{"id":3977,"date":"2026-09-04T08:14:39","date_gmt":"2026-09-04T08:14:39","guid":{"rendered":"https:\/\/nbaem.com\/?p=3977"},"modified":"2026-08-23T04:16:51","modified_gmt":"2026-08-23T04:16:51","slug":"what-elements-are-magnetic","status":"publish","type":"post","link":"https:\/\/nbaem.com\/et\/what-elements-are-magnetic\/","title":{"rendered":"What Elements Are Magnetic Top Magnetic Metals Guide"},"content":{"rendered":"<h2>The Science Behind Magnetic Elements<\/h2>\n<p>Engineers and material designers frequently ask us why specific elements exhibit strong magnetic pull while others remain functionally non-responsive. Magnetism originates at the subatomic level, dictated by electron configuration, orbital shell filling, and quantum mechanical interactions.<\/p>\n<h3>Unpaired Electron Spins and Atomic Dipoles<\/h3>\n<p>An element&#8217;s macro-level magnetic capability depends directly on its subatomic electron structure.<\/p>\n<ul>\n<li style=\"list-style-type: none;\">\n<ul>\n<li><strong>d-Orbital and f-Orbital Mechanics:<\/strong> In transition metals and rare-earth elements, incompletely filled d-orbitals and f-orbitals harbor <strong>unpaired electron spins<\/strong>.<\/li>\n<li><strong>Net Magnetic Dipoles:<\/strong> When electrons are paired, their equal and opposite quantum spins cancel each other out. <strong>Unpaired electron spins<\/strong> generate an uncompensated magnetic moment, transforming individual atoms into microscopic magnetic dipoles.<\/li>\n<\/ul>\n<\/li>\n<\/ul>\n<h3>Exchange Interactions and Magnetic Domains<\/h3>\n<p>Individual atomic dipoles must cooperate to generate measurable field strength.<\/p>\n<ul>\n<li style=\"list-style-type: none;\">\n<ul>\n<li><strong>Exchange Coupling:<\/strong> Powerful quantum interactions force neighboring electron spins within a <strong>magnetic crystal lattice<\/strong> to align parallel to one another.<\/li>\n<li><strong>Magnetic Domains:<\/strong> These aligned atomic groups form microscopic magnetic domains. In an unmagnetized state, these domains point in random directions, canceling net field output. Applying an external field aligns these domains, dramatically raising overall <strong>magnetic permeability<\/strong>.<\/li>\n<\/ul>\n<\/li>\n<\/ul>\n<h3>Four Primary Types of Magnetic Behavior<\/h3>\n<p>We classify elemental magnetic behavior into four core structural categories based on orbital stability and field response:<\/p>\n<ul>\n<li style=\"list-style-type: none;\">\n<ul>\n<li><strong>Ferromagnetism:<\/strong> Strong, spontaneous alignment of atomic magnetic domains. <strong>Ferromagnetic elements<\/strong> exhibit high field amplification and retain permanent magnetization after external fields are removed.<\/li>\n<li><strong>Paramagnetism:<\/strong> Weak, temporary attraction to magnetic fields caused by scattered unpaired spins. <strong>Paramagnetic metals<\/strong> lose all measurable magnet strength instantly once the external magnetic field disappears.<\/li>\n<li><strong>Diamagnetism:<\/strong> A universal, extremely weak magnetic repulsion occurring in elements where all electrons are paired. Diamagnetism is present in all matter but is completely masked in materials displaying paramagnetic or ferromagnetic properties.<\/li>\n<li><strong>Ferrimagnetism:<\/strong> Occurs when adjacent magnetic sub-lattices align antiparallel but hold unequal magnetic moments, creating a permanent net magnetic dipole (commonly seen in structural oxides and ceramic compounds rather than pure metals).<\/li>\n<\/ul>\n<\/li>\n<\/ul>\n<h2>Ferromagnetic Elements and Rare-Earth Metals<\/h2>\n<p>Only a select few pure elements exhibit strong intrinsic magnetic properties at standard conditions. When evaluating <strong>what elements are magnetic<\/strong>, we categorize them into primary room-temperature transition metals and heavy rare-earth elements used for high-performance alloy stabilization.<\/p>\n<h3>Room-Temperature Transition Metals<\/h3>\n<p>At standard ambient room temperature (20\u00b0C \/ 68\u00b0F), only three elemental metals exhibit pure ferromagnetism:<\/p>\n<ul>\n<li style=\"list-style-type: none;\">\n<ul>\n<li><strong>Iron (Fe):<\/strong> Delivers the highest magnetic saturation among pure elements. It serves as the primary base for structural magnetic cores and electrical steels.<\/li>\n<li><strong>Cobalt (Co):<\/strong> Features the highest Curie temperature (1,121\u00b0C) of any element. We utilize cobalt to retain magnetic alignment and structural integrity under severe thermal stress.<\/li>\n<li><strong>Nickel (Ni):<\/strong> Combines moderate ferromagnetism with strong corrosion resistance and high initial permeability, making it critical for magnetic shielding and soft alloys.<\/li>\n<\/ul>\n<\/li>\n<\/ul>\n<p>When we engineer heavy-duty power transmission hardware like a <a href=\"https:\/\/nbaem.com\/et\/what-is-mining-magnetic-coupling-and-how-it-works\/\">mining magnetic coupling<\/a>, leveraging the fundamental properties of these transition metals ensures reliable torque transfer and long-term mechanical durability.<\/p>\n<h3>Rare-Earth Elements and Thermal Stabilizers<\/h3>\n<p>Heavy rare-earth metals possess localized unpaired 4f electrons, providing exceptional magnetic dipole moments:<\/p>\n<ul>\n<li style=\"list-style-type: none;\">\n<ul>\n<li><strong>Gadolinium (Gd):<\/strong> The only rare-earth element with a Curie point near ambient conditions (20\u00b0C \/ 293 K). It sits precisely on the border between ferromagnetism and paramagnetism at room temperature.<\/li>\n<li><strong>Dysprosium (Dy) and Terbium (Tb):<\/strong> Although only ferromagnetic at cryogenic temperatures in their pure elemental form, we incorporate Dy and Tb into sintered NdFeB magnet lattices. This grain-boundary diffusion process drastically boosts intrinsic coercivity ($H_{cj}$), protecting assemblies from high-temperature demagnetization.<\/li>\n<\/ul>\n<\/li>\n<\/ul>\n<h2>From Pure Elements to High-Performance Commercial Alloys<\/h2>\n<p>Understanding <strong>what elements are magnetic<\/strong> is only the foundation. In real-world industrial environments, pure ferromagnetic elements like iron, nickel, and cobalt rarely suffice due to substantial material limitations:<\/p>\n<ul>\n<li style=\"list-style-type: none;\">\n<ul>\n<li><strong>Low Coercivity:<\/strong> Pure metals demagnetize easily when exposed to reverse magnetic fields or mechanical impact.<\/li>\n<li><strong>High Corrosion Risk:<\/strong> Raw iron and pure rare-earth metals oxidize rapidly in ambient atmospheric conditions.<\/li>\n<li><strong>Thermal Instability:<\/strong> Pure elemental magnetic domains lose alignment at relatively low operational temperatures.<\/li>\n<\/ul>\n<\/li>\n<\/ul>\n<h3>Commercial Permanent Magnet Alloys<\/h3>\n<p>To overcome these limitations, we engineer hard magnetic materials by combining transition metals with rare earths. This alloy design delivers superior remanence and coercivity across distinct commercial magnet families:<\/p>\n<ul>\n<li style=\"list-style-type: none;\">\n<ul>\n<li><strong>Neodymium Iron Boron (Nd2Fe14B):<\/strong> Produces the highest maximum energy product for compact, high-torque designs, though it requires protective coatings against oxidation.<\/li>\n<li><strong>Samarium-Cobalt Alloys (SmCo):<\/strong> Offers exceptional heat tolerance and intrinsic corrosion resistance up to 350\u00b0C. When evaluating <a href=\"https:\/\/nbaem.com\/et\/samarium-cobalt-vs-neodymium-magnets\/\">samarium-cobalt vs neodymium magnets<\/a>, operating temperature limits and environmental exposure dictate the material selection.<\/li>\n<li><strong>AlNiCo and FeCrCo:<\/strong> Provide extreme Curie temperatures, low temperature coefficients, and superior machinability for specialized sensors and metering devices.<\/li>\n<li><strong>Ferrite (Ceramic):<\/strong> Delivers cost-effective, highly rust-proof performance for high-volume electrical and industrial applications.<\/li>\n<\/ul>\n<\/li>\n<\/ul>\n<p>Engineers often ask <a href=\"https:\/\/nbaem.com\/et\/are-samarium-cobalt-magnets-stronger-than-neodymium\/\">are samarium-cobalt magnets stronger than neodymium<\/a> for heavy-duty drive systems. While NdFeB offers higher raw power at room temperature, SmCo retains far greater structural magnetic strength in elevated thermal environments.<\/p>\n<h2>Thermal Limits and Curie Temperature<\/h2>\n<p>The Curie temperature ($T_C$) is the critical thermal threshold where ferromagnetic elements lose their permanent magnetic order and transition into a paramagnetic state. Above this temperature, thermal energy disrupts the exchange interactions that keep unpaired electron spins aligned in magnetic domains. Knowing what elements are magnetic and their thermal boundaries helps us engineer assemblies that withstand extreme operational conditions without catastrophic loss of remanence.<\/p>\n<h3>Curie Temperature vs. Working Temperature Limits<\/h3>\n<p>While pure elements like Iron, Cobalt, and Nickel define baseline atomic thermal thresholds, commercial alloys are tailored for specific industrial working environments.<\/p>\n<table>\n<thead>\n<tr>\n<th style=\"text-align: left;\">Material \/ Grade<\/th>\n<th style=\"text-align: left;\">Material Type<\/th>\n<th style=\"text-align: left;\">Curie Temperature ($T_C$)<\/th>\n<th style=\"text-align: left;\">Max Operating Temp<\/th>\n<th style=\"text-align: left;\">Thermal Characteristic<\/th>\n<\/tr>\n<\/thead>\n<tbody>\n<tr>\n<td style=\"text-align: left;\"><strong>Cobalt (Co)<\/strong><\/td>\n<td style=\"text-align: left;\">Pure Element<\/td>\n<td style=\"text-align: left;\">1121\u00b0C (2050\u00b0F)<\/td>\n<td style=\"text-align: left;\">~500\u00b0C<\/td>\n<td style=\"text-align: left;\">Highest thermal stability of all pure metals<\/td>\n<\/tr>\n<tr>\n<td style=\"text-align: left;\"><strong>Iron (Fe)<\/strong><\/td>\n<td style=\"text-align: left;\">Pure Element<\/td>\n<td style=\"text-align: left;\">770\u00b0C (1418\u00b0F)<\/td>\n<td style=\"text-align: left;\">~350\u00b0C<\/td>\n<td style=\"text-align: left;\">High baseline threshold; prone to oxidation<\/td>\n<\/tr>\n<tr>\n<td style=\"text-align: left;\"><strong>Nickel (Ni)<\/strong><\/td>\n<td style=\"text-align: left;\">Pure Element<\/td>\n<td style=\"text-align: left;\">358\u00b0C (676\u00b0F)<\/td>\n<td style=\"text-align: left;\">~150\u00b0C<\/td>\n<td style=\"text-align: left;\">Low pure-element thermal limit<\/td>\n<\/tr>\n<tr>\n<td style=\"text-align: left;\"><strong>AlNiCo Alloys<\/strong><\/td>\n<td style=\"text-align: left;\">Commercial Alloy<\/td>\n<td style=\"text-align: left;\">800\u00b0C \u2013 860\u00b0C<\/td>\n<td style=\"text-align: left;\">450\u00b0C \u2013 530\u00b0C<\/td>\n<td style=\"text-align: left;\">Outstanding thermal resistance; low coercivity<\/td>\n<\/tr>\n<tr>\n<td style=\"text-align: left;\"><strong>Samarium-Cobalt (SmCo)<\/strong><\/td>\n<td style=\"text-align: left;\">Rare-Earth Alloy<\/td>\n<td style=\"text-align: left;\">700\u00b0C \u2013 800\u00b0C<\/td>\n<td style=\"text-align: left;\">250\u00b0C \u2013 550\u00b0C<\/td>\n<td style=\"text-align: left;\">Best high-temperature permanent magnet<\/td>\n<\/tr>\n<tr>\n<td style=\"text-align: left;\"><strong>Ferrite \/ Ceramic<\/strong><\/td>\n<td style=\"text-align: left;\">Oxide Alloy<\/td>\n<td style=\"text-align: left;\">450\u00b0C<\/td>\n<td style=\"text-align: left;\">250\u00b0C<\/td>\n<td style=\"text-align: left;\">Moderate heat tolerance, cost-effective<\/td>\n<\/tr>\n<tr>\n<td style=\"text-align: left;\"><strong>Neodymium (NdFeB)<\/strong><\/td>\n<td style=\"text-align: left;\">Rare-Earth Alloy<\/td>\n<td style=\"text-align: left;\">310\u00b0C \u2013 400\u00b0C<\/td>\n<td style=\"text-align: left;\">80\u00b0C \u2013 220\u00b0C<\/td>\n<td style=\"text-align: left;\">High magnetic energy density; review the <a href=\"https:\/\/nbaem.com\/et\/what-is-the-difference-between-n52-and-n55-magnets\/\">difference between N52 and N55 magnets<\/a> to select temperature-rated grades<\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n<h3>Industrial Demagnetization Risks<\/h3>\n<p>Maintaining magnetic performance in high-stress applications requires managing three primary demagnetization drivers:<\/p>\n<ul>\n<li style=\"list-style-type: none;\">\n<ul>\n<li><strong>Thermal Degradation:<\/strong> Operating near maximum working limits causes reversible flux losses. Exceeding $T_C$ leads to permanent, irreversible loss of magnetization.<\/li>\n<li><strong>Opposing External Fields:<\/strong> Strong reverse magnetic fields can overcome low-coercivity materials, flipping domain alignments permanently.<\/li>\n<li><strong>Mechanical Shock &amp; Vibration:<\/strong> Heavy impacts and physical stresses disrupt domain boundaries in brittle rare-earth lattices, lowering total magnetic field strength over time.<\/li>\n<\/ul>\n<\/li>\n<\/ul>\n<h2>Engineering &amp; Industrial Applications<\/h2>\n<p>Determining what elements are magnetic in raw form is only the first step; bringing them into real-world industrial hardware requires advanced metallurgy and precise structural engineering. We engineer raw ferromagnetic elements and rare-earth alloys into high-performance components tailored for demanding industrial systems.<\/p>\n<h3>Electric Motors &amp; E-Mobility<\/h3>\n<p>Electric vehicle (EV) powertrains demand maximal torque density and continuous efficiency under harsh thermal cycles.<\/p>\n<ul>\n<li style=\"list-style-type: none;\">\n<ul>\n<li><strong>Permanent Magnet Synchronous Motors (PMSM):<\/strong> Modern EV drive motors rely heavily on Neodymium-Iron-Boron (NdFeB) grades to deliver high flux density in compact footprints. Selecting the right <a href=\"https:\/\/nbaem.com\/et\/what-motor-magnets-used-in-permanent-magnet-motors\/\">motor magnets used in permanent magnet motors<\/a> guarantees high demagnetization resistance during sudden load spikes.<\/li>\n<li><strong>High-Efficiency Lamination Cores:<\/strong> Stator and rotor stacks built from ultra-thin silicon steel laminations suppress eddy current losses, maximizing overall drivetrain efficiency and battery range.<\/li>\n<\/ul>\n<\/li>\n<\/ul>\n<h3>Medical &amp; Precision Technology<\/h3>\n<p>Precision medical devices and automated equipment demand ultra-stable, highly uniform magnetic fields.<\/p>\n<ul>\n<li style=\"list-style-type: none;\">\n<ul>\n<li><strong>NMR &amp; MRI Systems:<\/strong> High-field imaging platforms require custom magnetic circuits with tight spatial tolerances to maintain field uniformity across the entire scanning volume.<\/li>\n<li><strong>Medical Robotics:<\/strong> Micro-actuators rely on compact, power-dense magnetic assemblies for ultra-precise movement. Leveraging specialized <a href=\"https:\/\/nbaem.com\/et\/microrobot-and-neodymium-magnets\/\">neodymium magnets in microrobotics<\/a> enables accurate spatial positioning and responsive force feedback in minimally invasive surgical tools.<\/li>\n<\/ul>\n<\/li>\n<\/ul>\n<h3>Renewable Energy &amp; Heavy Industry<\/h3>\n<p>Heavy equipment relies on hard-magnetic materials to sustain high mechanical stress, extreme weather, and continuous duty cycles.<\/p>\n<ul>\n<li style=\"list-style-type: none;\">\n<ul>\n<li><strong>Direct-Drive Wind Turbines:<\/strong> Eliminating gearboxes, utility-scale wind generators use tons of heavy-grade rare-earth magnets to deliver long life cycles and minimal maintenance in offshore environments.<\/li>\n<li><strong>Halbach Arrays:<\/strong> Arranging permanent magnets in specific spatial patterns focuses the magnetic field strictly on one side, doubling peak field strength for specialized linear propulsion systems and maglev track guidance.<\/li>\n<li><strong>Industrial Separators &amp; Pot Magnets:<\/strong> Heavy-duty magnetic separators remove tramp metal from raw material streams to protect downstream crushers, while pot magnets offer high holding forces for heavy lifting jigs and structural clamping.<\/li>\n<\/ul>\n<\/li>\n<\/ul>\n<h2>Custom Magnetic Engineering &amp; Manufacturing Solutions<\/h2>\n<p>Knowing <strong>what elements are magnetic<\/strong> is only the baseline. Converting raw magnetic elements into high-performance industrial components demands precise engineering, advanced processing, and reliable supply chain management. We bridge the gap between raw material science and high-spec enterprise applications.<\/p>\n<h3>14+ Years of Material &amp; R&amp;D Expertise<\/h3>\n<p>We bring over 14 years of hands-on experience in magnetic material design, R&amp;D, and global sourcing. Our engineering team customizes alloy compositions to optimize magnetic permeability, coercivity, and thermal stability for demanding B2B applications.<\/p>\n<h3>Full-Spectrum Manufacturing Capabilities<\/h3>\n<p>We manage the full production lifecycle to deliver consistent component quality:<br \/>\n<strong>Raw Rare-Earth Processing:<\/strong> Direct sourcing and refining of high-grade rare-earth permanent magnets.<br \/>\n<strong>Custom Magnetic Assemblies:<\/strong> Designing structural assemblies and selecting optimal <a href=\"https:\/\/nbaem.com\/et\/what-magnet-materials-are-best-for-halbach-arrays\/\">magnet materials for Halbach arrays<\/a> and rotor systems.<br \/>\n<strong>Surface Treatments:<\/strong> Custom plating and coatings to prevent oxidation and environmental degradation.<\/p>\n<h3>Precision Motor Lamination Cores<\/h3>\n<p>We design and fabricate high-efficiency <strong>motor lamination cores<\/strong> engineered to reduce eddy current losses in demanding motion control setups:<br \/>\n<strong>Drone Motors:<\/strong> Ultra-lightweight lamination stacks delivering maximum power-to-weight performance.<br \/>\n<strong>Servo Systems:<\/strong> High-torque density designs optimized for industrial automation and robotics.<br \/>\n<strong>Automotive &amp; EV:<\/strong> Precision lamination stacks built for permanent magnet synchronous motors (PMSM).<\/p>\n<h3>Quality &amp; Compliance Standards<\/h3>\n<p>Every component meets strict global automotive and industrial quality protocols:<br \/>\n<strong>ISO 9001 &amp; ISO 14001:<\/strong> Certified quality and environmental management systems.<br \/>\n<strong>ISO\/TS16949:<\/strong> Automotive-grade manufacturing controls and tolerance standards.<br \/>\n<strong>PPAP Level 3:<\/strong> Full Production Part Approval Process documentation for seamless OEM integration.<\/p>\n<h2>Frequently Asked Questions: What Elements Are Magnetic?<\/h2>\n<h3>Is Stainless Steel Magnetic?<\/h3>\n<p>It depends on the specific crystal structure of the alloy:<br \/>\n<strong>Austenitic (300 Series):<\/strong> Grades like 304 and 316 feature a face-centered cubic structure that renders them non-magnetic in their annealed state. Heavy cold working, however, can induce minor ferromagnetism.<br \/>\n<strong>Ferritic &amp; Martensitic (400 Series):<\/strong> Grades like 410 and 430 maintain a body-centered cubic lattice, making them naturally ferromagnetic.<\/p>\n<h3>Why Isn&#8217;t Copper or Aluminum Magnetic?<\/h3>\n<p>Neither metal possesses the required unpaired electron spins or crystal domain alignment needed for ferromagnetism. Copper is weakly diamagnetic and slightly repels magnetic fields, whereas aluminum is weakly paramagnetic. To dive deeper into non-ferrous behavior, see our technical breakdown on <a href=\"https:\/\/nbaem.com\/et\/is-aluminum-a-magnetic-material\/\">is aluminum a magnetic material<\/a> under standard operating conditions.<\/p>\n<h3>Are All Rare-Earth Elements Magnetic by Themselves?<\/h3>\n<p>No. Although lanthanides have unpaired 4f orbital electrons, most only exhibit ferromagnetism at cryogenic temperatures. Gadolinium is the sole rare-earth element that remains ferromagnetic near room temperature (up to 20\u00b0C \/ 68\u00b0F). Others, such as dysprosium, terbium, and neodymium, must be alloyed with transition metals like iron and cobalt to achieve stable room-temperature magnetism.<\/p>\n<h3>How Do Temperature Fluctuations Affect Magnet Performance in Motor Applications?<\/h3>\n<p>Thermal energy increases atomic vibration, which disrupts electron spin alignment and degrades magnetic flux density:<br \/>\n<strong>Reversible Loss:<\/strong> Operating within maximum rated temperatures causes minor, temporary drops in remanence that fully recover upon cooling.<br \/>\n<strong>Irreversible Demagnetization:<\/strong> Exceeding maximum working limits or approaching the Curie temperature alters domain structures permanently, causing thermal torque degradation and permanent efficiency loss in motor lamination cores.<\/p>\n<div id=\"references\">\n<h2>Related Sources<\/h2>\n<ul>\n<li><a href=\"https:\/\/www.supermagnete.de\/eng\/magnetism\/Exchange-interaction\" target=\"_blank\" rel=\"noopener noreferrer\">https:\/\/www.supermagnete.de\/eng\/magnetism\/Exchange-interaction<\/a><\/li>\n<li><a href=\"https:\/\/www.first4magnets.com\/information-and-articles\/grades-of-different-magnet-materials\" target=\"_blank\" rel=\"noopener noreferrer\">https:\/\/www.first4magnets.com\/information-and-articles\/grades-of-different-magnet-materials<\/a><\/li>\n<li><a href=\"https:\/\/www.supermagnete.de\/eng\/magnetism\/Curie-temperature\" target=\"_blank\" rel=\"noopener noreferrer\">https:\/\/www.supermagnete.de\/eng\/magnetism\/Curie-temperature<\/a><\/li>\n<li><a href=\"https:\/\/physicsexperiments.eu\/1775\/curie-temperature-of-ferromagnetic-materials\" target=\"_blank\" rel=\"noopener noreferrer\">https:\/\/physicsexperiments.eu\/1775\/curie-temperature-of-ferromagnetic-materials<\/a><\/li>\n<\/ul>\n<\/div>","protected":false},"excerpt":{"rendered":"<p>What elements are magnetic Learn the main magnetic metals iron nickel cobalt and rare earths plus easy differences between magnetic and nonmagnetic<\/p>","protected":false},"author":1,"featured_media":3976,"comment_status":"open","ping_status":"open","sticky":false,"template":"","format":"standard","meta":{"om_disable_all_campaigns":false,"_mi_skip_tracking":false,"footnotes":""},"categories":[1],"tags":[],"class_list":["post-3977","post","type-post","status-publish","format-standard","has-post-thumbnail","hentry","category-uncategorized"],"jetpack_featured_media_url":"https:\/\/nbaem.com\/wp-content\/uploads\/2026\/08\/Ferromagnetic_elements_periodic_table_BSo.webp","_links":{"self":[{"href":"https:\/\/nbaem.com\/et\/wp-json\/wp\/v2\/posts\/3977","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/nbaem.com\/et\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/nbaem.com\/et\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/nbaem.com\/et\/wp-json\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/nbaem.com\/et\/wp-json\/wp\/v2\/comments?post=3977"}],"version-history":[{"count":2,"href":"https:\/\/nbaem.com\/et\/wp-json\/wp\/v2\/posts\/3977\/revisions"}],"predecessor-version":[{"id":3992,"href":"https:\/\/nbaem.com\/et\/wp-json\/wp\/v2\/posts\/3977\/revisions\/3992"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/nbaem.com\/et\/wp-json\/wp\/v2\/media\/3976"}],"wp:attachment":[{"href":"https:\/\/nbaem.com\/et\/wp-json\/wp\/v2\/media?parent=3977"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/nbaem.com\/et\/wp-json\/wp\/v2\/categories?post=3977"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/nbaem.com\/et\/wp-json\/wp\/v2\/tags?post=3977"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}