2001
DOI: 10.1016/s0927-7757(01)00729-4
|View full text |Cite
|
Sign up to set email alerts
|

Thin double layer theory of the wide-frequency range dielectric dispersion of suspensions of non-conducting spherical particles including surface conductivity of the stagnant layer

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1
1

Citation Types

3
121
2

Year Published

2005
2005
2020
2020

Publication Types

Select...
6
2

Relationship

0
8

Authors

Journals

citations
Cited by 108 publications
(127 citation statements)
references
References 18 publications
3
121
2
Order By: Relevance
“…Each sphere i with radius R i is located at the position r i . The polarizability of the sphere i can be expressed as α i = 4π« 0 «R 3 i K i , where K i is the polarization coefficient that can be calculated both analytically (42) and numerically (43). Two spheres representing the lobes on the same dimer are subject to the geometric constraint of fixed bond length L = r i − r j .…”
Section: Significancementioning
confidence: 99%
See 1 more Smart Citation
“…Each sphere i with radius R i is located at the position r i . The polarizability of the sphere i can be expressed as α i = 4π« 0 «R 3 i K i , where K i is the polarization coefficient that can be calculated both analytically (42) and numerically (43). Two spheres representing the lobes on the same dimer are subject to the geometric constraint of fixed bond length L = r i − r j .…”
Section: Significancementioning
confidence: 99%
“…The polarization coefficient K i for particle i is calculated based on the low-frequency thin double-layer polarization theory (42). Fig.…”
Section: Significancementioning
confidence: 99%
“…Only numerical methods are available if this is the physical nature of the system under study. The reader is referred to [13][14][15][16]61,62,[67][68][69]. Figure 7 illustrates how important the effect of SLC on Re[ε * r (ω)] can be for the same conditions as in Fig.…”
Section: Dielectric Dispersion and ζ-Potential: Models Amentioning
confidence: 99%
“…Here, we focus on a simplified model [73] that allows the calculation of the volume-fraction dependence of both the low-frequency value of the real part of δε * r , and of the characteristic time τ α of the α-relaxation. The starting point is the assumption that L D , the length scale over which ionic diffusion takes place around the particle, can be averaged in the following way between the values of a very dilute (L D ≈ a) and a very concentrated (L D ≈ b -a; b is half the average distance between the centers of neighboring particles) dispersion: (67) or, in terms of the particle volume fraction (68) From these expressions, the simplified model allows us to obtain the dielectric increment at low frequency as follows. Let us call (69) the specific (i.e., per unit volume fraction) dielectric increment (for ω → 0).…”
Section: Nondilute Suspensions Of Nonconducting Spherical Particles Wmentioning
confidence: 99%
“…This result thus also indicates that the aggregation happens when the volume fraction is bigger than 0.08. It is well known that relaxation amplitude, for example, ⌬ l ͑= l − m ͒, increases with increasing volume fraction, [35][36][37] but dielectric increment denotes the relaxation amplitude per unit volume and thereby is only decided by the induced dipole coefficient of a single particle. As the volume fraction increases, ion concentration in the bulk solution increases, then more counterions will reside in the stagnant layer of EDL and fewer counterions will be left in the diffuse layer.…”
Section: The Dispersion State Of Palladium Nanoparticle Chain In Tmentioning
confidence: 99%