Volume (J,) and solute (J,) fluxes through Phaseolus root systems were observed over a 24-hour period. The volume flux was varied in a pressure chamber by altering the hydrostatic pressure in 10 steps, from 0 to OA meppascals. All root systems showed strong diurnal peaks in volume flux. The five transport coefficients (,, w, J,*, L., and x*) were estimated from a nonlinear least squares algorithm. Analysis of the data revealed that all the coefficients exhibited a diurnal rhythm. When the total differential of the volume flux was considered it was possible to show that the diurnal changes in volume flux were due to a complex interaction between the diurnally shifting coefficients with the role of each highly dependent on the level of volume flux. At low volume fluxes, w, J,*, and T* accounted for nearly all the diurnal change in volume flux.At high volume fluxes, however, the major influence shifted to L. and i*, while w and J,* became relatively unimportant. Thus, w* was the only coefficient of interest across the entire range of J, and appeared to be the single most important one in determining the diurnal rhythm of J, under conditions of a constant applied pressure.Since the first report of Hofmeister in 1862 (see Vaadia [27]) of the diurnal fluctuations of both root pressure and exudation rates, the phenomenon has been repeatedly demonstrated (more recently [11-13, 18, 21, 24, 27 (0600-2000) at the top of the plants. The plants, selected for size at the time of the experiments, averaged about 2230 cm2 projected leaf area as measured with a LI-CORI model 3100 leaf area meter, and about 3150 cm2 root surface area. Each root system was decapitated and sealed into a pressure chamber with the cut stump protruding through the lid and the roots surrounded by aerated nutrient solution (70 = 35 kPa)2 as previously described (5). The plants were placed in the chamber at about 1600 h, brought to the specified pressure and temperature (25 ± 0.25C), and allowed to equilibrate. Beginning at midnight, measurements of volume flow and ion flow from the cut stump were started and continued at 10-min intervals for the next 24 h. The volume flow was measured by weighing the exudate on an electronic balance. Concentration of the exudate was estimated from the electrical conductivity and expressed as KCI equivalents. The ion flow was then calculated as the product of the volume flow and the concentration. Using Newman's technique (19) on each root size class, surface areas were measured as described earlier (7)