理论最大效率 fuel cell 燃料电池的热效率取决于吉布斯自由能变化 (ΔG) 与电化学反应焓变 (ΔH) 的比值,即 ηthermo = ΔG/ΔH。关键在于,燃料电池并非热机,因此不受卡诺效率极限的限制,理论上可以实现更高的转换效率。

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理论最大效率 fuel cell 燃料电池的热效率取决于吉布斯自由能变化 (ΔG) 与电化学反应焓变 (ΔH) 的比值,即 ηthermo = ΔG/ΔH。关键在于,燃料电池并非热机,因此不受卡诺效率极限的限制,理论上可以实现更高的转换效率。
The Gibbs free energy, [latex]\Delta G[/latex], represents the maximum amount of non-expansion work that can be extracted from a thermodynamically closed system at constant temperature and pressure. In a fuel cell, this work is the electrical work performed. The change in enthalpy, [latex]\Delta H[/latex], represents the total heat content of the reaction, which is the energy released during combustion. The difference between these two values, [latex]T\Delta S[/latex] (where T is temperature and [latex]\Delta S[/latex] is the change in entropy), represents the unavoidable waste heat generated by the reaction even under ideal, reversible conditions.
In contrast, a heat engine’s maximum efficiency is dictated by the Carnot limit, [latex]\eta_C = 1 – \frac{T_{cold}}{T_{hot}}[/latex], which depends on the temperature difference between its hot and cold reservoirs. For a typical 氢燃料 cell operating at standard conditions, the 热力学 燃料电池的效率约为 83%,而实际内燃机的效率很难超过 40%。虽然燃料电池的理论效率很高,但实际应用中的设备会受到多种不可逆损耗,或称“极化”,从而降低其实际效率。这些损耗包括活化损耗(引发反应所需的能量)、欧姆损耗(离子和电子流动的阻力)以及传质损耗(反应物无法及时输送到反应位点)。
燃料电池的热力学效率
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