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Botany · Ch 7 — Transport in Plants

Long Distance Transport of Water

7.3

Long Distance Transport of Water

Why Long-Distance Transport Cannot Rely on Diffusion

A simple classroom demonstration makes the transport route visible: standing a cut twig bearing white flowers in coloured water, then later cutting across the stem, shows the dye has travelled specifically through the vascular bundles — more precisely through the xylem. But why is a dedicated vascular system needed at all, rather than just diffusion?

Diffusion is far too slow over any real distance. Moving a molecule across a single plant cell (roughly 50 micrometres) by diffusion takes about 2.5 seconds — scaling that same rate up to cover just one metre would take an impractically long time. Wherever the site where a substance is made or absorbed is far from where it is actually needed or stored, diffusion (and even active transport across one membrane) simply cannot keep up, so a faster, dedicated transport system is essential.

That system moves substances by mass flow (also called bulk flow): dissolved or suspended substances are carried together, en masse, at the same overall pace — like a river carrying everything within it — driven by a difference in pressure between two points. This is fundamentally different from diffusion, where each substance moves independently according to its own gradient. Bulk flow can be driven by a positive hydrostatic pressure gradient (comparable to water pushed through a garden hose) or by a negative hydrostatic pressure gradient (comparable to suction through a straw). …