Pawlus S, Paluch M, Sekula M, Ngai K L, Rzoska S J, Ziolo J
Institute of Physics, Silesian University, Uniwersytecka 4, 400-07 Katowice, Poland.
Phys Rev E Stat Nonlin Soft Matter Phys. 2003 Aug;68(2 Pt 1):021503. doi: 10.1103/PhysRevE.68.021503. Epub 2003 Aug 12.
Dielectric relaxation measurements have been used to study the crossover in dynamics with temperature and pressure, onset of breakdown of the Debye-Stokes-Einstein law, and the relation between the alpha and the beta relaxations in diethyl phthalate. The measurements made over 10 decades in frequency and a broad range of temperature and pressure enable the dc conductivity and the alpha- and the beta-relaxations to be studied altogether. The isobaric data show that the alpha-relaxation time tau(alpha) has temperature dependence that crosses over from one Vogel-Fulcher-Tammann-Hesse form to another at T(B) approximately 227 K and tau(alpha) approximately 10(-2) s. The dc conductivity sigma exhibits similar crossover at the same T(B). At temperatures above T(B), tau(alpha) and sigma have the same temperature dependence, but below T(B) they become different and the Debye-Stokes-Einstein law breaks down. The breadth of the alpha relaxation is nearly constant for T<T(B), but decreases with increasing temperature for T>T(B). The time dependence of tau(beta) is Arrhenius, which when extrapolated to higher temperatures intersects tau(alpha) at T(beta) nearly coincident with T(B). Isothermal measurements at various applied pressures when compared with isobaric data show that the shape of the alpha-relaxation depends only on tau(alpha), and not on the T and P combinations. At a constant temperature, while tau(alpha) increases rapidly with pressure, the beta-relaxation time tau(beta) is insensitive to applied pressure. This behavior is exactly the same as found in 1,1(')-bis (p-methoxyphenyl) cyclohexane. The findings are discussed in the framework of the coupling model.
介电弛豫测量已被用于研究动力学随温度和压力的转变、德拜 - 斯托克斯 - 爱因斯坦定律的击穿起始,以及邻苯二甲酸二乙酯中α弛豫和β弛豫之间的关系。在频率跨越10个数量级以及较宽温度和压力范围内进行的测量,使得能够同时研究直流电导率以及α弛豫和β弛豫。等压数据表明,α弛豫时间τ(α)具有温度依赖性,在约227 K和τ(α)约为10⁻² s时,从一种Vogel - Fulcher - Tammann - Hesse形式转变为另一种形式。直流电导率σ在相同的T(B)处表现出类似的转变。在高于T(B)的温度下,τ(α)和σ具有相同的温度依赖性,但在低于T(B)时它们变得不同,并且德拜 - 斯托克斯 - 爱因斯坦定律失效。对于T < T(B),α弛豫的宽度几乎恒定,但对于T > T(B),它随温度升高而减小。τ(β)的时间依赖性是阿仑尼乌斯型的,当外推到更高温度时,在T(β)处与τ(α)相交,T(β)几乎与T(B)重合。与等压数据相比,在各种施加压力下的等温测量表明,α弛豫的形状仅取决于τ(α),而不取决于T和P的组合。在恒定温度下,虽然τ(α)随压力迅速增加,但β弛豫时间τ(β)对施加压力不敏感。这种行为与在1,1'-双(对甲氧基苯基)环己烷中发现的完全相同。研究结果在耦合模型的框架内进行了讨论。