Volumen 13, Número 4, Octubre - Diciembre, 2025, Páginas 150 al 166-1908175-63500DOI: https://doi.org/10.37787/9jwj3173ARTÍCULO ORIGINAL Determinación del ciclo teórico Otto mediante fichas técnicas de motores monocilíndricosDetermination of the theoretical Otto cycle using technical data sheets of single-cylinder enginesPariacurí, B. , Olivera, M. y Lozada, E. RESUMENLos motores de combustión interna cumplen un papel muy importante en nuestra sociedad, ya que son fundamentales en el transporte y la industria, muchas de estas máquinas son monocilíndricos y de baja cilindrada. En este contexto, el presente estudio tiene como objetivo principal determinar el ciclo teórico Otto mediante fichas técnicas proporcionadas por el fabricante. La metodología combina parte cualitativa y cuantitativa, la primera evalúa de manera gráfica los ciclos teóricos y su comportamiento de cada uno, la segunda, analiza la eficiencia, presiones, volumen, temperatura y energía transferidas para cada ciclo Otto estimado. Los resultados demuestran que los cuatro motores tienen eficiencias térmicas similares (entre 58.5% y 60.2%), sin embargo, el motor XTZ 125 destaca con una eficiencia (60.2%), concluyendo que la relación de compresión, es esencial para determinar su eficiencia, y que, a mayor cilindrada, no necesariamente va a ser más eficiente el motor. Esto es corroborado con el valor del calor rechazado que en el motor XTZ 125 es 323.701 kJ/kg, siendo el mínimo en relación a los cuatro motores estudiados, teniendo éxito en convertir gran parte del calor cedido en trabajo.Palabras clave: Ciclo Otto; motores; monocilíndricos; MCI; termodinámica.ABSTRACTInternal combustion engines play a very important role in our society, since they are essential in transportation and industry, many of these machines are single-cylinder and low-displacement. In this context, the main objective of this study is to determine the theoretical Otto cycle using technical sheets provided by the manufacturer. The methodology combines qualitative and quantitative parts, the first graphically evaluates the theoretical cycles and their behavior of each one, the second analyzes the efficiency, pressures, volume, temperature and energy transferred for each estimated Otto cycle. The results show that the four engines have similar thermal efficiencies (between 58.5% and 60.2%), however, the XTZ 125 engine stands out with an efficiency (60.2%), concluding that the compression ratio is essential to determine its efficiency, and that, a larger displacement, not necessarily the engine will be more efficient. This is corroborated by the value of the rejected heat which in the XTZ 125 engine is 323,701 kJ/kg, being the minimum in relation to the four engines studied, succeeding in converting a large part of the heat released into work.Keywords: Otto cycle; engines; single-cylinder; MCI; thermodynamics.* Autor para correspondenciaINTRODUCCIÓNEl ciclo termodinámico teórico es un esquema didáctico, donde se formula una serie de teorías básicas, que se correlacionan con el ciclo operativo teórico, para obtener mediante cálculos sencillos, parámetros de importancia básica ADDIN ZOTERO_ITEM CSL_CITATION {"citationID":"eBFqHIY7","properties":{"formattedCitation":"(Erazo & Viteri, 2018)","plainCitation":"(Erazo & Viteri, 2018)","noteIndex":0},"citationItems":[{"id":1467,"uris":["http://zotero.org/users/local/BP6I2uqk/items/XB6KDMGQ"],"itemData":{"id":1467,"type":"thesis","abstract":"In this document it is shown a methodology for determination of power, work and indicated mean pressure of an atmospheric Otto engine, respect to altitude above sea level by means of a thermodynamic analysis, using for this purpose the information provided by sensors that equipped the electronic fuel injection system and air – fuel ratio determined by lambda factor (λ), which is obtained with a gas analyzer. Indicated and operating parameters that have directly influence on engine performance have been determined, and in the same way is established a test protocol to obtain the variables for the calculation of these indicated parameters. As a result of the research is obtained a correlation between indicated parameters obtained in static test and altitude increasing, showing an average loss of zero point five percent for each hundred meters of high.","event-place":"Quito","language":"Español","license":"openAccess","note":"Accepted: 2018-11-23T20:30:21Z","number-of-pages":"219","publisher":"Escuela Politécnica Nacional","publisher-place":"Quito","source":"bibdigital.epn.edu.ec","title":"Análisis termodinámico de los parámetros indicados de un motor de ciclo Otto aspiración natural con sistema de inyección electrónica en función de la altitud sobre el nivel del mar","URL":"https://bibdigital.epn.edu.ec/handle/15000/19868","author":[{"family":"Erazo","given":"D"},{"family":"Viteri","given":"A"}],"accessed":{"date-parts":[["2025",9,16]]},"issued":{"date-parts":[["2018"]]}}}],"schema":"https://github.com/citation-style-language/schema/raw/master/csl-citation.json"} (Erazo & Viteri, 2018). Para los ciclos ideales se asume que los procesos de compresión y potencia son adiabáticos y reversibles, y que cualquier transferencia de calor convectiva, conductiva o radiactiva a la pared del cilindro durante el proceso de disipación de calor puede ignorarse; además, la pérdida de calor a través de la pared del cilindro ocurre únicamente durante la combustión y que es proporcional a la temperatura promedio tanto del fluido de trabajo como de la pared del cilindro ADDIN ZOTERO_ITEM CSL_CITATION {"citationID":"2gAwuzbJ","properties":{"formattedCitation":"(Hou, 2007)","plainCitation":"(Hou, 2007)","noteIndex":0},"citationItems":[{"id":1392,"uris":["http://zotero.org/users/local/BP6I2uqk/items/2YYJZVNB"],"itemData":{"id":1392,"type":"article-journal","container-title":"Energy Conversion and Management","DOI":"10.1016/j.enconman.2006.11.001","ISSN":"01968904","issue":"5","journalAbbreviation":"Energy Conversion and Management","language":"en","license":"https://www.elsevier.com/tdm/userlicense/1.0/","page":"1683-1690","source":"DOI.org (Crossref)","title":"Comparison of performances of air standard Atkinson and Otto cycles with heat transfer considerations","volume":"48","author":[{"family":"Hou","given":"Sh"}],"issued":{"date-parts":[["2007",5]]}}}],"schema":"https://github.com/citation-style-language/schema/raw/master/csl-citation.json"} (Hou, 2007).El ciclo Otto de aire estándar es el ciclo idealizado para motores de combustión interna de encendido por chispa. Este ciclo se muestra en los diagramas P-V y T-s. El motor de encendido por chispa se modela con el ciclo Otto ADDIN ZOTERO_ITEM CSL_CITATION {"citationID":"Abq8LphJ","properties":{"formattedCitation":"(Zohuri, 2018)","plainCitation":"(Zohuri, 2018)","noteIndex":0},"citationItems":[{"id":1389,"uris":["http://zotero.org/users/local/BP6I2uqk/items/ZI4V4M2F"],"itemData":{"id":1389,"type":"book","ISBN":"978-0-12-814519-7","publisher":"Elsevier Inc.","source":"Library Genesis","title":"Physics of Cryogenics : An Ultralow Temperature Phenomenon","title-short":"Physics of cryogenics","URL":"https://doi.org/10.1016/B978-0-12-814519-7.00013-6","author":[{"family":"Zohuri","given":"Bahman"}],"accessed":{"date-parts":[["2025",6,1]]},"issued":{"date-parts":[["2018"]]}}}],"schema":"https://github.com/citation-style-language/schema/raw/master/csl-citation.json"} (Zohuri, 2018). Otra estudio acota que el ciclo Otto es un equilibrio entre eficiencia teórica y viabilidad práctica, predominando en motores de gasolina pese a sus limitaciones termodinámicas; además, concluye que el ciclo Otto (modelo ideal de los MECH) supera al ciclo de Carnot tanto en eficiencia como en trabajo útil por ciclo bajo ADDIN ZOTERO_ITEM CSL_CITATION {"citationID":"oJP2fEx5","properties":{"formattedCitation":"(Kroetz, 2024)","plainCitation":"(Kroetz, 2024)","noteIndex":0},"citationItems":[{"id":1429,"uris":["http://zotero.org/users/local/BP6I2uqk/items/EL9Y428U"],"itemData":{"id":1429,"type":"article-journal","abstract":"The reversibility of the Carnot Cycle makes it the most efficient thermodynamic cycle to convert energy as heat into work operating between two thermal reservoirs at different temperatures. The Otto cycle represents an idealization of the processes in the spark-ignition 4-stroke internal combustion engine operation. Some aspects of these two crucial thermodynamic cycles will be presented here in a comparative manner. This highlights why the Carnot Cycle does not offer advantages over the Otto Cycle in the operation of real thermal engines when we consider the efficiency and work done per cycle dependent on the compression ratio of the cycles.","container-title":"Revista Brasileira de Ensino de Física","DOI":"https://doi.org/10.1590/1806-9126-RBEF-2023-0318","ISSN":"1806-1117, 1806-9126","journalAbbreviation":"Rev. Bras. Ensino Fís.","language":"en","note":"publisher: Sociedade Brasileira de Física","page":"e20230318","source":"SciELO","title":"Revisiting and comparing the Carnot Cycle and the Otto Cycle","volume":"46","author":[{"family":"Kroetz","given":"T"}],"issued":{"date-parts":[["2024",2,23]]}}}],"schema":"https://github.com/citation-style-language/schema/raw/master/csl-citation.json"} (Kroetz, 2024).Otro análisis adicional muestra los efectos de la transferencia de vibración de la pared del cilindro en el ciclo Otto. Además; deriva la relación entre el trabajo neto (o potencia) y la eficiencia. Otro punto importante, es que deriva el trabajo máximo y la eficiencia correspondiente, y sus análisis detallados de los efectos se muestran mediante cálculos numéricos. Sus resultados proporcionan una guía importante para la evaluación y mejora del rendimiento de los motores Otto ADDIN ZOTERO_ITEM CSL_CITATION {"citationID":"kTCwxMZv","properties":{"formattedCitation":"(Chen et\\uc0\\u160{}al., 1998)","plainCitation":"(Chen et al., 1998)","noteIndex":0},"citationItems":[{"id":1412,"uris":["http://zotero.org/users/local/BP6I2uqk/items/R4F3EUKY"],"itemData":{"id":1412,"type":"article-journal","abstract":"Finite-time thermodynamic analysis of an air-standard Otto cycle is performed in this paper. The relation between net work output and efficiency of the cycle is derived. The maximum net work output and the corresponding efficiency bound of the cycle with heat transfer considerations are also found. Detailed numerical examples are given. The result obtained herein provides a guide to the performance evaluation and improvement for practical Otto engines.","container-title":"Energy Conversion and Management","DOI":"10.1016/S0196-8904(97)10003-6","ISSN":"0196-8904","issue":"7","journalAbbreviation":"Energy Conversion and Management","page":"643-648","source":"ScienceDirect","title":"Heat transfer effects on the net work output and efficiency characteristics for an air-standard Otto cycle","volume":"39","author":[{"family":"Chen","given":"L."},{"family":"Wu","given":"Ch."},{"family":"Sun","given":"F."},{"family":"Cao","given":"Sh."}],"issued":{"date-parts":[["1998",5,1]]}}}],"schema":"https://github.com/citation-style-language/schema/raw/master/csl-citation.json"} (Chen et al., 1998).También; otro autor resalta comparaciones de las relaciones de compresión, las eficiencias y el trabajo de los ciclos Otto y Diésel ideales en condiciones que producen el máximo trabajo por ciclo. Las relaciones de compresión que maximizan el trabajo del ciclo Diésel resultan siempre superiores a las del ciclo Otto en las mismas condiciones de operación, aunque las eficiencias térmicas son prácticamente idénticas. Las relaciones de compresión que maximizan el trabajo de los ciclos Otto y Diésel se comparan favorablemente con las relaciones de compresión empleadas en los motores de producción correspondientes ADDIN ZOTERO_ITEM CSL_CITATION {"citationID":"3nsuqZJW","properties":{"formattedCitation":"(Klein, 1991)","plainCitation":"(Klein, 1991)","noteIndex":0},"citationItems":[{"id":1407,"uris":["http://zotero.org/users/local/BP6I2uqk/items/LPPGLIGW"],"itemData":{"id":1407,"type":"article-journal","abstract":"Comparisons of the compression ratios, efficiencies, and work of the ideal Otto and Diesel cycles are presented at conditions that yield maximum work per cycle. The compression ratios that maximize the work of the Diesel cycle are found always to be higher than those for the Otto cycle at the same operating conditions, although the thermal efficiencies are nearly identical. The compression ratios that maximize the work of the Otto and Diesel cycles compare well with the compression ratios employed in corresponding production engines.","container-title":"Journal of Engineering for Gas Turbines and Power","DOI":"10.1115/1.2906270","ISSN":"0742-4795, 1528-8919","issue":"4","language":"en","page":"511-513","source":"DOI.org (Crossref)","title":"An Explanation for Observed Compression Ratios in Internal Combustion Engines","volume":"113","author":[{"family":"Klein","given":"S. A."}],"issued":{"date-parts":[["1991",10,1]]}}}],"schema":"https://github.com/citation-style-language/schema/raw/master/csl-citation.json"} (Klein, 1991).En definitiva, el modelo ideal (ciclo Otto) es una herramienta muy importante para entender los principios termodinámicos debido a que revelan lo esencial, son el primer paso en un proceso secuencial que va desde la teoría hasta un motor real y pasa por modelos semi-ideales, simulaciones avanzadas y prototipos. Por ello, nuestra investigación se centra en aplicar la termodinámica teórica a motores de encendido por chispa (MECH), utilizando fichas técnicas de vehículos comerciales disponibles en el mercado. Por tanto, la hipótesis central de esta investigación infiere si es posible solo utilizar únicamente datos de fichas técnicas para estimar con precisión aceptable el comportamiento termodinámico ideal de un MECH, sin necesidad de recurrir a datos experimentales específicos del motor. Además; nuestro objetivo principal es graficar el ciclo teórico Otto y determinar los parámetros más relevantes de este tipo de motores monocilíndricos a partir de sus DataSheet.MATERIALES Y MÉTODOS Esta sección se enfocó en describir teóricamente lo que implica un ciclo Otto ideal, que parámetros son necesarios para poder simularlo de manera teórica. A continuación, se presenta un diagrama que explica y desglosa el desarrollo de esta investigación. Figura SEQ Figura \* ARABIC 1Diagrama de flujo-3810-381000Nota. El diagrama muestra la secuencia metodológica empleada para la obtención y análisis de resultados termodinámicos, desde la recopilación de datos hasta la formulación de conclusiones. Elaboración propia.Análisis aire-estándarSegún Moran y Shapiro ADDIN ZOTERO_ITEM CSL_CITATION {"citationID":"1te6VIvI","properties":{"formattedCitation":"(2018)","plainCitation":"(2018)","noteIndex":0},"citationItems":[{"id":1415,"uris":["http://zotero.org/users/local/BP6I2uqk/items/PX3UCAIZ"],"itemData":{"id":1415,"type":"book","abstract":"Este libro ha evolucionado a lo largo de muchos años de enseñanza de la asignatura tanto para no graduados como postgraduados. Explicaciones claras y completas, junto a numerosos ejemplos bien desarrollados, hacen el texto agradable y casi idóneo para el aprendizaje por parte del estudiante.","edition":"2","event-place":"Barcelona etc.","ISBN":"978-84-291-4313-3","language":"Español","number-of-pages":"688","publisher":"Reverté","publisher-place":"Barcelona etc.","source":"Amazon","title":"Fundamentos de Termodinámica Técnica","author":[{"family":"Moran","given":"M"},{"family":"Shapiro","given":"H"}],"translator":[{"family":"Turégano","given":"J"}],"issued":{"date-parts":[["2018"]]}},"suppress-author":true}],"schema":"https://github.com/citation-style-language/schema/raw/master/csl-citation.json"} (2018) muestra puntos importantes para el análisis del ciclo teórico Otto:El fluido de trabajo es una cantidad fija de aire considerado gas ideal.Los procesos de combustión son reemplazados por la absorción de calor de una fuente externa. No existen procesos de admisión y escape como en un motor real. El ciclo se completa con un proceso de cesión de calor a volumen constante mientras el pistón está en el punto muerto inferior. 493374068565415200152Todos los procesos son internamente reversibles. El calor específico se considera constante y con un valor igual a su valor a temperatura ambiente.Ciclo Termodinámico OttoMoran et al., ADDIN ZOTERO_ITEM CSL_CITATION {"citationID":"V6VojJ25","properties":{"formattedCitation":"(2015)","plainCitation":"(2015)","noteIndex":0},"citationItems":[{"id":1410,"uris":["http://zotero.org/users/local/BP6I2uqk/items/YS9NUFHV"],"itemData":{"id":1410,"type":"book","edition":"8","event-place":"Asia","ISBN":"978-1-118-96088-2","language":"English","number-of-pages":"867","publisher":"John Wiley & Sons Singapore Pte. Ltd.","publisher-place":"Asia","source":"Library Genesis","title":"Principles of Engineering Thermodynamics","title-short":"Principles of Engineering Thermodynamics","author":[{"family":"Moran","given":"M"},{"family":"Shapiro","given":"H"},{"family":"Boettner","given":"D"},{"family":"Bailey","given":"M"}],"accessed":{"date-parts":[["2025",6,6]]},"issued":{"date-parts":[["2015"]]}},"suppress-author":true}],"schema":"https://github.com/citation-style-language/schema/raw/master/csl-citation.json"} (2015) describen el ciclo Otto mediante cuatro procesos característicos:Proceso 1-2 es una compresión isoentrópica del aire, cuando el pistón se desplaza desde el punto muerto inferior (PMI) hasta el punto muerto superior (PMS). Proceso 2-3 el aire absorbe calor a volumen constante, desde una fuente externa, mientras el pistón está en el punto muerto superior (PMS). Este proceso representa la ignición de la mezcla aire-combustible y la combustión rápida. Proceso 3-4 es una expansión isoentrópica (carrera de trabajo). Proceso 4-1 a volumen constante, en el cual el aire cede calor mientras el pistón está en el punto muerto inferior.Figura SEQ Figura \* ARABIC 2Ciclo Otto Aire-Estándar. Nota: Tomado de Advanced Thermodynamics for Engineers (p. 46) por Winterbone y Turan ADDIN ZOTERO_ITEM CSL_CITATION {"citationID":"xZ7FjHlw","properties":{"formattedCitation":"(2015)","plainCitation":"(2015)","noteIndex":0},"citationItems":[{"id":1422,"uris":["http://zotero.org/users/local/BP6I2uqk/items/MJ4NEITK"],"itemData":{"id":1422,"type":"book","abstract":"Advanced Thermodynamics for Engineers, Second Edition introduces the basic concepts of thermodynamics and applies them to a wide range of technologies. Authors Desmond Winterbone and Ali Turan also include a detailed study of combustion to show how the chemical energy in a fuel is converted into thermal energy and emissions; analyze fuel cells to give an understanding of the direct conversion of chemical energy to electrical power; and provide a study of property relationships to enable more sophisticated analyses to be made of irreversible thermodynamics, allowing for new ways of efficiently covering energy to power (e.g. solar energy, fuel cells). Worked examples are included in most of the chapters, followed by exercises with solutions. By developing thermodynamics from an explicitly equilibrium perspective and showing how all systems attempt to reach equilibrium (and the effects of these systems when they cannot), Advanced Thermodynamics for Engineers, Second Edition provides unparalleled insight into converting any form of energy into power. The theories and applications of this text are invaluable to students and professional engineers of all disciplines.Includes new chapter that introduces basic terms and concepts for a firm foundation of studyFeatures clear explanations of complex topics and avoids complicated mathematical analysisUpdated chapters with recent advances in combustion, fuel cells, and more Solutions manual will be provided for end-of-chapter problems","edition":"1","event-place":"Amsterdam Paris etc","ISBN":"978-0-444-63373-6","language":"Inglés","number-of-pages":"578","publisher":"Elsevier Inc.","publisher-place":"Amsterdam Paris etc","source":"Amazon","title":"Advanced Thermodynamics for Engineers","author":[{"family":"Winterbone","given":"D"},{"family":"Turan","given":"A"}],"issued":{"date-parts":[["2015"]]}},"suppress-author":true}],"schema":"https://github.com/citation-style-language/schema/raw/master/csl-citation.json"} (2015), Ed. Elsevier Inc.Figura SEQ Figura \* ARABIC 3Diagrama de un ciclo Otto de presión-volumen y temperatura-entropía Nota: Tomado de Termodinámica (p. 334), por Manrique, J. ADDIN ZOTERO_ITEM CSL_CITATION {"citationID":"aFZbz0UP","properties":{"formattedCitation":"(2001)","plainCitation":"(2001)","noteIndex":0},"citationItems":[{"id":1386,"uris":["http://zotero.org/users/local/BP6I2uqk/items/4LGZUFPP"],"itemData":{"id":1386,"type":"book","abstract":"De manera clara y pormenorizada se presenta esta obra. En ella se exponen todos los temas que comprende la termodinámica, desde las unidades básicas relacionadas con los fenómenos de transformación de la energía hasta los distintos ciclos termodinámicos y su aplicación en la industria. La termodinámica es una materia fundamental en la preparación del ingeniero, la termodinámica trata acerca de los cambios de estado de la materia y sus limitaciones, así como de las diferentes propiedades de las sustancias. Para entenderla es necesario tener una comprensión cabal de la teoría -leyes de la termodinámica-, así como resolver problemas prácticos, de aplicaciones industriales, que supongan la mejor aplicación de ésta, Por ello, en esta obra se explican con rigurosidad los fenómenos termodinámicos -el equlibrio entre fases, el trabajo, la entalpía, la transferencia de calor, entre otros-, se desglosan las fórmulas matemáticas que los denotan y se destaca la importancia que tiene cada uno de ellos en el aprovechamiento de la energía. A la vez para reafirmar los conocimientos, al final de cada capítulo se presentan numerosos ejercicios, resueltos y por resolver, con los que el estudiante de ingeniería, de licenciatura o de posgrado, puede reafirmar y aplicar conceptos aprendidos.","edition":"3","event-place":"México","ISBN":"970-613-633-9","language":"Español","note":"p.","number-of-pages":"546","publisher":"Alfaomega","publisher-place":"México","source":"Amazon","title":"Termodinámica","title-short":"Termodinamica","URL":"https://www.amazon.com/-/es/Termodin%C3%A1mica-Jos%C3%A9-Manrique/dp/9706136339","author":[{"family":"Manrique","given":"J."}],"issued":{"date-parts":[["2001"]]}},"suppress-author":true}],"schema":"https://github.com/citation-style-language/schema/raw/master/csl-citation.json"} (2001), Ed. Alfaomega.48992595576311530153Ecuaciones de Aire-Estándar[1-2] Proceso Isoentrópico T2T1=p2p1k-1k( SEQ ( \* ARABIC 1)T2T1=V1V2k-1=rk-1( SEQ ( \* ARABIC 2)p2p1=V1V2k( SEQ ( \* ARABIC 3)[2-3] Proceso Isócoro o Isovolumétricop2T2=p3T3( SEQ ( \* ARABIC 4)[3-4] Proceso Isoentrópico T4T3=p4p3k-1k( SEQ ( \* ARABIC 5)T4T3=V3V4k-1=1rk-1( SEQ ( \* ARABIC 6)p4p3=V3V4k=1rk( SEQ ( \* ARABIC 7)[4-1] Proceso Isócoro o Isovolumétricop4T4=p1T1( SEQ ( \* ARABIC 8)Donde:"k" es la relación de calores específicos, k=cpcv"cp" es el calor específico a presión constante, 1.0031kJkg.K "cv" es el calor específico a volumen constante, 0.7165kJkg.K"r" es la relación de compresión y V3 = V2 y V4 = V1, r=V1V2=V4V3 Determinación de T3486075815111661540154En un ciclo Otto ideal, no hay pérdidas irreversibles. Sin embargo, en un ciclo Otto real, la irreversibilidad de la transferencia de calor entre el fluido de trabajo y la pared del cilindro es considerable. Suponemos que la pérdida de calor a través de la pared del cilindro es proporcional a la temperatura promedio tanto del fluido de trabajo como de la pared del cilindro, y que la temperatura de la pared es constante. El calor añadido al fluido de trabajo por combustión por unidad de masa de fluido de trabajo se expresa en la siguiente expresión lineal ADDIN ZOTERO_ITEM CSL_CITATION {"citationID":"LjVluRqp","properties":{"formattedCitation":"(Chen et\\uc0\\u160{}al., 1998; Hou, 2007; Klein, 1991)","plainCitation":"(Chen et al., 1998; Hou, 2007; Klein, 1991)","noteIndex":0},"citationItems":[{"id":1412,"uris":["http://zotero.org/users/local/BP6I2uqk/items/R4F3EUKY"],"itemData":{"id":1412,"type":"article-journal","abstract":"Finite-time thermodynamic analysis of an air-standard Otto cycle is performed in this paper. The relation between net work output and efficiency of the cycle is derived. The maximum net work output and the corresponding efficiency bound of the cycle with heat transfer considerations are also found. Detailed numerical examples are given. The result obtained herein provides a guide to the performance evaluation and improvement for practical Otto engines.","container-title":"Energy Conversion and Management","DOI":"10.1016/S0196-8904(97)10003-6","ISSN":"0196-8904","issue":"7","journalAbbreviation":"Energy Conversion and Management","page":"643-648","source":"ScienceDirect","title":"Heat transfer effects on the net work output and efficiency characteristics for an air-standard Otto cycle","volume":"39","author":[{"family":"Chen","given":"L."},{"family":"Wu","given":"Ch."},{"family":"Sun","given":"F."},{"family":"Cao","given":"Sh."}],"issued":{"date-parts":[["1998",5,1]]}},"label":"page"},{"id":1392,"uris":["http://zotero.org/users/local/BP6I2uqk/items/2YYJZVNB"],"itemData":{"id":1392,"type":"article-journal","container-title":"Energy Conversion and Management","DOI":"10.1016/j.enconman.2006.11.001","ISSN":"01968904","issue":"5","journalAbbreviation":"Energy Conversion and Management","language":"en","license":"https://www.elsevier.com/tdm/userlicense/1.0/","page":"1683-1690","source":"DOI.org (Crossref)","title":"Comparison of performances of air standard Atkinson and Otto cycles with heat transfer considerations","volume":"48","author":[{"family":"Hou","given":"Sh"}],"issued":{"date-parts":[["2007",5]]}},"label":"page"},{"id":1407,"uris":["http://zotero.org/users/local/BP6I2uqk/items/LPPGLIGW"],"itemData":{"id":1407,"type":"article-journal","abstract":"Comparisons of the compression ratios, efficiencies, and work of the ideal Otto and Diesel cycles are presented at conditions that yield maximum work per cycle. The compression ratios that maximize the work of the Diesel cycle are found always to be higher than those for the Otto cycle at the same operating conditions, although the thermal efficiencies are nearly identical. The compression ratios that maximize the work of the Otto and Diesel cycles compare well with the compression ratios employed in corresponding production engines.","container-title":"Journal of Engineering for Gas Turbines and Power","DOI":"10.1115/1.2906270","ISSN":"0742-4795, 1528-8919","issue":"4","language":"en","page":"511-513","source":"DOI.org (Crossref)","title":"An Explanation for Observed Compression Ratios in Internal Combustion Engines","volume":"113","author":[{"family":"Klein","given":"S. A."}],"issued":{"date-parts":[["1991",10,1]]}},"label":"page"}],"schema":"https://github.com/citation-style-language/schema/raw/master/csl-citation.json"} (Chen et al., 1998; Hou, 2007; Klein, 1991). Donde “α” y “β” son dos constantes relacionadas con la transferencia de calor y la combustión.T3=α+cv-βT2(cv+β)( SEQ ( \* ARABIC 9)La relación entre el trabajo neto (o potencia) y la eficiencia es una función de "∝", " β " y “T1”. Los rangos típicos de los tres parámetros son "∝" = 2500-4500 kJ/kg, "β" = 0.3-1.8 kJ/(kg.K) y T1 = 300-370 K. El rango de temperatura correspondiente a T3 es de 1500-3000 K.Expresiones para energías transferidasCon el objeto de realizar un análisis termodinámico sencillo, el ciclo Otto estándar de aire implica varias simplificaciones y suposiciones; el medio de trabajo no cambia de composición química y permanece dentro del sistema, la adición de calor a volumen constante se realiza de forma equivalente a la combustión de la mezcla aire-combustible, los procesos de compresión y expansión son isoentrópicos y los calores específicos ideales son constantes ADDIN ZOTERO_ITEM CSL_CITATION {"citationID":"GXNld4gZ","properties":{"formattedCitation":"(Manrique, 2001)","plainCitation":"(Manrique, 2001)","noteIndex":0},"citationItems":[{"id":1386,"uris":["http://zotero.org/users/local/BP6I2uqk/items/4LGZUFPP"],"itemData":{"id":1386,"type":"book","abstract":"De manera clara y pormenorizada se presenta esta obra. En ella se exponen todos los temas que comprende la termodinámica, desde las unidades básicas relacionadas con los fenómenos de transformación de la energía hasta los distintos ciclos termodinámicos y su aplicación en la industria. La termodinámica es una materia fundamental en la preparación del ingeniero, la termodinámica trata acerca de los cambios de estado de la materia y sus limitaciones, así como de las diferentes propiedades de las sustancias. Para entenderla es necesario tener una comprensión cabal de la teoría -leyes de la termodinámica-, así como resolver problemas prácticos, de aplicaciones industriales, que supongan la mejor aplicación de ésta, Por ello, en esta obra se explican con rigurosidad los fenómenos termodinámicos -el equlibrio entre fases, el trabajo, la entalpía, la transferencia de calor, entre otros-, se desglosan las fórmulas matemáticas que los denotan y se destaca la importancia que tiene cada uno de ellos en el aprovechamiento de la energía. A la vez para reafirmar los conocimientos, al final de cada capítulo se presentan numerosos ejercicios, resueltos y por resolver, con los que el estudiante de ingeniería, de licenciatura o de posgrado, puede reafirmar y aplicar conceptos aprendidos.","edition":"3","event-place":"México","ISBN":"970-613-633-9","language":"Español","note":"p.","number-of-pages":"546","publisher":"Alfaomega","publisher-place":"México","source":"Amazon","title":"Termodinámica","title-short":"Termodinamica","URL":"https://www.amazon.com/-/es/Termodin%C3%A1mica-Jos%C3%A9-Manrique/dp/9706136339","author":[{"family":"Manrique","given":"J."}],"issued":{"date-parts":[["2001"]]}}}],"schema":"https://github.com/citation-style-language/schema/raw/master/csl-citation.json"} (Manrique, 2001).El ciclo Otto de Aire-Estándar consta de dos procesos en los que hay trabajo pero no transferencia de calor (Procesos 1-2 y 3-4) y dos procesos en los que hay calor transferido pero no trabajo (Procesos 2-3 y 4-1) ADDIN ZOTERO_ITEM CSL_CITATION {"citationID":"bzEcayo3","properties":{"formattedCitation":"(Manrique, 2001; Moran et\\uc0\\u160{}al., 2015; Moran & Shapiro, 2018)","plainCitation":"(Manrique, 2001; Moran et al., 2015; Moran & Shapiro, 2018)","noteIndex":0},"citationItems":[{"id":1386,"uris":["http://zotero.org/users/local/BP6I2uqk/items/4LGZUFPP"],"itemData":{"id":1386,"type":"book","abstract":"De manera clara y pormenorizada se presenta esta obra. En ella se exponen todos los temas que comprende la termodinámica, desde las unidades básicas relacionadas con los fenómenos de transformación de la energía hasta los distintos ciclos termodinámicos y su aplicación en la industria. La termodinámica es una materia fundamental en la preparación del ingeniero, la termodinámica trata acerca de los cambios de estado de la materia y sus limitaciones, así como de las diferentes propiedades de las sustancias. Para entenderla es necesario tener una comprensión cabal de la teoría -leyes de la termodinámica-, así como resolver problemas prácticos, de aplicaciones industriales, que supongan la mejor aplicación de ésta, Por ello, en esta obra se explican con rigurosidad los fenómenos termodinámicos -el equlibrio entre fases, el trabajo, la entalpía, la transferencia de calor, entre otros-, se desglosan las fórmulas matemáticas que los denotan y se destaca la importancia que tiene cada uno de ellos en el aprovechamiento de la energía. A la vez para reafirmar los conocimientos, al final de cada capítulo se presentan numerosos ejercicios, resueltos y por resolver, con los que el estudiante de ingeniería, de licenciatura o de posgrado, puede reafirmar y aplicar conceptos aprendidos.","edition":"3","event-place":"México","ISBN":"970-613-633-9","language":"Español","note":"p.","number-of-pages":"546","publisher":"Alfaomega","publisher-place":"México","source":"Amazon","title":"Termodinámica","title-short":"Termodinamica","URL":"https://www.amazon.com/-/es/Termodin%C3%A1mica-Jos%C3%A9-Manrique/dp/9706136339","author":[{"family":"Manrique","given":"J."}],"issued":{"date-parts":[["2001"]]}},"label":"page"},{"id":1410,"uris":["http://zotero.org/users/local/BP6I2uqk/items/YS9NUFHV"],"itemData":{"id":1410,"type":"book","edition":"8","event-place":"Asia","ISBN":"978-1-118-96088-2","language":"English","number-of-pages":"867","publisher":"John Wiley & Sons Singapore Pte. Ltd.","publisher-place":"Asia","source":"Library Genesis","title":"Principles of Engineering Thermodynamics","title-short":"Principles of Engineering Thermodynamics","author":[{"family":"Moran","given":"M"},{"family":"Shapiro","given":"H"},{"family":"Boettner","given":"D"},{"family":"Bailey","given":"M"}],"accessed":{"date-parts":[["2025",6,6]]},"issued":{"date-parts":[["2015"]]}},"label":"page"},{"id":1415,"uris":["http://zotero.org/users/local/BP6I2uqk/items/PX3UCAIZ"],"itemData":{"id":1415,"type":"book","abstract":"Este libro ha evolucionado a lo largo de muchos años de enseñanza de la asignatura tanto para no graduados como postgraduados. Explicaciones claras y completas, junto a numerosos ejemplos bien desarrollados, hacen el texto agradable y casi idóneo para el aprendizaje por parte del estudiante.","edition":"2","event-place":"Barcelona etc.","ISBN":"978-84-291-4313-3","language":"Español","number-of-pages":"688","publisher":"Reverté","publisher-place":"Barcelona etc.","source":"Amazon","title":"Fundamentos de Termodinámica Técnica","author":[{"family":"Moran","given":"M"},{"family":"Shapiro","given":"H"}],"translator":[{"family":"Turégano","given":"J"}],"issued":{"date-parts":[["2018"]]}},"label":"page"}],"schema":"https://github.com/citation-style-language/schema/raw/master/csl-citation.json"} (Manrique, 2001; Moran et al., 2015; Moran & Shapiro, 2018).Las siguientes ecuaciones muestran el trabajo y la transferencia de calor:W12m=u2-u1( SEQ ( \* ARABIC 10)W34m=u3-u4( SEQ ( \* ARABIC 11)Q23m=u3-u2=cvT3-T2( SEQ ( \* ARABIC 12)Q41m=u4-u1=cvT4-T1;<0( SEQ ( \* ARABIC 13)Donde:"u" Energía interna (kJ/kg) Este dato se extrae de la “Tabla A-22” ADDIN ZOTERO_ITEM CSL_CITATION {"citationID":"LsV7Irov","properties":{"formattedCitation":"(Moran & Shapiro, 2018)","plainCitation":"(Moran & Shapiro, 2018)","noteIndex":0},"citationItems":[{"id":1415,"uris":["http://zotero.org/users/local/BP6I2uqk/items/PX3UCAIZ"],"itemData":{"id":1415,"type":"book","abstract":"Este libro ha evolucionado a lo largo de muchos años de enseñanza de la asignatura tanto para no graduados como postgraduados. Explicaciones claras y completas, junto a numerosos ejemplos bien desarrollados, hacen el texto agradable y casi idóneo para el aprendizaje por parte del estudiante.","edition":"2","event-place":"Barcelona etc.","ISBN":"978-84-291-4313-3","language":"Español","number-of-pages":"688","publisher":"Reverté","publisher-place":"Barcelona etc.","source":"Amazon","title":"Fundamentos de Termodinámica Técnica","author":[{"family":"Moran","given":"M"},{"family":"Shapiro","given":"H"}],"translator":[{"family":"Turégano","given":"J"}],"issued":{"date-parts":[["2018"]]}}}],"schema":"https://github.com/citation-style-language/schema/raw/master/csl-citation.json"} (Moran & Shapiro, 2018)."cv" es el calor específico a volumen constante, 0.7165kJkg.K"T" temperatura, K.48415076635081550155Eficiencia del ciclo OttoPara el ciclo Otto el rendimiento térmico crece cuando la relación de compresión aumenta; además, el aumento del rendimiento térmico cuando crece la relación de compresión se manifiesta en las expresiones desarrolladas para un sistema de aire-estándar ADDIN ZOTERO_ITEM CSL_CITATION {"citationID":"Qwi5xKge","properties":{"formattedCitation":"(Moran et\\uc0\\u160{}al., 2015)","plainCitation":"(Moran et al., 2015)","noteIndex":0},"citationItems":[{"id":1410,"uris":["http://zotero.org/users/local/BP6I2uqk/items/YS9NUFHV"],"itemData":{"id":1410,"type":"book","edition":"8","event-place":"Asia","ISBN":"978-1-118-96088-2","language":"English","number-of-pages":"867","publisher":"John Wiley & Sons Singapore Pte. Ltd.","publisher-place":"Asia","source":"Library Genesis","title":"Principles of Engineering Thermodynamics","title-short":"Principles of Engineering Thermodynamics","author":[{"family":"Moran","given":"M"},{"family":"Shapiro","given":"H"},{"family":"Boettner","given":"D"},{"family":"Bailey","given":"M"}],"accessed":{"date-parts":[["2025",6,6]]},"issued":{"date-parts":[["2015"]]}}}],"schema":"https://github.com/citation-style-language/schema/raw/master/csl-citation.json"} (Moran et al., 2015).η=1-T1T2( SEQ ( \* ARABIC 14)η=1-1r(k-1)( SEQ ( \* ARABIC 15)Selección y datos extraídos fichas técnicas de motores MonocilíndricosPara la selección de los motores se ha tomado en cuenta la popularidad de estos vehículos en la zona nororiente del Perú, específicamente en la provincia de Jaén, donde predominan vehículos hindúes y japoneses, debido a que son motores robustos y fuertes, ideales para soportar las características geográficas agrestes donde se desempeñan estos vehículos. También, se recopila la información técnica de motores monocilíndricos, incluyendo parámetros como tipo de motor, cilindrada, peso, relación de compresión. Los datos provienen de fichas técnicas oficiales de fabricantes, garantizando precisión y confiabilidad para su uso en comparativas, estudios de eficiencia o aplicaciones en ingeniería.Tabla SEQ Tabla \* ARABIC 1Motor Apache RTR 180Datos de Ficha Técnica Apache - RTR - 180 - Race EditionTipo 4 TiemposCilindrada (VD)177.4cm3Peso 139.0KgRelación de compresión "r" 9.5 Fuente: Extraído de la Ficha Técnica Apache RTR 180, Bajaj ADDIN ZOTERO_ITEM CSL_CITATION {"citationID":"yyayPfFN","properties":{"formattedCitation":"(2023)","plainCitation":"(2023)","noteIndex":0},"citationItems":[{"id":1436,"uris":["http://zotero.org/users/local/BP6I2uqk/items/NDVKS2RY"],"itemData":{"id":1436,"type":"document","title":"APACHE-RTR-180-Race Edition","URL":"https://tvsperu.com/wp-content/uploads/2023/02/APACHE-RTR-180-RE.pdf","author":[{"family":"Bajaj","given":""}],"accessed":{"date-parts":[["2025",6,18]]},"issued":{"date-parts":[["2023"]]}},"suppress-author":true}],"schema":"https://github.com/citation-style-language/schema/raw/master/csl-citation.json"} (2023).Tabla SEQ Tabla \* ARABIC 2Motor CG 150 Titán – Honda.Datos de Ficha Técnica CG 150 Titán – HondaTipo 4 TiemposCilindrada (VD)149.2cm3Peso seco del motor27.7Kg Relación de comprensión “r”9.5 Fuente: Extraído del Manual de Taller CG 150 Titán, Honda ADDIN ZOTERO_ITEM CSL_CITATION {"citationID":"L3eEzF0i","properties":{"formattedCitation":"(2004)","plainCitation":"(2004)","noteIndex":0},"citationItems":[{"id":1433,"uris":["http://zotero.org/users/local/BP6I2uqk/items/DYXZD55A"],"itemData":{"id":1433,"type":"document","language":"Español","publisher":"Departamento de Servicios de Posventa","title":"MANUAL DE TALLER CG150 TITAN KS/ES/ESD","author":[{"family":"Honda","given":""}],"issued":{"date-parts":[["2004"]]}},"suppress-author":true}],"schema":"https://github.com/citation-style-language/schema/raw/master/csl-citation.json"} (2004).47942505871411560156Tabla SEQ Tabla \* ARABIC 3 Motor CGL 125 - Honda.Datos de Ficha Técnica CGL 125 – HondaTipo 4 TiemposCilindrada (VD)124.1cm3Peso seco del motor29.8KgRelación de compresión "r"9.0 Fuente: Extraído del Manual de Taller CGL 125, Honda ADDIN ZOTERO_ITEM CSL_CITATION {"citationID":"NfwmRyZf","properties":{"formattedCitation":"(2001)","plainCitation":"(2001)","noteIndex":0},"citationItems":[{"id":1431,"uris":["http://zotero.org/users/local/BP6I2uqk/items/HV4DQZ5F"],"itemData":{"id":1431,"type":"document","abstract":"Este manual de servicio describe los procedimientos de servicio para la CGL125 1WH/2WH/3WH.","language":"Español","publisher":"Departamento de Publicaciones de Servicio","source":"HSA - Honda South America.","title":"MANUAL TALLER CGL125 1/2/3WH","author":[{"family":"Honda","given":""}],"issued":{"date-parts":[["2001"]]}},"suppress-author":true}],"schema":"https://github.com/citation-style-language/schema/raw/master/csl-citation.json"} (2001).Tabla SEQ Tabla \* ARABIC 4Motor XTZ Yamaha 125Datos de Ficha Técnica XTZ - Yamaha 125Tipo 4 TiemposCilindrada (VD)124.0cm3Peso 118.0KgRelación de compresión "r"10.0 Fuente: Extraído de la Ficha Técnica XTZ 125, Yamaha ADDIN ZOTERO_ITEM CSL_CITATION {"citationID":"jeSvd7wM","properties":{"formattedCitation":"(2025)","plainCitation":"(2025)","noteIndex":0},"citationItems":[{"id":1439,"uris":["http://zotero.org/users/local/BP6I2uqk/items/T4D4STAV"],"itemData":{"id":1439,"type":"document","title":"XTZ125 Yamaha | Moto todo terreno | Yamaha Motor","URL":"https://www.yamaha-motor.com.pe/xtz125/product/600004","author":[{"family":"Yamaha","given":""}],"accessed":{"date-parts":[["2025",6,18]]},"issued":{"date-parts":[["2025"]]}},"suppress-author":true}],"schema":"https://github.com/citation-style-language/schema/raw/master/csl-citation.json"} (2025).RESULTADOSAnálisis gráficoLos resultados muestran que los cuatro motores tienen eficiencias térmicas similares (entre 58.5% y 60.2%), lo que significa que convierten aproximadamente el 60% de la energía del combustible en movimiento útil, mientras que el 40% restante se pierde como calor. El motor más eficiente es el XTZ-125 (60.2%) gracias a su mayor relación de compresión (10), que comprime más la mezcla de aire y combustible, generando mayor presión y aprovechando mejor la energía. En cambio, el CGL 125 (58.5%) tiene la menor eficiencia al comprimir menos la mezcla (relación 9), lo que reduce su rendimiento.Las curvas de los diagramas P-V reflejan este comportamiento: a mayor compresión, más altas son las líneas de presión (como la XTZ 125), lo que indica un mejor aprovechamiento de la energía. Aunque las diferencias son mínimas (1-2%), esto da como resultado un menor consumo de combustible y más potencia. En resumen, la eficiencia depende de qué tan bien el motor comprime la mezcla antes de quemarla, y estos resultados ayudan a entender por qué algunos motores son más eficientes que otros.4908116682993157015793345034544000Figura SEQ Figura \* ARABIC 4Análisis Gráfico de motores Monocilíndricos. Nota: Este gráfico evidencia de manera didáctica los diagramas P-V; además, fue realizado con GNU Octave, versión 9.3.0.Análisis NuméricoPara el presente análisis, se emplean las principales constantes termodinámicas que se muestran en la siguiente tabla:Tabla SEQ Tabla \* ARABIC 5Constantes asumidas para el análisis termodinámico.ConstantesValoresIntervalosUnidadesk1.4--∝3500[2500-4500]kJ/kgcv0.7165-kJ/(kg.K)β1.05[0.3-1.8]kJ/(kg.K)P11.00-BarT1300-KNota: Esta tabla muestra “∝” y “β” son promedios de los intervalos según Chen et al. ADDIN ZOTERO_ITEM CSL_CITATION {"citationID":"ABEqXsPW","properties":{"formattedCitation":"(1998)","plainCitation":"(1998)","noteIndex":0},"citationItems":[{"id":1412,"uris":["http://zotero.org/users/local/BP6I2uqk/items/R4F3EUKY"],"itemData":{"id":1412,"type":"article-journal","abstract":"Finite-time thermodynamic analysis of an air-standard Otto cycle is performed in this paper. The relation between net work output and efficiency of the cycle is derived. The maximum net work output and the corresponding efficiency bound of the cycle with heat transfer considerations are also found. Detailed numerical examples are given. The result obtained herein provides a guide to the performance evaluation and improvement for practical Otto engines.","container-title":"Energy Conversion and Management","DOI":"10.1016/S0196-8904(97)10003-6","ISSN":"0196-8904","issue":"7","journalAbbreviation":"Energy Conversion and Management","page":"643-648","source":"ScienceDirect","title":"Heat transfer effects on the net work output and efficiency characteristics for an air-standard Otto cycle","volume":"39","author":[{"family":"Chen","given":"L."},{"family":"Wu","given":"Ch."},{"family":"Sun","given":"F."},{"family":"Cao","given":"Sh."}],"issued":{"date-parts":[["1998",5,1]]}},"suppress-author":true}],"schema":"https://github.com/citation-style-language/schema/raw/master/csl-citation.json"} (1998)Procedimiento de cálculo482295914817561580158Se va a tomar en cuenta las características técnicas del motor Apache 180 y seguidamente se muestran Tablas 6 y 7 hechas en el programa Microsoft Office Excel Profesional Plus 2016, donde utilizando las fórmulas matemáticas presentadas en el apartado anterior, se realiza el cálculo correspondiente.Teniendo en cuenta lo siguiente:r=VmaxVmin=VD+VcVc( SEQ ( \* ARABIC 16)Sí. V1=VmaxV2=Vmin=VcVD=CilindradaCálculo del volumen inicial “V1”, teniendo en cuenta el siguiente gráfico.238421547180500Figura SEQ Figura \* ARABIC 5Esquema de un motor alternativo.Nota: Tomado de Motores de combustióninterna alternativos (p. 47) por Payri y Desantes ADDIN ZOTERO_ITEM CSL_CITATION {"citationID":"Qv07PUx7","properties":{"formattedCitation":"(2011)","plainCitation":"(2011)","noteIndex":0},"citationItems":[{"id":1129,"uris":["http://zotero.org/users/local/BP6I2uqk/items/AK9DW97F"],"itemData":{"id":1129,"type":"book","event-place":"Barcelona","ISBN":"978-84-291-4802-2","publisher":"Reverte","publisher-place":"Barcelona","title":"Motores de combustión interna alternativos","author":[{"family":"Payri","given":"F"},{"family":"Desantes","given":"J. M."}],"issued":{"date-parts":[["2011"]]}},"suppress-author":true}],"schema":"https://github.com/citation-style-language/schema/raw/master/csl-citation.json"} (2011), Ed. Reverte.490801521619741590159Vmax=VD+Vc( SEQ ( \* ARABIC 17)V1=VD+V2( SEQ ( \* ARABIC 18)VD=V1-V1r( SEQ ( \* ARABIC 19)VD=V11-1r( SEQ ( \* ARABIC 20)V1=VD1-1r=VD*rr-1( SEQ ( \* ARABIC 21)V1=VD*rr-1=177.4*9.59.5-1=198.271 cm3Punto “2”r=V1V2 →V2=V1r → V2=198.2719.5=20.871 cm3p2p1=V1V2k→p2=p1V1V2k→p2=p1rk→p2=1*9.51.4=23.378 barT2T1=V1V2k-1→T2=T1V1V2k-1→T2=T1rk-1→ T2=3009.51.4 -1=738.262 KPunto “3”T3=α+cv-βT2(cv+β)=3500+0.7165-1.05*738.262(0.7165+1.05)=1841.941 Kp2T2=p3T3→ p3=T3p2T2→p3=1841.94123.378738.262=58.328 barV3=V2=20.871 cm3Punto “4”p4p3=V3V4k→ p4=p3rk→ p4=58.328(9.5)1.4=2.495 barT4T3=V3V4k-1→T4=T3rk-1→T4=1841.941(9.5)1.4-1=748.491 KV4=V1=198.27148992598470231600160Seguidamente evaluamos las energías transferidas, según tablas de Energía interna "u" (kJ/kg) Este dato se extrae de la “Tabla A-22” de Moran y Shapiro ADDIN ZOTERO_ITEM CSL_CITATION {"citationID":"4pyqq3iZ","properties":{"formattedCitation":"(2018)","plainCitation":"(2018)","noteIndex":0},"citationItems":[{"id":1415,"uris":["http://zotero.org/users/local/BP6I2uqk/items/PX3UCAIZ"],"itemData":{"id":1415,"type":"book","abstract":"Este libro ha evolucionado a lo largo de muchos años de enseñanza de la asignatura tanto para no graduados como postgraduados. Explicaciones claras y completas, junto a numerosos ejemplos bien desarrollados, hacen el texto agradable y casi idóneo para el aprendizaje por parte del estudiante.","edition":"2","event-place":"Barcelona etc.","ISBN":"978-84-291-4313-3","language":"Español","number-of-pages":"688","publisher":"Reverté","publisher-place":"Barcelona etc.","source":"Amazon","title":"Fundamentos de Termodinámica Técnica","author":[{"family":"Moran","given":"M"},{"family":"Shapiro","given":"H"}],"translator":[{"family":"Turégano","given":"J"}],"issued":{"date-parts":[["2018"]]}},"suppress-author":true}],"schema":"https://github.com/citation-style-language/schema/raw/master/csl-citation.json"} (2018).W12m=u2-u1= 542.637-214.070=328.567 kJkgW34m=u3-u4=1527.211-550.787=976.424 kJkgQ23m=u3-u2=1527.211-542.637=984.574 kJkgQ41m=u4-u1=550.787-214.070=336.717 kJkgFinalmente, la eficiencia térmica “η” se calcula con la siguiente formulas:η=1-1rk-1=1-19.51.4-1=59.4 %η=1-T1T2=1-300738.262=59.4 %La eficiencia térmica “η”Los motores Apache 180 y CG 150 Titán comparten la misma eficiencia (59.4%), debido a su idéntica relación de compresión (9.5). El motor CGL 125 tiene la menor eficiencia (58.5%), coherente con su menor relación de compresión (9:1), también; el motor XTZ 125 destaca con la mayor eficiencia (60.2%), gracias a su mayor compresión (10).Presiones y TemperaturasPicos de presión:El motor XTZ 125 alcanza la presión máxima más alta (61.3 bar en P3), seguido por el Apache/CG 150 (58.3 bar). Esto explica su mejor rendimiento: a mayor compresión, mayor presión de combustión y aprovechamiento de energía.Temperaturas:Todos los motores superan los 1800 K durante la combustión (T3), pero el motor XTZ 125 mantiene mejor relación presión-temperatura.48607585678901610161Volúmenes y ExpansiónLos motores con mayor cilindrada (Apache: 177.4 cm³, CG 150: 149.2 cm³) tienen volúmenes iniciales (V1) mayores, pero esto no afecta directamente a la eficiencia. La clave está en la relación de compresión: el motor XTZ 125 reduce más su volumen durante la compresión (V2 = 13.78 cm³ vs. ~17 cm³ en otros), generando mayor presión.Tabla SEQ Tabla \* ARABIC 6Puntos principales del ciclo Otto.Resultados Motor Apache 180 Volumen (cm3) Temperatura (K) Presión (bar)η=59.4%V1198.271T1300P11V220.871T2738.26P223.378V320.871T31841.94P358.328V4198.271T4748.49P42.495  Resultados Motor CG 150 Titan Volumen (cm3) Temperatura (K) Presión (bar)η=59.4%V1166.753T1300P11V217.553T2738.26P223.378V317.553T31841.94P358.328V4166.753T4748.49P42.495  Resultados Motor CGL 125 Volumen (cm3) Temperatura (K) Presión (bar)η=58.5%V1139.613T1300P11V215.513T2722.47P221.674V315.513T31844.92P355.348V4139.613T4766.09P42.554  Resultados Motor XTZ 125 Volumen (cm3) Temperatura (K) Presión (bar)η=60.2%V1137.778T1300P11  V213.778T2753.57P225.119V313.778T31839.05P361.302V4137.778T4732.14P42.440  49570106731331620162Nota: Los puntos son resultado de fórmulas termodinámicas presentadas.Energías TransferidasEl siguiente cuadro presenta las energías transferidas (trabajo y calor) por unidad de masa (kJ/kg) para cuatro motores de 4 tiempos (4T) diferentes: Apache 180 - RTR, CG 150 Titán - Honda, CGL 125 - Honda y XTZ 125 - Yamaha. Estos valores corresponden a las etapas del ciclo termodinámico que sigue el motor bajo el ciclo Otto.4866707719602116300163Tabla SEQ Tabla \* ARABIC 7Energías transferidas para los motores estudiados.Energía transferidas Apache 180 – RTR ΔTΔuResultadoUnidadesTrabajo W12/m738.262300542.637214.070328.567kJ/kgW34/m1841.941748.491527.211550.787976.424kJ/kgTransferencia de calor Q23/m1841.941738.2621527.211542.637984.574kJ/kgQ41/m748.491300550.787214.070336.717kJ/kgEnergía transferidas CG 150 Titán – Honda ΔTΔuResultadoUnidadesTrabajo W12/m738.262300542.637214.070328.567kJ/kgW34/m1841.941748.4911527.211550.787976.424kJ/kgTransferencia de calor Q23/m1841.941738.2621527.211542.637984.574kJ/kgQ41/m748.491300550.787214.070336.717kJ/kgEnergías transferidas CGL 125 – Honda ΔTΔuResultadoUnidadesTrabajo W12/m722.467300530.099214.070316.029kJ/kgW34/m1844.923766.0931530.054564.919965.135kJ/kgTransferencia de calor Q23/m1844.923722.4671530.054530.099999.955kJ/kgQ41/m766.093300564.9190214.0700350.8490kJ/kgEnergías transferidas XTZ 125 – Yamaha ΔTΔuResultadoUnidadesTrabajo W12/m753.566300554.853214.070340.783kJ/kgW34/m1839.052732.1401524.454537.771986.683kJ/kgTransferencia de calor Q23/m1839.052753.5661524.454554.853969.601kJ/kgQ41/m732.140300537.771214.070323.701kJ/kgNota: Los puntos son resultado de fórmulas de energías transferidas.La tabla muestra resultados teóricamente analizados, donde las diferencias entre Δu muestran el desempeño termodinámico de cada motor. También, se muestra que el motor Apache 180 (mayor cilindrada) tiene una transferencia de energía (Q23/m = 984.574 kJ/kg) y destaca la XTZ 125 su eficiencia con un menor calor rechazado (Q41/m = 323.701 kJ/kg). Cabe resaltar, que inyectar mayor calor, no significa que tenga un mejor rendimiento. El Apache 180 debería ser más potente, pero los datos no reflejan ventajas frente a los 125cc. Podría deberse a ajustes en parámetros como relación de compresión o sistemas de enfriamiento. En cambio; el motor CGL 125 y la CG 150 logra mayor Q23/m, pero su alto Q41/m sugiere ineficiencias en la conversión de calor a trabajo.DISCUSIÓNEn esta investigación evidencia que la relación de compresión es un parámetro importante en los motores de combustión interna, en este caso la Yamaha XTZ 125, tuvo una mayor eficiencia, a pesar de que es un motor de baja cilindrada, además, su calor rechazado es mínimo, en comparación con la Apache 180, que, a pesar de contar con una cilindrada superior, su rendimiento es menor y su calor rechazado es mayor. Si una máquina cuenta con un mayor calor rechazo evidencia que ha tenido ineficiencias al momento de convertir el calor cedido en trabajo. En tal sentido Chicurel ADDIN ZOTERO_ITEM CSL_CITATION {"citationID":"HnInnAjn","properties":{"formattedCitation":"(1991)","plainCitation":"(1991)","noteIndex":0},"citationItems":[{"id":1442,"uris":["http://zotero.org/users/local/BP6I2uqk/items/Q4KNDKXY"],"itemData":{"id":1442,"type":"article-journal","abstract":"A novel Otto cycle engine concept, in which intake and compression are carried out in a compressor unit separate from the expansion unit, is presented. The compressor is driven via a continuously-variable transmission whose speed ratio determines the power output. Pumping as well as rubbing friction losses are reduced. Also compression work is reduced by increasing the heat rejection during this phase of the cycle. A regenerator is used to transfer heat from the exhaust gases to the compressed combustible mixture. Dilution of the combustible mixture is minimal, so permitting a lowering of the fuel-air ratios at idling and low load conditions. The proposed system includes the capability of supercharged operation.","container-title":"Applied Energy","DOI":"10.1016/0306-2619(91)90069-A","ISSN":"0306-2619","issue":"2","journalAbbreviation":"Applied Energy","page":"105-116","source":"ScienceDirect","title":"A modified Otto cycle engine for fuel economy","volume":"38","author":[{"family":"Chicurel","given":"R."}],"issued":{"date-parts":[["1991",1,1]]}},"suppress-author":true}],"schema":"https://github.com/citation-style-language/schema/raw/master/csl-citation.json"} (1991) menciona que la compresión es una etapa muy importante, que está ligado a la relación de compresión, en esa investigación la compresión se realiza en una unidad compresora separada de la unidad de expansión, ofreciendo una reducción significativa en el consumo de combustible. En comparación, con nuestros resultados se evidencia que, a mayor relación de compresión, mejora la eficiencia del motor.489925910196421640164Otro aspecto resaltante, es que esta investigación se enfocó en analizar de manera teórica el comportamiento de estos motores a través de sus fichas técnicas, con fines didácticos. Además, se emplearon las fórmulas para un ciclo Otto de aire estándar. Según Ge et al. ADDIN ZOTERO_ITEM CSL_CITATION {"citationID":"tXnw0f30","properties":{"formattedCitation":"(2005)","plainCitation":"(2005)","noteIndex":0},"citationItems":[{"id":1445,"uris":["http://zotero.org/users/local/BP6I2uqk/items/U5GLILAS"],"itemData":{"id":1445,"type":"article-journal","abstract":"The performance of an air-standard Otto cycle with heat transfer loss and variable specific heats of working fluid is analyzed by using finite-time thermodynamics. The relations between the power output and the compression ratio, between the thermal efficiency and the compression ratio, as well as the optimal relation between power output and the efficiency of the cycle are derived by detailed numerical examples. Moreover, the effects of heat transfer loss and variable specific heats of working fluid on the cycle performance are analyzed. The results show that the effects of heat transfer loss and variable specific heats of working fluid on the cycle performance are obvious, and they should be considered in practice cycle analysis. The results obtained in this paper may provide guidance for the design of practice internal combustion engines.","container-title":"International Journal of Thermal Sciences","DOI":"10.1016/j.ijthermalsci.2004.10.001","ISSN":"1290-0729","issue":"5","journalAbbreviation":"International Journal of Thermal Sciences","page":"506-511","source":"ScienceDirect","title":"Thermodynamic simulation of performance of an Otto cycle with heat transfer and variable specific heats of working fluid","volume":"44","author":[{"family":"Ge","given":"Y"},{"family":"Chen","given":"L"},{"family":"Sun","given":"F"},{"family":"Wu","given":"Ch"}],"issued":{"date-parts":[["2005",5,1]]}},"suppress-author":true}],"schema":"https://github.com/citation-style-language/schema/raw/master/csl-citation.json"} (2005), los resultados teóricos obtenidos pueden servir de guía para el diseño de motores de combustión interna de forma práctica.CONCLUSIONESSe concluyó que los ciclos termodinámicos Otto de aire estándar, se pueden graficar a través de las fichas técnicas de fabricante y asumiendo algunas constantes debidamente fundamentadas.También se afirma que la relación de compresión del motor Otto, es esencial para determinar su eficiencia por eso se priorizan para su uso urbano por su agilidad y ligereza, un claro ejemplo es la XTZ 125 y la Apache 180 populares en la región nororiental del Perú.Finalmente, se aprecia que la eficiencia de un motor es buena, cuando el calor rechazado es mínimo, en este estudio la XTZ solo rechazó (323.701 kJ/kg), demostrando que aprovechó en mayor medida el calor inyectado en la cámara de combustión, transformándolo en trabajo.REFERENCIAS BIBLIOGRÁFICAS ADDIN ZOTERO_BIBL {"uncited":[],"omitted":[],"custom":[]} CSL_BIBLIOGRAPHY Bajaj. (2023). APACHE-RTR-180-Race Edition. https://tvsperu.com/wp-content/uploads/2023/02/APACHE-RTR-180-RE.pdfChen, L., Wu, Ch., Sun, F., & Cao, Sh. (1998). Heat transfer effects on the net work output and efficiency characteristics for an air-standard Otto cycle. Energy Conversion and Management, 39(7), 643-648. https://doi.org/10.1016/S0196-8904(97)10003-6Chicurel, R. (1991). A modified Otto cycle engine for fuel economy. Applied Energy, 38(2), 105-116. https://doi.org/10.1016/0306-2619(91)90069-AErazo, D., & Viteri, A. (2018). Análisis termodinámico de los parámetros indicados de un motor de ciclo Otto aspiración natural con sistema de inyección electrónica en función de la altitud sobre el nivel del mar [Escuela Politécnica Nacional]. https://bibdigital.epn.edu.ec/handle/15000/19868Ge, Y., Chen, L., Sun, F., & Wu, C. (2005). Thermodynamic simulation of performance of an Otto cycle with heat transfer and variable specific heats of working fluid. International Journal of Thermal Sciences, 44(5), 506-511. https://doi.org/10.1016/j.ijthermalsci.2004.10.001483188211351461650165Honda. (2001). MANUAL TALLER CGL125 1/2/3WH. Departamento de Publicaciones de Servicio.Honda. (2004). MANUAL DE TALLER CG150 TITAN KS/ES/ESD. Departamento de Servicios de Posventa.Hou, S. (2007). Comparison of performances of air standard Atkinson and Otto cycles with heat transfer considerations. Energy Conversion and Management, 48(5), 1683-1690. https://doi.org/10.1016/j.enconman.2006.11.001Klein, S. A. (1991). An Explanation for Observed Compression Ratios in Internal Combustion Engines. Journal of Engineering for Gas Turbines and Power, 113(4), 511-513. https://doi.org/10.1115/1.2906270Kroetz, T. (2024). Revisiting and comparing the Carnot Cycle and the Otto Cycle. Revista Brasileira de Ensino de Física, 46, e20230318. https://doi.org/10.1590/1806-9126-RBEF-2023-0318Manrique, J. (2001). Termodinámica (3.a ed.). Alfaomega. https://www.amazon.com/-/es/Termodin%C3%A1mica-Jos%C3%A9-Manrique/dp/9706136339Moran, M., & Shapiro, H. (2018). Fundamentos de Termodinámica Técnica (J. Turégano, Trad.; 2.a ed.). Reverté.Moran, M., Shapiro, H., Boettner, D., & Bailey, M. (2015). Principles of Engineering Thermodynamics (8.a ed.). John Wiley & Sons Singapore Pte. Ltd.Payri, F., & Desantes, J. M. (2011). Motores de combustión interna alternativos. Reverte.Winterbone, D., & Turan, A. (2015). Advanced Thermodynamics for Engineers (1.a ed.). Elsevier Inc.Yamaha. (2025). XTZ125 Yamaha | Moto todo terreno | Yamaha Motor. https://www.yamaha-motor.com.pe/xtz125/product/600004Zohuri, B. (2018). Physics of Cryogenics: An Ultralow Temperature Phenomenon. Elsevier Inc. https://doi.org/10.1016/B978-0-12-814519-7.00013-6487947424255671660166 Universidad Nacional de Jaén, Perú. Email: bekerpariacuri@gmail.com, olivera_aldana@unj.edu.pe Universidad Nacional de San Martín, Perú. Email: eelozada@unsm.edu.peDeterminación del ciclo teórico Otto mediante fichas técnicas de motores monocilíndricos0444500151+1Recibido:9/07/2025Aceptado:25/12/2025https://revistas.unj.edu.pe/index.php/pakamuros 150 Pariacurí et al.01206500iVBORw0KGgoAAAANSUhEUgAAAgsAAABPCAYAAABlCYadAAAAAXNSR0IArs4c6QAAAARnQU1BAACx jwv8YQUAAAAJcEhZcwAAIdUAACHVAQSctJ0AACP9SURBVHhe7Z13vJTVmcdjYtRYEltimpoYV5OY vtndfLKuSTab3U/KFjcNDaIBxUas2KJItxCqiFIURBFBEFCUjjRpAgIiIEVBvKj03jGz88zcZ+7z nvmd8vYhe/74fuadp/yeM/fOnfvM+573nI985Pd3Fzwej8fj8Xi0QKPH4/F4PB4PA40ej8fj8Xg8 DDR6PB6Px+PxMNDo8Xg8Ho/Hw0Cjx+PxeDweDwONnlT561//WgWK83g8Ho+nJoBGT6r4ZsHj8RyJ /LrL086fXzPfXBvwqTm/evDJim/yktUB3/Y9+6ry+Dnbnp+3LGBDcC7x8htvQTvB9n6T50F759Ez oF1FF7Np5+6Kfem7GwI+Qs2ZteKdiq1R9yGB2NyARk+q8JtAguI8Ho+nluBmAflUZLPQov/oQN7+ g4cCz+n4n+5+tHR84uXtSs9Pv/K+io/Yd+BAIN7WLHzrtodKccc3aVP4xQMDS8fsY01G2i/t+Wzh 2D/cWzq+ut+oir1535GFY+rttw0aW8lhxi1aWdGiRz7+/DUPlI4/eUW7wjdblsck875wbdnP9o82 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