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paraffin wax deposition and fouling

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For breakdown <strong>and</strong> removal to occur some transformation of the<br />

weakness).<br />

weakness the <strong>wax</strong> deposit breaks down <strong>and</strong> is removed from the tube<br />

— 67 —<br />

istic r<strong>and</strong>om fuctuations in <strong>paraffin</strong> deositicn <strong>and</strong> foulinT.<br />

shear forces. In <strong>paraffin</strong> <strong>wax</strong>es there exists a solid crystal<br />

in the establishment of regular crystal matrices, that is, time being<br />

<strong>wax</strong> deposit structure may take place, reducing its resistance to<br />

required for orientation. As the <strong>deposition</strong> is a rapid process there<br />

is added opportunity for weakness. As a result of cohesion loss or<br />

On breakdo’. <strong>and</strong> removal of deposits? only strongly held Crystals<br />

responsible for the creation of weak planes in the <strong>paraffin</strong> <strong>wax</strong><br />

surface, leaving a thin granular layer. (The granular layer probably<br />

It was considered possible that some similar transition might be<br />

represents a well oriented matrix of crystals with few planes of<br />

at low temperatures where the <strong>wax</strong> transformed into a new crystal<br />

transition (section 2.2.2) at temperatures below the melting point.<br />

lubricating layer around them. The deoosit will therefore be most<br />

kerosene solvent will be exuded from the crystals <strong>and</strong> form a<br />

near a <strong>deposition</strong> surface after rapid initial <strong>deposition</strong>, the<br />

deoosits. These weak planes could be formed near the rube waZ<br />

stresses as deposits build up, are probably the main factors<br />

structure.<br />

will ‘cc left on the tube surface, giving rise to the granular<br />

rapid cooling. As regular denser crystal structures are formed<br />

systems <strong>and</strong> strong structural network than crystals formed under<br />

structure. As sho in section 2.2.2. crystals formed under slow<br />

likely to break where transition has occurred near the tube wall.<br />

cooling were observed to have less tendency to form solvated<br />

causlnf the breakdon ana removal that give rise to the character<br />

The creation of planes of weakness <strong>and</strong> the increases in shear

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