{"id":43254,"date":"2021-07-02T17:00:00","date_gmt":"2021-07-02T16:00:00","guid":{"rendered":"http:\/\/cupblog.bluefusesystems.com\/?p=43254"},"modified":"2021-07-05T09:44:15","modified_gmt":"2021-07-05T08:44:15","slug":"making-waves-in-the-lab","status":"publish","type":"post","link":"https:\/\/www.cambridge.org\/core\/blog\/2021\/07\/02\/making-waves-in-the-lab\/","title":{"rendered":"Making Waves in the Lab"},"content":{"rendered":"<div id=\"bsf_rt_marker\"><\/div>\n<p>The term \u2018tsunami\u2019 is synonymous with gigantic and often catastrophic waves that destroy almost everything in their path. So, when Alban Sauret at UC Santa Barbara and his colleagues at FAST laboratory tried to create one in a lab setting, it would be fair to say they had their work cut out.<\/p>\n\n\n\n<figure class=\"wp-block-image size-large\"><img loading=\"lazy\" decoding=\"async\" width=\"1240\" height=\"715\" src=\"http:\/\/cupblog.bluefusesystems.com\/wp-content\/uploads\/2021\/07\/makins-waves-in-lab-1-1240x715.png\" alt=\"Diagram, engineering drawing\n\nDescription automatically generated\" class=\"wp-image-43255\" srcset=\"https:\/\/www.cambridge.org\/core\/blog\/wp-content\/uploads\/2021\/07\/makins-waves-in-lab-1-1240x715.png 1240w, https:\/\/www.cambridge.org\/core\/blog\/wp-content\/uploads\/2021\/07\/makins-waves-in-lab-1-420x242.png 420w, https:\/\/www.cambridge.org\/core\/blog\/wp-content\/uploads\/2021\/07\/makins-waves-in-lab-1-768x443.png 768w, https:\/\/www.cambridge.org\/core\/blog\/wp-content\/uploads\/2021\/07\/makins-waves-in-lab-1-1536x885.png 1536w, https:\/\/www.cambridge.org\/core\/blog\/wp-content\/uploads\/2021\/07\/makins-waves-in-lab-1-410x235.png 410w, https:\/\/www.cambridge.org\/core\/blog\/wp-content\/uploads\/2021\/07\/makins-waves-in-lab-1.png 1804w\" sizes=\"auto, (max-width: 1240px) 100vw, 1240px\" \/><\/figure>\n\n\n\n<p>The experimental setup consists of a column of granular material of varying height H<sub>0<\/sub> (9-39cm), varying width L<sub>0<\/sub> (5-20cm), but fixed transverse width of 15cm; which is released via a sliding gate mechanism into a pool of water with total length 2m. The idea is to recreate the situation of a collapsing cliff or landslide into the ocean \u2013 a common cause of tsunamis as seen in the 2018 partial collapse of Anak Krakatau in Indonesia \u2013 to try to understand and predict the properties of the waves generated in this fashion.<\/p>\n\n\n\n<p>Earlier work by the team showed that the velocity of the landslide as it enters the water is key in controlling the size of the wave, but little was known about the effects of the volume of the collapse and the water depth. In this <a href=\"https:\/\/www.cambridge.org\/core\/journals\/journal-of-fluid-mechanics\/article\/nonlinear-regimes-of-tsunami-waves-generated-by-a-granular-collapse\/3F38B26548B891FA9AE8A4018FF992A4\">latest <em>JFM<\/em> publication<\/a>, we see how the geometry of the initial collapse affects the characteristics of the resultant wave, with three distinctive regimes identified: the <em>bore wave (a)<\/em>, the <em>solitary wave (b)<\/em>, and the <em>non-linear transition wave (c)<\/em>.<\/p>\n\n\n\n<figure class=\"wp-block-image size-large\"><img loading=\"lazy\" decoding=\"async\" width=\"874\" height=\"1208\" src=\"http:\/\/cupblog.bluefusesystems.com\/wp-content\/uploads\/2021\/07\/makins-waves-in-lab-2.png\" alt=\"\" class=\"wp-image-43256\" srcset=\"https:\/\/www.cambridge.org\/core\/blog\/wp-content\/uploads\/2021\/07\/makins-waves-in-lab-2.png 874w, https:\/\/www.cambridge.org\/core\/blog\/wp-content\/uploads\/2021\/07\/makins-waves-in-lab-2-304x420.png 304w, https:\/\/www.cambridge.org\/core\/blog\/wp-content\/uploads\/2021\/07\/makins-waves-in-lab-2-768x1061.png 768w\" sizes=\"auto, (max-width: 874px) 100vw, 874px\" \/><\/figure>\n\n\n\n<p>The <em>bore wave <\/em>is typically seen for a large volume collapse into a shallow ocean, whilst the <em>solitary wave <\/em>occurs for landslides with smaller volume. The <em>non-linear transition wave<\/em> is seen for tall, thin collapses into a deeper ocean.<\/p>\n\n\n\n<p>The authors believe the grains \u201cact like a piston as they enter the water, the horizontal force of which governs the formation of the wave\u201d. This is consistent with shallow water theory in the first two regimes of <em>bore<\/em> and <em>solitary waves<\/em>, but the transition to deep water <em>non-linear waves<\/em> in the third regime requires additional understanding of the physical mechanisms present.<\/p>\n\n\n\n<p>The expected behaviour of the wave is determined by the local Froude number <em>F<sub>rf<\/sub>&nbsp;= v<sub>m<\/sub>&nbsp;\/ (g h<sub>0<\/sub>)<a>&nbsp;<\/a><\/em>which is based on the velocity of the collapsing front <em>V<sub>m<\/sub><\/em>, the depth of the water <em>h<sub>0,<\/sub><\/em> and gravitational acceleration <em>g<\/em>. For large values of the Froude number, <em>F<sub>rf<\/sub>&nbsp;<\/em>&gt; 0.87, <em>bore waves<\/em> are seen; for small values of <em>F<sub>rf<\/sub>&nbsp;<\/em>&lt; 0.35 we see <em>non-linear transition waves<\/em>; and for the intermediate range 0.35 &lt; <em>Frf <\/em>&lt; 0.87 <em>solitary waves occur<\/em>.<\/p>\n\n\n\n<p>Another interesting result found by the researchers was the apparent non-influence of the properties of the granular material. Conducting experiments with a series of different density and diameter grains, the resultant amplitude of the wave was unchanged. Understanding this \u2018non-effect\u2019 further, as well as the changing forces on the particles as they move from air to water remain the future challenges in this area of research.<\/p>\n\n\n\n<p>Ultimately, the hope is to be able to use this new knowledge to increase the complexity of tsunami prediction models, which currently rely on simplified models that do not capture the physics of the landslide as it enters the water. Comparisons of the team\u2019s experimental data with that from real-world case studies will be key to identifying the importance of the wave regimes on tsunami generation.<\/p>\n\n\n\n<p><strong>Sarlin, W., Morize, C., Sauret, A., &amp; Gondret, P. (2021). Nonlinear regimes of tsunami waves generated by a granular collapse.&nbsp;<em>Journal of Fluid Mechanics,<\/em>&nbsp;<em>919<\/em>, R6. <a href=\"doi:10.1017\/jfm.2021.400\">doi:10.1017\/jfm.2021.400<\/a><\/strong><\/p>\n\n\n\n<hr class=\"wp-block-separator\"\/>\n\n\n\n<p><\/p>\n\n\n\n<p><\/p>\n\n\n\n<p><\/p>\n","protected":false},"excerpt":{"rendered":"<p>When Alban Sauret and his colleagues at FAST laboratory tried to create a tsunami in a lab setting, it would be fair to say they had their work cut out.<\/p>\n","protected":false},"author":448,"featured_media":28622,"comment_status":"open","ping_status":"open","sticky":true,"template":"","format":"standard","meta":{"footnotes":""},"categories":[2248,2253,1],"tags":[1137,347,349,9114],"coauthors":[4015],"class_list":["post-43254","post","type-post","status-publish","format-standard","has-post-thumbnail","hentry","category-earth-environmental-science","category-mathematics","category-news","tag-fluid-dynamics","tag-fluid-mechanics","tag-journal-of-fluid-mechanics","tag-waves"],"aioseo_notices":[],"_links":{"self":[{"href":"https:\/\/www.cambridge.org\/core\/blog\/wp-json\/wp\/v2\/posts\/43254","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/www.cambridge.org\/core\/blog\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/www.cambridge.org\/core\/blog\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/www.cambridge.org\/core\/blog\/wp-json\/wp\/v2\/users\/448"}],"replies":[{"embeddable":true,"href":"https:\/\/www.cambridge.org\/core\/blog\/wp-json\/wp\/v2\/comments?post=43254"}],"version-history":[{"count":3,"href":"https:\/\/www.cambridge.org\/core\/blog\/wp-json\/wp\/v2\/posts\/43254\/revisions"}],"predecessor-version":[{"id":43260,"href":"https:\/\/www.cambridge.org\/core\/blog\/wp-json\/wp\/v2\/posts\/43254\/revisions\/43260"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/www.cambridge.org\/core\/blog\/wp-json\/wp\/v2\/media\/28622"}],"wp:attachment":[{"href":"https:\/\/www.cambridge.org\/core\/blog\/wp-json\/wp\/v2\/media?parent=43254"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.cambridge.org\/core\/blog\/wp-json\/wp\/v2\/categories?post=43254"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.cambridge.org\/core\/blog\/wp-json\/wp\/v2\/tags?post=43254"},{"taxonomy":"author","embeddable":true,"href":"https:\/\/www.cambridge.org\/core\/blog\/wp-json\/wp\/v2\/coauthors?post=43254"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}