Phenomenological and Theoretical Analysis of Relativistic Temperature Transformation and Relativistic Entropy

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If the process is isotherm the Boyles law is Lorentz invariant. Also equilibrium constant and Gibbs energy, activation energy, enthalpy entropy and extent of the reaction became Lorentz invariant." /> <meta name="citation_title" content="Phenomenological and Theoretical Analysis of Relativistic Temperature Transformation and Relativistic Entropy" /> <meta name="citation_doi" content="10.5281/zenodo.1334830" /> <meta name="citation_abstract_html_url" content="https://zenodo.org/records/1334830" /> <meta property="og:title" content="Phenomenological and Theoretical Analysis of Relativistic Temperature Transformation and Relativistic Entropy" /> <meta property="og:description" content="There are three possible effects of Special Theory of Relativity (STR) on a thermodynamic system. Planck and Einstein looked upon this process as isobaric; on the other hand Ott saw it as an adiabatic process. However plenty of logical reasons show that the process is isotherm. Our phenomenological consideration demonstrates that the temperature is invariant with Lorenz transformation. In that case process is isotherm, so volume and pressure are Lorentz covariant. If the process is isotherm the Boyles law is Lorentz invariant. Also equilibrium constant and Gibbs energy, activation energy, enthalpy entropy and extent of the reaction became Lorentz invariant." /> <meta property="og:url" content="https://zenodo.org/records/1334830" /> <meta property="og:site_name" content="Zenodo" /> <meta name="twitter:card" content="summary" /> <meta name="twitter:site" content="@zenodo_org" /> <meta name="twitter:title" content="Phenomenological and Theoretical Analysis of Relativistic Temperature Transformation and Relativistic Entropy" /> <meta name="twitter:description" content="There are three possible effects of Special Theory of Relativity (STR) on a thermodynamic system. Planck and Einstein looked upon this process as isobaric; on the other hand Ott saw it as an adiabatic process. However plenty of logical reasons show that the process is isotherm. Our phenomenological consideration demonstrates that the temperature is invariant with Lorenz transformation. In that case process is isotherm, so volume and pressure are Lorentz covariant. If the process is isotherm the Boyles law is Lorentz invariant. Also equilibrium constant and Gibbs energy, activation energy, enthalpy entropy and extent of the reaction became Lorentz invariant." /> <meta name="citation_pdf_url" content="https://zenodo.org/records/1334830/files/13452.pdf"/> <link rel="alternate" type="application/pdf" href="https://zenodo.org/records/1334830/files/13452.pdf"> <link rel="canonical" href="https://zenodo.org/records/1334830"> <title>Phenomenological and Theoretical Analysis of Relativistic Temperature Transformation and Relativistic Entropy</title> <link rel="shortcut icon" type="image/x-icon" href="/static/favicon.ico"/> <link rel="apple-touch-icon" sizes="120x120" href="/static/apple-touch-icon-120.png"/> <link rel="apple-touch-icon" sizes="152x152" href="/static/apple-touch-icon-152.png"/> <link rel="apple-touch-icon" sizes="167x167" href="/static/apple-touch-icon-167.png"/> <link rel="apple-touch-icon" sizes="180x180" href="/static/apple-touch-icon-180.png"/> <link rel="stylesheet" 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href="/search?q=metadata.creators.person_or_org.name%3A%22Marko+Popovic%22" > <span class="creatibutor-name">Marko Popovic</span></a> </li> </ul> </div> </div> </div> </section> </section> <section id="description" class="rel-mt-2 rich-input-content" aria-label="Record description"> <h2 id="description-heading" class="sr-only">Description</h2> <div style="word-wrap: break-word;"> <p>There are three possible effects of Special Theory of Relativity (STR) on a thermodynamic system. Planck and Einstein looked upon this process as isobaric; on the other hand Ott saw it as an adiabatic process. However plenty of logical reasons show that the process is isotherm. Our phenomenological consideration demonstrates that the temperature is invariant with Lorenz transformation. In that case process is isotherm, so volume and pressure are Lorentz covariant. If the process is isotherm the Boyles law is Lorentz invariant. Also equilibrium constant and Gibbs energy, activation energy, enthalpy entropy and extent of the reaction became Lorentz invariant.</p> </div> </section> <section id="record-files" class="rel-mt-2 rel-mb-3" aria-label="Files" ><h2 id="files-heading">Files</h2> <div class="ui accordion panel mb-10 open" href="#files-preview-accordion-panel"> <h3 class="active title panel-heading open m-0"> <div role="button" id="files-preview-accordion-trigger" aria-controls="files-preview-accordion-panel" aria-expanded="true" tabindex="0" class="trigger" aria-label="File preview" > <span id="preview-file-title">13452.pdf</span> <i class="angle right icon" aria-hidden="true"></i> </div> </h3> <div role="region" id="files-preview-accordion-panel" aria-labelledby="files-preview-accordion-trigger" class="active content preview-container pt-0 open" > <div> <iframe title="Preview" class="preview-iframe" id="preview-iframe" name="preview-iframe" src="/records/1334830/preview/13452.pdf?include_deleted=0" > 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Planck and Einstein\nlooked upon this process as isobaric; on the other hand Ott saw it as\nan adiabatic process. However plenty of logical reasons show that the\nprocess is isotherm. Our phenomenological consideration\ndemonstrates that the temperature is invariant with Lorenz\ntransformation. In that case process is isotherm, so volume and\npressure are Lorentz covariant. If the process is isotherm the Boyles\nlaw is Lorentz invariant. Also equilibrium constant and Gibbs energy,\nactivation energy, enthalpy entropy and extent of the reaction became\nLorentz invariant.", "identifier": "https://doi.org/10.5281/zenodo.1334830", "inLanguage": {"@type": "Language", "alternateName": "eng", "name": "English"}, "issue": "2", "license": "https://creativecommons.org/licenses/by/4.0/legalcode", "name": "Phenomenological and Theoretical Analysis of Relativistic Temperature Transformation and Relativistic Entropy", "publisher": {"@type": "Organization", "name": "Zenodo"}, "size": "211.85 KB", "url": "https://zenodo.org/records/1334830", "version": "13452", "volume": "1.0"}</script> <script src="/static/dist/js/invenio-app-rdm-landing-page-theme.9b56690388e335810f04.js"></script> <script src="/static/dist/js/9945.e11a5a6ff50535c72070.js"></script> <script src="/static/dist/js/1357.4e237807ffba81b213b0.js"></script> <script src="/static/dist/js/1644.2b2007bc83e4beeabfaf.js"></script> <script src="/static/dist/js/8962.cfabe841decd009221fd.js"></script> <script src="/static/dist/js/9300.a81535ba51a38f1472fe.js"></script> <script src="/static/dist/js/9693.dac033d778162b60d96f.js"></script> <script src="/static/dist/js/invenio-app-rdm-landing-page.024f3c02bb324ddef007.js"></script> <script src="/static/dist/js/previewer_theme.77f20174699c7786038a.js"></script> <script src="/static/dist/js/zenodo-rdm-citations.f6ca22bc7712ee9b03f7.js"></script> <div class="ui container info message cookie-banner hidden"> <i class="close icon"></i> <div> <i aria-hidden="true" class="info icon"></i> <p class="inline">This site uses cookies. 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Phenomenological and Theoretical Analysis of Relativistic Temperature Transformation and Relativistic Entropy