1981
DOI: 10.1016/0166-6622(81)80016-9
|View full text |Cite
|
Sign up to set email alerts
|

Forces between hydrophobic surfaces in aqueous electrolyte and surfactant solutions containing common air-borne impurities

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1

Citation Types

1
21
0

Year Published

1982
1982
2014
2014

Publication Types

Select...
7
1
1

Relationship

0
9

Authors

Journals

citations
Cited by 34 publications
(22 citation statements)
references
References 10 publications
1
21
0
Order By: Relevance
“…Of particular interest are the force spectroscopy measurements of ⌬x which provide a direct measure of the length scales of a transition state, which were hitherto unknown. For example, for protein folding the distance to the folding transition state, ⌬x f , was found to be between 8 Å (17) and 60 Å (23), in rough agreement with the expected role of long range hydrophobic forces (24). For protein unfolding ⌬x u was found to be much shorter, in the range of 1.7-2.5 Å (16,19,21).…”
mentioning
confidence: 52%
“…Of particular interest are the force spectroscopy measurements of ⌬x which provide a direct measure of the length scales of a transition state, which were hitherto unknown. For example, for protein folding the distance to the folding transition state, ⌬x f , was found to be between 8 Å (17) and 60 Å (23), in rough agreement with the expected role of long range hydrophobic forces (24). For protein unfolding ⌬x u was found to be much shorter, in the range of 1.7-2.5 Å (16,19,21).…”
mentioning
confidence: 52%
“…The values of constants used in the calculation of X-DLVO potentials are listed in Table 5 (Israelachvili, 2011;Israelachvili et al, 1981;Pandya et al, 1998;Verwey and Overbeek, 1948;Yukselen and Kaya, 2003). Fig.…”
Section: Calculation Of Extended Dlvo (X-dlvo) Potentials Between a Fmentioning
confidence: 99%
“…λ is the thickness of the formed layer around the charged surfaces in contact with water (0.3 nm for 1:1 electrolytes and 0.18 nm for 2:1 electrolytes) (Israelachvili, 2011;Israelachvili et al, 1981) and for acid-base interactions in water 0.6 nm was offered by Van Oss, κ is the inverse Debye screening length, and p ξ and s ξ are the surface potentials of the particle and silica surfaces respectively. It should be mentioned that 1:1 electrolyte means the cation to anion charge ratio is 1, such as monovalent salts like NaCl and KCl and 2:1 electrolyte means the ratio of cation to anion charge is 2 like CaCl 2 and MgCl 2 .…”
Section: Calculation Of Extended Dlvo (X-dlvo) Potentials Between a Fmentioning
confidence: 99%
“…The surface structural forces arising upon interaction between objects consisting of quartz and silica glass are most extensively studied. The intensity parameter and the correlation length for the quartz surface are as follows: K = (1-2) × 10 6 J/m 3 and l = 1-1.6 nm in the one-term isotherm [formula (6)] [14,35,36]. However, in our earlier work [37], we estimated the parameters of the structural component V s for different pH values and revealed that, at the isoelectric point, the parameters K and l are considerably larger and, correspondingly, the boundary layers are more extended.…”
Section: Investigation Of Electrical Surface Properties Of Particlesmentioning
confidence: 99%