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Case II drug transport with axial and radial release from a cylinder

After integration of (4.7), we obtain the following equations as well as the time for which each one is operating  [Pg.62]

This means that the smaller dimension of the cylinder (p or L) determines the duration of the phenomenon. [Pg.62]

The amount of drug released at any time t is given by the following mass-balance equation  [Pg.62]

Substituting (4.8) into (4.9), the following expression for mass q (t) as a function of time t is obtained  [Pg.62]


Figure 4.2 Case II drug transport with axial and radial release from a cylinder of height 2L and radius p at t = 0. Drug release takes place from all sides of the big cylinder. The drug mass is contained in the grey region. After time t the height of the cylinder is reduced to 2L and its radius to p (small cylinder). Figure 4.2 Case II drug transport with axial and radial release from a cylinder of height 2L and radius p at t = 0. Drug release takes place from all sides of the big cylinder. The drug mass is contained in the grey region. After time t the height of the cylinder is reduced to 2L and its radius to p (small cylinder).
This equation describes the entire fractional release curve for Case II drug transport with axial and radial release from a cylinder. Again, (4.10) indicates that the smaller dimension of the cylinder p or L) determines the total duration of the phenomenon. When p> L, (4.10) can be approximated by... [Pg.63]




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