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Reservoir and transdermal delivery systems

The total amount of material leaving the membrane, can be determined by calculating the flux at the external surface and integrating with respect to time  [Pg.238]

When the initial concentration within the membrane, Cp o, and the concentration at the external surface of the membrane, Cp,2, are both equal to zero. Equation 9-4 can be simplified considerably  [Pg.239]

The cumulative mass of drug released is plotted versus time for planar reservoir devices with a range of physical characteristics, which are determined principally by the diffusion coefficient for the drug in the polymer and the membrane thickness. The cumulative mass released on the y-axis is scaled by Mq = Ac iL and each of the separate curves represents the normalized mass released at a particular value of Dyp/ l (in min ). If Di p is equal to 1 x 10 cm /s, then these curves correspond to thicknesses (L) of 20, 40, 60, and 120 /xm (from left to right). [Pg.239]

In situations where the concentrations at each surface of the polymer, Cpj and Cp 2, are maintained for a sufficient period, the drug diffusion will achieve steady state, which can be identified by examining the limit of Equation 9-3 as too  [Pg.240]

At steady state, the rate of drug release from the membrane is  [Pg.240]


See other pages where Reservoir and transdermal delivery systems is mentioned: [Pg.236]   


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