不同质系统中的热力学状态:从纳米尺度到宏观尺度
Sankhadeep Bose1, Andrea Floris2, Mangaiyarkarasi Rajendiran3
1School of Mechanical Engineering, Vellore Institute of Technology, Vellore 632014, Tamil Nadu, India.
ACS omega
|April 28, 2025
概括
有限纳米系统由于空间变化而表现出独特的热力学行为,挑战标准模型. 这些不均的系统表现出持续的偏差和有限的温度相变,即使是在更大的尺度上.
科学领域:
- 热力学是一种热力学.
- 纳米科学是一个纳米科学.
- 统计力学 统计力学
背景情况:
- 标准热力学通常假定系统的同质性,这可能不适用于有限的纳米系统.
- 对于纳米级应用来说,了解非均系统中的热力学稳定性和相位过渡至关重要.
研究的目的:
- 分析有限的非同质纳米系统中热力学稳定状态和相变的机制.
- 研究系统大小对这些系统宏观行为的影响.
- 挑战同质系统代表有限的非同质系统的非对称极限的假设.
主要方法:
- 经典的分子动力学模拟.
- 在各种尺度上分析球形的莱纳德-斯纳米粒子.
- 检查一个和两个相平衡中的系统.
主要成果:
- 非同质的稳定状态是由密集变量的空间变化所支配,而不是同质系统中的广泛变量.
- 不同质系统中的密集变量从同质预测中持续偏离,无论大小如何.
- 同相过渡在有限的温度间隔中发生在两相平衡中,包括三相状态,这些状态不会随着尺寸的增加而消失.
结论:
- 边界效应显著影响有限纳米系统中的热力学稳定性和平衡机制.
- 非均的强度变量变化是单相平衡和有限温度相位过渡的关键.
- 现有的热力学模型可能需要修订,以考虑纳米系统中的非同质性和边界效应.
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