Based on the rapid progression in understanding the precise pathobiology underlying various neurological diseases, a number of promising new putative therapeutics have been developed for specific disorders that have been ineffectually treated or are not currently treatable. While these agents have been successful in reversing disease-related pathology in vitro and/or in animal models, they have not been successfully translated into clinically effective therapies. One of the largest obstacles to the successful conversion of putative therapeutics into effective treatments is the inability to deliver these agents past the CNS blood-brain barrier (BBB) in a reliable, targeted, and homogeneous way using currently available approaches for drug delivery, including systemic delivery, intrathecal and/or intraventricular distribution, and polymer implantation. 6,15,47,67,80 To surmount the limitations of available CNS drug delivery techniques, targeted direct perfusion of regions of the nervous system using the convection-enhanced delivery (CED) of infusate is increasingly used in research models of neurological disease and in clinical trials to treat neurological disorders. Because infusate is driven by a hydrostatic pressure differential (bulk flow), 7,67 CED can be used to bypass the BBB and distribute putative therapeutics to targeted regions. Further, convective bulk flow properties allow for homogeneous and reproducible perfusion of variably sized regions of the nervous system using compounds with a wide range of molecular weights. The development of co-infused surrogate imaging tracers now permits noninvasive real-time monitoring of convective delivery. We review the biophysical principles of convective flow and the technology, properties, and clinical applications of convective delivery in the CNS.
Biophysical Principles of Convective FlowWithin the extracellular space of the CNS, fluids and agents move either by diffusion or by bulk flow. Diffusive flux (J) depends on the concentration gradient (āC, where ā is the gradient operator), as stated by Fick's law, J = -DāC, where tissue diffusivity (D) is highly dependent on the molecular weight of the molecule. Unfortunately, effective diffusion times are long for macromolecular therapeutic agents, and transport depends on large concentration gradients, often requiring unacceptably high Convection-enhanced delivery (CED) is a bulk flow-driven process. Its properties permit direct, homogeneous, targeted perfusion of CNS regions with putative therapeutics while bypassing the blood-brain barrier. Development of surrogate imaging tracers that are co-infused during drug delivery now permit accurate, noninvasive real-time tracking of convective infusate flow in nervous system tissues. The potential advantages of CED in the CNS over other currently available drug delivery techniques, including systemic delivery, intrathecal and/or intraventricular distribution, and polymer implantation, have led to its application in research studies and clinical trials. The authors review t...