{"id":13147,"date":"2026-07-19T10:33:39","date_gmt":"2026-07-19T10:33:39","guid":{"rendered":"https:\/\/www.vedprep.com\/exams\/?p=13147"},"modified":"2026-07-19T10:33:39","modified_gmt":"2026-07-19T10:33:39","slug":"ampere-s-law","status":"publish","type":"post","link":"https:\/\/www.vedprep.com\/exams\/iit-jam\/ampere-s-law\/","title":{"rendered":"Ampere\u2019s Law 5 Proven Methods for IIT JAM Success"},"content":{"rendered":"<h1>Ampere\u2019s law 5 Proven Methods for IIT JAM Success<\/h1>\n<p>Ampere\u2019s law stands as a cornerstone of <a href=\"https:\/\/www.vedprep.com\/\">VedPrep<\/a>\u2019s comprehensive guide for IIT JAM Physics aspirants, particularly those tackling the challenging Electromagnetism unit. This fundamental principle bridges the gap between theoretical understanding and practical problem-solving in competitive examinations like IIT JAM, CSIR NET, and GATE. Whether you&#8217;re grappling with magnetic fields or current distributions, mastering Ampere\u2019s law will significantly elevate your exam performance.<\/p>\n<p>In this definitive guide, we break down Ampere\u2019s law into digestible components, explore its mathematical formulation, and demonstrate its real-world applications through carefully selected examples. By the end, you\u2019ll not only understand the law but also develop the confidence to apply it to any problem that appears in your IIT JAM examination.<\/p>\n<h2>Ampere\u2019s law explained for IIT JAM: The complete breakdown<\/h2>\n<p>Ampere\u2019s law represents a fundamental relationship in magnetostatics, connecting the magnetic field circulating around a closed loop to the electric current passing through that loop. This principle is mathematically expressed as:<\/p>\n<p>$$<br \/>\noint vec{B} cdot dvec{l} = mu_0 I_{enc}<br \/>\n$$<\/p>\n<p>Where:<\/p>\n<ul>\n<li><strong>$(vec{B})$<\/strong> represents the magnetic field vector<\/li>\n<li><strong>$mu_0)$<\/strong> is the magnetic constant (permeability of free space, $4pi times 10^{-7}$ T\u00b7m\/A)<\/li>\n<li><strong>$vec{l})$<\/strong> is the differential length element along the closed path<\/li>\n<li><strong>$oint)$<\/strong> denotes the line integral around the closed loop<\/li>\n<li><strong>$I_{enc})$<\/strong> is the total current enclosed by the loop<\/li>\n<\/ul>\n<p>This equation reveals that the circulation of the magnetic field around any closed path is directly proportional to the net current passing through the surface bounded by that path. For IIT JAM aspirants, this means that understanding Ampere\u2019s law is crucial for solving problems involving symmetrical current distributions.<\/p>\n<h2>Ampere\u2019s law statement and its mathematical representation<\/h2>\n<p>The formal statement of Ampere\u2019s law declares that the line integral of the magnetic field around any closed loop equals $\u03bc\u2080$ times the total current passing through the loop. This principle forms the foundation of magnetostatics and is essential for analyzing magnetic fields in various configurations.<\/p>\n<p>The mathematical representation of Ampere\u2019s law is:<\/p>\n<p>$$<br \/>\noint_C vec{B} cdot dvec{l} = mu_0 int_S vec{J} cdot dvec{A}<br \/>\n$$<\/p>\n<p>Where:<\/p>\n<ul>\n<li><strong>$C$<\/strong> is the closed loop<\/li>\n<li><strong>$S$<\/strong> is any surface bounded by loop $C$<\/li>\n<li><strong>$vec{J}$<\/strong> is the current density vector<\/li>\n<li><strong>$dvec{A}$<\/strong> is the differential area element<\/li>\n<\/ul>\n<p>For IIT JAM preparation, focus on the simplified form that applies to steady currents and symmetrical geometries. This version states that the magnetic field\u2019s circulation depends solely on the enclosed current, making it an invaluable tool for calculating magnetic fields in conductors, solenoids, and toroids.<\/p>\n<h2>Understanding magnetic fields: The foundation of Ampere\u2019s law<\/h2>\n<p>The magnetic field, denoted by $B$, represents a vector field that permeates space around magnets and current-carrying conductors. In the context of Ampere\u2019s law, understanding magnetic field properties becomes paramount for successful application.<\/p>\n<p>Magnetic fields exhibit several key characteristics:<\/p>\n<ul>\n<li><strong>Field lines<\/strong> form continuous loops that emerge from north poles and terminate at south poles<\/li>\n<li><strong>Field strength<\/strong> is proportional to the density of field lines<\/li>\n<li><strong>Field direction<\/strong> at any point is tangent to the field line at that location<\/li>\n<li><strong>Field lines never intersect<\/strong>, ensuring a unique direction at every point<\/li>\n<\/ul>\n<p>When applying Ampere\u2019s law, visualize the magnetic field configuration before selecting your Amperian loop. For IIT JAM problems, look for symmetrical distributions where the magnetic field remains constant along portions of your chosen path. This symmetry simplifies calculations and reduces computational complexity.<\/p>\n<h2>Ampere\u2019s law applications in IIT JAM: Real problem-solving scenarios<\/h2>\n<p>Ampere\u2019s law finds extensive applications in competitive examinations, particularly in scenarios involving:<\/p>\n<ul>\n<li><strong>Long straight conductors<\/strong>: Calculating magnetic field at various distances from the wire<\/li>\n<li><strong>Solenoids<\/strong>: Determining internal and external magnetic fields<\/li>\n<li><strong>Toroids<\/strong>: Analyzing magnetic field within circular current loops<\/li>\n<li><strong>Infinite planes<\/strong>: Evaluating magnetic fields from current sheets<\/li>\n<\/ul>\n<p>Consider the classic problem of finding the magnetic field inside a long solenoid carrying current $I$. Using Ampere\u2019s law with a rectangular Amperian loop that has one side inside the solenoid and the other outside:<\/p>\n<p>$$<br \/>\nB cdot L = mu_0 N I<br \/>\n$$<\/p>\n<p>Where $N$ represents the number of turns per unit length. This application demonstrates how Ampere\u2019s law transforms complex magnetic field calculations into straightforward algebraic manipulations.<\/p>\n<h2>Worked example: Applying Ampere\u2019s law to a cylindrical conductor<\/h2>\n<p>Let\u2019s solve a typical IIT JAM problem involving a long cylindrical conductor of radius $R$ carrying a uniformly distributed current $I$. Our goal is to find the magnetic field at a distance $r$ from the axis.<\/p>\n<p><strong>Step 1: Choose an Amperian loop<\/strong><\/p>\n<p>For $r &lt; R$ (inside the conductor):<\/p>\n<p>$$<br \/>\noint vec{B} cdot dvec{l} = B cdot 2pi r = mu_0 I_{enc} = mu_0 I frac{r^2}{R^2}<br \/>\n$$<\/p>\n<p>Solving for $B$:<\/p>\n<p>$$<br \/>\nB = frac{mu_0 I r}{2pi R^2}<br \/>\n$$<\/p>\n<p>For $r &gt; R$ (outside the conductor):<\/p>\n<p>$$<br \/>\noint vec{B} cdot dvec{l} = B cdot 2pi r = mu_0 I<br \/>\n$$<\/p>\n<p>Solving for $B$:<\/p>\n<p>$$<br \/>\nB = frac{mu_0 I}{2pi r}<br \/>\n$$<\/p>\n<p>This example illustrates how Ampere\u2019s law elegantly handles both internal and external magnetic field calculations for cylindrical conductors.<\/p>\n<h2>Common mistakes to avoid with Ampere\u2019s law in IIT JAM<\/h2>\n<p>Many students stumble when applying Ampere\u2019s law due to several recurring misconceptions:<\/p>\n<ul>\n<li><strong>Assuming symmetry where none exists<\/strong>: Ampere\u2019s law requires careful selection of Amperian loops that match the problem\u2019s symmetry<\/li>\n<li><strong>Incorrect current enclosure<\/strong>: Failing to account for all currents passing through the loop\u2019s surface<\/li>\n<li><strong>Direction errors<\/strong>: Misapplying the right-hand rule for current and magnetic field directions<\/li>\n<li><strong>Overlooking boundary conditions<\/strong>: Not considering field behavior at discontinuities<\/li>\n<li><strong>Unit confusion<\/strong>: Mixing up $\u03bc\u2080$ with other constants or misapplying units<\/li>\n<\/ul>\n<p>To avoid these pitfalls, always:<\/p>\n<ol>\n<li>Sketch the problem geometry before attempting calculations<\/li>\n<li>Verify your Amperian loop selection matches the symmetry<\/li>\n<li>Double-check current directions using the right-hand rule<\/li>\n<li>Confirm your final answer has appropriate units (Tesla for magnetic field)<\/li>\n<\/ol>\n<h2>Exam strategy: Mastering Ampere\u2019s law for IIT JAM success<\/h2>\n<p>To excel in IIT JAM examinations using Ampere\u2019s law, implement these proven strategies:<\/p>\n<ol>\n<li><strong>Practice symmetry identification<\/strong>: Train yourself to recognize symmetrical current distributions immediately<\/li>\n<li><strong>Develop Amperian loop intuition<\/strong>: Practice selecting optimal loops for various geometries<\/li>\n<li><strong>Time management<\/strong>: Allocate specific time slots for Ampere\u2019s law problems during mock tests<\/li>\n<li><strong>Formula memorization<\/strong>: Commit the fundamental equation to memory while understanding its derivation<\/li>\n<li><strong>Error analysis<\/strong>: Review incorrect solutions to identify pattern-based mistakes<\/li>\n<\/ol>\n<p>Remember that Ampere\u2019s law problems in IIT JAM typically test your ability to:<\/p>\n<ul>\n<li>Identify appropriate Amperian loops<\/li>\n<li>Calculate enclosed currents accurately<\/li>\n<li>Apply the right-hand rule correctly<\/li>\n<li>Simplify complex geometries using symmetry<\/li>\n<\/ul>\n<h2>Advanced concepts: Beyond basic Ampere\u2019s law applications<\/h2>\n<p>While the basic form of Ampere\u2019s law suffices for most IIT JAM problems, understanding its extensions provides deeper insight:<\/p>\n<p><strong>Ampere-Maxwell law<\/strong> incorporates displacement current for time-varying fields:<\/p>\n<p>$$<br \/>\noint_C vec{B} cdot dvec{l} = mu_0 left(I_{enc} + epsilon_0 frac{dPhi_E}{dt}right)<br \/>\n$$<\/p>\n<p>This generalization becomes crucial when dealing with electromagnetic waves and changing electric fields, though it\u2019s rarely tested in IIT JAM\u2019s magnetostatics section.<\/p>\n<p><strong>Vector potential formulation<\/strong> provides an alternative approach using:<\/p>\n<p>$$<br \/>\nvec{B} = nabla times vec{A}<br \/>\n$$<\/p>\n<p>Where $(vec{A})$ represents the magnetic vector potential. This formulation often simplifies calculations for complex geometries.<\/p>\n<h2>IIT JAM syllabus alignment: Where Ampere\u2019s law fits in<\/h2>\n<p>Ampere\u2019s law appears prominently in the IIT JAM Physics syllabus under the Electromagnetism unit, specifically in the Magnetostatics section. This topic typically accounts for 5-10% of the total marks in the examination, making it a high-yield area for preparation.<\/p>\n<p>The syllabus emphasizes:<\/p>\n<ul>\n<li>Statement and mathematical formulation of Ampere\u2019s law<\/li>\n<li>Applications to symmetrical current distributions<\/li>\n<li>Calculation of magnetic fields in various geometries<\/li>\n<li>Relationship between Ampere\u2019s law and other electromagnetic principles<\/li>\n<\/ul>\n<p>For comprehensive preparation, refer to standard textbooks like <strong>David J. Griffiths<\/strong>\u2019 &#8220;Introduction to Electrodynamics&#8221; and <strong>John David Jackson<\/strong>\u2019s &#8220;Classical Electrodynamics&#8221; for advanced topics.<\/p>\n<h2>Practical tips for IIT JAM preparation with Ampere\u2019s law<\/h2>\n<p>To maximize your Ampere\u2019s law preparation for IIT JAM:<\/p>\n<ul>\n<li><strong>Daily practice<\/strong>: Solve at least 2-3 Ampere\u2019s law problems daily during your preparation period<\/li>\n<li><strong>Concept mapping<\/strong>: Create visual diagrams showing magnetic field patterns for different current configurations<\/li>\n<li><strong>Formula sheets<\/strong>: Maintain a concise reference sheet with key equations and constants<\/li>\n<li><strong>Mock tests<\/strong>: Take timed mock tests focusing specifically on Ampere\u2019s law applications<\/li>\n<li><strong>Peer discussion<\/strong>: Explain concepts to fellow aspirants to reinforce your understanding<\/li>\n<\/ul>\n<p>Remember that consistency beats intensity. Regular, focused practice will build the intuition needed to tackle even the most challenging Ampere\u2019s law problems in your IIT JAM examination.<\/p>\n<h2>Additional resources for Ampere\u2019s law mastery<\/h2>\n<p>Enhance your understanding with these valuable resources:<\/p>\n<ul>\n<li><strong>Video lectures<\/strong>: <a href=\"https:\/\/www.youtube.com\/watch?v=GrmJ9D1xLjo\" rel=\"nofollow noopener\" target=\"_blank\">Ampere\u2019s law explained visually<\/a> provides intuitive explanations of key concepts<\/li>\n<li><strong>Interactive simulations<\/strong>: PhET\u2019s &#8220;Magnet and Compass&#8221; simulation helps visualize magnetic field patterns<\/li>\n<li><strong>Problem banks<\/strong>: Solve past IIT JAM papers and test series questions specifically targeting Ampere\u2019s law<\/li>\n<li><strong>Conceptual guides<\/strong>: <a href=\"https:\/\/www.vedprep.com\/\">VedPrep<\/a>\u2019s detailed explanations and step-by-step solutions<\/li>\n<\/ul>\n<p>These resources complement your textbook learning and provide multiple perspectives on Ampere\u2019s law applications.<\/p>\n<h2>Conclusion: Your path to Ampere\u2019s law mastery for IIT JAM<\/h2>\n<p>Ampere\u2019s law represents more than just another equation to memorize\u2014it\u2019s a powerful tool that unlocks the mysteries of magnetic fields and current interactions. By mastering this fundamental principle, you position yourself for success not only in IIT JAM but also in your future physics endeavors.<\/p>\n<p>Remember that understanding comes through practice. Each problem you solve builds neural pathways that transform abstract concepts into intuitive understanding. As you progress through your IIT JAM preparation, you\u2019ll find that Ampere\u2019s law becomes second nature, allowing you to tackle complex problems with confidence and precision.<\/p>\n<p>Start today by selecting one Ampere\u2019s law problem and working through it methodically. Build momentum through consistent practice, and soon you\u2019ll be solving problems that once seemed impossible. Your IIT JAM success begins with mastering the fundamentals\u2014and Ampere\u2019s law is one of the most fundamental tools in your physics toolkit.<\/p>\n<section class=\"vedprep-faq\">\n<h2>Frequently Asked Questions about Ampere\u2019s law for IIT JAM<\/h2>\n<h3>Core Understanding<\/h3>\n<div class=\"faq-item\">\n<h4>What exactly is Ampere\u2019s law?<\/h4>\n<p>Ampere\u2019s law states that the line integral of the magnetic field around any closed loop equals $\u03bc\u2080$ times the total current passing through the loop. This fundamental principle in magnetostatics relates magnetic field circulation to enclosed current, forming the basis for calculating magnetic fields in various symmetrical configurations.<\/p>\n<\/div>\n<div class=\"faq-item\">\n<h4>How is Ampere\u2019s law mathematically expressed?<\/h4>\n<p>Ampere\u2019s law is mathematically represented as $\u222e vec{B} \u00b7 dvec{l} = \u03bc\u2080 I_{enc}$, where the left side represents the magnetic field\u2019s circulation around a closed path and the right side shows the proportionality to enclosed current through the magnetic constant $\u03bc\u2080$.<\/p>\n<\/div>\n<div class=\"faq-item\">\n<h4>What are the key limitations of Ampere\u2019s law?<\/h4>\n<p>Ampere\u2019s law applies strictly to static currents and steady magnetic fields. It doesn\u2019t account for time-varying electric fields or displacement currents, which require the Ampere-Maxwell law extension for complete accuracy in dynamic situations.<\/p>\n<\/div>\n<div class=\"faq-item\">\n<h4>Why is Ampere\u2019s law significant in Electricity and Magnetism?<\/h4>\n<p>Ampere\u2019s law provides the quantitative relationship between electric currents and the magnetic fields they generate. This principle enables physicists and engineers to calculate magnetic fields in conductors, solenoids, and other current-carrying structures, making it indispensable for both theoretical understanding and practical applications.<\/p>\n<\/div>\n<div class=\"faq-item\">\n<h4>How does Ampere\u2019s law relate specifically to Magnetostatics?<\/h4>\n<p>Ampere\u2019s law serves as the foundational equation in magnetostatics, which studies magnetic fields produced by steady (time-independent) currents. In magnetostatic scenarios, Ampere\u2019s law enables the calculation of magnetic field distributions without requiring knowledge of time-varying components.<\/p>\n<\/div>\n<div class=\"faq-item\">\n<h4>What are the units of the magnetic constant $\u03bc\u2080$?<\/h4>\n<p>The magnetic constant $\u03bc\u2080$ has units of henries per meter (H\/m) or equivalently tesla meters per ampere (T\u00b7m\/A). Its exact value is $4\u03c0 \u00d7 10^{-7}$ H\/m, which appears in all Ampere\u2019s law calculations involving SI units.<\/p>\n<\/div>\n<div class=\"faq-item\">\n<h4>What does the line integral represent in Ampere\u2019s law?<\/h4>\n<p>The line integral in Ampere\u2019s law represents the total magnetic circulation around a closed path, which equals the sum of magnetic field components parallel to the path multiplied by path length elements. This circulation directly correlates with the total current enclosed by the path.<\/p>\n<\/div>\n<h3>Exam Application<\/h3>\n<div class=\"faq-item\">\n<h4>How can I apply Ampere\u2019s law to solve IIT JAM problems effectively?<\/h4>\n<p>To apply Ampere\u2019s law in IIT JAM examinations, first identify the problem\u2019s symmetry, then select an appropriate Amperian loop where the magnetic field remains constant along portions of the path. Calculate the enclosed current carefully and apply the right-hand rule to determine field direction before solving for the magnetic field.<\/p>\n<\/div>\n<div class=\"faq-item\">\n<h4>What types of problems typically use Ampere\u2019s law in IIT JAM?<\/h4>\n<p>IIT JAM examinations commonly feature Ampere\u2019s law problems involving long straight wires, infinite current sheets, solenoids, toroids, and cylindrical conductors. These problems test your ability to identify symmetry, select optimal Amperian loops, and calculate magnetic fields using the fundamental law.<\/p>\n<\/div>\n<div class=\"faq-item\">\n<h4>How do I find the magnetic field inside a solenoid using Ampere\u2019s law?<\/h4>\n<p>To find the magnetic field inside a solenoid, select a rectangular Amperian loop with one side parallel to the solenoid\u2019s axis inside the coil and the other side outside. The line integral simplifies to $B\u00b7L = \u03bc\u2080NI$, where $N$ represents turns per unit length, yielding $B = \u03bc\u2080NI$ for the internal field.<\/p>\n<\/div>\n<div class=\"faq-item\">\n<h4>How can I determine magnetic field direction using Ampere\u2019s law?<\/h4>\n<p>Use the right-hand rule in conjunction with Ampere\u2019s law: point your thumb in the direction of the current flow, and your fingers will curl in the direction of the magnetic field. This rule helps determine both the field\u2019s direction and the sign of enclosed current in your calculations.<\/p>\n<\/div>\n<div class=\"faq-item\">\n<h4>What\u2019s the approach for applying Ampere\u2019s law to a current-carrying wire?<\/h4>\n<p>For a long straight wire carrying current $I$, choose a circular Amperian loop centered on the wire. The magnetic field remains constant along this path, so the line integral becomes $B\u00b72\u03c0r = \u03bc\u2080I$, yielding $B = \u03bc\u2080I\/(2\u03c0r)$ at distance $r$ from the wire.<\/p>\n<\/div>\n<h3>Common Mistakes<\/h3>\n<div class=\"faq-item\">\n<h4>What are the most common mistakes when applying Ampere\u2019s law?<\/h4>\n<p>Common errors include selecting Amperian loops that don\u2019t match the problem\u2019s symmetry, miscalculating enclosed currents, applying the right-hand rule incorrectly, overlooking boundary conditions at material interfaces, and confusing $\u03bc\u2080$ with other electromagnetic constants.<\/p>\n<\/div>\n<div class=\"faq-item\">\n<h4>How can I avoid errors in calculating the line integral?<\/h4>\n<p>Avoid calculation errors by carefully choosing Amperian loops where the magnetic field is constant along portions of the path. Verify that your selected loop actually encloses the current you\u2019re accounting for, and double-check your right-hand rule application for direction consistency.<\/p>\n<\/div>\n<div class=\"faq-item\">\n<h4>What\u2019s frequently misunderstood about Ampere\u2019s law applications?<\/h4>\n<p>A widespread misconception is that Ampere\u2019s law can be applied to any current distribution without considering symmetry. In reality, the law\u2019s power comes from its application to symmetrical problems where the magnetic field remains constant along portions of the Amperian loop.<\/p>\n<\/div>\n<div class=\"faq-item\">\n<h4>What happens if I choose the wrong Amperian loop?<\/h4>\n<p>Selecting an inappropriate Amperian loop typically leads to complex integrals that can\u2019t be simplified, resulting in incorrect magnetic field calculations. The loop must match the problem\u2019s symmetry to exploit the law\u2019s full power in competitive examination settings.<\/p>\n<\/div>\n<h3>Advanced Concepts<\/h3>\n<div class=\"faq-item\">\n<h4>How does Ampere\u2019s law connect to Maxwell\u2019s equations?<\/h4>\n<p>Ampere\u2019s law appears as one of Maxwell\u2019s four fundamental equations, specifically in its extended form that includes the displacement current term. This connection ensures the consistency of electromagnetic theory across both static and dynamic scenarios.<\/p>\n<\/div>\n<div class=\"faq-item\">\n<h4>What role does Ampere\u2019s law play in electromagnetic theory?<\/h4>\n<p>Ampere\u2019s law provides the quantitative bridge between electric currents and magnetic fields, forming the cornerstone of classical electromagnetism. This principle enables the calculation of magnetic field distributions in complex geometries and underpins much of electrical engineering and physics applications.<\/p>\n<\/div>\n<div class=\"faq-item\">\n<h4>How can Ampere\u2019s law be extended for dynamic fields?<\/h4>\n<p>Ampere\u2019s law extends to dynamic fields through the Ampere-Maxwell law, which adds the displacement current term $\u03b5\u2080(d\u03a6_E\/dt)$ to account for time-varying electric fields. This generalization ensures the law\u2019s validity across all electromagnetic scenarios.<\/p>\n<\/div>\n<div class=\"faq-item\">\n<h4>Can Ampere\u2019s law handle non-static currents?<\/h4>\n<p>Ampere\u2019s law in its original form only applies to static currents. For non-static (time-varying) currents, you must use the Ampere-Maxwell law extension, which incorporates the displacement current to maintain mathematical consistency in dynamic situations.<\/p>\n<\/div>\n<\/section>\n","protected":false},"excerpt":{"rendered":"<p>Ampere&#8217;s Law is a fundamental concept in electromagnetism that allows students to understand and quantify the magnetic field around closed loops. This law is a cornerstone in understanding various electromagnetic phenomena and has numerous applications in physics and engineering. It is particularly useful for IIT JAM and other competitive exams.<\/p>\n","protected":false},"author":12,"featured_media":13146,"comment_status":"open","ping_status":"open","sticky":false,"template":"","format":"standard","meta":{"_acf_changed":false,"footnotes":"","_debug_hook_fired":"2026-07-19 10:33:40","rank_math_seo_score":0},"categories":[23],"tags":[8502,8503,8504,8505,2923,2922],"class_list":["post-13147","post","type-post","status-publish","format-standard","has-post-thumbnail","hentry","category-iit-jam","tag-ampere-s-law-for-iit-jam","tag-ampere-s-law-for-iit-jam-notes","tag-ampere-s-law-for-iit-jam-questions","tag-ampere-s-law-for-iit-jam-study-material","tag-competitive-exams","tag-vedprep","entry","has-media"],"acf":[],"rank_math_title":"Ampere\u2019s Law 5 Proven Methods for IIT JAM Success","rank_math_description":"Ampere\u2019s law is a fundamental concept in magnetostatics essential for IIT JAM preparation","rank_math_focus_keyword":"Ampere\u2019s law","_links":{"self":[{"href":"https:\/\/www.vedprep.com\/exams\/wp-json\/wp\/v2\/posts\/13147","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/www.vedprep.com\/exams\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/www.vedprep.com\/exams\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/www.vedprep.com\/exams\/wp-json\/wp\/v2\/users\/12"}],"replies":[{"embeddable":true,"href":"https:\/\/www.vedprep.com\/exams\/wp-json\/wp\/v2\/comments?post=13147"}],"version-history":[{"count":1,"href":"https:\/\/www.vedprep.com\/exams\/wp-json\/wp\/v2\/posts\/13147\/revisions"}],"predecessor-version":[{"id":30229,"href":"https:\/\/www.vedprep.com\/exams\/wp-json\/wp\/v2\/posts\/13147\/revisions\/30229"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/www.vedprep.com\/exams\/wp-json\/wp\/v2\/media\/13146"}],"wp:attachment":[{"href":"https:\/\/www.vedprep.com\/exams\/wp-json\/wp\/v2\/media?parent=13147"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.vedprep.com\/exams\/wp-json\/wp\/v2\/categories?post=13147"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.vedprep.com\/exams\/wp-json\/wp\/v2\/tags?post=13147"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}