10 A stock solution of cyanidin
chloride (1.50 ꢂ 10ꢀ4 M) in acidied ethanol was prepared as
described above.
Nevertheless, if the reverse pH jump is carried out within 1
min of delay aer the direct jump, the re-appearance of (some)
avylium cation can be monitored by stopped ow, Fig. 4. As
reported previously, the reverse pH jump converts all A into AH+
within a few milliseconds (mixing time of the stopped ow),
accounting for the absorbance of avylium/quinoidal base aer
the delay (75%).6 The rst observable kinetic process corresponds
to the recovery of more AH+ (16%) from B, since at low pH values
hydration step is faster than tautomerization (change of regime).
Direct pH jumps (from pH 1 to higher pH values) were carried
out by pippeting 0.250 mL of cyanidin stock solution into a
quartz cuvette, then rapidly adding 2.25 mL of a universal buffer
at the target pH value, and start collecting UV-vis spectra
immediately. This corresponds to a 10-fold dilution and the
analyzed solutions were therefore 10% in EtOH (v/v). Minor pH
adjustments were made by adding a few microliters of aqueous
HCl 10 M or NaOH 1 M solutions. The ionic strength was kept
constant. Reverse pH jumps (from higher pH values to pH 1) were
performed by adding 0.100 mL HCl (10 M) to cyanidin solutions
that previously underwent direct pH jumps. Throughout the
whole experiment the temperature was kept at 20 ꢃC.
The HPLC system was a Merck-Hitachi comprising a L-6200A
pump, a L-4500 Diode Array Detector, a L-5025 column oven, a D-
6000 interface controlled with the DSM soware, and a Rheo-
dyne 7125 manual injection valve with a 20 mL injection loop. The
analysis was performed in a Phenomenex Gemini column (C18,
150 ꢂ 4.6 mm, 3 mm). The solvents used were A (water : formic
Fig. 1 pH dependent absorption spectra obtained 20 ms after a pH
acid, 9 : 1, v/v) and B (water : formic acid : methanol, 4 : 1 : 5, jump followed by stopped flow.
This journal is © The Royal Society of Chemistry 2014
RSC Adv., 2014, 4, 18939–18944 | 18941