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J. C. Cañadas

Publications and source records attributed to J. C. Cañadas.

3 recordsLinked to original sources

Double glass transition in polyethylene naphthalate structural relaxation by MDSC, BDS and TSDC

In this work, we present an experimental study of the primary and secondary relaxations of the semi-crystalline polymer polyethylene naphthalate (PEN), by Modulated Differential Scanning Calorimetry (MDSC), Thermally Stimulated Depolarization Currents (TSDC) and Broadband Dielectric Spectroscopy (BDS), and how they are affected by physical aging. Three dipolar relaxation modes can be observed: (from slowest to fastest) the primary $α$ relaxation, which vitrifies at the glass transition temperature, $T_{gα}$, and two secondary relaxations, named $β^*$ and $β$. MDSC results show how the secondary $β^*$ relaxation also vitrifies, giving rise to an additional glass transition at $T_{gβ^*} < T_{gα}$. In fact, the $α$ and $β^*$ relaxations can be considered as part of a very broad and distributed relaxation. Its main part is the primary $α$ relaxation with a shoulder at the high-frequency region corresponding to a complex secondary $β^*$ relaxation. BDS results about the $β^*$ can be modeled by a main contribution ($β_3^*$) and two additional ones ($β_1^*$ and $β_2^*$) with a weaker dielectric strength. TSDC results show that each single mode of the relaxation has its own glass transition temperature and they are compatible with the structure inferred by BDS. This scenario gives rise to an extended glass transition dually centered in the $T_{gβ^*} \sim 305$ K and $T_{gα} \sim 387$ K. temperatures.

cond-mat.mtrl-sci↗

Comparison of pulsed electroacoustic and thermally stimulated depolarization current measurements of thermally poled PET electrets

We have compared measurements of a set of polyethylene terephthalate (PET) electret samples by means of pulsed electroacoustic method (PEA) and thermally stimulated depolarization current (TSDC) techniques. Experimental parameters such as the combined thermal and electrical history and the electrode type have been selected in order to correlate the polarization mechanisms revealed by TSDC with the charge profile measured by PEA in five different cases. Existing deconvolution procedures for PEA have been improved as a means to enhance the calibration of PEA signals in the case of thin samples. Samples where the $α$ dipolar relaxation or the $ρ$ space charge relaxation is activated show a uniform polarization that manifests itself as image charge at the electrodes. In the experiments where external charge carriers are injected into the sample, the same poling procedure has been tested under different electrode configurations. Charge profiles are qualitatively similar in all of them but the depolarization currents show clearly different behavior. These differences are explained, on the one hand, by the different blocking behavior of vacuum-deposited aluminum electrodes with regards to electrodes with a thin air gap and, on the other hand, by the distinct behavior of electrodes with an air gap for both directions of the charge carriers. Numerical analysis of the polarization of TSDC peaks and charge per unit area of charge profiles supports this interpretation and confirms the relationship between both measurement techniques. All in all, PEA in combination with TSDC turns out to be a useful technique in the study of thermally poled electrets, either in the study of relaxations or of external charge.

cond-mat.mtrl-sci↗

Effects of UV radiation on the charge trapping capability of PET

Poly(ethylene terephthalate) (PET), as most dielectric materials, is able to retain space charge in traps. This allows the material to attain an almost-permanent polarization when space charge is displaced by an external electric field or it is injected from an electrode. We have studied the influence of UV irradiation on the charge trapping capability of PET in samples exposed for different periods of time, up to 10 weeks. The pulsed electro-acoustic technique (PEA) has been used to determine the charge profile. The injected charge that the material is able to retain on the irradiated surface increases with irradiation time. This indicates the formation of new traps. An extensive characterization of these localized states has been performed by thermally stimulated depolarization currents (TSDC) technique. Parameters of charge relaxation kinetics have been obtained fitting spectra of the $ρ_c$ peak, related to injected charge, to the general order kinetics model. A relaxation map analysis shows that relaxation times become more distributed and the activation energy decreases as irradiation time is increased. The activation energy decreases approximately by 10% after 10 weeks of exposition. These results show that UV irradiation creates additional traps on the treated surface, which agrees with PEA results, and that these traps are shallower and their energy depth distribution is wider than in the case of pre-existing traps.

cond-mat.mtrl-sci↗