21.2
Motores de calor
Um motor de calor é um dispositivo usado para extrair calor de uma fonte e convertê-lo em trabalho mecânico, que é então utilizado para várias aplicaç…
Uma máquina térmica é uma máquina usada para extrair calor de uma fonte e depois convertê-lo parcialmente em trabalho na forma de energia mecânica.
Os componentes de um motor térmico são um reservatório quente atuando como fonte, uma substância de trabalho para transferência de calor durante a operação cíclica e um reservatório frio atuando como dissipador.
Quando a substância de trabalho extrai calor da fonte, apenas uma parte significativa do calor é utilizada para fazer algum trabalho útil, e o calor restante é transferido para a pia.
Em um motor térmico reversível ideal, a mudança na energia interna do sistema é zero.
Usando a primeira lei da termodinâmica, uma expressão para o trabalho extraído do motor térmico é obtida.
A eficiência térmica do motor térmico é dada como a razão entre esse trabalho e a quantidade de calor absorvida da fonte.
Em motores térmicos práticos, essa eficiência é sempre menor que a unidade, pois é impossível converter todo o calor em trabalho; sempre há alguma perda de calor.
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Q1: What are the main components of a heat engine?
A heat engine consists of three essential components: a hot reservoir that serves as the heat source, a working substance that transfers heat during cyclic operation, and a cold reservoir acting as the heat sink. The working substance absorbs heat from the hot reservoir, converts part of it into useful mechanical work, and rejects the remaining heat to the cold reservoir.
Q2: How is thermal efficiency calculated in a heat engine?
Thermal efficiency is defined as the ratio of useful work output to the total heat absorbed from the hot reservoir during each cycle. It represents what we get out divided by what we put in. In practical heat engines, efficiency is always less than unity because it is impossible to convert all absorbed heat into work; some heat is always lost to the cold reservoir.
Q3: Why can't a heat engine convert all heat into work?
According to the first law of thermodynamics, in an ideal reversible heat engine, the change in internal energy is zero. This means the heat absorbed must equal the work done plus the heat rejected. Therefore, some heat must always be transferred to the cold reservoir, making it thermodynamically impossible to achieve 100% efficiency or convert all heat into mechanical work.
Q4: What is the difference between ideal and practical heat engines?
An ideal reversible heat engine operates with zero change in internal energy and represents the theoretical maximum efficiency. Practical heat engines always have efficiency less than this ideal value due to irreversibilities such as friction, heat losses through engine walls, and incomplete combustion. Real engines like power plants and internal combustion engines cannot achieve the theoretical efficiency of reversible engines.
Q5: How do power plants and internal combustion engines function as heat engines?
Power plants use steam generated at high temperatures to drive electric generators, then release waste heat to the atmosphere or water bodies as the cold reservoir. Internal combustion engines use a hot gas-air mixture to push pistons and produce mechanical work, similarly rejecting heat to the surrounding atmosphere. Both extract heat from a high-temperature source and convert part of it into useful work.
Q6: What role do the hot and cold reservoirs play in heat engine operation?
The hot reservoir at temperature Th provides the heat energy Qh that drives the engine, while the cold reservoir at temperature Tc receives the rejected heat Qc. The temperature difference between these reservoirs enables the engine to perform work W. Without both reservoirs at different temperatures, no net work can be extracted from the system.
Q7: What does the first law of thermodynamics tell us about heat engine operation?
The first law of thermodynamics states that energy is conserved: the heat absorbed from the source equals the work output plus the heat rejected to the sink. For an ideal reversible heat engine, the internal energy change is zero, confirming this energy balance. This fundamental principle explains why efficiency must always be less than unity in any real heat engine.