Transvascular and interstitial fluid movements are involved in many im
portant biological processes such as convective macromolecular transpo
rt and contribute to the mechanical behavior of tissue. Although intim
ately coupled, there is a tendency in the literature to regard these t
wo fluid-transport mechanisms separately; if the interaction is consid
ered, the description is usually confined to the local level (e.g., tr
ansvascular or interstitial perivascular). A general framework present
ed here combines transvascular and interstitial fluid movement with th
e mechanics of soft tissue and integrates macro- and microscopic views
of the phenomena. On the macroscopic level interstitial fluid transpo
rt is described by adapting the field equations of the poroelastic the
ory using average field variables defined on a scale of several blood
vessel diameters (approximate to 1 mm), while transvascular transport
is described by a generalized Starling's law. As an example, the model
equations have been specialized for a spherical solid tumor and an an
alytical solution is presented for the transient redistribution of int
erstitial fluid following a rapid change in vascular pressure or flow.
The model describes the overall average profiles of the interstitial
fluid pressure and velocity, as well as the dilatation, displacement a
nd stress of the solid matrix. Moreover on a smaller length scale the
model can describe the local fluid movement (perivascular) using the a
verage field variables as boundary conditions. The basic theory provid
es new insight into understanding the fluid transport in biological ti
ssues and a valuable tool for determining relevant fluid-transport par
ameters. Implications for improving drug delivery to solid tumors are
also discussed.