kinetic studies of retinol addition radicals · 2011-01-07 · kinetic absorption profile for the...
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Kinetic studies of retinol addition radicals
Ali El-Agamey,*a,b,c Shunichi Fukuzumi,*a,d K. Razi Naqvi,e and David J McGarveyb
aDepartment of Material and Life Science, Graduate School of Engineering, Osaka
University, Suita, Osaka 565-0871, Japan; bSchool of Physical and Geographical
Sciences, Keele University, Keele, Staffordshire, ST5 5BG, UK; cChemistry Department,
Faculty of Science, Mansoura University, New Damietta, Damietta, Egypt; dDepartment
of Bioinspired Science, Ewha Womans University, Seoul 120-750, Korea; eDepartment
of Physics, Norwegian University of Science and Technology (NTNU), N-7491,
Trondheim, Norway.
*Corresponding authors: Ali El-Agamey (Osaka University); Shunichi
Fukuzumi (Osaka University)
E-mails: [email protected]; [email protected] Tel. No.: +81-
0668797369; Fax No.: +81-0668797370
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Contents
Fig. S1 Transient spectra of 2-PyrS• obtained following 266 nm laser photolysis of 2, 2`-dipyridyl disulfide (~3.0 × 10–4 M) in air-saturated methanol (laser energy ~7 mJ). The inset shows the transient profiles at 380 and 490 nm.
Fig. S2 Transient absorption spectra obtained following LFP (266 nm) of phenyl disulfide (~6 × 10–4 M) in air-saturated methanol (laser energy ~10 mJ). Fig. S3 Normalized kinetic absorption profiles for the decay of PhS• at 450 nm in air- and argon-saturated methanol (laser energy ~4 mJ). Fig. S4 Transient spectra of 2-PyrS-retinol• obtained following 266 nm laser photolysis of 2, 2`-dipyridyl disulfide (~3.0 × 10–4 M) in the presence of retinol (~5.0 × 10–5 M) in air-saturated methanol at room temperature (laser energy ~4 mJ). The inset shows a kinetic absorption profile for the decay of 2-PyrS-retinol• at 380 nm. Fig. S5 Transient spectra of PhS-retinol• obtained following 266 nm laser photolysis of phenyl disulfide (~6 × 10–4 M) in the presence of retinol (~5.0 × 10–5 M) in air-saturated methanol at room temperature (laser energy ~4 mJ). The inset shows a kinetic absorption profile for the decay of PhS-retinol• at 380 nm. Fig. S6 Transient spectra of 4-PyrS-retinol• obtained following 266 nm laser photolysis of 4, 4`-dipyridyl disulfide (~1.0 × 10–4 M) in the presence of retinol (~4.0 × 10–5 M) in air-saturated cyclohexane at room temperature (laser energy ~4 mJ). The inset shows a kinetic absorption profile for the decay of 4-PyrS-retinol• at 380 nm. Fig. S7 Transient spectra of 4-PyrS-retinol• obtained following 266 nm laser photolysis of 4, 4`-dipyridyl disulfide (~2.0 × 10–4 M) in the presence of retinol (~4.0 × 10–5 M) in argon-saturated methanol at room temperature (laser energy ~4 mJ). The inset shows a kinetic absorption profile for the decay of 4-PyrS-retinol• at 380 nm.
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Fig. S8 Plots of pseudo-first order rate constants (kobs) for formation of PhS-retinol•, 4-PyrS-retinol• or 2-PyrS-retinol• at 380 nm, from the reaction of retinol with phenyl disulfide, 4, 4`-dipyridyl disulfide or 2, 2`-dipyridyl disulfide, respectively in air-saturated methanol versus the concentration of retinol (laser energy ~4.0 mJ). Fig. S9 Kinetic absorption profiles for the formation of 4-PyrS-retinol• at 380 nm at various retinol concentrations formed following 266 nm laser photolysis (laser energy ∼4 mJ) of 4, 4`-dipyridyl disulfide (~2.0 × 10–4 M) in the presence of retinol in air-saturated methanol. Fig. S10 Kinetic absorption profiles for the formation of 2-PyrS-retinol• at 380 nm at various retinol concentrations formed following 266 nm laser photolysis (laser energy ∼4 mJ) of 2, 2`-dipyridyl disulfide (~3.0 × 10–4 M) in the presence of retinol in air-saturated methanol. Fig. S11 Kinetic absorption profiles for the formation of PhS-retinol• at 380 nm at various retinol concentrations formed following 266 nm laser photolysis (laser energy ∼4 mJ) of phenyl disulfide (~6.0 × 10–4 M) in the presence of retinol in air-saturated methanol. Fig. S12 Arrhenius plot for the slow growth (at 380 nm) generated from the reaction of 4-PyrS• (4,4`-dipyridyl disulfide ~2 × 10–4 M) and retinol (~8.0 × 10–5 M), in argon-saturated methanol (laser energy ~4 mJ). Fig. S13 Transient spectra of 4-PyrS-retinol• obtained following 266 nm laser photolysis of 4, 4`-dipyridyl disulfide (~2.0 × 10–4 M) in the presence of retinol (~4.0 × 10–5 M) in air-saturated methanol at 334 K (laser energy ~4 mJ). The inset shows a kinetic absorption profile of 4-PyrS-retinol• at 380 nm. Fig. S14 Eyring plots for the slow growth (at 380 nm) generated from the reaction of 4-PyrS• or 2-PyrS• with retinol (~8.0 × 10–5 M), in argon-saturated methanol (laser energy ~4 mJ). Fig. S15 Transient profiles, at 380 nm, for 4-PyrS-retinol• and 4-PyrS• in argon-saturated methanol at 334 K (laser energy ~4 mJ).
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Fig. S16 Transient profiles, at 380 nm, for 2-PyrS-retinol• and 2-PyrS• in argon-saturated methanol at 334 K (laser energy ~4 mJ). Fig. S17 Transient profile of PhS-retinol•, at 380 nm, following 266 nm laser photolysis (laser energy ~4 mJ) of phenyl disulfide (~6 × 10–4 M) in the presence of retinol (~9.0 × 10–5 M), in argon-saturated methanol at 333 K. Fig. S18 Normalized kinetic absorption profiles for the decay of 4-PyrS-retinol• at 380 nm in methanol at various oxygen concentrations (5, 21, 50 and 100%) formed following 266 nm laser photolysis (laser energy ~4 mJ) of 4, 4`-dipyridyl disulfide (~2 × 10–4 M) in the presence of retinol (~8.0 × 10–5 M). The inset shows plots of pseudo-first order rate constants (kobs) for the fast and slow decay of 4-PyrS-retinol•, at 380 nm, versus the oxygen concentration. Fig. S19 The influence of temperature on the normalized transient profiles, at 380 nm, of 2-PyrS-retinol• following 266 nm laser photolysis (laser energy ~4 mJ) of 2, 2`-dipyridyl disulfide (~3.0 × 10–4 M) in the presence of retinol (~8 × 10–5 M), in air-saturated methanol. Fig. S20 Plots of pseudo-first order rate constants (kobs) for the fast and slow decay of PhS-retinol• at 380 nm, generated following 266 nm laser photolysis of phenyl disulfide (~6 × 10–4 M) with retinol (~9.0 × 10–5 M) in methanol, versus the oxygen concentration (laser energy ~4 mJ). The inset shows normalized kinetic absorption profiles for the decay of PhS-retinol•, at 380 nm, at various oxygen concentrations (1, 5, 21, 50, 100% and argon). Fig. S21 The influence of temperature on the normalized transient profiles, at 380 nm, of PhS-retinol• following 266 nm laser photolysis (laser energy ~4 mJ) of phenyl disulfide (~6 × 10–4 M) in the presence of retinol (~9.0 × 10–5 M), in air-saturated methanol. Table S1: Values of kobs for the slow absorption rise at 380 nm following 266 nm LFP (laser energy ~4 mJ) of 4, 4`-dipyridyl disulfide (~2 × 10–4 M) in the presence of retinol (~8.0 × 10–5 M), in argon-saturated methanol at different temperatures.
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Table S2: Values of kobs for the slow absorption rise at 380 nm following 266 nm LFP (laser energy ~4 mJ) of 2, 2`-dipyridyl disulfide (~3.0 × 10–4 M) in the presence of retinol (~8.0 × 10–5 M), in argon-saturated methanol at different temperatures.
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0
0.01
0.02
0.03
400 440 480 520
0.47 µs3.19 µs8.14 µs16.59 µs87.20 µs
Wavelength/ nm
ΔA
0
0.02
0 25 50 75 100
380 nm490 nmΔ
At/ µs
Fig. S1 Transient spectra of 2-PyrS• obtained following 266 nm laser photolysis of 2, 2`-dipyridyl disulfide (~3.0 × 10–4 M) in air-saturated methanol (laser energy ~7 mJ). The inset shows the transient profiles at 380 and 490 nm.
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0
0.02
0.04
400 450 500 550
0.52 µs2.58 µs6.92 µs17.7 µs88.0 µs
Wavelength/ nm
ΔA
Fig. S2 Transient absorption spectra obtained following LFP (266 nm) of phenyl disulfide (~6 × 10–4 M) in air-saturated methanol (laser energy ~10 mJ).
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0
0.005
0.01
0.015
0 25 50 75 100
ArgonAir
ΔA
t/ µs
Fig. S3 Normalized kinetic absorption profiles for the decay of PhS• at 450 nm in air- and argon-saturated methanol (laser energy ~4 mJ).
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0
0.04
0.08
0.12
0.16
360 405 450 495 540 585 630
0.04 ms0.2 ms0.5 ms1.0 ms
Wavelength/ nm
ΔA 0
0.05
0.1
0 1 2
380 nm
ΔA
t/ ms
Fig. S4 Transient spectra of 2-PyrS-retinol• obtained following 266 nm laser photolysis of 2, 2`-dipyridyl disulfide (~3.0 × 10–4 M) in the presence of retinol (~5.0 × 10–5 M) in air-saturated methanol at room temperature (laser energy ~4 mJ). The inset shows a kinetic absorption profile for the decay of 2-PyrS-retinol• at 380 nm.
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0
0.04
0.08
0.12
0.16
360 405 450 495 540 585 630
0.07 ms0.3 ms1.0 ms1.5 ms
Wavelength/ nm
ΔA 0
0.05
0.1
0 1 2
380 nm
ΔA
t/ ms
Fig. S5 Transient spectra of PhS-retinol• obtained following 266 nm laser photolysis of phenyl disulfide (~6 × 10–4 M) in the presence of retinol (~5.0 × 10–5 M) in air-saturated methanol at room temperature (laser energy ~4 mJ). The inset shows a kinetic absorption profile for the decay of PhS-retinol• at 380 nm.
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0
0.04
0.08
0.12
0.16
360 405 450 495
0.1 ms0.4 ms0.7 ms1.62 ms
Wavelength/ nm
ΔA 0
0.06
0.12
0 1 2
380 nm
ΔA
t/ ms
Fig. S6 Transient spectra of 4-PyrS-retinol• obtained following 266 nm laser photolysis of 4, 4`-dipyridyl disulfide (~1.0 × 10–4 M) in the presence of retinol (~4.0 × 10–5 M) in air-saturated cyclohexane at room temperature (laser energy ~4 mJ). The inset shows a kinetic absorption profile for the decay of 4-PyrS-retinol• at 380 nm.
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0
0.04
0.08
0.12
0.16
360 405 450 495 540 585 630
0.02 ms0.12 ms1.5 ms
Wavelength/ nm
ΔA 0
0.04
0.08
0 30 60 90
380 nm
ΔA
t/ ms
Fig. S7 Transient spectra of 4-PyrS-retinol• obtained following 266 nm laser photolysis of 4, 4`-dipyridyl disulfide (~2.0 × 10–4 M) in the presence of retinol (~4.0 × 10–5 M) in argon-saturated methanol at room temperature (laser energy ~4 mJ). The inset shows a kinetic absorption profile for the decay of 4-PyrS-retinol• at 380 nm.
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0
2
4
6
0 25 50 75
Phenyl disulfide4, 4`-Dipyridyl disulfide2, 2`-Dipyridyl disulfide
k obs/ 1
05 s-1
[retinol]/ µM
Fig. S8 Plots of pseudo-first order rate constants (kobs) for formation of PhS-retinol•, 4-PyrS-retinol• or 2-PyrS-retinol• at 380 nm, from the reaction of retinol with phenyl disulfide, 4, 4`-dipyridyl disulfide or 2, 2`-dipyridyl disulfide, respectively in air-saturated methanol versus the concentration of retinol (laser energy ~4.0 mJ).
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0
0.05
0 15 30 45
1.3 x 10-5 M
2.6 x 10-5 M
ΔA
t/ µs
Fig. S9 Kinetic absorption profiles for the formation of 4-PyrS-retinol• at 380 nm at various retinol concentrations formed following 266 nm laser photolysis (laser energy ∼4 mJ) of 4, 4`-dipyridyl disulfide (~2.0 × 10–4 M) in the presence of retinol in air-saturated methanol.
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0
0.05
0.1
0.15
0 15 30 45
2.7 x 10-5 M
4.5 x 10-5 M
ΔA
t/ µs
Fig. S10 Kinetic absorption profiles for the formation of 2-PyrS-retinol• at 380 nm at various retinol concentrations formed following 266 nm laser photolysis (laser energy ∼4 mJ) of 2, 2`-dipyridyl disulfide (~3.0 × 10–4 M) in the presence of retinol in air-saturated methanol.
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0
0.05
0.1
0 30 60 90
4.3 x 10-5 M
6.0 x 10-5 M
8.0 x 10-5 M
ΔA
t/ µs
Fig. S11 Kinetic absorption profiles for the formation of PhS-retinol• at 380 nm at various retinol concentrations formed following 266 nm laser photolysis (laser energy ∼4 mJ) of phenyl disulfide (~6.0 × 10–4 M) in the presence of retinol in air-saturated methanol.
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7
8
9
10
0.003 0.0032 0.0034
ln(k
β/ s-1
)
K/ T
Fig. S12 Arrhenius plot for the slow growth (at 380 nm) generated from the reaction of 4-PyrS• (4,4`-dipyridyl disulfide ~2 × 10–4 M) and retinol (~8.0 × 10–5 M), in argon-saturated methanol (laser energy ~4 mJ).
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0
0.04
0.08
0.12
360 405 450
0.33 µs21.0 µs130 µs436 µs
Wavelength/ nm
ΔA 0
0.05
0.1
0 150 300 450
380 nmΔA
t/ µs
Fig. S13 Transient spectra of 4-PyrS-retinol• obtained following 266 nm laser photolysis of 4, 4`-dipyridyl disulfide (~2.0 × 10–4 M) in the presence of retinol (~4.0 × 10–5 M) in air-saturated methanol at 334 K (laser energy ~4 mJ). The inset shows a kinetic absorption profile of 4-PyrS-retinol• at 380 nm.
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-22
-21
-20
-19
0.003 0.0032 0.0034
4, 4`-dipyridyl disulfide2, 2`-dipyridyl disulfide
ln(k
β hT
-1k b-1
)
K/ T
Fig. S14 Eyring plots for the slow growth (at 380 nm) generated from the reaction of 4-PyrS• or 2-PyrS• with retinol (~8.0 × 10–5 M), in argon-saturated methanol (laser energy ~4 mJ).
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0.04
0.08
0.12
0 0.2 0.4 0.6 0.8 1
retinol and 4, 4`-dipyridyl disulfide 4, 4`-dipyridyl disulfide onlyΔ
A
t/ ms
Fig. S15 Transient profiles, at 380 nm, for 4-PyrS-retinol• and 4-PyrS• in argon-saturated methanol at 334 K (laser energy ~4 mJ).
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0.04
0.08
0.12
0.16
0 0.2 0.4 0.6
retinol and 2, 2`-dipyridyl disulfide2, 2`-dipyridyl disulfide onlyΔ
A
t/ ms
Fig. S16 Transient profiles, at 380 nm, for 2-PyrS-retinol• and 2-PyrS• in argon-saturated methanol at 334 K (laser energy ~4 mJ).
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0.05
0.1
0.15
0 150 300 450
ΔA
t/ µs
Fig. S17 Transient profile of PhS-retinol•, at 380 nm, following 266 nm laser photolysis (laser energy ~4 mJ) of phenyl disulfide (~6 × 10–4 M) in the presence of retinol (~9.0 × 10–5 M), in argon-saturated methanol at 333 K.
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0.12
0 0.5 1 1.5 2 2.5
5 %21 %50 %100 %
ΔA
t/ ms
0
5
10
15
20
0 0.005 0.01
Fast stepSlow step
k obs/ 1
03 s-1
[O2]/ M
Fig. S18 Normalized kinetic absorption profiles for the decay of 4-PyrS-retinol• at 380 nm in methanol at various oxygen concentrations (5, 21, 50 and 100%) formed following 266 nm laser photolysis (laser energy ~4 mJ) of 4, 4`-dipyridyl disulfide (~2 × 10–4 M) in the presence of retinol (~8.0 × 10–5 M). The inset shows plots of pseudo-first order rate constants (kobs) for the fast and slow decay of 4-PyrS-retinol•, at 380 nm, versus the oxygen concentration.
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0
0.04
0.08
0.12
0.16
0 3 6 9
297 K323 K333 K
ΔA
t/ ms
Fig. S19 The influence of temperature on the normalized transient profiles, at 380 nm, of 2-PyrS-retinol• following 266 nm laser photolysis (laser energy ~4 mJ) of 2, 2`-dipyridyl disulfide (~3.0 × 10–4 M) in the presence of retinol (~8 × 10–5 M), in air-saturated methanol.
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0
2
4
6
0 0.005 0.01
Fast stepSlow step
k obs/ 1
03 s-1
[O2]/ M
0
0.08
0.16
0 2.5 5 7.5 10
Argon1 %5 %21 %50 %100 %Δ
At/ ms
Fig. S20 Plots of pseudo-first order rate constants (kobs) for the fast and slow decay of PhS-retinol• at 380 nm, generated following 266 nm laser photolysis of phenyl disulfide (~6 × 10–4 M) with retinol (~9.0 × 10–5 M) in methanol, versus the oxygen concentration (laser energy ~4 mJ). The inset shows normalized kinetic absorption profiles for the decay of PhS-retinol•, at 380 nm, at various oxygen concentrations (1, 5, 21, 50, 100% and argon).
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0
0.03
0.06
0 2.5 5 7.5 10
301 K334 K
ΔA
t/ ms
Fig. S21 The influence of temperature on the normalized transient profiles, at 380 nm, of PhS-retinol• following 266 nm laser photolysis (laser energy ~4 mJ) of phenyl disulfide (~6 × 10–4 M) in the presence of retinol (~9.0 × 10–5 M), in air-saturated methanol.
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Table S1: Values of kobs for the slow absorption rise at 380 nm following 266 nm LFP (laser energy ~4 mJ) of 4, 4`-dipyridyl disulfide (~2 × 10–4 M) in the presence of retinol (~8.0 × 10–5 M), in argon-saturated methanol at different temperatures.
T/K kobs for the slow absorption rise/ s-1
334 1.78 × 104 327 1.10 × 104 321 7.45 × 103 311 4.25 × 103 296 1.39 × 103
Table S2: Values of kobs for the slow absorption rise at 380 nm following 266 nm LFP (laser energy ~4 mJ) of 2, 2`-dipyridyl disulfide (~3.0 × 10–4 M) in the presence of retinol (~8.0 × 10–5 M), in argon-saturated methanol at different temperatures.
T/K kobs for the slow absorption rise/ s-1
334 3.29 × 104 327 2.14 × 104 321 1.60 × 104 311 8.55 × 103 296 3.48 × 103
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