International Journal of Polymer Science

International Journal of Polymer Science / 2011 / Article

Research Article | Open Access

Volume 2011 |Article ID 627195 |

Maria Larkowska, Michael Wuebbenhorst, Stanislaw Kucharski, "Spirooxazine Photoisomerization and Relaxation in Polymer Matrices", International Journal of Polymer Science, vol. 2011, Article ID 627195, 6 pages, 2011.

Spirooxazine Photoisomerization and Relaxation in Polymer Matrices

Academic Editor: Qijin Zhang
Received21 Mar 2011
Accepted17 Jun 2011
Published14 Aug 2011


9′-Hydroxy-1,3,3-trimethylspiro[indoline-2,3′[3H]naphtha[2,1-b]-1,4oxazine] (SPO-7OH) was used in studies of photochromic transformations in polymer matrices. Illumination with UV lamp caused opening the spirostructure of the oxazine with formation of open merocyanine species absorbing at ca. 610 nm. The kinetic studies of thermal relaxation of the open form showed that this process can be described with a biexponential function including both photochemical reaction and rheological behaviour of the polymeric environment. Basing on Arrhenius plot of the rate constant ascribed to the photochemical reaction, the activation energy was determined, which was 66.1 and 84.7 kJ/mole for poly(methyl methacrylate-co-butyl methacrylate) and poly(vinylpyrrolidone) matrix, respectively.

1. Introduction

Extensive research has been devoted to gain insight into transformation of photochromic molecules induced by light [1, 2]. Reversible rearrangement of bistable molecules occurs in photochemical or thermal way. Significantly different molecular states can exist as thermodynamically stable ones. The photoisomers differ in their physical properties such as absorption spectra, refractive indices, dielectric constants, geometrical structure, and oxidation/reduction potential [3]. Interests devoted to photochromic materials have been expanded because of their potential applications in optical devices and memories [46].

Among the most important categories of photochromic molecules there are spirocompounds which can induce excellent colouration during irradiation [79]. UV light excitation occurs to be relatively strong to cause photocleavage of the C–O spirobond of the spirooxazine which leads to the coloured merocyanine; the latter can exist in four isomeric forms [1012]. The mechanism of the reversible photochromic transformation of spirooxazines involves the photochemical process of ring opening of spirocompound yielding merocyanines and thermal or photochemical relaxation process of closing ring of the merocyanines [13]. The process of reversible isomerization is presented in Figure 1.

Studies on photochromism of spirooxazines have been carried out in various organic solvents as well as in different media, such as polymer matrices, liposomal membranes, monolayers, and bilayer-clay matrices [8]. The lifetimes of excited state of the spiroform and subsequent open form depend on temperature [1416]. The polarity of polymer matrices is of great importance because of possible interactions between polymer chain and tautomeric form of merocyanine [12, 17].

In this paper the main attention was focused on investigation of the temperature influence on reversible isomerization of spirooxazine in polymer matrices. Two polymers with different glass transition temperature and polarity were used as matrices, and concentration of the dye was 30% by weight. The temperature dependence was controlled by measurement of UV-Vis absorption spectra. It is to mention that spirooxazines belong to the photochromic dyes sensitive to UV range of radiation [10, 18, 19].

2. Experimental

2.1. Materials

9′-Hydroxy-1,3,3-trimethylspiro[indoline-2,3′[3H]naphtha[2,1-b]-1,4oxazine] (SPO-7OH) was synthesized using previously described procedures [18, 19]. 1-Nitrosonaphthalene-2,7-diol (5.28 mmnol, 1.00 g) was dissolved in 100 mL ethanol. 1,3,3-Trimethyl-2-methyleneindoline (4.80 mmol, 0.83 g) was added, and the reaction mixture was refluxed with stirring for 5 hours. The resulting product was purified by silica gel column chromatography using chloroform as an eluent. Yield of SPO-7OH was 41% (0.68 g).

Poly(methyl methacrylate-co-butyl methacrylate) (P(MMA-BMA)) and poly(vinylpyrrolidone) (PVP) were purchased from Sigma-Aldrich.

Polymer films containing spirooxazine dye (SPO-7OH) were prepared by spin coating technique. The materials were deposited on glass plates using 6% solution of P(MMA-BMA) or 3% solution of PVP in chloroform. The concentration of photochromic compounds (SPO-7OH) in polymers was 30%. The samples were annealed at 423 K for 8 hours. The thicknesses of polymer films were in the range of 200–400 nm depending on concentration of polymer solutions. The resulting films were kept in dark before measurement.

2.2. Optical Experiments

UV-Vis spectra were recorded using DT-MINI-2-GS Mikropack UV-VIS-NIR LIGHTSOURCE. The polymer films were irradiated with 365 nm diode light (type H2A1-H365) providing 25 mW power. The samples were kept at constant temperature during illumination and thermal relaxation, and the temperature was controlled by DC HEATER SUPPLY.

3. Results and Discussion

3.1. Absorption Spectra of Spirooxazine Photochromic System

The measurements of UV-Vis spectra were carried out using thin polymer films containing spirooxazine (SPO-7OH) on glass plates. The absorption spectra of SPO-7OH in P(MMA-BMA) during illumination with UV diode light and thermal relaxation are presented in Figures 2 and 3, respectively.

Spirooxazine showed maximum absorption peak in the range of ca. 344–350 nm, depending on the polymer matrix. Upon UV light excitation, the spiro-carbon-oxygen (C–O) bond of colorless ring-closed form breaks and the subsequent isomerization leads to colored ring-open isomers (merocyanine). The maximum absorption peak of merocyanine is located at 610 nm for PVP and at 613 nm for P(MMA-BMA) guest host system. The photoisomerization of photochromic materials is reversible. The metastable colored form is changed into ground state colourless form. The route from open to closed form of spirocompound took place as a thermal relaxation process. Influence of temperature on relaxation process was investigated. The measurements were carried out within the range of 303–333 K in steps of 10 K under strict temperature control. The UV-Vis spectra were recorded during heating and periodic illumination with 365 nm diode light. Spectral parameters are presented in Table 1.

SampleTemperature (K) 𝜆 m a x (nm) 𝐴 ( 𝑡 ) 𝑖 (a.u.) 𝑡 𝑖 (s) 𝐴 ( 𝑡 ) 𝑟 (a.u.) 𝑡 𝑟 (s)

SPO-7OH P(MMA-BMA)3036130.5692000.167200
SPO-7OH P(MMA-BMA)3136130.4022000.078200
SPO-7OH P(MMA-BMA)3236130.0202000.015200
SPO-7OH P(MMA-BMA)3336130.0842000.00080
SPO-7OH PVP3036100.1942000.115200
SPO-7OH PVP3136100.1702000.110200
SPO-7OH PVP3236100.1262000.083200
SPO-7OH PVP3336100.0842000.058200

𝐴 ( 𝑡 ) 𝑖 : absorbance of merocyanine measured after time 𝑡 𝑖 during illumination with light;
𝐴 ( 𝑡 ) 𝑟 : absorbance of merocyanine measured after time 𝑡 𝑟 during thermal relaxation.
3.2. Kinetics of the Thermal Relaxation Process

Kinetic characteristics of thermal relaxation process of SPO-7OH were presented by recording the maximum absorption band decay in two different polymer matrices. The typical curves of absorption growth and relaxation processes are showed in Figure 4.

Several kinetic models are known and used to explain relaxation processes [14, 20, 21]. Biexponential function describes relaxation process sufficiently well, so (1) was chosen to optimize thermal bleaching reaction converting merocyanines to their ground state ring-closed form: 𝐴(𝑡)=𝑎𝑒𝑘𝑎𝑡+𝑏𝑒𝑘𝑏𝑡,(1) where 𝐴(𝑡) is change of absorbance observed at time 𝑡; 𝑘𝑎 and 𝑘𝑏 represent the rate constants ascribed to the amplitude of 𝑎 and 𝑏, respectively. The first part of (1) is responsible for isomerization of chromophore, and the second part corresponds to material equilibration. The rate constants 𝑘𝑎 and 𝑘𝑏 determine the rate of open-closed isomerization and the rate of material reorientation, respectively.

The decay curves were fitted to biexponential decay model using a computer program. This biexponential model fits experimental points into calculated curve very well. All values of the constants are given in Table 2. Along with increase of temperature, there is observed an increase of rate constants and thereby relaxation process is significantly faster at higher temperature. Comparing the rate constants 𝑘𝑎 and 𝑘𝑏, it can be noticed that the first process is considerably faster than the second one. This means that the main influence on the rate of relaxation process has open-closed isomerization. However, the suppressing environment relaxation and kind of polymer matrices had a distinct effect that was evidenced by higher values of the rate constants in P(MMA-BMA) versus PVP in guest host system. The polarity of polymer matrices can influence the relaxation rate because of formation of the dipole-dipole interaction between merocyanine and side chains of polymers (Figure 5). The dipolar interactions are significantly stronger in PVP than in P(MMA-BMA). The differences in dipolar interactions of the polymers with merocyanine have a distinct effect on difference in stabilization of merocyanine forms. The relaxation process appeared to be slower when the interactions were more pronounced owing to the presence of nitrogen atoms in PVP polymer.

SampleTemperature (K) 𝑎 𝑘 𝑎 𝑏 𝑘 𝑏 𝑅

SPO-7OH P(MMA-MBA)3030.37980.02050.22400.00170.996
SPO-7OH P(MMA-MBA)3130.19920.05960.19300.00500.999
SPO-7OH P(MMA-MBA)3230.12450.10130.06070.00840.999
SPO-7OH P(MMA-MBA)3330.04670.23640.03630.04340.997
SPO-7OH PVP3030.10260.00230.18290.00010.999
SPO-7OH PVP3130.03640.00850.13450.00040.999
SPO-7OH PVP3230.02600.02250.10010.00110.999
SPO-7OH PVP3330.01160.04770.06930.00110.999

The Arrhenius equation (2) was used to determine activation energy (𝐸𝑎) of relaxation process corresponding to the faster step: 𝑘ln𝑎=ln𝑘0𝐸𝑎𝑅1𝑇.(2)

The Arrhenius plots for thermal bleaching of SPO-7OH in polymer matrices were shown in Figure 6. The calculated values of rate constants (𝑘𝑎) fit the Arrhenius plots with very good precision, so it was possible to determine values of energy barrier which were presented in Table 3. It can be noticed that activation energy in relaxation process of SPO-7OH in P(MMA-BMA) is lower than that in PVP which is consistent with expectation.

Sample 𝑘 0 [s−1] 𝐸 𝑎 [kJ·mol−1]

SPO-7OH P(MMA-BMA)5.46·10966.10
SPO-7OH PVP1.03·101284.72

4. Conclusions

The illumination of spirooxazine containing polymer matrix resulted in formation of open merocyanine species absorbing at ca. 610 nm. The reverse process could be described as composed of two stages: first one as a photochemical closing of merocyanine form and the second one as the polymer matrix rheological cooperation response. The Arrhenius plot of the reaction rate constant of the first stage made it possible to determine activation energy of this process that was 66.1 and 84.7 kJ/mole in poly(methyl methacrylate-co-butyl methacrylate) and poly(vinylpyrrolidone) matrix, respectively.


This work was supported by the grant of Chemistry Department of Wrocław University of Technology, Wrocław (Poland), and Catholic University of Leuven (Belgium).


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Copyright © 2011 Maria Larkowska et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

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