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The Carnot Cycle and the Second Law of Thermodynamics01:20

The Carnot Cycle and the Second Law of Thermodynamics

2.9K
The Carnot engine works between two heat reservoirs of fixed temperatures. The Carnot cycle begs the following question: Is it possible to devise a heat engine that is more efficient than a Carnot engine between two fixed temperatures? The answer lies in designing a Carnot refrigerator.
Since the individual steps in a Carnot cycle can be reversed, the entire cycle is, thus, reversible. If a Carnot cycle is reversed, it becomes a Carnot refrigerator. It extracts heat Qc from a cold reservoir at...
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The Carnot Cycle01:30

The Carnot Cycle

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Converting work to heat is an irreversible process, and the purpose of a heat engine is to reverse the effect partially. Heat engines aim to increase the efficiency of the reversal, that is, maximize the work retrieved from heat. If the efficiency of a heat engine were 100%, it would imply reversing the process completely without introducing any other effect. Thus, it would violate the second law of thermodynamics.
What could be the theoretical limit to the efficiency of a heat engine? The...
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Efficiency of The Carnot Cycle01:16

Efficiency of The Carnot Cycle

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The hypothetical Carnot cycle consists of an ideal gas subjected to two isothermal and two adiabatic processes. Since the internal energy of an ideal gas depends only on its temperature, which is the same before and after the completion of the Carnot cycle, there is no change in its internal energy. Hence, using the first law of thermodynamics, the total heat exchanged by the ideal gas equals the total work done. Thus, we can quantify the efficiency of the Carnot cycle via the heat exchanged...
2.8K
Internal Combustion Engine01:20

Internal Combustion Engine

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The internal combustion engine is a heat engine that uses the byproducts of combustion as the working fluid instead of using a heat transfer medium to transfer heat. The combustion is done in a way that produces high-pressure combustion products that can be expanded through a turbine or piston to create work. Internal combustion engines can again be categorized into three kinds: (1) spark ignition gasoline engines, most commonly used in automobiles, (2) compression ignition diesel engines that...
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Otto and Diesel Cycle01:27

Otto and Diesel Cycle

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An Otto engine is a four-stroke engine that uses a mixture of gasoline and air as the working fuel. The fuel is injected into the cylinder, and the piston is moved completely down so that the cylinder is at maximum volume. By moving the piston up, adiabatic compression takes place. The spark plug ignites the gasoline-air mixture, and the burning fuel adds heat to the system at a constant volume. The heated mixture expands adiabatically and gets further cooled by exhausting heat, and this cyclic...
2.1K
Heat Engines01:10

Heat Engines

3.0K
A heat engine is a device used to extract heat from a source and then convert it into mechanical work used for various applications. For example, a steam engine on an old-style train can produce the work needed for driving the train.
Whenever we consider heat engines (and associated devices such as refrigerators and heat pumps), we do not use the standard sign convention for heat and work. For convenience, we assume that the symbols Qh, Qc, and W represent only the amounts of heat transferred...
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Video Experimental Relacionado

Updated: Sep 10, 2025

A Rapid Method for Modeling a Variable Cycle Engine
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A Rapid Method for Modeling a Variable Cycle Engine

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Juegos de azar motor Carnot

Tarek Tohme1,2, Valentina Bedoya1, Costantino di Bello3

  • 1ICTP-The Abdus Salam International Centre for Theoretical Physics, Strada Costiera 11, 34151 Trieste, Italy.

Physical review letters
|August 27, 2025
PubMed
Resumen
Este resumen es generado por máquina.

Este estudio introduce un nuevo motor de calor coloidal con un sistema de retroalimentación que convierte completamente el calor absorbido en trabajo. Este diseño innovador supera la eficiencia y la potencia del motor Carnot estándar, incluso a su potencia máxima.

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Área de la Ciencia:

  • La termodinámica
  • Mecánica estadística
  • Física coloidal

Sus antecedentes:

  • Los sistemas coloidales ofrecen una plataforma única para estudiar los principios termodinámicos a escala microscópica.
  • Los motores térmicos tradicionales se enfrentan a limitaciones en la eficiencia y la potencia, particularmente más allá del límite cuasiestático.
  • Las estrategias de control de retroalimentación pueden potencialmente mejorar el rendimiento de los motores térmicos microscópicos.

Objetivo del estudio:

  • Desarrollar un modelo teórico para un motor de calor coloidal impulsado por un protocolo de retroalimentación.
  • Demostrar la capacidad del motor para lograr la conversión completa del calor absorbido en trabajo.
  • Analizar el rendimiento del motor en términos de potencia y eficiencia en comparación con un ciclo de Carnot.

Principales métodos:

  • Modelado teórico basado en el primer paso y la teoría martingale.
  • Introducción de un protocolo de retroalimentación inspirado en las estrategias de juego, que incluye apagadas repentinas.
  • Derivación de las expresiones analíticas de potencia y eficiencia.
  • Simulaciones numéricas para validar los resultados teóricos.

Principales resultados:

  • El protocolo de retroalimentación propuesto permite la conversión total del calor neto en trabajo extraído.
  • El motor demuestra una mayor potencia y eficiencia en comparación con un ciclo de Carnot estándar.
  • El motor supera la eficiencia de Carnot a su máxima potencia.
  • Se derivaron expresiones analíticas para la potencia y la eficiencia, válidas más allá del límite cuasiestático.

Conclusiones:

  • El motor de calor coloidal controlado por retroalimentación desarrollado ofrece un rendimiento superior a los diseños convencionales.
  • El modelo teórico proporciona un marco para comprender y optimizar los motores térmicos microscópicos.
  • Los hallazgos destacan el potencial de las estrategias de retroalimentación para mejorar la eficiencia termodinámica y la potencia en los sistemas a nanoescala.