{"id":5126,"date":"2025-02-12T11:24:18","date_gmt":"2025-02-12T09:24:18","guid":{"rendered":"https:\/\/www.nanosensors.com\/blog\/?p=5126"},"modified":"2025-02-12T11:27:42","modified_gmt":"2025-02-12T09:27:42","slug":"mechanical-disassembly-of-human-picobirnavirus-like-particles-indicates-that-cargo-retention-is-tuned-by-the-rna-coat-protein-interaction","status":"publish","type":"post","link":"https:\/\/www.nanosensors.com\/blog\/mechanical-disassembly-of-human-picobirnavirus-like-particles-indicates-that-cargo-retention-is-tuned-by-the-rna-coat-protein-interaction\/","title":{"rendered":"Mechanical disassembly of human picobirnavirus like particles indicates that cargo retention is tuned by the RNA-coat protein interaction"},"content":{"rendered":"<p>The idea of using virus-like particles as nanocarriers for heterologous cargo transport and delivery requires controlling the stability of the container\u2013cargo system.*<\/p>\n<p>In particular, the conditions of the cargo delivery entail tailoring the escape of the molecular payload when the virus particle is disassembled. What happens to the internalized molecules when the nanocage is opened? *<\/p>\n<p>To this end, it is necessary to control the cargo\u2013container interaction which, in turn, would tune the retention of cargo when the disassembly of the nanocarrier takes place. Thus, it is necessary to develop nanocarrier systems that facilitate the control of the cargo retention conditions as a function of its interaction with the nano-container.*<\/p>\n<p>In the article \u201c<em>Mechanical disassembly of human picobirnavirus like particles indicates that cargo retention is tuned by the RNA\u2013coat protein interaction<\/em>\u201d Mar\u00eda J. Rodr\u00edguez-Espinosa, Javier M. Rodr\u00edguez, Jos\u00e9 R. Cast\u00f3n and Pedro J. de Pablo describe how they designed three mutants of human picobirnavirus where the RNA\u2013coat protein interaction, observed previously via cryo-electron microscopy, is modified by changing the N-terminal end of the coat protein.<br \/>\nThe authors used atomic force microscopy (AFM) for inducing the mechanical unpacking of the RNA internalized in particles of each mutant.*<\/p>\n<p>Their experiments crack-opened individual particles in real time to monitor the cargo release. Among other results, Mar\u00eda J. Rodr\u00edguez-Espinosa et al. have measured that an increment in the N-terminal length by just 8% increases the cargo retention of partially disrupted particles by a factor of 10 with respect to the wild type. *<\/p>\n<p>This study elucidates the interplay between the RNA\u2013coat protein interaction of each mutant and their capacity for cargo retention during disassembly.*<\/p>\n<p>For mechanical fatigue experiments, rectangular AFM cantilevers (NANOSENSORS\u2122, <a href=\"https:\/\/www.nanosensors.com\/uploads\/media\/files\/0001\/05\/99a5bb03a57561c33fc8374eca2747fdb83ff15d.pdf\" target=\"_blank\" rel=\"noopener\">uniqprobe<\/a> <a href=\"https:\/\/www.nanosensors.com\/uniqprobe-uniform-quality-contact-or-dynamic-mode-for-biology-in-dynamic-ac-mode-afm-tip-qp-BioAC\" target=\"_blank\" rel=\"noopener\">qp-BioAC<\/a> AFM probes with three different AFM cantilevers per chip) with nominal spring constants of 0.05 and 0.1 N m\u22121 were used.<\/p>\n<p>The small variation of AFM cantilever force constant and resonance frequency of all types of the <a href=\"https:\/\/www.nanosensors.com\/uploads\/media\/files\/0001\/05\/99a5bb03a57561c33fc8374eca2747fdb83ff15d.pdf\" target=\"_blank\" rel=\"noopener\">uniqprobe<\/a> AFM probes series \u00a0makes them the ideal AFM probes for biology and life science applications.<\/p>\n<div id=\"attachment_4238\" style=\"width: 628px\" class=\"wp-caption alignright\"><a href=\"https:\/\/d218f3btfcac6d.cloudfront.net\/wp-content\/uploads\/2022\/11\/28103557\/NANOSENSORS-uniqprobe-qp-fast-AFM-probe-3.jpg\"><img loading=\"lazy\" decoding=\"async\" aria-describedby=\"caption-attachment-4238\" class=\"size-full wp-image-4238\" src=\"https:\/\/d218f3btfcac6d.cloudfront.net\/wp-content\/uploads\/2022\/11\/28103557\/NANOSENSORS-uniqprobe-qp-fast-AFM-probe-3.jpg\" alt=\"NANOSENSORS uniqprobe qp-BioAC AFM probe top view (SEM image)These oft, drift-reduced AFM probes have become very popular among our users who appreciate the small variation of AFM cantilever force constant and resonance frequency. The partial coating of the uniqprobes designed for liquid environments has the advantage of preserving the mechanical properties of the AFM cantilevers while maintaining high optical reflection. Further benefits of the uniqprobe coating are stress-free AFM cantilevers with considerably less bending and reduced drift particularly for measurements in liquid environments. These properties make the AFM probes of the NANOSENSORS uniqprobe series ideal for applications in biology and life-sciences.\" width=\"618\" height=\"420\" data-wp-pid=\"4238\" srcset=\"https:\/\/d218f3btfcac6d.cloudfront.net\/wp-content\/uploads\/2022\/11\/28103557\/NANOSENSORS-uniqprobe-qp-fast-AFM-probe-3.jpg 618w, https:\/\/d218f3btfcac6d.cloudfront.net\/wp-content\/uploads\/2022\/11\/28103557\/NANOSENSORS-uniqprobe-qp-fast-AFM-probe-3-300x204.jpg 300w, https:\/\/d218f3btfcac6d.cloudfront.net\/wp-content\/uploads\/2022\/11\/28103557\/NANOSENSORS-uniqprobe-qp-fast-AFM-probe-3-464x315.jpg 464w\" sizes=\"auto, (max-width: 618px) 100vw, 618px\" \/><\/a><p id=\"caption-attachment-4238\" class=\"wp-caption-text\">NANOSENSORS uniqprobe qp-BioAC AFM probe top view (SEM image)<\/p><\/div>\n<p>The AFM cantilevers were calibrated using Sader&#8217;s method.<\/p>\n<p>Mechanical fatigue experiments were carried out on single particles, taking consecutive images at a low and constant force of \u223c50 pN, below its breaking force. Images were processed and analyzed frame-by-frame using WSxM software39 to obtain additional information about the topography transformation of virus particles during the experiments. The mechanical fatigue experiments were performed in 10 \u039445-CP, 18 CP VLPs and 10 Ht-CP VLPs. Enough frames were obtained until the disruption of the particles took place. The variations over time of the VLPs area and height increments were monitored from the initial value 0 for each frame (Fig. 5).*<\/p>\n<p>In mechanical fatigue experiments, the AFM tip erodes the VLPs gradually while imaging (Fig. 5(A) and Movies SM1\u2013SM3, ESI\u2020 in the cited article), removing the virus material which can be either adhered by the surface or diffused to the liquid environment. Monitoring the area covered with debris for each hPBV variant reveals that RNA helps to keep the capsomer debris attached to the HOPG surface after being lost from the capsid during the mechanical fatigue procedure (Fig. 5(B) in the cited article).*<a href=\"https:\/\/www.nanosensors.com\/blog\/wp-content\/uploads\/2025\/02\/Fig-5-from-Maria-J-Rodriguez-Espinosa-et-al-2023-uniqprobe-qp-BioAC-AFM-probes-blog.jpg\"><img loading=\"lazy\" decoding=\"async\" class=\"size-full wp-image-5131\" src=\"https:\/\/www.nanosensors.com\/blog\/wp-content\/uploads\/2025\/02\/Fig-5-from-Maria-J-Rodriguez-Espinosa-et-al-2023-uniqprobe-qp-BioAC-AFM-probes-blog.jpg\" alt=\"Fig. 5 from Mar\u00eda J. Rodr\u00edguez-Espinosa et al. 2023:Analysis of individual virus particles unpacking under mechanical fatigue. (A) Evolution of individual particles under mechanical fatigue for the three variants: \u039445-CP (left), CP (center) and Ht-CP (right). Scale bar: 25 nm. The initial frame shows the intact particle, the intermediate frame reveals some damage and the last frame is the image of the final collapsed state. The entire fatigue process can be visualized in Movies SM1, SM2 and SM3 (ESI\u2020) for \u039445-CP, CP and Ht-CP, respectively. The color of the height scale is the same as shown in Fig. 2. (B) Evolution of the particle surrounding the covered area with debris for each VLP: 10 \u039445-CP VLPs (left), 18 CP VLPs (center) and 10 Ht-CP VLPs (right). (C) Evolution of the particle height for each virus particle, grouped by the hPBV variant. The dotted dark lines indicate the rate of collapse (RoC) ratio fitting for three cases in \u039445-CP (left, \u22127 nm per frame), CP (center, \u22126 nm per frame) and Ht-CP (right, \u22120.5 nm per frame), see the text. (D) Lost volume for each virus particle, classified by the hPBV variant. The dotted dark lines indicate the RoC ratio fitting for three cases in \u039445-CP (left, \u221221\u2006000 nm3 per frame), CP (center, \u221221\u2006000 nm3 per frame) and Ht-CP (right, \u22122000 nm3 per frame), see the text. The elapsed time for 1 frame is 120 seconds, resulting in 2 hours 30 minutes for the 80 frames of the x axes. For mechanical fatigue experiments, rectangular cantilevers (NANOSENSORS\u2122, uniqprobe qp-BioAC AFM probes) with nominal spring constants of 0.05 and 0.1 N m\u22121 were used. \" width=\"2000\" height=\"1740\" data-wp-pid=\"5131\" srcset=\"https:\/\/www.nanosensors.com\/blog\/wp-content\/uploads\/2025\/02\/Fig-5-from-Maria-J-Rodriguez-Espinosa-et-al-2023-uniqprobe-qp-BioAC-AFM-probes-blog.jpg 2000w, https:\/\/www.nanosensors.com\/blog\/wp-content\/uploads\/2025\/02\/Fig-5-from-Maria-J-Rodriguez-Espinosa-et-al-2023-uniqprobe-qp-BioAC-AFM-probes-blog-300x261.jpg 300w, https:\/\/www.nanosensors.com\/blog\/wp-content\/uploads\/2025\/02\/Fig-5-from-Maria-J-Rodriguez-Espinosa-et-al-2023-uniqprobe-qp-BioAC-AFM-probes-blog-1024x891.jpg 1024w, https:\/\/www.nanosensors.com\/blog\/wp-content\/uploads\/2025\/02\/Fig-5-from-Maria-J-Rodriguez-Espinosa-et-al-2023-uniqprobe-qp-BioAC-AFM-probes-blog-768x668.jpg 768w, https:\/\/www.nanosensors.com\/blog\/wp-content\/uploads\/2025\/02\/Fig-5-from-Maria-J-Rodriguez-Espinosa-et-al-2023-uniqprobe-qp-BioAC-AFM-probes-blog-1536x1336.jpg 1536w, https:\/\/www.nanosensors.com\/blog\/wp-content\/uploads\/2025\/02\/Fig-5-from-Maria-J-Rodriguez-Espinosa-et-al-2023-uniqprobe-qp-BioAC-AFM-probes-blog-362x315.jpg 362w\" sizes=\"auto, (max-width: 2000px) 100vw, 2000px\" \/><\/a><\/p>\n<p>Fig. 5 from Mar\u00eda J. Rodr\u00edguez-Espinosa et al. 2023:<br \/>\nAnalysis of individual virus particles unpacking under mechanical fatigue.<br \/>\n(A) Evolution of individual particles under mechanical fatigue for the three variants: \u039445-CP (left), CP (center) and Ht-CP (right). Scale bar: 25 nm. The initial frame shows the intact particle, the intermediate frame reveals some damage and the last frame is the image of the final collapsed state. The entire fatigue process can be visualized in Movies SM1, SM2 and SM3 (ESI\u2020) for \u039445-CP, CP and Ht-CP, respectively. The color of the height scale is the same as shown in Fig. 2. (B) Evolution of the particle surrounding the covered area with debris for each VLP: 10 \u039445-CP VLPs (left), 18 CP VLPs (center) and 10 Ht-CP VLPs (right). (C) Evolution of the particle height for each virus particle, grouped by the hPBV variant. The dotted dark lines indicate the rate of collapse (RoC) ratio fitting for three cases in \u039445-CP (left, \u22127 nm per frame), CP (center, \u22126 nm per frame) and Ht-CP (right, \u22120.5 nm per frame), see the text. (D) Lost volume for each virus particle, classified by the hPBV variant. The dotted dark lines indicate the RoC ratio fitting for three cases in \u039445-CP (left, \u221221\u2006000 nm3 per frame), CP (center, \u221221\u2006000 nm3 per frame) and Ht-CP (right, \u22122000 nm3 per frame), see the text. The elapsed time for 1 frame is 120 seconds, resulting in 2 hours 30 minutes for the 80 frames of the x axes.<\/p>\n<p>&nbsp;<\/p>\n<div id=\"attachment_5132\" style=\"width: 2010px\" class=\"wp-caption alignleft\"><a href=\"https:\/\/www.nanosensors.com\/blog\/wp-content\/uploads\/2025\/02\/Fig-6-from-Maria-J-Rodriguez-Espinosa-et-al-2023-blog.jpg\"><img loading=\"lazy\" decoding=\"async\" aria-describedby=\"caption-attachment-5132\" class=\"size-full wp-image-5132\" src=\"https:\/\/www.nanosensors.com\/blog\/wp-content\/uploads\/2025\/02\/Fig-6-from-Maria-J-Rodriguez-Espinosa-et-al-2023-blog.jpg\" alt=\"Fig. 6 from Mar\u00eda J. Rodr\u00edguez-Espinosa et al. 2023:Model depicting the RNA cargo retention for each VLP variant. The \u039445-CP VLP structure (A) does not show externalized cargo. The CP VLP structure (B) shows shorter N-terminals compared to the Ht-CP structure (C), which implies less RNA cargo retention compared to the Ht-CP structure. The cartoons in blue, green and pink colors represent coat protein, RNA and N-terminal, respectively. \" width=\"2000\" height=\"773\" data-wp-pid=\"5132\" srcset=\"https:\/\/www.nanosensors.com\/blog\/wp-content\/uploads\/2025\/02\/Fig-6-from-Maria-J-Rodriguez-Espinosa-et-al-2023-blog.jpg 2000w, https:\/\/www.nanosensors.com\/blog\/wp-content\/uploads\/2025\/02\/Fig-6-from-Maria-J-Rodriguez-Espinosa-et-al-2023-blog-300x116.jpg 300w, https:\/\/www.nanosensors.com\/blog\/wp-content\/uploads\/2025\/02\/Fig-6-from-Maria-J-Rodriguez-Espinosa-et-al-2023-blog-1024x396.jpg 1024w, https:\/\/www.nanosensors.com\/blog\/wp-content\/uploads\/2025\/02\/Fig-6-from-Maria-J-Rodriguez-Espinosa-et-al-2023-blog-768x297.jpg 768w, https:\/\/www.nanosensors.com\/blog\/wp-content\/uploads\/2025\/02\/Fig-6-from-Maria-J-Rodriguez-Espinosa-et-al-2023-blog-1536x594.jpg 1536w, https:\/\/www.nanosensors.com\/blog\/wp-content\/uploads\/2025\/02\/Fig-6-from-Maria-J-Rodriguez-Espinosa-et-al-2023-blog-600x232.jpg 600w\" sizes=\"auto, (max-width: 2000px) 100vw, 2000px\" \/><\/a><p id=\"caption-attachment-5132\" class=\"wp-caption-text\">Fig. 6 from Mar\u00eda J. Rodr\u00edguez-Espinosa et al. 2023:<br \/>Model depicting the RNA cargo retention for each VLP variant. The \u039445-CP VLP structure (A) does not show externalized cargo. The CP VLP structure (B) shows shorter N-terminals compared to the Ht-CP structure (C), which implies less RNA cargo retention compared to the Ht-CP structure. The cartoons in blue, green and pink colors represent coat protein, RNA and N-terminal, respectively.<\/p><\/div>\n<p>*Mar\u00eda J. Rodr\u00edguez-Espinosa, Javier M. Rodr\u00edguez, Jos\u00e9 R. Cast\u00f3n and Pedro J. de Pablo<br \/>\n<strong>Mechanical disassembly of human picobirnavirus like particles indicates that cargo retention is tuned by the RNA\u2013coat protein interaction<\/strong><br \/>\nNanoscale Horizons, 2023, 8, 1665-1676<br \/>\nDOI: <a href=\"https:\/\/doi.org\/10.1039\/D3NH00195D\" target=\"_blank\" rel=\"noopener\">https:\/\/doi.org\/10.1039\/D3NH00195D<\/a><\/p>\n<p>&nbsp;<\/p>\n<p>The article \u201c<em>Mechanical disassembly of human picobirnavirus like particles indicates that cargo retention is tuned by the RNA\u2013coat protein interaction<\/em>\u201d by Mar\u00eda J. Rodr\u00edguez-Espinosa, Javier M. Rodr\u00edguez, Jos\u00e9 R. Cast\u00f3n and Pedro J. de Pablo is licensed under a Creative Commons Attribution 3.0 International License, which permits use, sharing, adaptation, distribution and reproduction in any medium or format, as long as you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons license, and indicate if changes were made. The images or other third-party material in this article are included in the article\u2019s Creative Commons license, unless indicated otherwise in a credit line to the material. If material is not included in the article\u2019s Creative Commons license and your intended use is not permitted by statutory regulation or exceeds the permitted use, you will need to obtain permission directly from the copyright holder. To view a copy of this license, visit https:\/\/creativecommons.org\/licenses\/by\/3.0\/.<\/p>\n","protected":false},"excerpt":{"rendered":"<p>The idea of using virus-like particles as nanocarriers for heterologous cargo transport and delivery requires controlling the stability of the container\u2013cargo system.* In particular, the conditions of the cargo delivery entail tailoring the escape of the molecular payload when the virus particle is disassembled. What happens to the internalized molecules when the nanocage is opened?&hellip;&nbsp;<a href=\"https:\/\/www.nanosensors.com\/blog\/mechanical-disassembly-of-human-picobirnavirus-like-particles-indicates-that-cargo-retention-is-tuned-by-the-rna-coat-protein-interaction\/\" class=\"\" rel=\"bookmark\">Read More &raquo;<span class=\"screen-reader-text\">Mechanical disassembly of human picobirnavirus like particles indicates that cargo retention is tuned by the RNA-coat protein interaction<\/span><\/a><\/p>\n","protected":false},"author":2,"featured_media":5140,"comment_status":"closed","ping_status":"closed","sticky":false,"template":"","format":"standard","meta":{"neve_meta_sidebar":"","neve_meta_container":"","neve_meta_enable_content_width":"off","neve_meta_content_width":70,"neve_meta_title_alignment":"","neve_meta_author_avatar":"","neve_post_elements_order":"","neve_meta_disable_header":"","neve_meta_disable_footer":"","neve_meta_disable_title":"","footnotes":""},"categories":[16],"tags":[880,17,1135,18,448,339,398,19,84,1136,527,1127,85,1129,1133,1134,1125,1131,1128,327,557,255,1130,181,1132,83,340,447,50,498,1137,1126,1140,442,539,481,1138,728,1139],"class_list":{"0":"post-5126","1":"post","2":"type-post","3":"status-publish","4":"format-standard","5":"has-post-thumbnail","6":"hentry","7":"category-science-technology","8":"tag-afm-cantilevers","9":"tag-afm-probes","10":"tag-afm-tip-indentation","11":"tag-afm-tips","12":"tag-afm","15":"tag-atomic-force-microscopy","16":"tag-biology","17":"tag-biology-afm-probes","18":"tag-biotechnology","19":"tag-heterologous-cargo-transport","20":"tag-life-sciences","21":"tag-macromolecular-structures","22":"tag-mechanical-fatigue","23":"tag-mechanical-fatigue-experiments","24":"tag-nanobiotechnology","25":"tag-nanocage","26":"tag-nanocarriers","27":"tag-nanoindentation","28":"tag-nanoscale","29":"tag-nanoscience","30":"tag-picobirnavirus","31":"tag-qp-bioac","32":"tag-rna","33":"tag-soft-cantilevers","34":"tag-spm","36":"tag-uniqprobe","37":"tag-uniqprobes","38":"tag-virus-material","39":"tag-virus-like-particles","40":"tag-1140","41":"tag-442","42":"tag-539","43":"tag-481","44":"tag-1138","45":"tag-728","46":"tag-1139"},"_links":{"self":[{"href":"https:\/\/www.nanosensors.com\/blog\/wp-json\/wp\/v2\/posts\/5126","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/www.nanosensors.com\/blog\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/www.nanosensors.com\/blog\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/www.nanosensors.com\/blog\/wp-json\/wp\/v2\/users\/2"}],"replies":[{"embeddable":true,"href":"https:\/\/www.nanosensors.com\/blog\/wp-json\/wp\/v2\/comments?post=5126"}],"version-history":[{"count":10,"href":"https:\/\/www.nanosensors.com\/blog\/wp-json\/wp\/v2\/posts\/5126\/revisions"}],"predecessor-version":[{"id":5138,"href":"https:\/\/www.nanosensors.com\/blog\/wp-json\/wp\/v2\/posts\/5126\/revisions\/5138"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/www.nanosensors.com\/blog\/wp-json\/wp\/v2\/media\/5140"}],"wp:attachment":[{"href":"https:\/\/www.nanosensors.com\/blog\/wp-json\/wp\/v2\/media?parent=5126"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.nanosensors.com\/blog\/wp-json\/wp\/v2\/categories?post=5126"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.nanosensors.com\/blog\/wp-json\/wp\/v2\/tags?post=5126"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}