{"id":179,"date":"2017-08-08T21:15:35","date_gmt":"2017-08-08T21:15:35","guid":{"rendered":"https:\/\/home.physics.wisc.edu\/gilbert2\/?page_id=179"},"modified":"2026-03-09T02:30:03","modified_gmt":"2026-03-09T02:30:03","slug":"nacre-research","status":"publish","type":"page","link":"https:\/\/home.physics.wisc.edu\/gilbert\/nacre-research\/","title":{"rendered":"Nacre"},"content":{"rendered":"<h1 style=\"margin-top:var(--wp--preset--spacing--50);margin-bottom:var(--wp--preset--spacing--20);\" class=\"is-style-mini-bar wp-block-post-title\">Nacre<\/h1><div id=\"\" class=\"wp-block-group alignfull has-background  has-base-background-color\" style=\"margin-top:0;margin-bottom:0; padding-top:var(--wp--preset--spacing--40); padding-bottom:var(--wp--preset--spacing--60);\"><div class=\"wp-block-group__inner-container is-layout-constrained wp-block-group-is-layout-constrained\"><div class=\"wp-block-columns alignnone is-layout-flex wp-container-core-columns-is-layout-9d6595d7 wp-block-columns-is-layout-flex\"><div class=\"wp-block-column is-layout-flow wp-block-column-is-layout-flow\" ><div class=\"wp-block-group\"><div class=\"wp-block-group__inner-container is-layout-constrained wp-block-group-is-layout-constrained\">The nacre layer, or mother of pearl, at the inner surface of the abalone shell and of other mollusk shells and pearls (see images below and <a href=\"\/gilbert\/nacre\/sample_compendium.html\">in the sample compendium<\/a>) has a fracture resistance 3000 times greater than that of aragonite, the pure mineral of which it is composed. The toughening effect is due to well-defined nanolayers of organics at the interfaces between micro-tablets of aragonite (JD Currey 1977, 2005).\r\n\r\nNacre formation is poorly understood at the molecular level, and this piqued our interest in this material, exploring the organic-mineral interface (Gilbert 2005, Metzler 2010, Metzler 2010).\r\n\r\nWe strive to understand the fundamental mechanisms leading to the formation of the beautiful, extraordinarily efficient, self-assembling natural structures in nacre. We recently discovered a new polarization-dependent imaging contrast (PIC) mechanism, also known as linear dichroism. The PIC-mapping method we developed (DeVol 2014) showed that adjacent stacks of co-oriented tablets have different crystallographic c-axis orientations, and consequently the nacre growth direction cannot be identified with the c-axis (Metzler 2007). The appearance of the columns also inspired new models for the formation mechanism of nacre (Gilbert 2008).\r\n\r\nOur hypothesis is that the physical structure of nacre is affected by the environmental conditions at the time of nacre deposition. We are currently exploring this possibility (Olson 2012, Olson 2012, Gilbert 2015 in preparation).\r\n\r\nWe recently discovered that nacre forms via two amorphous precursor phases, similar to those found in sea urchin biominerals, and not proto-aragonite (DeVol 2015).\r\n\r\n<figure id=\"attachment_194\" class=\"wp-caption alignnone\" style=\"max-width: 300px;\" aria-label=\"Polarization-dependent imaging contrast in a side view of red abalone nacre. Different gray levels correspond to different c-axis orientations with respect to the illuminating x-ray polarization vector. Immediately adjacent columns are mis-aligned in c-axis direction. Data from ref. 5.\"><a href=\"\/gilbert\/wp-content\/uploads\/sites\/3\/2017\/08\/nacre-2008-larger.jpg\"><img loading=\"lazy\" decoding=\"async\" class=\"size-medium wp-image-194\" src=\"\/gilbert\/wp-content\/uploads\/sites\/3\/2017\/08\/nacre-2008-larger-300x168.jpg\" alt=\"\" width=\"300\" height=\"168\" srcset=\"https:\/\/home.physics.wisc.edu\/gilbert\/wp-content\/uploads\/sites\/3\/2017\/08\/nacre-2008-larger-300x168.jpg 300w, https:\/\/home.physics.wisc.edu\/gilbert\/wp-content\/uploads\/sites\/3\/2017\/08\/nacre-2008-larger-768x430.jpg 768w, https:\/\/home.physics.wisc.edu\/gilbert\/wp-content\/uploads\/sites\/3\/2017\/08\/nacre-2008-larger.jpg 946w\" sizes=\"auto, (max-width: 300px) 100vw, 300px\" \/><\/a><figcaption class=\"wp-caption-text\">Polarization-dependent imaging contrast in a side view of red abalone nacre. Different gray levels correspond to different c-axis orientations with respect to the illuminating x-ray polarization vector. Immediately adjacent columns are mis-aligned in c-axis direction. Data from ref. 5.<\/figcaption><\/figure>\r\n<h2>GG Publications on Nacre<\/h2>\r\n<ol class=\"reftext\">\r\n \t<li>P.U.P.A. Gilbert, Bradley H. Frazer and M. Abrecht.\r\nThe organic-mineral interface in biominerals.\r\nReviews in Mineralogy and Geochemistry. In: Molecular Geomicrobiology. Vol 59. JF Banfield, KH Nealson, J. Cervini-Silva (eds), Mineralogical Society of America, Washington DC, p 157-185 (2005). <a href=\"\/gilbert\/wp-content\/uploads\/sites\/3\/2017\/08\/92.pdf\">PDF<\/a><\/li>\r\n \t<li>Rebecca A. Metzler, Mike Abrecht, Ronke M. Olabisi, Daniel Ariosa, Christopher J. Johnson, Bradley H. Frazer, Susan N. Coppersmith, P.U.P.A. Gilbert.\r\nColumnar Nacre Architecture and Possible Formation Mechanism.\r\nPhys. Rev. Lett. 98, 268102-1\/4 (2007). <a href=\"\/gilbert\/wp-content\/uploads\/sites\/3\/2017\/08\/102.pdf\">PDF<\/a> <i>Also featured in Science 317, 175 (2007).<\/i> <a href=\"\/gilbert\/wp-content\/uploads\/sites\/3\/2017\/08\/102a.pdf\">PDF<\/a><i><\/i><\/li>\r\n \t<li>Rebecca A. Metzler, Dong Zhou, Mike Abrecht, Jau-Wern Chiou, Jinghua Guo, Daniel Ariosa, Susan N. Coppersmith, P.U.P.A. Gilbert.\r\nPolarization-dependent imaging contrast in abalone shells.\r\nPhys. Rev. B. 77, 064110-1\/9 (2008). <a href=\"\/gilbert\/wp-content\/uploads\/sites\/3\/2017\/08\/106.pdf\">PDF<\/a><\/li>\r\n \t<li>Dong Zhou, Rebecca A. Metzler, Tolek Tyliszczak, Jinghua Guo, Mike Abrecht, Susan N. Coppersmith, P.U.P.A. Gilbert.\r\nAssignment of polarization-dependent peaks in carbon K-edge spectra from biogenic and geologic aragonite.\r\nJ. Phys. Chem. B 112, 13128-13135 (2008). <a href=\"http:\/\/pubs.acs.org\/doi\/full\/10.1021\/jp803176z\">PDF<\/a><\/li>\r\n \t<li><b>P.U.P.A. Gilbert, Rebecca A. Metzler, Dong Zhou, Andreas Scholl, Andrew Doran, Anthony Young, Martin Kunz, Nobumichi Tamura, Susan N. Coppersmith.\r\nGradual Ordering in Red Abalone Nacre.\r\nJ. Am. Chem. Soc. 130, 17519-17527 (2008).<\/b> <a href=\"http:\/\/pubs.acs.org\/doi\/full\/10.1021\/ja8065495\">PDF<\/a> <a href=\"http:\/\/pubs.acs.org\/doi\/suppl\/10.1021\/ja8065495\">SI<\/a><\/li>\r\n \t<li>S. N. Coppersmith, P.U.P.A. Gilbert and R. A. Metzler.\r\nTheoretical characterization of a model of aragonite crystal orientation in red abalone nacre.\r\nJ. Phys. A: Math. Theor. 42, 125101 (2009). <a href=\"\/gilbert\/wp-content\/uploads\/sites\/3\/2017\/08\/113.pdf\">PDF<\/a><\/li>\r\n \t<li>RA Metzler, GA Tribello, M Parrinello, and PUPA Gilbert.\r\nAsprich peptides are occluded in calcite and permanently disorder biomineral crystals.\r\nJ. Am. Chem. Soc. 132, 11585-11591 (2010). <a href=\"http:\/\/pubs.acs.org\/doi\/abs\/10.1021\/ja103089r\">PDF<\/a><\/li>\r\n \t<li>RA Metzler, JS Evans, CE Killian, D. Zhou, TH Churchill, N Appathurai, SN Coppersmith, PUPA Gilbert.\r\nNacre Protein Fragment Templates Lamellar Aragonite Growth.\r\nJ. Am. Chem. Soc. 132, 6329-6334 (2010). <a class=\"reftext\" href=\"http:\/\/pubs.acs.org\/doi\/abs\/10.1021\/ja909735y\">PDF<\/a><\/li>\r\n \t<li><b>IC Olson, R Kozdon, JW Valley, and PUPA Gilbert.\r\nMollusk Shell Nacre Ultrastructure Correlates with Environmental Temperature and Pressure.\r\nJ. Am. Chem. Soc. 134, 7351-7358 (2012).<\/b> <a href=\"\/gilbert\/wp-content\/uploads\/sites\/3\/2017\/08\/127-cover.pdf\">COVER<\/a> <a class=\"reftext\" href=\"http:\/\/pubs.acs.org\/doi\/abs\/10.1021\/ja210808s\">PDF<\/a><\/li>\r\n \t<li>IC Olson and PUPA Gilbert.\r\nAragonite crystal orientation in mollusk shell nacre may depend on temperature. The angle spread of crystalline aragonite tablets records the water temperature at which nacre was deposited by Pinctada margaritifera.\r\nFaraday Discuss. 159, 421-432 (2012). <a class=\"reftext\" href=\"http:\/\/xlink.rsc.org\/?doi=C2FD20047C\">PDF<\/a><\/li>\r\n \t<li>PUPA Gilbert.\r\nPolarization-dependent Imaging Contrast (PIC) mapping reveals nanocrystal orientation patterns in carbonate biominerals.\r\nJ. Electr. Spectrosc. and Rel. Phenom. special issue on Photoelectron microscopy, Time-resolved pump-probe PES. Eds. M Kiskinova, A Scholl. Vol 185, pages 395-405 (2012). <a class=\"reftext\" href=\"http:\/\/www.sciencedirect.com\/science\/article\/pii\/S0368204812000564\">PDF<\/a><\/li>\r\n \t<li>IC Olson, AZ Blonsky, N Tamura, M Kunz, B Pokroy, CP Romao, MA White, and PUPA Gilbert.\r\nCrystal nucleation and near-epitaxial growth in nacre.\r\nJ. Struct. Biol. 184, 454-463 (2013). <a href=\"\/gilbert\/wp-content\/uploads\/sites\/3\/2017\/08\/JSBcover.pdf\">COVER<\/a> <a class=\"reftext\" href=\"http:\/\/dx.doi.org\/10.1016\/j.jsb.2013.10.002\">PDF<\/a><\/li>\r\n \t<li><b>RT DeVol, C-Y Sun, MA Marcus, SN Coppersmith, SCB Myneni, and PUPA Gilbert.\r\nNanoscale transforming mineral phases in fresh nacre.\r\nJ Am Chem Soc, 137, 13325-13333 (2015).<\/b> <a class=\"reftext\" href=\"http:\/\/pubs.acs.org\/doi\/abs\/10.1021\/jacs.5b07931\">PDF<\/a>\r\nHighlighted in Science 350, 648 (2015). <a class=\"reftext\" href=\"http:\/\/www.sciencemag.org\/content\/350\/6261\/647.3.full?ct=ct\">PDF<\/a><\/li>\r\n<\/ol>\r\n<ol>\r\n \t<li>AJ Lew, CA Stifler, A Tits, CA Schmidt, A Scholl, A Cantamessa, L M\u00fcller, Y Delaunois, P Comp\u00e8re, D Ruffoni, MJ Buehler*, PUPA Gilbert*.\r\nA molecular scale understanding of misorientation toughening in corals and seashells.\r\nDOI: <a href=\"https:\/\/doi.org\/10.1002\/adma.202300373\">10.1002\/adma.202300373<\/a>\r\n<em>Advanced Materials <\/em><strong>35<\/strong>, 2300373 (2023). <a href=\"https:\/\/onlinelibrary.wiley.com\/toc\/15214095\/2023\/35\/28\">INSIDE COVER<\/a> <a href=\"https:\/\/doi.org\/10.1002\/adma.202300373\">PDF<\/a><\/li>\r\n<\/ol>\r\nAlso see stories from UW NEWS July 2, 2007 by Jill Sakai\r\n<a href=\"http:\/\/www.news.wisc.edu\/13904\">Mother-of-pearl: Classic beauty and remarkable strength<\/a>\r\nand October 20, 2015 by Terrance Devitt\r\n<a href=\"http:\/\/news.wisc.edu\/24112\">Mother-of-pearl&#8217;s genesis identified in mineral&#8217;s transformation<\/a>\r\n\r\nClick on the images below for a description.\u00a0 Many more images can be found in the <a href=\"\/gilbert\/nacre\/sample_compendium.html\">nacre sample compendium<\/a>.<\/div><\/div><figure class=\"wp-block-gallery has-nested-images columns-default is-cropped wp-block-gallery-1 is-layout-flex wp-block-gallery-is-layout-flex\"><figure data-wp-context=\"{&quot;imageId&quot;:&quot;69e97efc4947e&quot;}\" data-wp-interactive=\"core\/image\" data-wp-key=\"69e97efc4947e\" class=\"wp-block-image size-large wp-lightbox-container\"><img loading=\"lazy\" decoding=\"async\" width=\"500\" height=\"372\" data-wp-class--hide=\"state.isContentHidden\" data-wp-class--show=\"state.isContentVisible\" data-wp-init=\"callbacks.setButtonStyles\" data-wp-on--click=\"actions.showLightbox\" data-wp-on--load=\"callbacks.setButtonStyles\" data-wp-on-window--resize=\"callbacks.setButtonStyles\" data-id=\"186\" src=\"https:\/\/home.physics.wisc.edu\/gilbert\/wp-content\/uploads\/sites\/3\/2017\/08\/nacre1.gif\" alt=\"\" class=\"wp-image-186\"\/><button\n\t\t\tclass=\"lightbox-trigger\"\n\t\t\ttype=\"button\"\n\t\t\taria-haspopup=\"dialog\"\n\t\t\taria-label=\"Enlarge\"\n\t\t\tdata-wp-init=\"callbacks.initTriggerButton\"\n\t\t\tdata-wp-on--click=\"actions.showLightbox\"\n\t\t\tdata-wp-style--right=\"state.imageButtonRight\"\n\t\t\tdata-wp-style--top=\"state.imageButtonTop\"\n\t\t>\n\t\t\t<svg xmlns=\"http:\/\/www.w3.org\/2000\/svg\" width=\"12\" height=\"12\" fill=\"none\" viewBox=\"0 0 12 12\">\n\t\t\t\t<path fill=\"#fff\" d=\"M2 0a2 2 0 0 0-2 2v2h1.5V2a.5.5 0 0 1 .5-.5h2V0H2Zm2 10.5H2a.5.5 0 0 1-.5-.5V8H0v2a2 2 0 0 0 2 2h2v-1.5ZM8 12v-1.5h2a.5.5 0 0 0 .5-.5V8H12v2a2 2 0 0 1-2 2H8Zm2-12a2 2 0 0 1 2 2v2h-1.5V2a.5.5 0 0 0-.5-.5H8V0h2Z\" \/>\n\t\t\t<\/svg>\n\t\t<\/button><figcaption class=\"wp-element-caption\">Photograph of the inner side of a green abalone (Haliotis fulgens) shell, showing the iridescent nacre. Shell diameter is ~20 cm.<\/figcaption><\/figure><figure data-wp-context=\"{&quot;imageId&quot;:&quot;69e97efc49d4b&quot;}\" data-wp-interactive=\"core\/image\" data-wp-key=\"69e97efc49d4b\" class=\"wp-block-image size-large wp-lightbox-container\"><img loading=\"lazy\" decoding=\"async\" width=\"200\" height=\"149\" data-wp-class--hide=\"state.isContentHidden\" data-wp-class--show=\"state.isContentVisible\" data-wp-init=\"callbacks.setButtonStyles\" data-wp-on--click=\"actions.showLightbox\" data-wp-on--load=\"callbacks.setButtonStyles\" data-wp-on-window--resize=\"callbacks.setButtonStyles\" data-id=\"187\" src=\"https:\/\/home.physics.wisc.edu\/gilbert\/wp-content\/uploads\/sites\/3\/2017\/08\/SEM-nacre.gif\" alt=\"\" class=\"wp-image-187\"\/><button\n\t\t\tclass=\"lightbox-trigger\"\n\t\t\ttype=\"button\"\n\t\t\taria-haspopup=\"dialog\"\n\t\t\taria-label=\"Enlarge\"\n\t\t\tdata-wp-init=\"callbacks.initTriggerButton\"\n\t\t\tdata-wp-on--click=\"actions.showLightbox\"\n\t\t\tdata-wp-style--right=\"state.imageButtonRight\"\n\t\t\tdata-wp-style--top=\"state.imageButtonTop\"\n\t\t>\n\t\t\t<svg xmlns=\"http:\/\/www.w3.org\/2000\/svg\" width=\"12\" height=\"12\" fill=\"none\" viewBox=\"0 0 12 12\">\n\t\t\t\t<path fill=\"#fff\" d=\"M2 0a2 2 0 0 0-2 2v2h1.5V2a.5.5 0 0 1 .5-.5h2V0H2Zm2 10.5H2a.5.5 0 0 1-.5-.5V8H0v2a2 2 0 0 0 2 2h2v-1.5ZM8 12v-1.5h2a.5.5 0 0 0 .5-.5V8H12v2a2 2 0 0 1-2 2H8Zm2-12a2 2 0 0 1 2 2v2h-1.5V2a.5.5 0 0 0-.5-.5H8V0h2Z\" \/>\n\t\t\t<\/svg>\n\t\t<\/button><figcaption class=\"wp-element-caption\">SEM micrograph of a fractured nacre surface, from the gastropod red abalone (Haliotis rufescens). Nacre tablets are 400 nm thick, and appear in a side view. The 400-nm layering is the origin of nacre&#039;s iridescence. Scale bar is 5 &mu;m. <\/figcaption><\/figure><figure data-wp-context=\"{&quot;imageId&quot;:&quot;69e97efc4a54c&quot;}\" data-wp-interactive=\"core\/image\" data-wp-key=\"69e97efc4a54c\" class=\"wp-block-image size-large wp-lightbox-container\"><img loading=\"lazy\" decoding=\"async\" width=\"500\" height=\"332\" data-wp-class--hide=\"state.isContentHidden\" data-wp-class--show=\"state.isContentVisible\" data-wp-init=\"callbacks.setButtonStyles\" data-wp-on--click=\"actions.showLightbox\" data-wp-on--load=\"callbacks.setButtonStyles\" data-wp-on-window--resize=\"callbacks.setButtonStyles\" data-id=\"188\" src=\"https:\/\/home.physics.wisc.edu\/gilbert\/wp-content\/uploads\/sites\/3\/2017\/08\/nautilus.jpg\" alt=\"\" class=\"wp-image-188\" srcset=\"https:\/\/home.physics.wisc.edu\/gilbert\/wp-content\/uploads\/sites\/3\/2017\/08\/nautilus.jpg 500w, https:\/\/home.physics.wisc.edu\/gilbert\/wp-content\/uploads\/sites\/3\/2017\/08\/nautilus-300x199.jpg 300w\" sizes=\"auto, (max-width: 500px) 100vw, 500px\" \/><button\n\t\t\tclass=\"lightbox-trigger\"\n\t\t\ttype=\"button\"\n\t\t\taria-haspopup=\"dialog\"\n\t\t\taria-label=\"Enlarge\"\n\t\t\tdata-wp-init=\"callbacks.initTriggerButton\"\n\t\t\tdata-wp-on--click=\"actions.showLightbox\"\n\t\t\tdata-wp-style--right=\"state.imageButtonRight\"\n\t\t\tdata-wp-style--top=\"state.imageButtonTop\"\n\t\t>\n\t\t\t<svg xmlns=\"http:\/\/www.w3.org\/2000\/svg\" width=\"12\" height=\"12\" fill=\"none\" viewBox=\"0 0 12 12\">\n\t\t\t\t<path fill=\"#fff\" d=\"M2 0a2 2 0 0 0-2 2v2h1.5V2a.5.5 0 0 1 .5-.5h2V0H2Zm2 10.5H2a.5.5 0 0 1-.5-.5V8H0v2a2 2 0 0 0 2 2h2v-1.5ZM8 12v-1.5h2a.5.5 0 0 0 .5-.5V8H12v2a2 2 0 0 1-2 2H8Zm2-12a2 2 0 0 1 2 2v2h-1.5V2a.5.5 0 0 0-.5-.5H8V0h2Z\" \/>\n\t\t\t<\/svg>\n\t\t<\/button><figcaption class=\"wp-element-caption\">Nautilus pompilius, a cephalopod. The inner surface of the shell is nacre. Shell diameter is ~18 cm. Courtesy of Pupa Gilbert, University of Wisconsin, Madison. <\/figcaption><\/figure><figure data-wp-context=\"{&quot;imageId&quot;:&quot;69e97efc4ac6a&quot;}\" data-wp-interactive=\"core\/image\" data-wp-key=\"69e97efc4ac6a\" class=\"wp-block-image size-large wp-lightbox-container\"><img loading=\"lazy\" decoding=\"async\" width=\"360\" height=\"240\" data-wp-class--hide=\"state.isContentHidden\" data-wp-class--show=\"state.isContentVisible\" data-wp-init=\"callbacks.setButtonStyles\" data-wp-on--click=\"actions.showLightbox\" data-wp-on--load=\"callbacks.setButtonStyles\" data-wp-on-window--resize=\"callbacks.setButtonStyles\" data-id=\"191\" src=\"https:\/\/home.physics.wisc.edu\/gilbert\/wp-content\/uploads\/sites\/3\/2017\/08\/pinctada_margaritifera.jpg\" alt=\"\" class=\"wp-image-191\" srcset=\"https:\/\/home.physics.wisc.edu\/gilbert\/wp-content\/uploads\/sites\/3\/2017\/08\/pinctada_margaritifera.jpg 360w, https:\/\/home.physics.wisc.edu\/gilbert\/wp-content\/uploads\/sites\/3\/2017\/08\/pinctada_margaritifera-300x200.jpg 300w\" sizes=\"auto, (max-width: 360px) 100vw, 360px\" \/><button\n\t\t\tclass=\"lightbox-trigger\"\n\t\t\ttype=\"button\"\n\t\t\taria-haspopup=\"dialog\"\n\t\t\taria-label=\"Enlarge\"\n\t\t\tdata-wp-init=\"callbacks.initTriggerButton\"\n\t\t\tdata-wp-on--click=\"actions.showLightbox\"\n\t\t\tdata-wp-style--right=\"state.imageButtonRight\"\n\t\t\tdata-wp-style--top=\"state.imageButtonTop\"\n\t\t>\n\t\t\t<svg xmlns=\"http:\/\/www.w3.org\/2000\/svg\" width=\"12\" height=\"12\" fill=\"none\" viewBox=\"0 0 12 12\">\n\t\t\t\t<path fill=\"#fff\" d=\"M2 0a2 2 0 0 0-2 2v2h1.5V2a.5.5 0 0 1 .5-.5h2V0H2Zm2 10.5H2a.5.5 0 0 1-.5-.5V8H0v2a2 2 0 0 0 2 2h2v-1.5ZM8 12v-1.5h2a.5.5 0 0 0 .5-.5V8H12v2a2 2 0 0 1-2 2H8Zm2-12a2 2 0 0 1 2 2v2h-1.5V2a.5.5 0 0 0-.5-.5H8V0h2Z\" \/>\n\t\t\t<\/svg>\n\t\t<\/button><figcaption class=\"wp-element-caption\">Pinctada margaritifera, a bivalve, also known as the &quot;black pearl oyster&quot;. Notice at the center of the image, a seeded and fully grown pearl making the mollusk&#039;s pocket bulge. This bivalve, cultured for pearl production in French Polynesia, has a diameter of 10 cm. <\/figcaption><\/figure><figure data-wp-context=\"{&quot;imageId&quot;:&quot;69e97efc4b3a8&quot;}\" data-wp-interactive=\"core\/image\" data-wp-key=\"69e97efc4b3a8\" class=\"wp-block-image size-large wp-lightbox-container\"><img loading=\"lazy\" decoding=\"async\" width=\"360\" height=\"240\" data-wp-class--hide=\"state.isContentHidden\" data-wp-class--show=\"state.isContentVisible\" data-wp-init=\"callbacks.setButtonStyles\" data-wp-on--click=\"actions.showLightbox\" data-wp-on--load=\"callbacks.setButtonStyles\" data-wp-on-window--resize=\"callbacks.setButtonStyles\" data-id=\"192\" src=\"https:\/\/home.physics.wisc.edu\/gilbert\/wp-content\/uploads\/sites\/3\/2017\/08\/black_pearls.jpg\" alt=\"\" class=\"wp-image-192\" srcset=\"https:\/\/home.physics.wisc.edu\/gilbert\/wp-content\/uploads\/sites\/3\/2017\/08\/black_pearls.jpg 360w, https:\/\/home.physics.wisc.edu\/gilbert\/wp-content\/uploads\/sites\/3\/2017\/08\/black_pearls-300x200.jpg 300w\" sizes=\"auto, (max-width: 360px) 100vw, 360px\" \/><button\n\t\t\tclass=\"lightbox-trigger\"\n\t\t\ttype=\"button\"\n\t\t\taria-haspopup=\"dialog\"\n\t\t\taria-label=\"Enlarge\"\n\t\t\tdata-wp-init=\"callbacks.initTriggerButton\"\n\t\t\tdata-wp-on--click=\"actions.showLightbox\"\n\t\t\tdata-wp-style--right=\"state.imageButtonRight\"\n\t\t\tdata-wp-style--top=\"state.imageButtonTop\"\n\t\t>\n\t\t\t<svg xmlns=\"http:\/\/www.w3.org\/2000\/svg\" width=\"12\" height=\"12\" fill=\"none\" viewBox=\"0 0 12 12\">\n\t\t\t\t<path fill=\"#fff\" d=\"M2 0a2 2 0 0 0-2 2v2h1.5V2a.5.5 0 0 1 .5-.5h2V0H2Zm2 10.5H2a.5.5 0 0 1-.5-.5V8H0v2a2 2 0 0 0 2 2h2v-1.5ZM8 12v-1.5h2a.5.5 0 0 0 .5-.5V8H12v2a2 2 0 0 1-2 2H8Zm2-12a2 2 0 0 1 2 2v2h-1.5V2a.5.5 0 0 0-.5-.5H8V0h2Z\" \/>\n\t\t\t<\/svg>\n\t\t<\/button><figcaption class=\"wp-element-caption\">Tahitian black pearls, produced by Pinctada margaritifera, as shown in the previous image. The shape, diameter, and color of the pearls determine their jewelry quality. Here 8 very precious, perfectly spherical pearls are shown, with diameter 8 mm, and assorted colors. <\/figcaption><\/figure><\/figure><\/div><\/div><\/div><\/div>","protected":false},"excerpt":{"rendered":"<p>The nacre layer, or mother of pearl, at the inner surface of the abalone shell and of other mollusk shells and pearls (see images below) has a fracture resistance 3000 times greater than that of aragonite, the pure mineral of which it is composed. The toughening effect is due to well-defined nanolayers of organics at&hellip;<\/p>\n","protected":false},"author":1,"featured_media":0,"parent":0,"menu_order":0,"comment_status":"closed","ping_status":"closed","template":"","meta":{"_acf_changed":false,"_uw_migration_status":"in-progress","_uw_gutenberg_post_content_before_migration":"","footnotes":""},"class_list":["post-179","page","type-page","status-publish","hentry"],"acf":[],"_links":{"self":[{"href":"https:\/\/home.physics.wisc.edu\/gilbert\/wp-json\/wp\/v2\/pages\/179","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/home.physics.wisc.edu\/gilbert\/wp-json\/wp\/v2\/pages"}],"about":[{"href":"https:\/\/home.physics.wisc.edu\/gilbert\/wp-json\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"https:\/\/home.physics.wisc.edu\/gilbert\/wp-json\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/home.physics.wisc.edu\/gilbert\/wp-json\/wp\/v2\/comments?post=179"}],"version-history":[{"count":15,"href":"https:\/\/home.physics.wisc.edu\/gilbert\/wp-json\/wp\/v2\/pages\/179\/revisions"}],"predecessor-version":[{"id":1194,"href":"https:\/\/home.physics.wisc.edu\/gilbert\/wp-json\/wp\/v2\/pages\/179\/revisions\/1194"}],"wp:attachment":[{"href":"https:\/\/home.physics.wisc.edu\/gilbert\/wp-json\/wp\/v2\/media?parent=179"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}