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Chapter II Solution Growth….<br />

stable equilibrium with its vapor, which is neither super-saturated nor under-<br />

saturated, then a step in equilibrium on the crystal surface will exhibit a<br />

constant mean direction h , inclined at an angle θ to the principle direction<br />

given by the following expression,<br />

tan θ = n+ n- (2.1)<br />

Where, n+ and n- are the numbers of kinks of opposite sign per atom spacing.<br />

The potential energy considerations suggest that at absolute zero<br />

temperature, a step will tend to remain as straight as possible.<br />

As the temperature increases from absolute zero, the component<br />

molecules will start vibrating relative to one another. As the temperature<br />

increases the vibrations become progressively stronger. Now the scenario<br />

changes, some molecules will be able to overcome the energy that binds<br />

them to the crystal and will jump in the space surrounding it. In this manner, a<br />

certain vapor concentration, which is the average number of vapor molecules<br />

per unit volume, will occur in contact with the crystal surface. With comparison<br />

to the other molecules, the molecules positioned at the kink are more prone to<br />

depart from the crystal and vaporize. The molecules at the kinks are bound by<br />

three molecules. Moreover, the molecules on the straight portions of the step<br />

are bound by four molecules and those on the flat portions of the surface by<br />

five. The energy required for a molecule to leave the kink position such as A<br />

in figure (2.3 a) is equal to the evaporation energy W. Two different processes<br />

will occur simultaneously; in one some molecules will be leaving the crystal<br />

and in the other one the molecules will be arriving at the crystal from the<br />

58

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