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Pharmaceutical Manufacturing Handbook: Production and

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906 PHARMACEUTICAL PREFORMULATION<br />

properties (brittleness, elasticity), density, size, shape, surface area, moisture content,<br />

direction <strong>and</strong> rate of shear, storage container dimension, <strong>and</strong> particle – wall interaction<br />

[19] .<br />

It is a property of all powders to resist the differential movement between particles<br />

when subjected to external stresses. A bulk powder is somewhat analogous to<br />

a non - Newtonian liquid, which exhibits plastic fl ow <strong>and</strong> sometimes dilatancy if the<br />

particles being infl uenced by attractive forces. Accordingly, powders may be free<br />

fl owing or cohesive ( “ sticky ” ). The resistance is to free fl ow is due to the cohesive<br />

forces between particles [18] . Three principal types of interparticular forces are<br />

forces due to electrostatic changing, van der Waals forces, <strong>and</strong> forces due to moisture.<br />

Electrostatic forces are dependent on the nature of the particles, in particular<br />

their conductivity. Van der Waals forces are the most important forces for most<br />

pharmaceutical powders. These forces are inversely proportional to the square of<br />

the distance between the two particles <strong>and</strong> hence diminish rapidly as particle size<br />

<strong>and</strong> separation increase. Powders with particles below 50 μ m will generally exhibit<br />

irregular or no fl ow due to van der Waals forces. Particle shape is also important;<br />

for example, the force between a sphere <strong>and</strong> a plane surface is about twice that<br />

between two equal - sized spheres. At low relative humidity, moisture produces a<br />

layer of adsorbed vapor on the surface of particles. Above a critical humidity, typically<br />

in the range 65 – 80%, it will form water liquid bridges between particles. Where<br />

a liquid bridge forms, it will give rise to an attractive force between the particles<br />

due to surface tension or capillary forces. The role of the formulator is to ensure<br />

that the fl ow properties of the powder are suffi cient to enable its use on modern<br />

pharmaceutical equipment, powder hoppers, <strong>and</strong> fl ow through orifi ces in the tablet<br />

production.<br />

It is important that the powder fl ows from the hopper to the fi lling station of the<br />

tablet machine at an appropriate rate <strong>and</strong> without segregation occurring. There are<br />

two types of fl ow that can occur from a powder hopper: core fl ow <strong>and</strong> mass fl ow [2] .<br />

Figure 6 shows the two different powder fl ow patterns in hoppers. When a small<br />

amount of powder is allowed to leave the hopper, there is a defi ned region in which<br />

downward movement takes place <strong>and</strong> the top surface begins to fall in the center. A<br />

core fl ow hopper is characterized by the existence of dead spaces during discharge.<br />

A mass fl ow hopper is one in which all the material is in motion during discharge,<br />

in particular the areas adjacent to the hopper wall. As a small amount of powder is<br />

discharged, the whole bulk of the powder will move downward. Whether core fl ow<br />

or mass fl ow is achieved is dependent on the design of the hopper (geometry <strong>and</strong><br />

wall material) <strong>and</strong> the fl ow properties of the powder.<br />

Powder fl ow into orifi ces is also important when fi lling dies in tablet machines<br />

<strong>and</strong> in certain types of capsule - fi lling machines. For a given material, the fl ow into<br />

or through an orifi ce is dependent on the particle size (Figure 7 ). In general, as the<br />

particle size increases, the powder fl ow rate also increases. However, there is practically<br />

no fl ow if the particle size is below 50 μ m or above 1200 μ m. The Carr index<br />

gives us the guidance for powder fl owability. A lower Carr index of excipients is<br />

more desirable for acceptable powder fl ow. At the lower end of the particle size<br />

range, cohesive forces will result in poor fl ow. Powders with particles below 50 μ m<br />

will generally exhibit irregular or no fl ow due to van der Waals forces. As the particle<br />

size increases, the fl ow rate increases until a maximum is achieved, at an orifi ce<br />

diameter – particle diameter ratio of 20 – 30. As the particle size continues to increase,

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