{"id":977,"date":"2020-03-11T20:44:54","date_gmt":"2020-03-12T00:44:27","guid":{"rendered":"http:\/\/www.nuclearphysicslab.com\/npl\/?page_id=977"},"modified":"2023-05-22T19:15:45","modified_gmt":"2023-05-22T23:15:45","slug":"trinitite","status":"publish","type":"page","link":"http:\/\/www.nuclearphysicslab.com\/npl\/npl-home\/spectroscopy\/gamma-ray-spectroscopy\/trinitite\/","title":{"rendered":"Trinitite"},"content":{"rendered":"\n<p class=\"has-text-align-center\"><em>Author: Tim<\/em><\/p>\n\n\n\n<p>Trinitite is the sand-turned-glass remnant of the first atomic bomb, the Trinity test, detonated July 16th, 1945 in Alamogordo NM, deep in the White Sands Missile Range.  The test shot was a demonstration of the plutonium based implosion-type nuclear device.  It worked.  During the shot a subcritical shell of 239Pu was compressed into a super-critical assembly that fissioned for about 80 generations before it &#8220;self-disassembled.&#8221; That all occurred within a few microseconds.  During the brief event an intense burst of neutrons were generated and activated many of the nearby materials.  In addition to neutron activated materials, some of the core obviously fissioned, leaving behind many fission products, some that have long half lives.  Finally, most of the 239Pu core went unused, and was scattered about.<\/p>\n\n\n\n<p>The updraft of fireball sucked the desert sand into the fire ball, melting it and mixing and churning in the activation products, the fission products, and un-spent core materials.  As the explosion evolved, the sand-fission product stew rained back down on the cold desert floor, solidifying into a green glass.  Today, it is mildly radioactive and will make a geiger counter respond.  <\/p>\n\n\n\n<p>Gathering a largish quantity, here about two pounds, we can perform long, background-subtracted, counts (48 hours or more) in a low-background shield.  It is interested to see what we can pull out of the spectrum.  <\/p>\n\n\n\n<p>This particular sample Tim purchased from a custodian of the Wallace Smith Collection.<\/p>\n\n\n\n<figure class=\"wp-block-image size-large\"><a href=\"http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/IMG_4445.jpg\"><img loading=\"lazy\" width=\"2448\" height=\"3264\" src=\"http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/IMG_4445.jpg\" alt=\"\" class=\"wp-image-978\" srcset=\"http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/IMG_4445.jpg 2448w, http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/IMG_4445-1875x2500.jpg 1875w, http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/IMG_4445-768x1024.jpg 768w, http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/IMG_4445-1152x1536.jpg 1152w, http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/IMG_4445-1536x2048.jpg 1536w, http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/IMG_4445-203x270.jpg 203w\" sizes=\"(max-width: 2448px) 100vw, 2448px\" \/><\/a><figcaption>A Marinelli beaker, which aims to optimize the sample&#8217;s geometry to make best use of the HPGe detector.<\/figcaption><\/figure>\n\n\n\n<figure class=\"wp-block-image size-large\"><a href=\"http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/IMG_4446.jpg\"><img loading=\"lazy\" width=\"2448\" height=\"3264\" src=\"http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/IMG_4446.jpg\" alt=\"\" class=\"wp-image-979\" srcset=\"http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/IMG_4446.jpg 2448w, http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/IMG_4446-1875x2500.jpg 1875w, http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/IMG_4446-768x1024.jpg 768w, http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/IMG_4446-1152x1536.jpg 1152w, http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/IMG_4446-1536x2048.jpg 1536w, http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/IMG_4446-203x270.jpg 203w\" sizes=\"(max-width: 2448px) 100vw, 2448px\" \/><\/a><figcaption>The detector, ready to receive the sample.<\/figcaption><\/figure>\n\n\n\n<figure class=\"wp-block-image size-large\"><a href=\"http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/IMG_4447.jpg\"><img loading=\"lazy\" width=\"2448\" height=\"3264\" src=\"http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/IMG_4447.jpg\" alt=\"\" class=\"wp-image-980\" srcset=\"http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/IMG_4447.jpg 2448w, http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/IMG_4447-1875x2500.jpg 1875w, http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/IMG_4447-768x1024.jpg 768w, http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/IMG_4447-1152x1536.jpg 1152w, http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/IMG_4447-1536x2048.jpg 1536w, http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/IMG_4447-203x270.jpg 203w\" sizes=\"(max-width: 2448px) 100vw, 2448px\" \/><\/a><figcaption>Demonstrating the &#8220;fill factor&#8221; of the detector in Marinelli beaker re-entrant volume.<\/figcaption><\/figure>\n\n\n\n<figure class=\"wp-block-image size-large\"><a href=\"http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/IMG_4448.jpg\"><img loading=\"lazy\" width=\"2448\" height=\"3264\" src=\"http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/IMG_4448.jpg\" alt=\"\" class=\"wp-image-981\" srcset=\"http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/IMG_4448.jpg 2448w, http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/IMG_4448-1875x2500.jpg 1875w, http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/IMG_4448-768x1024.jpg 768w, http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/IMG_4448-1152x1536.jpg 1152w, http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/IMG_4448-1536x2048.jpg 1536w, http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/IMG_4448-203x270.jpg 203w\" sizes=\"(max-width: 2448px) 100vw, 2448px\" \/><\/a><figcaption>The Trinitite has been carefully packed into the Marinelli beaker to achieve greatest density.<\/figcaption><\/figure>\n\n\n\n<figure class=\"wp-block-image size-large\"><a href=\"http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/IMG_4450.jpg\"><img loading=\"lazy\" width=\"2448\" height=\"3264\" src=\"http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/IMG_4450.jpg\" alt=\"\" class=\"wp-image-982\" srcset=\"http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/IMG_4450.jpg 2448w, http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/IMG_4450-1875x2500.jpg 1875w, http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/IMG_4450-768x1024.jpg 768w, http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/IMG_4450-1152x1536.jpg 1152w, http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/IMG_4450-1536x2048.jpg 1536w, http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/IMG_4450-203x270.jpg 203w\" sizes=\"(max-width: 2448px) 100vw, 2448px\" \/><\/a><figcaption>The larger pieces on top.<\/figcaption><\/figure>\n\n\n\n<figure class=\"wp-block-image size-large\"><a href=\"http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/IMG_4451.jpg\"><img loading=\"lazy\" width=\"2448\" height=\"3264\" src=\"http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/IMG_4451.jpg\" alt=\"\" class=\"wp-image-983\" srcset=\"http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/IMG_4451.jpg 2448w, http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/IMG_4451-1875x2500.jpg 1875w, http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/IMG_4451-768x1024.jpg 768w, http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/IMG_4451-1152x1536.jpg 1152w, http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/IMG_4451-1536x2048.jpg 1536w, http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/IMG_4451-203x270.jpg 203w\" sizes=\"(max-width: 2448px) 100vw, 2448px\" \/><\/a><\/figure>\n\n\n\n<figure class=\"wp-block-image size-large\"><a href=\"http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/IMG_4452-copy.jpg\"><img loading=\"lazy\" width=\"2448\" height=\"3264\" src=\"http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/IMG_4452-copy.jpg\" alt=\"\" class=\"wp-image-1097\" srcset=\"http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/IMG_4452-copy.jpg 2448w, http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/IMG_4452-copy-1875x2500.jpg 1875w, http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/IMG_4452-copy-768x1024.jpg 768w, http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/IMG_4452-copy-1152x1536.jpg 1152w, http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/IMG_4452-copy-1536x2048.jpg 1536w, http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/IMG_4452-copy-203x270.jpg 203w\" sizes=\"(max-width: 2448px) 100vw, 2448px\" \/><\/a><figcaption>Ready to count.<\/figcaption><\/figure>\n\n\n\n<figure class=\"wp-block-image size-large\"><a href=\"http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/IMG_4454.jpg\"><img loading=\"lazy\" width=\"3264\" height=\"2448\" src=\"http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/IMG_4454.jpg\" alt=\"\" class=\"wp-image-1098\" srcset=\"http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/IMG_4454.jpg 3264w, http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/IMG_4454-768x576.jpg 768w, http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/IMG_4454-1536x1152.jpg 1536w, http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/IMG_4454-2048x1536.jpg 2048w, http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/IMG_4454-360x270.jpg 360w\" sizes=\"(max-width: 3264px) 100vw, 3264px\" \/><\/a><\/figure>\n\n\n\n<figure class=\"wp-block-image size-large\"><a href=\"http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/Screen-Shot-2020-03-11-at-8.19.49-PM.png\"><img loading=\"lazy\" width=\"2192\" height=\"1776\" src=\"http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/Screen-Shot-2020-03-11-at-8.19.49-PM.png\" alt=\"\" class=\"wp-image-1100\" srcset=\"http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/Screen-Shot-2020-03-11-at-8.19.49-PM.png 2192w, http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/Screen-Shot-2020-03-11-at-8.19.49-PM-768x622.png 768w, http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/Screen-Shot-2020-03-11-at-8.19.49-PM-1536x1244.png 1536w, http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/Screen-Shot-2020-03-11-at-8.19.49-PM-2048x1659.png 2048w, http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/Screen-Shot-2020-03-11-at-8.19.49-PM-333x270.png 333w\" sizes=\"(max-width: 2192px) 100vw, 2192px\" \/><\/a><\/figure>\n\n\n\n<p>Pursuing a needle in a haystack, Bill Kolb said I should still be able to find Co60 in Trinitite.  After a 48 hour count, there is in fact a hint.  That Co60 was formed during the evaporation of the Trinity test tower.  This is remarkable, as the half life of Co-60 is only 5.27 years, 12.3 half lives ago&#8230; or 0.02% of this original Co-60 remaining.<\/p>\n\n\n\n<p>There are plenty of other interesting lines, such as Cs-137, Eu-152, Ba-133 and more.<\/p>\n\n\n\n<figure class=\"wp-block-image size-large\"><a href=\"http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/Screen-Shot-2020-03-18-at-9.05.23-PM.png\"><img loading=\"lazy\" width=\"3088\" height=\"1690\" src=\"http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/Screen-Shot-2020-03-18-at-9.05.23-PM.png\" alt=\"\" class=\"wp-image-2267\" srcset=\"http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/Screen-Shot-2020-03-18-at-9.05.23-PM.png 3088w, http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/Screen-Shot-2020-03-18-at-9.05.23-PM-768x420.png 768w, http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/Screen-Shot-2020-03-18-at-9.05.23-PM-1536x841.png 1536w, http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/Screen-Shot-2020-03-18-at-9.05.23-PM-2048x1121.png 2048w, http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/Screen-Shot-2020-03-18-at-9.05.23-PM-493x270.png 493w\" sizes=\"(max-width: 3088px) 100vw, 3088px\" \/><\/a><figcaption>This is a 48-hour long, background subtracted count of the Trinitite filled Marinelli Beaker.<\/figcaption><\/figure>\n\n\n\n<figure class=\"wp-block-image size-large\"><a href=\"http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/Screen-Shot-2020-03-18-at-9.11.50-PM.png\"><img loading=\"lazy\" width=\"3320\" height=\"1964\" src=\"http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/Screen-Shot-2020-03-18-at-9.11.50-PM.png\" alt=\"\" class=\"wp-image-2268\" srcset=\"http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/Screen-Shot-2020-03-18-at-9.11.50-PM.png 3320w, http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/Screen-Shot-2020-03-18-at-9.11.50-PM-768x454.png 768w, http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/Screen-Shot-2020-03-18-at-9.11.50-PM-1536x909.png 1536w, http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/Screen-Shot-2020-03-18-at-9.11.50-PM-2048x1212.png 2048w, http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/Screen-Shot-2020-03-18-at-9.11.50-PM-456x270.png 456w\" sizes=\"(max-width: 3320px) 100vw, 3320px\" \/><\/a><figcaption>Log Scale: The two regions of interest highlighted in red are the two lines of Co-60.<\/figcaption><\/figure>\n\n\n\n<figure class=\"wp-block-image size-large\"><a href=\"http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/Screen-Shot-2020-03-18-at-9.11.28-PM.png\"><img loading=\"lazy\" width=\"3324\" height=\"1970\" src=\"http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/Screen-Shot-2020-03-18-at-9.11.28-PM.png\" alt=\"\" class=\"wp-image-2269\" srcset=\"http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/Screen-Shot-2020-03-18-at-9.11.28-PM.png 3324w, http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/Screen-Shot-2020-03-18-at-9.11.28-PM-768x455.png 768w, http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/Screen-Shot-2020-03-18-at-9.11.28-PM-1536x910.png 1536w, http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/Screen-Shot-2020-03-18-at-9.11.28-PM-2048x1214.png 2048w, http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/Screen-Shot-2020-03-18-at-9.11.28-PM-456x270.png 456w\" sizes=\"(max-width: 3324px) 100vw, 3324px\" \/><\/a><figcaption>Lin Scale: The two regions of interest highlighted in red are the two lines of Co-60.<\/figcaption><\/figure>\n\n\n\n<figure class=\"wp-block-image size-large\"><a href=\"http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/Screen-Shot-2020-03-18-at-9.10.51-PM.png\"><img loading=\"lazy\" width=\"3318\" height=\"1960\" src=\"http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/Screen-Shot-2020-03-18-at-9.10.51-PM.png\" alt=\"\" class=\"wp-image-2270\" srcset=\"http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/Screen-Shot-2020-03-18-at-9.10.51-PM.png 3318w, http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/Screen-Shot-2020-03-18-at-9.10.51-PM-768x454.png 768w, http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/Screen-Shot-2020-03-18-at-9.10.51-PM-1536x907.png 1536w, http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/Screen-Shot-2020-03-18-at-9.10.51-PM-2048x1210.png 2048w, http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/Screen-Shot-2020-03-18-at-9.10.51-PM-457x270.png 457w\" sizes=\"(max-width: 3318px) 100vw, 3318px\" \/><\/a><figcaption>Zoom in on the two  lines of Co-60.<\/figcaption><\/figure>\n\n\n\n<figure class=\"wp-block-image size-large\"><a href=\"http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/Screen-Shot-2020-03-18-at-9.12.25-PM.png\"><img loading=\"lazy\" width=\"3322\" height=\"1962\" src=\"http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/Screen-Shot-2020-03-18-at-9.12.25-PM.png\" alt=\"\" class=\"wp-image-2271\" srcset=\"http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/Screen-Shot-2020-03-18-at-9.12.25-PM.png 3322w, http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/Screen-Shot-2020-03-18-at-9.12.25-PM-768x454.png 768w, http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/Screen-Shot-2020-03-18-at-9.12.25-PM-1536x907.png 1536w, http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/Screen-Shot-2020-03-18-at-9.12.25-PM-2048x1210.png 2048w, http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/Screen-Shot-2020-03-18-at-9.12.25-PM-457x270.png 457w\" sizes=\"(max-width: 3322px) 100vw, 3322px\" \/><\/a><figcaption>Many lines of Eu-152, and of course Cs-137<\/figcaption><\/figure>\n\n\n\n<p>Ba-133 is interesting because it was formed from the barium in the baratol high explosive compound used in the Trinity explosion.<\/p>\n\n\n\n<figure class=\"wp-block-image size-large\"><a href=\"http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/Screen-Shot-2020-03-18-at-10.22.35-PM.png\"><img loading=\"lazy\" width=\"3086\" height=\"1692\" src=\"http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/Screen-Shot-2020-03-18-at-10.22.35-PM.png\" alt=\"\" class=\"wp-image-2279\" srcset=\"http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/Screen-Shot-2020-03-18-at-10.22.35-PM.png 3086w, http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/Screen-Shot-2020-03-18-at-10.22.35-PM-768x421.png 768w, http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/Screen-Shot-2020-03-18-at-10.22.35-PM-1536x842.png 1536w, http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/Screen-Shot-2020-03-18-at-10.22.35-PM-2048x1123.png 2048w, http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/Screen-Shot-2020-03-18-at-10.22.35-PM-492x270.png 492w\" sizes=\"(max-width: 3086px) 100vw, 3086px\" \/><\/a><figcaption>Gamma ray lines belonging to Ba-133<\/figcaption><\/figure>\n\n\n\n<figure class=\"wp-block-image size-large\"><a href=\"http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/Screen-Shot-2020-03-18-at-10.21.52-PM.png\"><img loading=\"lazy\" width=\"3088\" height=\"1690\" src=\"http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/Screen-Shot-2020-03-18-at-10.21.52-PM.png\" alt=\"\" class=\"wp-image-2275\" srcset=\"http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/Screen-Shot-2020-03-18-at-10.21.52-PM.png 3088w, http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/Screen-Shot-2020-03-18-at-10.21.52-PM-768x420.png 768w, http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/Screen-Shot-2020-03-18-at-10.21.52-PM-1536x841.png 1536w, http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/Screen-Shot-2020-03-18-at-10.21.52-PM-2048x1121.png 2048w, http:\/\/www.nuclearphysicslab.com\/npl\/wp-content\/uploads\/Screen-Shot-2020-03-18-at-10.21.52-PM-493x270.png 493w\" sizes=\"(max-width: 3088px) 100vw, 3088px\" \/><\/a><figcaption>Gamma ray lines belonging to Ba-133<\/figcaption><\/figure>\n","protected":false},"excerpt":{"rendered":"<p>Author: Tim Trinitite is the sand-turned-glass remnant of the first atomic bomb, the Trinity test, detonated July 16th, 1945 in Alamogordo NM, deep in the White Sands Missile Range. The test shot was a demonstration of the plutonium based implosion-type nuclear device. It worked. During the shot a subcritical shell of 239Pu was compressed&#8230;<\/p>\n<p class=\"read-more\"><a class=\"btn btn-default\" href=\"http:\/\/www.nuclearphysicslab.com\/npl\/npl-home\/spectroscopy\/gamma-ray-spectroscopy\/trinitite\/\"> Read More<span class=\"screen-reader-text\">  Read More<\/span><\/a><\/p>\n","protected":false},"author":3,"featured_media":206,"parent":25,"menu_order":5,"comment_status":"open","ping_status":"closed","template":"","meta":{"advanced-sidebar-menu\/link-title":"","advanced-sidebar-menu\/exclude-page":false},"categories":[49],"tags":[],"_links":{"self":[{"href":"http:\/\/www.nuclearphysicslab.com\/npl\/wp-json\/wp\/v2\/pages\/977"}],"collection":[{"href":"http:\/\/www.nuclearphysicslab.com\/npl\/wp-json\/wp\/v2\/pages"}],"about":[{"href":"http:\/\/www.nuclearphysicslab.com\/npl\/wp-json\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"http:\/\/www.nuclearphysicslab.com\/npl\/wp-json\/wp\/v2\/users\/3"}],"replies":[{"embeddable":true,"href":"http:\/\/www.nuclearphysicslab.com\/npl\/wp-json\/wp\/v2\/comments?post=977"}],"version-history":[{"count":14,"href":"http:\/\/www.nuclearphysicslab.com\/npl\/wp-json\/wp\/v2\/pages\/977\/revisions"}],"predecessor-version":[{"id":2284,"href":"http:\/\/www.nuclearphysicslab.com\/npl\/wp-json\/wp\/v2\/pages\/977\/revisions\/2284"}],"up":[{"embeddable":true,"href":"http:\/\/www.nuclearphysicslab.com\/npl\/wp-json\/wp\/v2\/pages\/25"}],"wp:featuredmedia":[{"embeddable":true,"href":"http:\/\/www.nuclearphysicslab.com\/npl\/wp-json\/wp\/v2\/media\/206"}],"wp:attachment":[{"href":"http:\/\/www.nuclearphysicslab.com\/npl\/wp-json\/wp\/v2\/media?parent=977"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"http:\/\/www.nuclearphysicslab.com\/npl\/wp-json\/wp\/v2\/categories?post=977"},{"taxonomy":"post_tag","embeddable":true,"href":"http:\/\/www.nuclearphysicslab.com\/npl\/wp-json\/wp\/v2\/tags?post=977"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}