my comsol work

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    Introduction

    This example describes the operation of a drug delivery system that supplies

    a variable

    concentration of a water soluble drug. A droplet with a xed volume of water

    travels

    down a capillary tube at a constant velocity. Part of the capillary wall consists

    of a

    permeable membrane separating the interior of the capillary from a

    concentrated

    solution of the drug. As the drop passes by the membrane, the drug dissolves

    into the

    water. To model this process a constant ux of the drug is assumed on the

    capillary

    wall for the duration of its contact with the membrane. By altering the droplet

    velocity,

    the nal concentration of the drug in the drop can be adusted.

    WORKING

    !n the "odel #i$ard window, clic% the &' Axisymmetric button.

    & !n the (elect Physics tree, select )luid )low*"ultiphase )low*Two+Phase)low, "oving

    "esh*aminar Two+Phase )low, "oving "esh -tpfmm.

    / 0lic% the Add button.

    1 0lic% the (tudy button.

    2 !n the tree, select Preset (tudies*Time 'ependent.

    3 0lic% the 'one button.

    GEOMETRY

    !mport the model geometry.

    4 !n the "odel Builder window, under 0omponent 4 clic% 5eometry 4.

    & !n the 5eometry settings window, locate the 6nits section.

    / )rom the ength unit list, choose mm.

    Import

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    4 7n the 8ome toolbar, clic% !mport.

    & !n the !mport settings window, locate the !mport section.

    / 0lic% the Browse button.

    1 Browse to the model9s "odel ibrary folder and double+clic% the le

    drug:delivery:mm.mphbin.

    2 0lic% the !mport button.

    DEFINITION

    "odel 'enition

    The droplet is visible near the top of the geometry. The hori$ontal lines

    across the capillary are included to assist with meshing.

    The drop is initially stationary at the top of the domain, but accelerates

    rapidly to a constant velocity before it reaches the permeable membrane.

    The

    permeable part of the capillary is not visible as part of the geometry as it is

    represented

    by a function applied to the boundary condition. !t is located between $;

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    dru!,

    - Mo$"% d"$i*"rd t'rou!' dru! incr"&%"% .it' tim",

    - Mo$"% d"$i*"r"d d"cr"&%"% .it' t'" *"$ocit/ o+ t'" dru!drop$"t,