The dielectric properties of human erythrocytes (red blood cells) suspended in whole blood and in isotonic media at various volume fractions (haematocrits) have been studied in the frequency range 0.2-10 MHz, in which the so-called beta-dispersion due to the Maxwell-Wagner effect is known to occur. The capacitance and conductance at 25 degrees C were measured by an instrument interfaced to a computer. The rectangular sample cavity (1 mi volume) contained four pure gold electrode pins, and the sample could be circulated by a roller pump. The frequency-dependence of the permittivity and conductivity were fitted by non-linear least squares regression. Corrections were applied for non-linearity in the dielectric increment at high haematocrit, and for electrode polarisation when diluting the blood in saline. Data were interpreted in terms of a simple equivalent resistor-capacitor circuit. From the measured haematological values the specific membrane capacitance (C-m) and the conductivities internal and external to the cells (sigma'(i) and sigma'(o) respectively) were estimated. The conductivities behaved in a predictable manner with a mean of 0.458 S.m(-1) (s.d. +/- 0.044) for sigma'(i), whereas the value of C-m (and indeed the actual capacitance of the suspension) was dependent on the amount of plasma present. Hence, in stationary normal (anticoagulated) whole blood samples, C-m was as high as 2.98 mu F.cm(-2) (s.d. +/- 0.40), in contrast to about 0.9 mu F.cm(-2) in blood diluted more than two-fold (to less than 20% hct) in isotonic media. The high value remained when the diluent was plasma. The C-m value returned to a high value when washed erythrocytes were reconstituted with plasma, provided that this was present at above a critical or threshold concentration of about 30 vol% in the medium, irrespective of the haematocrit in the range studied (15-44%). The C-m remained low in serum. When added to washed cells in saline, purified fibrinogen had no effect. However, high C-m values were obtained by fibrinogen supplementation to serum and diluted plasma. Applying moderate flow to whole blood approximately halved its high C-m value in an exponential manner with flow rate, whilst the C-m of washed cells (31-67% hct) slightly increased, and converged to the value for whole blood under flow. We interpret the high apparent C-m value in stationary samples to be a result of rapid cell aggregation in the presence of plasma, where rouleaux formation takes place before visible sedimentation sets in.