Disperse Systems and Suspensions Flashcards

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Vocabulary practice flashcards covering definitions, terminology, electrical double layer properties, DLVO theory, and sedimentation behavior in pharmaceutical disperse systems and suspensions.

Last updated 11:36 AM on 10/5/26
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20 Terms

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Disperse system

A system in which one component (the dispersed phase) is dispersed through another (the continuous phase), where the individual phases do not change state.

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Lipophilic

Having an affinity for, tending to combine with, or capable of dissolving in lipids.

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Hydrophilic

Having an affinity for, tending to combine with, or capable of dissolving in aqueous systems.

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Lyophobic

Having an aversion for the continuous solvent type.

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Lyophilic

Having an affinity for the continuous solvent type.

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Colloidal suspension

A suspension system in which the dispersed solid particles have a diameter up to 1 mˉm1\text{ }\bar{\text{m}}\text{m} (specifically up to 1 mˉm1\text{ }\bar{\text{m}}\text{m} in particle size).

<p>A suspension system in which the dispersed solid particles have a diameter up to $$1\text{ }\bar{\text{m}}\text{m}$$ (specifically up to $$1\text{ }\bar{\text{m}}\text{m}$$ in particle size).</p>
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Coarse dispersion

A suspension system in which the dispersed solid particles have a size greater than 1 mˉm1\text{ }\bar{\text{m}}\text{m}.

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Pharmaceutical suspension

A liquid system consisting of solid drug particles dispersed throughout an insoluble liquid phase, with typical particle sizes ranging from 0.1 mˉm0.1\text{ }\bar{\text{m}}\text{m} to 10 mˉm10\text{ }\bar{\text{m}}\text{m}.

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Chloramphenicol palmitate

An insoluble form of chloramphenicol formulated into an oral suspension to mask the unpleasant taste of the soluble drug form.

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Stern layer

The fixed inner layer of strongly attached counter-ions immediately adjacent to a charged particle surface within the electrical double layer.

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Diffuse layer

The outer region of an electrical double layer where mobile ions decay in concentration toward the bulk solution.

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Zeta potential

The electrical potential existing at the slipping or shear plane between the moving particle with its attached layer and the bulk liquid phase.

<p>The electrical potential existing at the slipping or shear plane between the moving particle with its attached layer and the bulk liquid phase.</p>
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DLVO theory

A theory describing particle interaction where total potential energy (VTV_T) is the additive sum of van der Waals attractive forces (VAV_A) and electrostatic repulsive forces (VRV_R): VT=VA+VRV_T = V_A + V_R.

<p>A theory describing particle interaction where total potential energy ($$V_T$$) is the additive sum of van der Waals attractive forces ($$V_A$$) and electrostatic repulsive forces ($$V_R$$): $$V_T = V_A + V_R$$.</p>
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Primary minimum

A deep minimum in total potential energy at close particle distance where attractive forces dominate, leading to initial flocculation and subsequent coagulation.

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Primary maximum

An energy barrier in DLVO theory where electrostatic repulsive forces exceed attractive forces, preventing particle collision and maintaining deflocculation.

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Secondary minimum

A shallow energy minimum occurring at larger inter-particulate distances where weak attractive forces produce loose aggregates (floccules), representing the desired state for pharmaceutical suspensions.

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Coagulation

An undesirable process where suspended particles collide and adhere closely to form larger permanent aggregates at the primary potential energy minimum.

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Deflocculation

A state in which individual particles remain separate from one another due to repulsive forces exceeding attractive forces at the primary energy maximum.

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Brownian motion

Random thermal motion relevant for suspended particles up to 1 mˉm1\text{ }\bar{\text{m}}\text{m} to 2 mˉm2\text{ }\bar{\text{m}}\text{m} in size that aids diffusion and improves dosage uniformity.

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Stokes' equation

The equation determining gravitational sedimentation velocity (vv) for particles larger than 0.5 mˉm0.5\text{ }\bar{\text{m}}\text{m}: v=d2g(ρ−ρ0)18νv = \frac{d^2 g (\rho - \rho_0)}{18 \nu}.