{"id":209207,"date":"2025-04-28T16:16:40","date_gmt":"2025-04-28T16:16:40","guid":{"rendered":"https:\/\/learnexams.com\/blog\/?p=209207"},"modified":"2025-04-28T16:16:48","modified_gmt":"2025-04-28T16:16:48","slug":"a-gas-contained-in-a-piston-cylinder-assembly-undergoes-two-processes","status":"publish","type":"post","link":"https:\/\/www.learnexams.com\/blog\/2025\/04\/28\/a-gas-contained-in-a-piston-cylinder-assembly-undergoes-two-processes\/","title":{"rendered":"A gas contained in a piston-cylinder assembly undergoes two processes"},"content":{"rendered":"\n<p>A gas contained in a piston-cylinder assembly undergoes two processes, A and B, between the same end states, 1 and 2, where p1 =1bar, V1 = 1m3, U1 =400kJ and p * 2 = 10 bar, V2 = 0.1 m3, U2 = 450 kJ: Process A: Constant-volume process from state 1 to a pressure of 10 bar, followed by a constantpressure process to state 2. Process B: Process from 1 to 2 during which the pressure-volume relation is pV = constant. Kinetic and potential effects can be ignored. For each of the processes A and B, (a) sketch the process on p-V coordinates, (b) evaluate the work, in kJ, and (c) evaluate the heat transfer, in kJ.<\/p>\n\n\n\n<p><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-ast-global-color-6-color\"><strong>The correct answer and explanation is :<\/strong><\/mark><\/p>\n\n\n\n<p>Alright, let\u2019s work through this carefully.<\/p>\n\n\n\n<hr class=\"wp-block-separator has-alpha-channel-opacity\"\/>\n\n\n\n<h3 class=\"wp-block-heading\">First, <strong>given data<\/strong>:<\/h3>\n\n\n\n<ul class=\"wp-block-list\">\n<li>State 1:<br>( p_1 = 1\\, \\text{bar} = 100\\, \\text{kPa} )<br>( V_1 = 1\\, \\text{m}^3 )<br>( U_1 = 400\\, \\text{kJ} )<\/li>\n\n\n\n<li>State 2:<br>( p_2 = 10\\, \\text{bar} = 1000\\, \\text{kPa} )<br>( V_2 = 0.1\\, \\text{m}^3 )<br>( U_2 = 450\\, \\text{kJ} )<\/li>\n<\/ul>\n\n\n\n<hr class=\"wp-block-separator has-alpha-channel-opacity\"\/>\n\n\n\n<h2 class=\"wp-block-heading\">(a) Sketch on <strong>p-V Diagram<\/strong>:<\/h2>\n\n\n\n<ul class=\"wp-block-list\">\n<li><strong>Process A<\/strong>:<\/li>\n\n\n\n<li>Step 1: Constant <strong>volume<\/strong> compression (vertical line up on p-V diagram) from 1 bar to 10 bar.<\/li>\n\n\n\n<li>Step 2: Constant <strong>pressure<\/strong> compression (horizontal line left) from ( V_1 = 1\\, \\text{m}^3 ) to ( V_2 = 0.1\\, \\text{m}^3 ) at ( p = 10\\, \\text{bar} ).<\/li>\n\n\n\n<li><strong>Process B<\/strong>:<\/li>\n\n\n\n<li>( pV = \\text{constant} ) (a hyperbolic curve, called an isothermal-like shape but NOT necessarily isothermal).<\/li>\n<\/ul>\n\n\n\n<hr class=\"wp-block-separator has-alpha-channel-opacity\"\/>\n\n\n\n<h2 class=\"wp-block-heading\">(b) <strong>Work done (W)<\/strong><\/h2>\n\n\n\n<h3 class=\"wp-block-heading\">Process A:<\/h3>\n\n\n\n<ul class=\"wp-block-list\">\n<li>Step 1 (constant volume):<br>( W = 0 ) (because ( dV = 0 ))<\/li>\n\n\n\n<li>Step 2 (constant pressure):<br>[<br>W = p (V_2 &#8211; V_1)<br>]<br>Substituting values:<br>[<br>W = 1000\\, \\text{kPa} \\times (0.1 &#8211; 1) \\, \\text{m}^3 = 1000 \\times (-0.9) = -900\\, \\text{kJ}<br>]<\/li>\n<\/ul>\n\n\n\n<blockquote class=\"wp-block-quote is-layout-flow wp-block-quote-is-layout-flow\">\n<p>So, <strong>Work for Process A<\/strong> = <strong>(-900) kJ<\/strong><\/p>\n<\/blockquote>\n\n\n\n<hr class=\"wp-block-separator has-alpha-channel-opacity\"\/>\n\n\n\n<h3 class=\"wp-block-heading\">Process B:<\/h3>\n\n\n\n<p>Since ( pV = \\text{constant} ), it is a <strong>polytropic process<\/strong> with ( n = 1 ).<\/p>\n\n\n\n<p>Work formula for ( n = 1 ) process:<br>[<br>W = p_1 V_1 \\ln\\left( \\frac{V_2}{V_1} \\right)<br>]<\/p>\n\n\n\n<p>Substituting:<br>[<br>W = (100\\, \\text{kPa})(1\\, \\text{m}^3) \\ln\\left( \\frac{0.1}{1} \\right)<br>]<br>[<br>= 100 \\times \\ln(0.1)<br>]<br>[<br>= 100 \\times (-2.3026)<br>]<br>[<br>= -230.26\\, \\text{kJ}<br>]<\/p>\n\n\n\n<blockquote class=\"wp-block-quote is-layout-flow wp-block-quote-is-layout-flow\">\n<p>So, <strong>Work for Process B<\/strong> = <strong>(-230.26) kJ<\/strong><\/p>\n<\/blockquote>\n\n\n\n<hr class=\"wp-block-separator has-alpha-channel-opacity\"\/>\n\n\n\n<h2 class=\"wp-block-heading\">(c) <strong>Heat transfer (Q)<\/strong><\/h2>\n\n\n\n<p>From <strong>First Law of Thermodynamics<\/strong>:<br>[<br>Q = \\Delta U + W<br>]<br>where:<br>[<br>\\Delta U = U_2 &#8211; U_1 = 450 &#8211; 400 = 50\\, \\text{kJ}<br>]<\/p>\n\n\n\n<hr class=\"wp-block-separator has-alpha-channel-opacity\"\/>\n\n\n\n<h3 class=\"wp-block-heading\">Process A:<\/h3>\n\n\n\n<p>[<br>Q_A = \\Delta U + W_A<br>]<br>[<br>Q_A = 50 + (-900)<br>]<br>[<br>Q_A = -850\\, \\text{kJ}<br>]<\/p>\n\n\n\n<hr class=\"wp-block-separator has-alpha-channel-opacity\"\/>\n\n\n\n<h3 class=\"wp-block-heading\">Process B:<\/h3>\n\n\n\n<p>[<br>Q_B = \\Delta U + W_B<br>]<br>[<br>Q_B = 50 + (-230.26)<br>]<br>[<br>Q_B = -180.26\\, \\text{kJ}<br>]<\/p>\n\n\n\n<hr class=\"wp-block-separator has-alpha-channel-opacity\"\/>\n\n\n\n<h1 class=\"wp-block-heading\"><strong>Summary of Results:<\/strong><\/h1>\n\n\n\n<figure class=\"wp-block-table\"><table class=\"has-fixed-layout\"><thead><tr><th><\/th><th>Work (kJ)<\/th><th>Heat Transfer (kJ)<\/th><\/tr><\/thead><tbody><tr><td>Process A<\/td><td>-900<\/td><td>-850<\/td><\/tr><tr><td>Process B<\/td><td>-230.26<\/td><td>-180.26<\/td><\/tr><\/tbody><\/table><\/figure>\n\n\n\n<hr class=\"wp-block-separator has-alpha-channel-opacity\"\/>\n\n\n\n<h2 class=\"wp-block-heading\"><strong>Explanation (300+ words):<\/strong><\/h2>\n\n\n\n<p>This problem involves analyzing two different thermodynamic processes that take a gas between the same starting and ending conditions, but using different paths. In Process A, the gas first undergoes a constant volume compression, meaning the piston is locked, and the pressure increases from 1 bar to 10 bar without any volume change. Since the volume doesn\u2019t change, no work is done during this step (( W = 0 )). After reaching 10 bar, the gas is compressed at constant pressure from a volume of 1 m\u00b3 to 0.1 m\u00b3. For a constant pressure process, the work is simply the pressure multiplied by the volume change. Here, because the volume is decreasing, the work comes out negative, meaning the system is compressed.<\/p>\n\n\n\n<p>In Process B, the gas undergoes a process where ( pV ) remains constant. This is known as a polytropic process with ( n = 1 ). The work done during this process involves integrating ( p \\, dV ) while keeping ( pV = \\text{constant} ), leading to the logarithmic formula for work. The work is again negative because the volume is decreasing during compression, although it is a smaller magnitude compared to Process A.<\/p>\n\n\n\n<p>Once the work is known for each process, we use the first law of thermodynamics to find the heat transfer: ( Q = \\Delta U + W ). The internal energy change ( \\Delta U ) is positive, meaning the gas absorbs internal energy, but because the work terms are negative and larger in magnitude, the heat transfer ends up being negative for both processes. A negative heat transfer indicates that the system loses heat to the surroundings.<\/p>\n\n\n\n<p>The results show that Process A requires more compression work (\u2013900 kJ) compared to Process B (\u2013230.26 kJ), and correspondingly, loses more heat. This highlights how the path between states significantly affects work and heat interactions even if the initial and final states are identical.<\/p>\n\n\n\n<hr class=\"wp-block-separator has-alpha-channel-opacity\"\/>\n","protected":false},"excerpt":{"rendered":"<p>A gas contained in a piston-cylinder assembly undergoes two processes, A and B, between the same end states, 1 and 2, where p1 =1bar, V1 = 1m3, U1 =400kJ and p * 2 = 10 bar, V2 = 0.1 m3, U2 = 450 kJ: Process A: Constant-volume process from state 1 to a pressure of [&hellip;]<\/p>\n","protected":false},"author":1,"featured_media":0,"comment_status":"closed","ping_status":"closed","sticky":false,"template":"","format":"standard","meta":{"site-sidebar-layout":"default","site-content-layout":"","ast-site-content-layout":"default","site-content-style":"default","site-sidebar-style":"default","ast-global-header-display":"","ast-banner-title-visibility":"","ast-main-header-display":"","ast-hfb-above-header-display":"","ast-hfb-below-header-display":"","ast-hfb-mobile-header-display":"","site-post-title":"","ast-breadcrumbs-content":"","ast-featured-img":"","footer-sml-layout":"","ast-disable-related-posts":"","theme-transparent-header-meta":"","adv-header-id-meta":"","stick-header-meta":"","header-above-stick-meta":"","header-main-stick-meta":"","header-below-stick-meta":"","astra-migrate-meta-layouts":"default","ast-page-background-enabled":"default","ast-page-background-meta":{"desktop":{"background-color":"","background-image":"","background-repeat":"repeat","background-position":"center center","background-size":"auto","background-attachment":"scroll","background-type":"","background-media":"","overlay-type":"","overlay-color":"","overlay-opacity":"","overlay-gradient":""},"tablet":{"background-color":"","background-image":"","background-repeat":"repeat","background-position":"center center","background-size":"auto","background-attachment":"scroll","background-type":"","background-media":"","overlay-type":"","overlay-color":"","overlay-opacity":"","overlay-gradient":""},"mobile":{"background-color":"","background-image":"","background-repeat":"repeat","background-position":"center center","background-size":"auto","background-attachment":"scroll","background-type":"","background-media":"","overlay-type":"","overlay-color":"","overlay-opacity":"","overlay-gradient":""}},"ast-content-background-meta":{"desktop":{"background-color":"var(--ast-global-color-5)","background-image":"","background-repeat":"repeat","background-position":"center center","background-size":"auto","background-attachment":"scroll","background-type":"","background-media":"","overlay-type":"","overlay-color":"","overlay-opacity":"","overlay-gradient":""},"tablet":{"background-color":"var(--ast-global-color-5)","background-image":"","background-repeat":"repeat","background-position":"center center","background-size":"auto","background-attachment":"scroll","background-type":"","background-media":"","overlay-type":"","overlay-color":"","overlay-opacity":"","overlay-gradient":""},"mobile":{"background-color":"var(--ast-global-color-5)","background-image":"","background-repeat":"repeat","background-position":"center center","background-size":"auto","background-attachment":"scroll","background-type":"","background-media":"","overlay-type":"","overlay-color":"","overlay-opacity":"","overlay-gradient":""}},"footnotes":""},"categories":[25],"tags":[],"class_list":["post-209207","post","type-post","status-publish","format-standard","hentry","category-exams-certification"],"_links":{"self":[{"href":"https:\/\/www.learnexams.com\/blog\/wp-json\/wp\/v2\/posts\/209207","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/www.learnexams.com\/blog\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/www.learnexams.com\/blog\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/www.learnexams.com\/blog\/wp-json\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/www.learnexams.com\/blog\/wp-json\/wp\/v2\/comments?post=209207"}],"version-history":[{"count":0,"href":"https:\/\/www.learnexams.com\/blog\/wp-json\/wp\/v2\/posts\/209207\/revisions"}],"wp:attachment":[{"href":"https:\/\/www.learnexams.com\/blog\/wp-json\/wp\/v2\/media?parent=209207"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.learnexams.com\/blog\/wp-json\/wp\/v2\/categories?post=209207"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.learnexams.com\/blog\/wp-json\/wp\/v2\/tags?post=209207"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}