Abstract
In this chapter broadband dielectric spectroscopy (BDS) is employed to polymeric blend systems. In its modern form BDS can cover an extraordinary broad frequency range from 10−4 to 1012 Hz. Therefore, molecular and collective dipolar fluctuations, charge transport, and polarization effects at inner phase boundaries can be investigated in detail including its temperature dependence. In the first part of the chapter, the theoretical basics of dielectric spectroscopy are briefly introduced covering both static and dynamic aspects. This section is followed by short description of the various experimental techniques to cover this broad frequency range. To provide the knowledge to understand the dielectric behavior of polymeric blend systems, the dielectric features of amorphous homopolymers are discussed in some detail. This concerns an introduction of the most important relaxation processes observed for these polymers (localized fluctuations, segmental dynamics related to the dynamic glass transition, chain relaxation), a brief introduction to the conductivity of disordered systems as well as polarization effects at phase boundaries. Theoretical models for each process are shortly discussed. In the last paragraph the dielectric behavior of polymer blends is reviewed where special attention is paid to binary systems for the sake of simplicity. In detail the dielectric behavior of binary miscible blends is described. The two most important experimental facts like the broadening of the dielectric relaxation spectra and the dynamic heterogeneity of the segmental dynamics are addressed in depth. Appropriate theoretical approaches like the temperature-driven concentration fluctuation model and the self-concentration idea are introduced.
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List of Important Symbols and Abbreviations
- aT
-
Shift factor
- C
-
Concentration
- C1, C2
-
Parameters of the WLF equation
- D
-
Dielectric displacement
- E
-
Electric field strength
- EA, ΔE
-
Activation energy, barrier heights
- f
-
Frequency
- fi
-
Relaxation rate at maximal loss, i = β, α, n
- f∞i
-
Preexponential factor, i = β, α, n
- Φi
-
Volume fraction
- ϕi
-
Weight fraction
- g, gintra
-
Dipolar correlation coefficients
- ΔGM
-
Free energy of mixing
- Γ*
-
Reflection coefficient
- I, J
-
Current, Current density
- kB
-
Boltzmann constant, kB = 1.380662 10−23 J K−1; kB = R/NA
- M, MW
-
Molecular weight, weight average
- NA
-
Avogadro number (NA = 6.022 1023 mol−1)
- R
-
Gas constant R = 8.314 kJ mol−1
- SC
-
Configurational entropy
- ΔSM
-
Mixing entropy
- σ*, σ′, σ′
-
Complex conductivity, real and imaginary part
- T
-
Temperature
- T0
-
Vogel temperature, ideal glass transition temperature
- Tg
-
Glass transition temperature
- tan δ
-
Dielectric loss tangent
- β, γ
-
Shape parameter of the HN function
- ε0
-
Permittivity of vacuum (ε0 = 8.854 10−12 As V−1 m−1)
- ε*, ε′, ε′
-
Complex dielectric function, real and imaginary part
- Δεi
-
Dielectric relaxation strength, i = β, α, n,
- ζ
-
Monomeric friction coefficient
- ξ
-
Correlation length
- κ
-
Flory/Huggins interaction parameter
- μ
-
Dipole moment
- ω
-
Angular frequency (ω = 2*π*f)
- τ
-
Relaxation time
- τHN
-
Relaxation time of the HN function
- τe
-
Time constant for conduction
- PEO
-
Poly(ethylene oxide)
- PI
-
Cis-1,4-Polyisorene
- PMMA
-
Poly(methyl methacrylate)
- PPG
-
Poly(propylene glycol)
- PS
-
Polystyrene
- PVAC
-
Poly(vinyl acetate)
- PVME
-
Poly(vinyl methylether)
- PoClS
-
Poly(o-chlorostyrene)
- PVC
-
Poly(vinyl chloride)
- U
-
Voltage, different meanings
- Z *S (ω); Z *R (ω)
-
Sample impedance; Reference impedance
- <…>
-
Correlation function; Averaged quantities
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Yin, H., Schönhals, A. (2014). Broadband Dielectric Spectroscopy on Polymer Blends. In: Utracki, L., Wilkie, C. (eds) Polymer Blends Handbook. Springer, Dordrecht. https://doi.org/10.1007/978-94-007-6064-6_14
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