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Influence of the Processes Parameters on the Properties of The ...

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Chapter 3.<br />

Analytical Methods and Designs <str<strong>on</strong>g>of</str<strong>on</strong>g> Experiments<br />

tensi<strong>on</strong> causes low wetting properties. A high solid surface energy (mostly hydrophilic), <strong>on</strong> <str<strong>on</strong>g>the</str<strong>on</strong>g> o<str<strong>on</strong>g>the</str<strong>on</strong>g>r hand,<br />

means that <str<strong>on</strong>g>the</str<strong>on</strong>g> interfaces between <str<strong>on</strong>g>the</str<strong>on</strong>g> solid material and <str<strong>on</strong>g>the</str<strong>on</strong>g> air are not favourable in a <str<strong>on</strong>g>the</str<strong>on</strong>g>rmodynamic sense.<br />

<strong>The</strong>refore, high surface energy solids are easily wetted by liquids (cf. Figure 3.20). Wetting <str<strong>on</strong>g>of</str<strong>on</strong>g> a solid<br />

eliminates <str<strong>on</strong>g>the</str<strong>on</strong>g> solid-air interface in favour <str<strong>on</strong>g>of</str<strong>on</strong>g> <str<strong>on</strong>g>the</str<strong>on</strong>g> solid-liquid interface. Interacti<strong>on</strong>s between <str<strong>on</strong>g>the</str<strong>on</strong>g> solid surface<br />

and <str<strong>on</strong>g>the</str<strong>on</strong>g> liquid are resulting in a lowering <str<strong>on</strong>g>of</str<strong>on</strong>g> energy state, which is a more favourable state [Lazghab et al.,<br />

2005; Shaw, 1992].<br />

Figure 3.20: Wetting <str<strong>on</strong>g>of</str<strong>on</strong>g> hydrophilic and hydrophobic samples.<br />

6.2.1 Surface Tensi<strong>on</strong>s <str<strong>on</strong>g>of</str<strong>on</strong>g> Liquids<br />

Different liquids may be used in surface tensi<strong>on</strong> measurements but in general chosen liquids have<br />

relatively low viscosity and low volatility. Van der Waals forces result to <str<strong>on</strong>g>the</str<strong>on</strong>g> additi<strong>on</strong> <str<strong>on</strong>g>of</str<strong>on</strong>g> different<br />

comp<strong>on</strong>ents: d dispersive and nd n<strong>on</strong> dispersive or attractive forces (polar forces and hydrogen b<strong>on</strong>ds). We<br />

can write: = d + nd .<br />

In some apolar molecules, <str<strong>on</strong>g>the</str<strong>on</strong>g>re exist important intermolecular forces but no permanent dipolar<br />

moment. When two molecules are in <str<strong>on</strong>g>the</str<strong>on</strong>g> proximity, instantaneous dipoles interact via L<strong>on</strong>d<strong>on</strong> forces. In<br />

polar molecules, permanent attractive forces create special arrangement increasing stability <str<strong>on</strong>g>of</str<strong>on</strong>g> <str<strong>on</strong>g>the</str<strong>on</strong>g> couple<br />

(Debye and Keesom forces). Interacti<strong>on</strong>s between apolar molecules and polar surface are limited to <str<strong>on</strong>g>the</str<strong>on</strong>g>se<br />

attractive interacti<strong>on</strong>s and nd L polar forces are c<strong>on</strong>stituted by <str<strong>on</strong>g>the</str<strong>on</strong>g> sum <str<strong>on</strong>g>of</str<strong>on</strong>g> <str<strong>on</strong>g>the</str<strong>on</strong>g>se two forces. A special attenti<strong>on</strong><br />

must be paid when a hydrogen atom is linked to an electr<strong>on</strong>egative atom. <strong>The</strong> electr<strong>on</strong>egative atom exerts an<br />

important attractive force <strong>on</strong> <str<strong>on</strong>g>the</str<strong>on</strong>g> unique hydrogen atom and forms hydrogen b<strong>on</strong>ds. Also, even if <str<strong>on</strong>g>the</str<strong>on</strong>g>se types<br />

<str<strong>on</strong>g>of</str<strong>on</strong>g> relati<strong>on</strong>ships fit for <str<strong>on</strong>g>the</str<strong>on</strong>g> dispersi<strong>on</strong> forces, and possibly also for some polar (Debye and Keesom forces),<br />

<str<strong>on</strong>g>the</str<strong>on</strong>g>y are not so good for acid/base and hydrogen b<strong>on</strong>ding.<br />

For this, Oss [2006, 1994] have proposed o<str<strong>on</strong>g>the</str<strong>on</strong>g>r combinati<strong>on</strong>s <str<strong>on</strong>g>of</str<strong>on</strong>g> surface energies. <strong>The</strong> argument is<br />

that <str<strong>on</strong>g>of</str<strong>on</strong>g>ten, <str<strong>on</strong>g>the</str<strong>on</strong>g> polar (Keesom and Debye) forces are weak, and can be included in <str<strong>on</strong>g>the</str<strong>on</strong>g> dispersive<br />

c<strong>on</strong>tributi<strong>on</strong>. <strong>The</strong> "combined" c<strong>on</strong>tributi<strong>on</strong> is denoted by LW (Lifschitz-van der Waals). In additi<strong>on</strong>, <str<strong>on</strong>g>the</str<strong>on</strong>g>re is<br />

a short-range interacti<strong>on</strong> that is caused by acid-base interacti<strong>on</strong>s (hydrogen b<strong>on</strong>ding is a type <str<strong>on</strong>g>of</str<strong>on</strong>g> Acid-Base).<br />

In that case, we write: = LW + AB .<br />

<strong>The</strong>re are several comm<strong>on</strong> methods described in <str<strong>on</strong>g>the</str<strong>on</strong>g> literature for measuring <str<strong>on</strong>g>the</str<strong>on</strong>g> surface tensi<strong>on</strong> <str<strong>on</strong>g>of</str<strong>on</strong>g><br />

liquids. <strong>The</strong> surface tensi<strong>on</strong>s <str<strong>on</strong>g>of</str<strong>on</strong>g> liquids can be directly determined by measuring <str<strong>on</strong>g>the</str<strong>on</strong>g> surface force with a Du<br />

Noüy ring or a Wilhelmy plate for example. <strong>The</strong> determinati<strong>on</strong> <str<strong>on</strong>g>of</str<strong>on</strong>g> surface energy is necessary indirect In<br />

literature, <str<strong>on</strong>g>the</str<strong>on</strong>g>re are several methods to measure <str<strong>on</strong>g>the</str<strong>on</strong>g>ir c<strong>on</strong>tact angle with a liquid [Petrie, 2000]. By using a<br />

given model, we <strong>on</strong>ly can estimate <str<strong>on</strong>g>the</str<strong>on</strong>g>ir surface energy.<br />

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