Petiole cooling is known to cause a temporary decline in mass transfer rate in sugar beet (2,8). The observed recovery of mass transfer rate may be explained in a number of ways. Increased loading in the source leaf might compensate for low velocity by increased solute concentration, or translocation velocity might return to the original rate because of a steepened pressure gradient, a reversal of the cause of increased resistance to flow, or a recovery in the metabolic process which supplies the energy to drive the translocation process. This report provides evidence that inhibition of mass transfer during petiole cooling is a result of decreased translocation velocity and that recovery occurs mainly because of a restoration of velocity.Sugar beet plants (Beta vulgaris, monogerm hybrid [SL129 X 133] ms X [SP6322-0]) and bean plants (Phaseolus vulgaris, var. Black Valentine) were grown in a controlled environment cabinet as described previously (3). Steady state labeling with 14CO2 was used to measure mass transfer rate (3). Labeled CO2 was supplied to a mature sugar beet leaf, and arrival was followed in a young leaf whereas in bean the 14CO2 was supplied to a primary leaf, and arrival of translocate was monitored using the terminal leaflet of a young trifoliate leaf (4).Velocity was measured by a pulse labeling technique for labeling photosynthate (5). As a consequence, it was necessary to devise a pulse labeling method for studying mass transfer in the same plants used for velocity measurements. The proportion of a 14CO pulse which was translocated out of the source leaf during the first 45 min was used as a measure of the relative mass transfer rate. The excellent agreement of the time course obtained by the two methods permitted use of pulse labeling to compare both mass transfer rate and apparent velocity in the same plant (Figs. 1, 2). The apparent velocity was based on the time required for first detection of a count rate above background in the sink leaf. The method gives an apparent velocity which includes the time for loading in the source leaf, for transit from source to sink, and the time required for the accumulated 14C translocate to reach the threshold of detection. The time required for the "4C pulse to reach a detectable level in the sink is related directly to the amount of labeled translocate which is exchanged out of the translocation system and is inversely related to the specific radioactivity of the 14C translocate. As the specific radioactivity of the translocate is increased, the time required to reach the detection threshold is shortened and the apparent velocity approaches a limit which includes principally loading time plus transit time (5). In the velocity measurements we used approximately 50 lic 14C per I This work was supported by United States Atomic Energy Commission Grant AT 11-1-2015.pulse, which was found to give a minimal amount of time for reaching the detection threshold. Loading constitutes a constant and presumably relatively small part of the time between supplying o...