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Drugs and the pharmaceutical sciences

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6 Quigley<br />

This inertial force depends directly upon <strong>the</strong> mass of <strong>the</strong> particle, <strong>and</strong> <strong>the</strong> square of its<br />

velocity. It is, <strong>the</strong>refore, more important with heavier particles. The inertial force is<br />

attenuated by <strong>the</strong> viscosity of <strong>the</strong> fluid, <strong>and</strong> is consequently influenced by temperature<br />

which is inversely related to viscosity. For this reason it is less effective in liquid than in<br />

gaseous contexts (Fig. 6).<br />

Brownian Motion<br />

Smaller particles, less heavy, are less influenced by inertia. However, <strong>the</strong>y are more<br />

affected by Brownian motion wherein <strong>the</strong>y are vectored from <strong>the</strong> fluid pathway to <strong>the</strong><br />

pore surface by collisions with <strong>the</strong> fluid’s molecules. The result is retention of <strong>the</strong><br />

particles by <strong>the</strong> filter surfaces <strong>the</strong>y impact.<br />

At all temperatures above absolute zero <strong>the</strong> various sections of all molecules are in<br />

constant motion; <strong>the</strong> various bonds being flexed, rotated, stretched, etc. The higher <strong>the</strong><br />

temperature, <strong>the</strong> greater <strong>the</strong> amplitude of <strong>the</strong> molecular motion. The significance of<br />

absolute zero is that only at that temperature or below is all molecular movement frozen.<br />

In <strong>the</strong>ir frenetic activity, <strong>the</strong> fluid molecules collide, perhaps repeatedly, with suspended<br />

particles. The latter are directed to new directions of travel within <strong>the</strong> fluid stream. As a<br />

result of <strong>the</strong>ir induced r<strong>and</strong>om <strong>and</strong> erratic movements, <strong>the</strong> particles have opportunities to<br />

encounter pore surfaces. This is <strong>the</strong> nature of Brownian or diffusional interception. It is<br />

favored by small size particles, <strong>and</strong> by <strong>the</strong> lower viscosities of <strong>the</strong> suspending fluids.<br />

Adsorptive Interactions<br />

The donating of electrons by one atom, possibly already part of a molecule, to ano<strong>the</strong>r<br />

one results in a strong bonding between <strong>the</strong> two atoms. This is <strong>the</strong> nature of <strong>the</strong> chemical<br />

bond. The same occurs from <strong>the</strong> sharing of electrons between two atoms. The atomic<br />

interactions resulting from electron sharing is called covalent bonding. By convention,<br />

electrons each represent a full negative charge. Thus, possessing more electrons than in<br />

its neutral state confers a negative charge upon an atom. Having fewer than <strong>the</strong> normal<br />

number of electrons in its possession gives an atom a plus or positive electrical charge.<br />

Matrix<br />

thick porous<br />

Depth straining<br />

FIGURE 6 Inertial impaction.<br />

Inertial<br />

impaction<br />

Surface<br />

retention<br />

“Tortuous<br />

path” pore<br />

Direction<br />

of flow

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