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.2019 Mar 12;116(11):4917-4922.
doi: 10.1073/pnas.1820318116. Epub 2019 Feb 25.

Vortex-induced dispersal of a plant pathogen by raindrop impact

Affiliations

Vortex-induced dispersal of a plant pathogen by raindrop impact

Seungho Kim et al. Proc Natl Acad Sci U S A..

Abstract

Raindrop impact on infected plants can disperse micron-sized propagules of plant pathogens (e.g., spores of fungi). Little is known about the mechanism of how plant pathogens are liberated and transported due to raindrop impact. We used high-speed photography to observe thousands of dry-dispersed spores of the rust fungusPuccinia triticina being liberated from infected wheat plants following the impact of a single raindrop. We revealed that an air vortex ring was formed during the raindrop impact and carried the dry-dispersed spores away from the surface of the host plant. The maximum height and travel distance of the airborne spores increased with the aid of the air vortex. This unique mechanism of vortex-induced dispersal dynamics was characterized to predict trajectories of spores. Finally, we found that the spores transported by the air vortex can reach beyond the laminar boundary layer of leaves, which would enable the long-distance transport of plant pathogens through the atmosphere.

Keywords: air vortex; drop impact; dry rust spore; plant pathogen; swirling trajectory.

Copyright © 2019 the Author(s). Published by PNAS.

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Conflict of interest statement

The authors declare no conflicts of interest.

Figures

Fig. 1.
Fig. 1.
(A) Rust-infected wheat leaf surface (Left) and SEM image of a uredinium (rust pustule containing urediniospores) (Right). Here, a pustule of spores is seen on the epidermis of the wheat leaf. (B) Dispersal of thousands of dry spores by drop impact when [Rd,Ud]= [1.6 mm, 2.4 m/s], whereRd,Ud are the radius and velocity of the impacting drop, respectively. (C) Visualization of dispersal patterns at [Rd,Ud]= [1.8 mm, 2.8 m/s]. (Inset) Dry-dispersed spores discharged by drop impact. (D) The numberNs and (E) dispersal distanceDdisp of dry spores versus impact velocityUd for a drop of 1.8-mm radius. The gray area inE corresponds to the calculated distance of dispersed spores without an air vortex. The filled bars and circles are for single spores only, whereas the open bars and circles are for all spores including spore agglomerates (more than one spore).
Fig. 2.
Fig. 2.
(A) Visualization of spores ofP.triticina motions moving around a wheat leaf when a raindrop of [Rd,Ud]= [1.6 mm, 2.4 m/s] impacts the leaf surface. Dry-dispersed wheat spores escape from the leaf, showing swirling trajectories during their dispersal (a solid curve with circles is obtained by tracking one spore). Each inset shows overlapping multiple images to visualize the trajectories of dry-dispersed spores (Movies S1 andS2). (B) Comparison of spore trajectories obtained from an experiment and from a ballistic model.
Fig. 3.
Fig. 3.
Visualization of the dispersal motion of glass beads (surrogates for spores) when [Rd,Ud]= [1.9 mm, 3.1 m/s]. Ballistic motion of the beads was observed only at the beginning stage of dispersal, but later spores exhibited a swirling motion (Movies S3 andS4).
Fig. 4.
Fig. 4.
(A) Smoke visualization of the air vortex with [Rd,Ud] = [1.4 mm, 3.3 m/s]. The white dashed curve represents the final shape of a drop and the solid curve indicates the intermediate shape of a spreading drop at the maximum spreading radius. (B) Schematic of the formation of an air vortex, driving spores to swirl around. (C) Magnitude of a circulationΓ versus an impact velocityUd depending on a drop radiusRd. (D)Γ is replotted according to our scaling law (Eq.2). (E) Contour map of a vorticity obtained from particle image velocimetry (PIV) measurements using glass beads with [Rd,Ud]= [1.9 mm, 3.1 m/s], showing the dissipation of the air vortex with elapsed times (seeSI Appendix, section D).
Fig. 5.
Fig. 5.
Experimental (circles) and theoretical (solid lines) footprints of glass beads, where [Rd,Ud] = [1.4 mm, 3.2 m/s]. (Inset) The actual trajectories of glass beads I, obtained from overlapping multiple images fromt = 0.4 to 76 ms.
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