Wettability of the leaf surface, surface tension of the liquid, and stomatal morphology control penetration of stomata by liquids. The critical surface tension of the lower leaf surface of Zebrina purpusii Bruckn. was estimated to be 25 to 30 dyne cm-'. Liquids having a surface tension less than 30 dyne cm'i gave zero contact angle on the leaf surface and infiltrated stomata spontaneously while liquids having a surface tension greater than 30 dyne cm-' did not wet the leaf surface and failed to infiltrate stomata. Considering stomata as conical capillaries, we were able to show that with liquids giving a finite contact angle, infiltration depended solely on the relationship between the magnitude of the contact angle and the wall angle of the aperture. Generally, spontaneous infiltration of stomata will take place when the contact angle is smaller than the wall angle of the aperture wall. The degree of stomatal opening (4, 6, 8, or 10 /m) was of little importance.Cuticular ledges present at the entrance to the outer vestibule and between the inner vestibule and substomatal chamber resulted in very small if not zero wall angles, and thus played a major role in excluding water from the intercellular space of leaves. We show why the degree of stomatal opening cannot be assessed by observing spontaneous infiltration of stomata by organic liquids of low surface tension.tionship between any of these parameters and penetration has been generally poor. In this paper we present a systematic assessment of stomatal penetration by liquids based on the theory of capillary rise. THEORY When a liquid enters a capillary of circular cross-section the pressure difference (P) across the liquid meniscus is represented by equation 1,where '/L represents the surface tension of the liquid and R, and RI the principal radii of curvature of the liquid meniscus (1). In a narrow cylindrical capillary the meniscus is a segment of a sphere; R, and R, are equal and can be expressed in terms of the advancing contact angle (09) (4,22,27) unless external pressure is applied (6, 7). Some organic liquids, however, are known to penetrate readily, which led to attempts to estimate the degree of stomatal opening from substomatal penetration of certain organic liquids (18,22,25). Reports concerned with the effect of surfactants on promoting penetration into stomata and the substomatal space by aqueous solutions are contradictory (3, 4. 11, 14). Surface tension, viscosity, contact angle, diameter of the stomatal aperture, final height and initial velocity of capillary rise have been implicated in controlling penetration of liquids into the stomatal pore and substomatal chamber (4,6,7,18,26,27) A liquid will rise in the capillary spontaneously only if P is positive. The sign of P is determined by the term cos O.,; P being positive when OA < 90', zero when 9A = 900 and negative when O., > 900. The magnitude of P increases as r decreases.For a conical capillary (Fig. 1)