{"id":1435,"date":"2021-06-01T05:00:00","date_gmt":"2021-06-01T09:00:00","guid":{"rendered":"https:\/\/sites.nd.edu\/biomechanics-in-the-wild\/?p=1435"},"modified":"2023-01-13T15:49:58","modified_gmt":"2023-01-13T19:49:58","slug":"innovative-plant-how-does-the-dandelion-drift-its-seeds","status":"publish","type":"post","link":"https:\/\/sites.nd.edu\/biomechanics-in-the-wild\/2021\/06\/01\/innovative-plant-how-does-the-dandelion-drift-its-seeds\/","title":{"rendered":"Innovative plant: How does the dandelion drift its seeds?"},"content":{"rendered":"\n<p class=\"wp-block-paragraph\">How far do you think a dandelion seed can drift from its base plant?<\/p>\n\n\n\n<!--more-->\n\n\n\n<p class=\"wp-block-paragraph\">The Common Dandelion (Taraxacum officinale) primarily relies on wind flow to scatter its seeds. The dandelion seed has a fluffy structure that enables it to hold the most prolonged wind-based dispersal record. Commonly the seeds land 2 meters away from their mother plant. Still, in windy, dry weather favored by the dandelion, the seeds can fly up to 30 kilometers and even far (150 kilometers in some conditions). The vital point in this extraordinary adventure of the dandelion is flying with a constant velocity and having a short descent time, which means it should stay stable in the air for a relatively long time.<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">A study tried to illuminate the mystery behind the dandelion seeds\u2019 ability to stay aloft in the air. Researchers attempted to mimic the dandelion flight using similarly structured<a href=\"http:\/\/www.nature.com\/articles\/s41586-018-0604-2\"> silicon disks<\/a> in a<a href=\"https:\/\/www.youtube.com\/watch?v=clKEdi-nXVw&amp;t=13s\"> wind tunnel<\/a> that simulated the airflow around the pappus. Pappus, the flying seed of the dandelion, consists of radially oriented filaments, each interacting with other adjacent ones, resulting in a reduction in the airflow. They compared the flight of natural seeds collected from one plant with several silicon disks with different porosities.<\/p>\n\n\n<div class=\"wp-block-image is-style-default\">\n<figure class=\"aligncenter size-medium\"><a href=\"https:\/\/doi.org\/10.1038\/s41586-018-0604-2\" target=\"_blank\" rel=\"noopener\"><img loading=\"lazy\" decoding=\"async\" width=\"300\" height=\"147\" src=\"https:\/\/sites.nd.edu\/biomechanics-in-the-wild\/files\/2021\/04\/1-300x147.png\" alt=\"Dandelion seeds and silicon disks in wind tunnel\" class=\"wp-image-1463\" srcset=\"https:\/\/sites.nd.edu\/biomechanics-in-the-wild\/files\/2021\/04\/1-300x147.png 300w, https:\/\/sites.nd.edu\/biomechanics-in-the-wild\/files\/2021\/04\/1-1024x503.png 1024w, https:\/\/sites.nd.edu\/biomechanics-in-the-wild\/files\/2021\/04\/1-768x377.png 768w, https:\/\/sites.nd.edu\/biomechanics-in-the-wild\/files\/2021\/04\/1-1536x754.png 1536w, https:\/\/sites.nd.edu\/biomechanics-in-the-wild\/files\/2021\/04\/1.png 1698w\" sizes=\"auto, (max-width: 300px) 100vw, 300px\" \/><\/a><figcaption class=\"wp-element-caption\">Wind tunnel experiment, modified from Cathal Cummins &amp; et al. 2018<\/figcaption><\/figure>\n<\/div>\n\n<div class=\"wp-block-image is-style-default\">\n<figure class=\"alignright size-medium\"><a href=\"https:\/\/onlinelibrary.wiley.com\/doi\/abs\/10.1111\/nph.16110\"><img loading=\"lazy\" decoding=\"async\" width=\"204\" height=\"300\" src=\"https:\/\/sites.nd.edu\/biomechanics-in-the-wild\/files\/2021\/04\/figure-3-4-204x300.png\" alt=\"vortex ring above pappus\" class=\"wp-image-1467\" srcset=\"https:\/\/sites.nd.edu\/biomechanics-in-the-wild\/files\/2021\/04\/figure-3-4-204x300.png 204w, https:\/\/sites.nd.edu\/biomechanics-in-the-wild\/files\/2021\/04\/figure-3-4.png 570w\" sizes=\"auto, (max-width: 204px) 100vw, 204px\" \/><\/a><figcaption class=\"wp-element-caption\">Pappus &amp; separated vortex ring, modified from Madeleine Seale &amp; et al. 2019<\/figcaption><\/figure>\n<\/div>\n\n\n<p class=\"wp-block-paragraph\">Their results showed that when pappus separates into the air,&nbsp; it forms an air bubble detached from its surface above it. This air bubble, known as a vortex, is unique to the dandelion seed. When the pappus is released in the air, it takes some time to reach a steady point, in which the vortex becomes symmetrical. An important feature affecting this symmetry is the porosity of the pappus, defined by the number of filaments and their dimension in each pappus\u2014 generally, the more the porosity, the steadier the flight. The best porosity for a<a href=\"http:\/\/aip.scitation.org\/doi\/10.1063\/5.0030894\"> stable vortex<\/a> ring is greater than 84.97%, and the vortex ring begins to separate as the porosity falls below 77.42%.&nbsp;The experiment also indicated that the vortex is axisymmetric in low velocities, but it begins to lose its symmetry as the Reynolds increases.<\/p>\n\n\n<div class=\"wp-block-image is-style-default\">\n<figure class=\"alignright size-medium is-resized\"><a href=\"https:\/\/www.pexels.com\/photo\/black-and-white-art-iphone-dark-3745895\/\"><img decoding=\"async\" src=\"https:\/\/sites.nd.edu\/biomechanics-in-the-wild\/files\/2021\/04\/pexels-enfantnocta-3745895-240x300.jpg\" alt=\"Pappus with water drops on it\" class=\"wp-image-1492\" width=\"200\" srcset=\"https:\/\/sites.nd.edu\/biomechanics-in-the-wild\/files\/2021\/04\/pexels-enfantnocta-3745895-240x300.jpg 240w, https:\/\/sites.nd.edu\/biomechanics-in-the-wild\/files\/2021\/04\/pexels-enfantnocta-3745895-819x1024.jpg 819w, https:\/\/sites.nd.edu\/biomechanics-in-the-wild\/files\/2021\/04\/pexels-enfantnocta-3745895-768x960.jpg 768w, https:\/\/sites.nd.edu\/biomechanics-in-the-wild\/files\/2021\/04\/pexels-enfantnocta-3745895-1229x1536.jpg 1229w, https:\/\/sites.nd.edu\/biomechanics-in-the-wild\/files\/2021\/04\/pexels-enfantnocta-3745895-1639x2048.jpg 1639w, https:\/\/sites.nd.edu\/biomechanics-in-the-wild\/files\/2021\/04\/pexels-enfantnocta-3745895-scaled.jpg 2048w\" sizes=\"(max-width: 240px) 100vw, 240px\" \/><\/a><figcaption class=\"wp-element-caption\">Pappus in moisture, photo by enfantnocta<\/figcaption><\/figure>\n<\/div>\n\n\n<p class=\"wp-block-paragraph\">This phenomenal plant has evolved techniques for mass germination, even in the<a href=\"https:\/\/onlinelibrary.wiley.com\/doi\/abs\/10.1111\/nph.16110\"> absence of wind<\/a>! Pappus\u2019s hairy structure enables it to attach to an animal\u2019s skin and <a href=\"http:\/\/link.springer.com\/10.1007\/s11104-019-04086-x\">soil<\/a> particles, assuring the dandelion to have enough seed dispersion during the flowering season. More interestingly, the dandelion is known to have an informed dispersal in response to environmental fluctuations. When the plant experiences root herbivory, it intensifies the seed dispersal. The flight distance may vary from meters to kilometers to assure good germination in the absence of threatening conditions. Imagine a rainy day; the moist<a href=\"https:\/\/www.ssrn.com\/abstract=3334428\"> weather condition<\/a> makes the pappus\u2019 bristles come close together, reducing the possibility of separating from the plant. The moisture makes the current spot a suitable choice to stay. So even the detached seeds prefer to fall close to their base plant.&nbsp;<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">It worth mentioning that this remarkable plant also inspired areas of science. In their study of <a href=\"https:\/\/arc.aiaa.org\/doi\/10.2514\/6.2020-2935\">Mars exploration<\/a>, researchers presented a primary model of a dandelion-inspired rover. Considering the harsh environmental condition on Mars, other excavators find the wind flow as an obstacle that results in damaged parts and incomplete missions. In contrast, the new dandelion-shaped rovers use the wind flow as an accelerating point to explore locations on Mars that other robots couldn\u2019t access.<\/p>\n\n\n<div class=\"wp-block-image is-style-default\">\n<figure class=\"aligncenter size-medium\"><a href=\"https:\/\/arc.aiaa.org\/doi\/10.2514\/6.2020-2935\"><img loading=\"lazy\" decoding=\"async\" width=\"279\" height=\"300\" src=\"https:\/\/sites.nd.edu\/biomechanics-in-the-wild\/files\/2021\/04\/figure-5-1-279x300.png\" alt=\"Dandelion-shaped Mars rovers\" class=\"wp-image-1475\" srcset=\"https:\/\/sites.nd.edu\/biomechanics-in-the-wild\/files\/2021\/04\/figure-5-1-279x300.png 279w, https:\/\/sites.nd.edu\/biomechanics-in-the-wild\/files\/2021\/04\/figure-5-1.png 396w\" sizes=\"auto, (max-width: 279px) 100vw, 279px\" \/><\/a><figcaption class=\"wp-element-caption\">Dandelion-shaped rovers ,modified from Michelle Sherman &amp; et al. 2020<\/figcaption><\/figure>\n<\/div>\n\n\n<p class=\"wp-block-paragraph\">Featured image from <a href=\"https:\/\/www.pexels.com\/photo\/nature-plant-flower-dandelion-36456\/\">White Dandelion<\/a> licensed under <a href=\"https:\/\/creativecommons.org\/publicdomain\/zero\/1.0\/\">CC0 1.0<\/a>. <\/p>\n","protected":false},"excerpt":{"rendered":"<p>How far do you think a dandelion seed can drift from its base plant?<\/p>\n","protected":false},"author":3935,"featured_media":1480,"comment_status":"closed","ping_status":"open","sticky":false,"template":"","format":"standard","meta":{"_monsterinsights_skip_tracking":false,"footnotes":""},"categories":[505480,505447],"tags":[380449,353229,505455,280588,44245],"class_list":["post-1435","post","type-post","status-publish","format-standard","has-post-thumbnail","hentry","category-2021-spring","category-text","tag-bio-inspired-design","tag-flying","tag-fluids","tag-plants","tag-robots"],"_links":{"self":[{"href":"https:\/\/sites.nd.edu\/biomechanics-in-the-wild\/wp-json\/wp\/v2\/posts\/1435","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/sites.nd.edu\/biomechanics-in-the-wild\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/sites.nd.edu\/biomechanics-in-the-wild\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/sites.nd.edu\/biomechanics-in-the-wild\/wp-json\/wp\/v2\/users\/3935"}],"replies":[{"embeddable":true,"href":"https:\/\/sites.nd.edu\/biomechanics-in-the-wild\/wp-json\/wp\/v2\/comments?post=1435"}],"version-history":[{"count":25,"href":"https:\/\/sites.nd.edu\/biomechanics-in-the-wild\/wp-json\/wp\/v2\/posts\/1435\/revisions"}],"predecessor-version":[{"id":3330,"href":"https:\/\/sites.nd.edu\/biomechanics-in-the-wild\/wp-json\/wp\/v2\/posts\/1435\/revisions\/3330"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/sites.nd.edu\/biomechanics-in-the-wild\/wp-json\/wp\/v2\/media\/1480"}],"wp:attachment":[{"href":"https:\/\/sites.nd.edu\/biomechanics-in-the-wild\/wp-json\/wp\/v2\/media?parent=1435"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/sites.nd.edu\/biomechanics-in-the-wild\/wp-json\/wp\/v2\/categories?post=1435"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/sites.nd.edu\/biomechanics-in-the-wild\/wp-json\/wp\/v2\/tags?post=1435"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}