{"id":2296,"date":"2018-04-30T07:44:10","date_gmt":"2018-04-29T23:44:10","guid":{"rendered":"https:\/\/gurumuda.net\/physics\/?p=2296"},"modified":"2023-08-08T13:07:58","modified_gmt":"2023-08-08T13:07:58","slug":"kinetic-theory-of-gas-and-first-law-of-thermodynamics-problems-and-solutions","status":"publish","type":"post","link":"https:\/\/gurumuda.net\/physics\/kinetic-theory-of-gas-and-first-law-of-thermodynamics-problems-and-solutions.htm","title":{"rendered":"Kinetic theory of gas and first law of thermodynamics \u2013 problems and solutions","gt_translate_keys":[{"key":"rendered","format":"text"}]},"content":{"rendered":"<p style=\"text-align: justify;\" align=\"justify\"><span style=\"font-size: 12pt; font-family: 'times new roman', times, serif;\">Kinetic theory of gas and first law of thermodynamics \u2013 problems and solutions<\/span><\/p>\n<p class=\"western\" style=\"text-align: justify;\" align=\"justify\"><span style=\"font-size: 12pt; font-family: 'times new roman', times, serif;\">1. Ideal gases are in a container with a volume of 4 liters and its pressure is 3 atm (1 atm = 10<sup>5<\/sup> N.m<sup>-2<\/sup>). The <a href=\"https:\/\/gurumuda.net\/physics\/ideal-gas-law-problems-and-solutions.htm\" target=\"_blank\" rel=\"noopener\">ideal gases<\/a> heated at a constant pressure from 27<sup>o<\/sup>C to 87<sup>o<\/sup>C. The <a href=\"https:\/\/gurumuda.net\/physics\/specific-heat-and-heat-capacity-problems-and-solutions.htm\" target=\"_blank\" rel=\"noopener\">heat capacity<\/a> of the gas is 9 J.K<sup>-1<\/sup>. What is the final volume of gases and the change of internal energy of gases?<\/span><\/p>\n<p class=\"western\" style=\"text-align: justify;\" align=\"justify\"><span style=\"font-family: 'times new roman', times, serif; font-size: 12pt;\">Solution<\/span><\/p>\n<p class=\"western\" style=\"text-align: justify;\" align=\"justify\"><span style=\"font-family: 'times new roman', times, serif; font-size: 12pt;\"><b>Isobaric process (constant pressure)<\/b><\/span><\/p>\n<p class=\"western\" style=\"text-align: justify;\" align=\"justify\"><span style=\"font-family: 'times new roman', times, serif; font-size: 12pt;\"><u>Known :<\/u><\/span><\/p>\n<p class=\"western\" style=\"text-align: justify;\" align=\"justify\"><span style=\"font-size: 12pt; font-family: 'times new roman', times, serif;\">The initial volume of gas (V<sub>1<\/sub>) = 4 liters<!--more--><\/span><\/p>\n<p class=\"western\" style=\"text-align: justify;\" align=\"justify\"><span style=\"font-size: 12pt; font-family: 'times new roman', times, serif;\">The initial <a href=\"https:\/\/gurumuda.net\/physics\/temperature-and-heat-problems-and-solutions.htm\" target=\"_blank\" rel=\"noopener\">temperature<\/a> of gas (T<sub>1<\/sub>) = 27<sup>o<\/sup>C + 273 = 300 K <\/span><\/p>\n<p class=\"western\" style=\"text-align: justify;\" align=\"justify\"><span style=\"font-size: 12pt; font-family: 'times new roman', times, serif;\">The final temperature of gas (T<sub>2<\/sub>) = 87<sup>o<\/sup>C + 273 = 360 K <\/span><\/p>\n<p class=\"western\" style=\"text-align: justify;\" align=\"justify\"><span style=\"font-size: 12pt; font-family: 'times new roman', times, serif;\">The pressure of gas (P) = 3 atm = 3 x 10<sup>5<\/sup> N.m<sup>-2<\/sup><\/span><\/p>\n<p class=\"western\" style=\"text-align: justify;\" align=\"justify\"><span style=\"font-size: 12pt; font-family: 'times new roman', times, serif;\">The heat capacity of gas (C) = 9 J.K<sup>-1<\/sup><\/span><\/p>\n<p class=\"western\" style=\"text-align: justify;\" align=\"justify\"><span style=\"font-size: 12pt; font-family: 'times new roman', times, serif;\"><u>Wanted :<\/u> The final volume of gas (V<sub>2<\/sub>) and the change of internal energy of gas (\u0394U)<\/span><\/p>\n<p class=\"western\" style=\"text-align: justify;\" align=\"justify\"><span style=\"font-family: 'times new roman', times, serif; font-size: 12pt;\"><u>Solution :<\/u><\/span><\/p>\n<p class=\"western\" style=\"text-align: justify;\" align=\"justify\"><span style=\"font-size: 12pt; font-family: 'times new roman', times, serif;\">Determine the final volume using the equation of <a href=\"https:\/\/gurumuda.net\/physics\/charless-law-constant-pressure-problems-and-solutions.htm\" target=\"_blank\" rel=\"noopener\">Charles&#8217;s law<\/a> (isobaric process or constant pressure) :<\/span><\/p>\n<p style=\"text-align: justify;\" align=\"justify\"><span style=\"font-size: 12pt; font-family: 'times new roman', times, serif;\"><img loading=\"lazy\" decoding=\"async\" class=\"aligncenter size-full wp-image-2297\" src=\"https:\/\/gurumuda.net\/physics\/wp-content\/uploads\/2018\/04\/Kinetic-theory-of-gas-and-thermodynamic-\u2013-problems-and-solutions-1.png\" alt=\"Kinetic theory of gas and thermodynamic \u2013 problems and solutions 1\" width=\"145\" height=\"241\" \/><\/span><\/p>\n<p class=\"western\" style=\"text-align: justify;\" align=\"justify\"><span style=\"font-family: 'times new roman', times, serif; font-size: 12pt;\"><u>The change in volume :<\/u><\/span><\/p>\n<p class=\"western\" style=\"text-align: justify;\" align=\"justify\"><span style=\"font-size: 12pt; font-family: 'times new roman', times, serif;\">1 liter = 0.001 m<sup>3 <\/sup><\/span><\/p>\n<p class=\"western\" style=\"text-align: justify;\" align=\"justify\"><span style=\"font-size: 12pt; font-family: 'times new roman', times, serif;\">Initial volume (V<sub>1<\/sub>) = 4 (0.001 m<sup>3<\/sup>) = 0.004 m<sup>3<\/sup><\/span><\/p>\n<p class=\"western\" style=\"text-align: justify;\" align=\"justify\"><span style=\"font-size: 12pt; font-family: 'times new roman', times, serif;\">Final volume (V<sub>2<\/sub>) = 4.8 (0.001 m<sup>3<\/sup>) = 0.0048 m<sup>3<\/sup><\/span><\/p>\n<p class=\"western\" style=\"text-align: justify;\" align=\"justify\"><span style=\"font-size: 12pt; font-family: 'times new roman', times, serif;\">The change in volume (\u0394V) = V<sub>2<\/sub> \u2013 V<sub>1 <\/sub>= 0.0048 m<sup>3<\/sup> \u2013 0.004 m<sup>3<\/sup> = 0.008 m<sup>3<\/sup>. <\/span><\/p>\n<p class=\"western\" style=\"text-align: justify;\" align=\"justify\"><span style=\"font-family: 'times new roman', times, serif; font-size: 12pt;\"><u>The change in temperature :<\/u><\/span><\/p>\n<p class=\"western\" style=\"text-align: justify;\" align=\"justify\"><span style=\"font-size: 12pt; font-family: 'times new roman', times, serif;\">The change in temperature (\u0394T) = T<sub>2<\/sub> \u2013 T<sub>1<\/sub> = 360 K &#8211; 300 K = 60 K <\/span><\/p>\n<p class=\"western\" style=\"text-align: justify;\" align=\"justify\"><span style=\"font-family: 'times new roman', times, serif; font-size: 12pt;\">Determine the change of the internal energy (\u0394U) of the ideal gas using the equation of the first law of thermodynamics.<\/span><\/p>\n<p class=\"western\" style=\"text-align: justify;\" align=\"justify\"><span style=\"font-family: 'times new roman', times, serif; font-size: 12pt;\">\u0394U = Q \u2013 W<\/span><\/p>\n<p class=\"western\" style=\"text-align: justify;\" align=\"justify\"><span style=\"font-family: 'times new roman', times, serif; font-size: 12pt;\"><i>\u0394U = the change of the internal energy, Q = heat, W = work<\/i><\/span><\/p>\n<p class=\"western\" style=\"text-align: justify;\" align=\"justify\"><span style=\"font-family: 'times new roman', times, serif; font-size: 12pt;\">Determine work (W) at constant pressure :<\/span><\/p>\n<p class=\"western\" style=\"text-align: justify;\" align=\"justify\"><span style=\"font-size: 12pt; font-family: 'times new roman', times, serif;\">W = P \u0394V = (3 x 10<sup>5<\/sup>)(0.0008) = (3 x 10<sup>1<\/sup>)(8) = (30)(8) = 240 Joule <\/span><\/p>\n<p class=\"western\" style=\"text-align: justify;\" align=\"justify\"><span style=\"font-family: 'times new roman', times, serif; font-size: 12pt;\">Determine heat (Q) using the equation of the heat capacity (C) :<\/span><\/p>\n<p class=\"western\" style=\"text-align: justify;\" align=\"justify\"><span style=\"font-size: 12pt; font-family: 'times new roman', times, serif;\">C = Q \/ \u0394T<\/span><\/p>\n<p class=\"western\" style=\"text-align: justify;\" align=\"justify\"><span style=\"font-family: 'times new roman', times, serif; font-size: 12pt;\">Q = (C)(\u0394T) = (9)(60) = 540 Joule<\/span><\/p>\n<p class=\"western\" style=\"text-align: justify;\" align=\"justify\"><span style=\"font-family: 'times new roman', times, serif; font-size: 12pt;\">Determine the change of the internal energy :<\/span><\/p>\n<p class=\"western\" style=\"text-align: justify;\" align=\"justify\"><span style=\"font-size: 12pt; font-family: 'times new roman', times, serif;\">\u0394U = Q \u2013 W = 540 Joule &#8211; 240 Joule = 300 Joule.<\/span><\/p>\n<p class=\"western\" style=\"text-align: justify;\" align=\"justify\"><span style=\"font-size: 12pt; font-family: 'times new roman', times, serif;\">2. 6 liters of ideal gases at 2 atm are in a container (1 atm = 10<sup>5<\/sup> N.m<sup>-2<\/sup>). The gas heated from 27<sup>o<\/sup>C to 77<sup>o<\/sup>C at a constant pressure. If the heat capacity of gas is 5 J.K<sup>-1<\/sup>, what is the final volume and the change of internal energy of the gas.<\/span><\/p>\n<p class=\"western\" style=\"text-align: justify;\" align=\"justify\"><span style=\"font-family: 'times new roman', times, serif; font-size: 12pt;\">Solution :<\/span><\/p>\n<p class=\"western\" style=\"text-align: justify;\" align=\"justify\"><span style=\"font-family: 'times new roman', times, serif; font-size: 12pt;\"><b><a href=\"https:\/\/gurumuda.net\/physics\/isobaric-thermodynamics-processes-problems-and-solutions.htm\" target=\"_blank\" rel=\"noopener\">Isobaric process<\/a> (constant pressure)<\/b><\/span><\/p>\n<p class=\"western\" style=\"text-align: justify;\" align=\"justify\"><span style=\"font-family: 'times new roman', times, serif; font-size: 12pt;\"><u>Known :<\/u><\/span><\/p>\n<p class=\"western\" style=\"text-align: justify;\" align=\"justify\"><span style=\"font-size: 12pt; font-family: 'times new roman', times, serif;\">The initial volume of the ideal gases (V<sub>1<\/sub>) = 6 liters<\/span><\/p>\n<p class=\"western\" style=\"text-align: justify;\" align=\"justify\"><span style=\"font-size: 12pt; font-family: 'times new roman', times, serif;\">The initial temperature of the ideal gases (T<sub>1<\/sub>) = 27<sup>o<\/sup>C + 273 = 300 K <\/span><\/p>\n<p class=\"western\" style=\"text-align: justify;\" align=\"justify\"><span style=\"font-size: 12pt; font-family: 'times new roman', times, serif;\">The final temperature of the ideal gases (T<sub>2<\/sub>) = 77<sup>o<\/sup>C + 273 = 350 K <\/span><\/p>\n<p class=\"western\" style=\"text-align: justify;\" align=\"justify\"><span style=\"font-size: 12pt; font-family: 'times new roman', times, serif;\">The pressure of the ideal gases (P) = 2 atm = 2 x 10<sup>5<\/sup> N.m<sup>-2<\/sup><\/span><\/p>\n<p class=\"western\" style=\"text-align: justify;\" align=\"justify\"><span style=\"font-size: 12pt; font-family: 'times new roman', times, serif;\">The heat capacity of gases (C) = 5 J.K<sup>-1<\/sup><\/span><\/p>\n<p class=\"western\" style=\"text-align: justify;\" align=\"justify\"><span style=\"font-size: 12pt; font-family: 'times new roman', times, serif;\"><u>Wanted:<\/u> The final volume of the gas (V<sub>2<\/sub>) and the change of internal energy of the gas (\u0394U)<\/span><\/p>\n<p class=\"western\" style=\"text-align: justify;\" align=\"justify\"><span style=\"font-family: 'times new roman', times, serif; font-size: 12pt;\"><u>Solution :<\/u><\/span><\/p>\n<p class=\"western\" style=\"text-align: justify;\" align=\"justify\"><span style=\"font-size: 12pt; font-family: 'times new roman', times, serif;\">Determine the final volume of gas using the equation of Charles&#8217;s law (isobaric process or constant pressure) :<\/span><\/p>\n<p style=\"text-align: justify;\" align=\"justify\"><span style=\"font-size: 12pt; font-family: 'times new roman', times, serif;\"><img loading=\"lazy\" decoding=\"async\" class=\"aligncenter size-full wp-image-2298\" src=\"https:\/\/gurumuda.net\/physics\/wp-content\/uploads\/2018\/04\/Kinetic-theory-of-gas-and-thermodynamic-\u2013-problems-and-solutions-2.png\" alt=\"Kinetic theory of gas and thermodynamic \u2013 problems and solutions 2\" width=\"140\" height=\"208\" \/><\/span><\/p>\n<p class=\"western\" style=\"text-align: justify;\" align=\"justify\"><span style=\"font-family: 'times new roman', times, serif; font-size: 12pt;\"><u>The change in volume :<\/u><\/span><\/p>\n<p class=\"western\" style=\"text-align: justify;\" align=\"justify\"><span style=\"font-size: 12pt; font-family: 'times new roman', times, serif;\">1 liter = 0.001 m<sup>3 <\/sup><\/span><\/p>\n<p class=\"western\" style=\"text-align: justify;\" align=\"justify\"><span style=\"font-size: 12pt; font-family: 'times new roman', times, serif;\">The initial volume (V<sub>1<\/sub>) = 6 (0.001 m<sup>3<\/sup>) = 0.006 m<sup>3<\/sup><\/span><\/p>\n<p class=\"western\" style=\"text-align: justify;\" align=\"justify\"><span style=\"font-size: 12pt; font-family: 'times new roman', times, serif;\">The final volume (V<sub>2<\/sub>) = 7 (0.001 m<sup>3<\/sup>) = 0.007 m<sup>3<\/sup><\/span><\/p>\n<p class=\"western\" style=\"text-align: justify;\" align=\"justify\"><span style=\"font-size: 12pt; font-family: 'times new roman', times, serif;\">The change in volume (\u0394V) = V<sub>2<\/sub> \u2013 V<sub>1<\/sub> = 0.007 m<sup>3<\/sup> \u2013 0.006 m<sup>3<\/sup> = 0.001 m<sup>3<\/sup><\/span><\/p>\n<p class=\"western\" style=\"text-align: justify;\" align=\"justify\"><span style=\"font-family: 'times new roman', times, serif; font-size: 12pt;\"><u>The change in temperature :<\/u><\/span><\/p>\n<p class=\"western\" style=\"text-align: justify;\" align=\"justify\"><span style=\"font-size: 12pt; font-family: 'times new roman', times, serif;\">The change in temperature (\u0394T) = T<sub>2<\/sub> \u2013 T<sub>1 <\/sub>= 350 K &#8211; 300 K = 50 K <\/span><\/p>\n<p class=\"western\" style=\"text-align: justify;\" align=\"justify\"><span style=\"font-family: 'times new roman', times, serif; font-size: 12pt;\">Determine the change of the internal energy (\u0394U) of the ideal gases using the equation of the first law of thermodynamics.<\/span><\/p>\n<p class=\"western\" style=\"text-align: justify;\" align=\"justify\"><span style=\"font-family: 'times new roman', times, serif; font-size: 12pt;\">\u0394U = Q \u2013 W<\/span><\/p>\n<p class=\"western\" style=\"text-align: justify;\" align=\"justify\"><span style=\"font-family: 'times new roman', times, serif; font-size: 12pt;\"><i>\u0394U = the change in the internal energy, Q = heat, W = work<\/i><\/span><\/p>\n<p class=\"western\" style=\"text-align: justify;\" align=\"justify\"><span style=\"font-family: 'times new roman', times, serif; font-size: 12pt;\">Determine work (W) at constant pressure :<\/span><\/p>\n<p class=\"western\" style=\"text-align: justify;\" align=\"justify\"><span style=\"font-size: 12pt; font-family: 'times new roman', times, serif;\">W = P \u0394V = (2 x 10<sup>5<\/sup>)(0.001) = (2 x 10<sup>2<\/sup>)(1) = (200)(1) = 200 Joule <\/span><\/p>\n<p class=\"western\" style=\"text-align: justify;\" align=\"justify\"><span style=\"font-family: 'times new roman', times, serif; font-size: 12pt;\">Determine heat (Q) using the equation of the heat capacity (C) :<\/span><\/p>\n<p class=\"western\" style=\"text-align: justify;\" align=\"justify\"><span style=\"font-size: 12pt; font-family: 'times new roman', times, serif;\">C = Q \/ \u0394T<\/span><\/p>\n<p class=\"western\" style=\"text-align: justify;\" align=\"justify\"><span style=\"font-family: 'times new roman', times, serif; font-size: 12pt;\">Q = (C)(\u0394T) = (5)(50) = 250 Joule<\/span><\/p>\n<p class=\"western\" style=\"text-align: justify;\" align=\"justify\"><span style=\"font-family: 'times new roman', times, serif; font-size: 12pt;\">Determine the change in the internal energy :<\/span><\/p>\n<p class=\"western\" style=\"text-align: justify;\" align=\"justify\"><span style=\"font-size: 12pt; font-family: 'times new roman', times, serif;\">\u0394U = Q \u2013 W = 250 Joule &#8211; 200 Joule = 50 Joule.<\/span><\/p>\n<ol>\n<li style=\"text-align: justify;\"><span style=\"font-size: 12pt; font-family: 'times new roman', times, serif;\"><strong>What are the main assumptions of the kinetic theory of gases?<\/strong><\/span>\n<ul>\n<li><span style=\"font-size: 12pt; font-family: 'times new roman', times, serif;\"><strong>Answer:<\/strong> The kinetic theory of gases assumes that: (a) Gases consist of a large number of tiny particles that are in constant random motion; (b) These particles are far apart relative to their size; (c) Collisions between gas particles, or between a particle and the walls of its container, are elastic (i.e., no kinetic energy is lost); (d) There are no intermolecular forces between gas particles; and (e) The average kinetic energy of the gas particles is directly proportional to the absolute temperature of the gas.<\/span><\/li>\n<\/ul>\n<\/li>\n<li style=\"text-align: justify;\"><span style=\"font-size: 12pt; font-family: 'times new roman', times, serif;\"><strong>How is the average kinetic energy of gas molecules related to the temperature of the gas?<\/strong><\/span>\n<ul>\n<li><span style=\"font-size: 12pt; font-family: 'times new roman', times, serif;\"><strong>Answer:<\/strong> The average kinetic energy of gas molecules is directly proportional to the absolute temperature (in Kelvin) of the gas. As the temperature increases, the average kinetic energy of the molecules also increases.<\/span><\/li>\n<\/ul>\n<\/li>\n<li style=\"text-align: justify;\"><span style=\"font-size: 12pt; font-family: 'times new roman', times, serif;\"><strong>What is the significance of absolute zero in terms of molecular motion?<\/strong><\/span>\n<ul>\n<li><span style=\"font-size: 12pt; font-family: 'times new roman', times, serif;\"><strong>Answer:<\/strong> Absolute zero (0 Kelvin) is theoretically the temperature at which all molecular motion stops. It represents the lowest possible temperature where nothing could be colder and no heat energy remains in a substance.<\/span><\/li>\n<\/ul>\n<\/li>\n<li style=\"text-align: justify;\"><span style=\"font-size: 12pt; font-family: 'times new roman', times, serif;\"><strong>What is the first law of thermodynamics in terms of internal energy, heat, and work?<\/strong><\/span>\n<ul>\n<li><span style=\"font-size: 12pt; font-family: 'times new roman', times, serif;\"><strong>Answer:<\/strong> The first law of thermodynamics states that the change in the internal energy of a system is equal to the heat added to the system minus the work done by the system on its surroundings: \u0394U = Q &#8211; W.<\/span><\/li>\n<\/ul>\n<\/li>\n<li style=\"text-align: justify;\"><span style=\"font-size: 12pt; font-family: 'times new roman', times, serif;\"><strong>In an isochoric process, what happens to the work done by or on the system?<\/strong><\/span>\n<ul>\n<li><span style=\"font-size: 12pt; font-family: 'times new roman', times, serif;\"><strong>Answer:<\/strong> In an isochoric process, the volume remains constant. Hence, there is no work done by or on the system, as work in such cases is given by the pressure-volume work, which would be zero if the volume doesn&#8217;t change.<\/span><\/li>\n<\/ul>\n<\/li>\n<li style=\"text-align: justify;\"><span style=\"font-size: 12pt; font-family: 'times new roman', times, serif;\"><strong>What does it mean when we say that a gas is &#8220;ideal&#8221;?<\/strong><\/span>\n<ul>\n<li><span style=\"font-size: 12pt; font-family: 'times new roman', times, serif;\"><strong>Answer:<\/strong> An &#8220;ideal&#8221; gas is one that follows the ideal gas law (PV = nRT) under all conditions of temperature and pressure. It also means that the gas follows the postulates of the kinetic theory perfectly, with no intermolecular forces and perfectly elastic collisions.<\/span><\/li>\n<\/ul>\n<\/li>\n<li style=\"text-align: justify;\"><span style=\"font-size: 12pt; font-family: 'times new roman', times, serif;\"><strong>How do real gases deviate from the behavior of ideal gases?<\/strong><\/span>\n<ul>\n<li><span style=\"font-size: 12pt; font-family: 'times new roman', times, serif;\"><strong>Answer:<\/strong> Real gases deviate from ideal behavior at high pressures and low temperatures. This is due to the presence of intermolecular forces and the finite size of gas molecules. The deviations are described by the van der Waals equation and other similar equations.<\/span><\/li>\n<\/ul>\n<\/li>\n<li>\n<p style=\"text-align: justify;\"><span style=\"font-size: 12pt; font-family: 'times new roman', times, serif;\"><strong>Why can the first law of thermodynamics be thought of as a conservation law?<\/strong><\/span><\/p>\n<ul>\n<li style=\"text-align: justify;\"><span style=\"font-size: 12pt; font-family: 'times new roman', times, serif;\"><strong>Answer:<\/strong> The first law of thermodynamics can be considered a conservation law because it states that energy cannot be created or destroyed, only transferred or converted from one form to another. This mirrors the principle of conservation of energy.<\/span><\/li>\n<\/ul>\n<\/li>\n<\/ol>\n","protected":false,"gt_translate_keys":[{"key":"rendered","format":"html"}]},"excerpt":{"rendered":"<p>Kinetic theory of gas and first law of thermodynamics \u2013 problems and solutions 1. Ideal gases are in a container with a volume of 4 liters and its pressure is 3 atm (1 atm = 105 N.m-2). The ideal gases heated at a constant pressure from 27oC to 87oC. The heat capacity of the gas &#8230; <a title=\"Kinetic theory of gas and first law of thermodynamics \u2013 problems and solutions\" class=\"read-more\" href=\"https:\/\/gurumuda.net\/physics\/kinetic-theory-of-gas-and-first-law-of-thermodynamics-problems-and-solutions.htm\" aria-label=\"Read more about Kinetic theory of gas and first law of thermodynamics \u2013 problems and solutions\">Read more<\/a><\/p>\n","protected":false,"gt_translate_keys":[{"key":"rendered","format":"html"}]},"author":1,"featured_media":0,"comment_status":"closed","ping_status":"closed","sticky":false,"template":"","format":"standard","meta":{"_seopress_titles_title":"","_seopress_titles_desc":"","_seopress_robots_index":"","_seopress_robots_follow":"","_seopress_robots_imageindex":"","_seopress_robots_snippet":"","_seopress_robots_primary_cat":"","_seopress_robots_breadcrumbs":"","_seopress_robots_freeze_modified_date":"","_seopress_robots_custom_modified_date":"","_seopress_robots_canonical":"","_seopress_social_fb_title":"","_seopress_social_fb_desc":"","_seopress_social_fb_img":"","_seopress_social_fb_img_attachment_id":0,"_seopress_social_fb_img_width":0,"_seopress_social_fb_img_height":0,"_seopress_social_twitter_title":"","_seopress_social_twitter_desc":"","_seopress_social_twitter_img":"","_seopress_social_twitter_img_attachment_id":0,"_seopress_social_twitter_img_width":0,"_seopress_social_twitter_img_height":0,"_seopress_redirections_value":"","_seopress_redirections_enabled":"","_seopress_redirections_enabled_regex":"","_seopress_redirections_logged_status":"","_seopress_redirections_param":"","_seopress_redirections_type":0,"_seopress_analysis_target_kw":"Kinetic theory of gas and first law of thermodynamics \u2013 problems and solutions","_seopress_news_disabled":"","_seopress_video_disabled":"","_seopress_video":[],"_seopress_pro_schemas_manual":[],"_seopress_pro_rich_snippets_disable_all":"","_seopress_pro_rich_snippets_disable":[],"_seopress_pro_schemas":[],"footnotes":""},"categories":[3],"tags":[],"class_list":["post-2296","post","type-post","status-publish","format-standard","hentry","category-solved-problems-in-basic-physics"],"gt_translate_keys":[{"key":"link","format":"url"}],"_links":{"self":[{"href":"https:\/\/gurumuda.net\/physics\/wp-json\/wp\/v2\/posts\/2296","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/gurumuda.net\/physics\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/gurumuda.net\/physics\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/gurumuda.net\/physics\/wp-json\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/gurumuda.net\/physics\/wp-json\/wp\/v2\/comments?post=2296"}],"version-history":[{"count":2,"href":"https:\/\/gurumuda.net\/physics\/wp-json\/wp\/v2\/posts\/2296\/revisions"}],"predecessor-version":[{"id":8612,"href":"https:\/\/gurumuda.net\/physics\/wp-json\/wp\/v2\/posts\/2296\/revisions\/8612"}],"wp:attachment":[{"href":"https:\/\/gurumuda.net\/physics\/wp-json\/wp\/v2\/media?parent=2296"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/gurumuda.net\/physics\/wp-json\/wp\/v2\/categories?post=2296"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/gurumuda.net\/physics\/wp-json\/wp\/v2\/tags?post=2296"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}