Pressure-dependent dielectric properties in a polyurethane elastomer

The dielectric responses of polyurethane films were investigated in the pressure range from atmospheric to 20 kpsi and in the frequency range from 0.05 Hz to 4 KHz at −50, 0, 29, 50, and 80 ◦ C, where T g is close to −15 ◦ C (α-relaxation) and where the glass temperature of the chain extender is abo...

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Published inJournal of the Korean Physical Society Vol. 70; no. 7; pp. 699 - 705
Main Authors Hwang, Seung Won, Shin, Jae Sup, Shin, Min Jae, Kim, Chy Hyung
Format Journal Article
LanguageEnglish
Published Seoul The Korean Physical Society 01.04.2017
Springer Nature B.V
한국물리학회
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ISSN0374-4884
1976-8524
DOI10.3938/jkps.70.699

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Abstract The dielectric responses of polyurethane films were investigated in the pressure range from atmospheric to 20 kpsi and in the frequency range from 0.05 Hz to 4 KHz at −50, 0, 29, 50, and 80 ◦ C, where T g is close to −15 ◦ C (α-relaxation) and where the glass temperature of the chain extender is about 80 ◦ C (I-relaxation). When a higher pressure was applied to the material, a lower dielectric constant (k’ ) was obtained owing to the suppression of polarization motions by the external pressure. However, k’ increased with rising pressure at temperatures above 50 ◦ C and at high frequencies due to the predominant thermal effect expanding the film outwards, where a dispersive α-relaxation occurred. Both α- and I-relaxations followed the pressure-frequency superposition principle with a different shifting factor, a ( p ), where the α-relaxation showed a faster migration of the relaxation time with changing pressure and a ( p ) values larger than those of I-relaxation. The two relaxations observed at 29 ◦ C demonstrated linear relations between 1/k’ and pressure and between ln a ( p ) and pressure, regardless of the film thickness.
AbstractList The dielectric responses of polyurethane films were investigated in the pressure range from atmospheric to 20 kpsi and in the frequency range from 0.05 Hz to 4 KHz at −50, 0, 29, 50, and 80 C, where Tg is close to −15 C (-relaxation) and where the glass temperature of the chain extender is about 80 C (I-relaxation). When a higher pressure was applied to the material, a lower dielectric constant (k0) was obtained owing to the suppression of polarization motions by the external pressure. However, k0 increased with rising pressure at temperatures above 50 C and at high frequencies due to the predominant thermal effect expanding the film outwards, where a dispersive -relaxation occurred. Both - and I-relaxations followed the pressure-frequency superposition principle with a different shifting factor, a(p), where the -relaxation showed a faster migration of the relaxation time with changing pressure and a(p) values larger than those of I-relaxation. The two relaxations observed at 29 C demonstrated linear relations between 1/k0 and pressure and between ln a(p) and pressure, regardless of the film thickness. KCI Citation Count: 0
The dielectric responses of polyurethane films were investigated in the pressure range from atmospheric to 20 kpsi and in the frequency range from 0.05 Hz to 4 KHz at −50, 0, 29, 50, and 80 ◦ C, where T g is close to −15 ◦ C (α-relaxation) and where the glass temperature of the chain extender is about 80 ◦ C (I-relaxation). When a higher pressure was applied to the material, a lower dielectric constant (k’ ) was obtained owing to the suppression of polarization motions by the external pressure. However, k’ increased with rising pressure at temperatures above 50 ◦ C and at high frequencies due to the predominant thermal effect expanding the film outwards, where a dispersive α-relaxation occurred. Both α- and I-relaxations followed the pressure-frequency superposition principle with a different shifting factor, a ( p ), where the α-relaxation showed a faster migration of the relaxation time with changing pressure and a ( p ) values larger than those of I-relaxation. The two relaxations observed at 29 ◦ C demonstrated linear relations between 1/k’ and pressure and between ln a ( p ) and pressure, regardless of the film thickness.
The dielectric responses of polyurethane films were investigated in the pressure range from atmospheric to 20 kpsi and in the frequency range from 0.05 Hz to 4 KHz at −50, 0, 29, 50, and 80 ◦ C, where Tg is close to −15 ◦ C (α-relaxation) and where the glass temperature of the chain extender is about 80 ◦ C (I-relaxation). When a higher pressure was applied to the material, a lower dielectric constant (k’ ) was obtained owing to the suppression of polarization motions by the external pressure. However, k’ increased with rising pressure at temperatures above 50 ◦ C and at high frequencies due to the predominant thermal effect expanding the film outwards, where a dispersive α-relaxation occurred. Both α- and I-relaxations followed the pressure-frequency superposition principle with a different shifting factor, a(p), where the α-relaxation showed a faster migration of the relaxation time with changing pressure and a(p) values larger than those of I-relaxation. The two relaxations observed at 29 ◦ C demonstrated linear relations between 1/k’ and pressure and between ln a(p) and pressure, regardless of the film thickness.
Author Kim, Chy Hyung
Hwang, Seung Won
Shin, Jae Sup
Shin, Min Jae
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Keywords Pressure-frequency superposition principle
Shifting factor
Hydrostatic pressure
Dielectric relaxation
Polyurethane elastomer
Language English
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Snippet The dielectric responses of polyurethane films were investigated in the pressure range from atmospheric to 20 kpsi and in the frequency range from 0.05 Hz to 4...
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SubjectTerms Dielectric properties
Elastomers
External pressure
Film thickness
Frequency ranges
Mathematical and Computational Physics
Particle and Nuclear Physics
Physics
Physics and Astronomy
Polyurethane resins
Pressure dependence
Pressure effects
Relaxation time
Superposition (mathematics)
Temperature effects
Theoretical
물리학
Title Pressure-dependent dielectric properties in a polyurethane elastomer
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