{"id":754,"date":"2023-03-08T11:40:02","date_gmt":"2023-03-08T11:40:02","guid":{"rendered":"https:\/\/doublelayer.eu\/vilab\/?p=754"},"modified":"2023-03-08T11:42:45","modified_gmt":"2023-03-08T11:42:45","slug":"creating-scientific-figures-with-versioning","status":"publish","type":"post","link":"https:\/\/doublelayer.eu\/vilab\/2023\/03\/08\/creating-scientific-figures-with-versioning\/","title":{"rendered":"Creating scientific figures with versioning"},"content":{"rendered":"\n<p>While working on the &#8220;<a rel=\"noreferrer noopener\" href=\"https:\/\/arxiv.org\/abs\/2301.13681\" target=\"_blank\">Potential of monolayer charge<\/a>&#8221; letter, we learned that saving figure versions is essential. In particular, while working on the first Figure (representing the concept), we started with this sketch as an intermediate of a cartoon from &#8220;<a rel=\"noreferrer noopener\" href=\"https:\/\/link.aps.org\/doi\/10.1103\/PhysRevLett.106.046102\" target=\"_blank\">Overscreening versus Crowding<\/a>&#8221; and MD snapshots from &#8220;<a rel=\"noreferrer noopener\" href=\"https:\/\/www.electrochem.org\/dl\/interface\/spr\/spr14\/spr14_p65_69.pdf\" target=\"_blank\">Interfaces between Charged Surfaces and Ionic Liquids<\/a>.&#8221;<\/p>\n\n\n\n<center><figure class=\"wp-block-image aligncenter size-full is-resized\"><img decoding=\"async\" src=\"https:\/\/doublelayer.eu\/vilab\/wp-content\/uploads\/2023\/03\/unnamed.png\" alt=\"\" class=\"wp-image-755\" width=\"360\" srcset=\"https:\/\/doublelayer.eu\/vilab\/wp-content\/uploads\/2023\/03\/unnamed.png 512w, https:\/\/doublelayer.eu\/vilab\/wp-content\/uploads\/2023\/03\/unnamed-300x120.png 300w, https:\/\/doublelayer.eu\/vilab\/wp-content\/uploads\/2023\/03\/unnamed-220x88.png 220w\" sizes=\"(max-width: 512px) 100vw, 512px\" \/><\/figure><\/center>\n\n\n\n<p>With chatGPT, we created a wavy electrode and arranged ions in Matplotlib. Then, we created over 30 versions in Inkscape, as shown in this animation (also made with guidance from chatGPT):<\/p>\n\n\n\n<center><figure class=\"wp-block-image size-large\" align=\"center\"><img decoding=\"async\" src=\"https:\/\/doublelayer.eu\/vilab\/wp-content\/uploads\/2023\/03\/output-4.gif\" alt=\"Versions of Figure 1\" width=\"360\"><\/figure><\/center>\n\n\n\n<p>It was crucial to have versions instead of working on the same file because we often reverted to previous versions after trying new visual elements. Our final figure illustrates that the Potential of Monolayer Charge (PMC) is right between overscreening and crowding regimes. Moreover, the PMC can fit into the electrochemical stability window by lowering its absolute value with varying ion area. Read more in the &#8220;<a rel=\"noreferrer noopener\" href=\"https:\/\/arxiv.org\/abs\/2301.13681\" target=\"_blank\">Potential of monolayer charge<\/a>&#8221; letter.<\/p>\n\n\n\n<center><figure class=\"wp-block-image size-large\"><img decoding=\"async\" src=\"https:\/\/doublelayer.eu\/vilab\/wp-content\/uploads\/2023\/03\/Figure_Final-1024x600.png\" alt=\"\" class=\"wp-image-766\" width=\"350\" srcset=\"https:\/\/doublelayer.eu\/vilab\/wp-content\/uploads\/2023\/03\/Figure_Final-1024x600.png 1024w, https:\/\/doublelayer.eu\/vilab\/wp-content\/uploads\/2023\/03\/Figure_Final-300x176.png 300w, https:\/\/doublelayer.eu\/vilab\/wp-content\/uploads\/2023\/03\/Figure_Final-768x450.png 768w, https:\/\/doublelayer.eu\/vilab\/wp-content\/uploads\/2023\/03\/Figure_Final-1536x900.png 1536w, https:\/\/doublelayer.eu\/vilab\/wp-content\/uploads\/2023\/03\/Figure_Final-220x129.png 220w, https:\/\/doublelayer.eu\/vilab\/wp-content\/uploads\/2023\/03\/Figure_Final.png 1996w\" sizes=\"(max-width: 1024px) 100vw, 1024px\" \/><\/figure><\/center>\n\n\n\n<p><\/p>\n","protected":false},"excerpt":{"rendered":"<p>While working on the &#8220;Potential of monolayer charge&#8221; letter, we learned that saving figure versions is essential. In particular, while working on the first Figure (representing the concept), we started with this sketch as an intermediate of a cartoon from &#8220;Overscreening versus Crowding&#8221; and MD snapshots from &#8220;Interfaces between Charged Surfaces and Ionic Liquids.&#8221; With&hellip; <a class=\"read-more\" href=\"https:\/\/doublelayer.eu\/vilab\/2023\/03\/08\/creating-scientific-figures-with-versioning\/\">Read More<\/a><\/p>\n","protected":false},"author":5,"featured_media":0,"comment_status":"closed","ping_status":"open","sticky":false,"template":"","format":"standard","meta":{"footnotes":""},"categories":[1],"tags":[],"class_list":["post-754","post","type-post","status-publish","format-standard","hentry","category-uncategorized"],"_links":{"self":[{"href":"https:\/\/doublelayer.eu\/vilab\/wp-json\/wp\/v2\/posts\/754","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/doublelayer.eu\/vilab\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/doublelayer.eu\/vilab\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/doublelayer.eu\/vilab\/wp-json\/wp\/v2\/users\/5"}],"replies":[{"embeddable":true,"href":"https:\/\/doublelayer.eu\/vilab\/wp-json\/wp\/v2\/comments?post=754"}],"version-history":[{"count":6,"href":"https:\/\/doublelayer.eu\/vilab\/wp-json\/wp\/v2\/posts\/754\/revisions"}],"predecessor-version":[{"id":769,"href":"https:\/\/doublelayer.eu\/vilab\/wp-json\/wp\/v2\/posts\/754\/revisions\/769"}],"wp:attachment":[{"href":"https:\/\/doublelayer.eu\/vilab\/wp-json\/wp\/v2\/media?parent=754"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/doublelayer.eu\/vilab\/wp-json\/wp\/v2\/categories?post=754"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/doublelayer.eu\/vilab\/wp-json\/wp\/v2\/tags?post=754"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}