Abstract:Friction and adhesion hysteresis experiments were
carried out on fluorocarbon surfactant monolayer-coated
surfaces using the surface forces apparatus. Measurements were
made as a function of temperature, load,
sliding velocity, and relaxation time, and the resulting properties are
contrasted with those of hydrocarbon
monolayers and also with bulk fluorocarbon surfaces (e.g., Teflon,
PTFE). The dynamic adhesion
measurements show that the adhesion hysteresis and friction of
fluorocarbon monolayer-coated surfaces… Show more
“…In order to investigate the static friction behaviors of confined lubricants, SFA stop-start experiments were performed by a number of authors [14,15,[18][19][20]30]. Figure 5 shows the example of a SFA stop-start experiment for the molecularly confined film of an asymmetric liquid lubricant, 1,3-dimethylbutyl octyl ether (DBOE) in the hard-wall thickness (D = 1.7 nm) [18,20].…”
Section: Static Friction (Stiction) Of Confined Liquid Lubricantsmentioning
confidence: 99%
“…Hence, the nucleation time τ n is the time required for the conformational (orientational) rearrangements of molecules from shear-ordered configuration to disordered liquid-like configuration and then to a static solid-like structure. The τ n is of course dependent on molecular mobility, and increasing applied load or decreasing temperature generally increases τ n because both effects decrease the molecular mobility in the film [14,18,20,30] (see Figure 6a). The brief mechanism discussed here is rather suitable to describe the behavior of asymmetric liquid molecules; symmetric liquids include some different features (discussed below).…”
Section: Static Friction (Stiction) Of Confined Liquid Lubricantsmentioning
When liquid molecules are confined in a narrow gap between smooth surfaces, their dynamic properties are completely different from those of the bulk. The molecular motions are highly restricted and the system exhibits solid-like responses when sheared slowly. This solidification behavior is very dependent on the molecular geometry (shape) of liquids because the solidification is induced by the packing of molecules into ordered structures in confinement. This paper reviews the measurements of confined structures and friction of symmetric and asymmetric liquid lubricants using the surface forces apparatus. The results show subtle and complex friction mechanisms at the molecular scale.
“…In order to investigate the static friction behaviors of confined lubricants, SFA stop-start experiments were performed by a number of authors [14,15,[18][19][20]30]. Figure 5 shows the example of a SFA stop-start experiment for the molecularly confined film of an asymmetric liquid lubricant, 1,3-dimethylbutyl octyl ether (DBOE) in the hard-wall thickness (D = 1.7 nm) [18,20].…”
Section: Static Friction (Stiction) Of Confined Liquid Lubricantsmentioning
confidence: 99%
“…Hence, the nucleation time τ n is the time required for the conformational (orientational) rearrangements of molecules from shear-ordered configuration to disordered liquid-like configuration and then to a static solid-like structure. The τ n is of course dependent on molecular mobility, and increasing applied load or decreasing temperature generally increases τ n because both effects decrease the molecular mobility in the film [14,18,20,30] (see Figure 6a). The brief mechanism discussed here is rather suitable to describe the behavior of asymmetric liquid molecules; symmetric liquids include some different features (discussed below).…”
Section: Static Friction (Stiction) Of Confined Liquid Lubricantsmentioning
When liquid molecules are confined in a narrow gap between smooth surfaces, their dynamic properties are completely different from those of the bulk. The molecular motions are highly restricted and the system exhibits solid-like responses when sheared slowly. This solidification behavior is very dependent on the molecular geometry (shape) of liquids because the solidification is induced by the packing of molecules into ordered structures in confinement. This paper reviews the measurements of confined structures and friction of symmetric and asymmetric liquid lubricants using the surface forces apparatus. The results show subtle and complex friction mechanisms at the molecular scale.
“…That is, these interferograms look identical for increasing and decreasing voltages. Yet, hydrocarbon and fluorocarbon-tailed monolayer films deposited by the Langmuir-Blodgett technique exhibit adhesion hysteresis in surface force apparatus experiments [29,30], as well as in similar experiments between polydimethyl siloxane and fluoroalkylsiloxane coated mica [31]. The proposed mechanisms for the hysteresis are chain interdigitation when surfactant films are in an amorphous state [29], and molecular as well as submolecular changes in a fluorocarbon surfactant due to the bulky fluorocarbon groups [30].…”
Section: Discussionmentioning
confidence: 99%
“…These results gives us information on the average amount of water on the surface, which we interpret in terms of a classical BET adsorption isotherm [30]. For the hydrophilic Si02 surface below 50% RH, a sub-monolayer film of water exists on the surface.…”
Section: Ldrd Fundamental Mechanisms Of Micrornachine Reliability Samentioning
confidence: 91%
“…We shall refer to these as the hydrophobic samples. ODTS has been investigated as a promising molecule for minimization of adhesion in MEMS [8,22,29,30]. The head group of the organosilane is hydrolyzable, which facilitates the formation of covalent siloxane bonding to the substrate hydroxyl groups as well as between neighboring silane molecules to form a well attached organosilane layer [31].…”
Section: A) Specimen Fabrication and Surface Treatmentmentioning
The sections in this article are
Introduction
Chemical Modification of
AFM
Tips
Sample Surfaces with Various Patterns
FFM
and
PFM
‐
AFM
Measurements
Friction and Adhesive Force Imaging as
CFM
CFM
of Patterned Surface Prepared by the
LB
Method
Friction Force Map in Phase‐separated
HC
‐
FC
Mixed
LB
Films with
Ca
2+
Counterions
CFM
of Patterned Surfaces Prepared by µ‐
CP
Effect of Experimental Environments and Surface Roughness
Other Approaches for
CFM
Concluding Remarks
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