在矿热电中,通过工程来实现载体 - 声子脱
Yunpeng Zheng1,2, Qinghua Zhang3, Caijuan Shi4
1State Key Laboratory of New Ceramics and Fine Processing, School of Materials Science and Engineering, Tsinghua University, Beijing, PR China.
Nature communications
|September 2, 2024
概括
热工程在矿热电学中将载体和声子脱. 这一策略显著提高了基于SrTiO3的材料的热电功率 (zT).
科学领域:
- 材料科学 材料科学 材料科学
- 固态物理 固态物理
- 能源转换 能源转换
背景情况:
- 热电材料直接转换热量和电力,其效率用功率 (zT) 表示量化.
- 热电材料的一个关键挑战是将电荷载体和声子传输脱,以优化zT.
- 基于甲酸 (SrTiO3) 的矿是典型的热电氧化物,具有改进潜力.
研究的目的:
- 引入和研究一种工程策略,用于在基于SrTiO3的热电中解载体和声子运输.
- 通过高设计,降低格子导热率并增强载体流动性.
- 评估热电性能,特别是工程矿的优点 (zT) 值.
主要方法:
- 使用高设计创建了新的矿组成.
- 测量和分析了格子的导热率.
- 计算了载体加权的移动性.
- 在各种温度下测量了热电功率 (zT).
主要成果:
- 格子的导热率降低到接近无形极限 (1.25 W m-1 K-1).
- Entropy 工程提高了载体加权移动性,达到 65 cm2 V-1 s-1.1.
- 权重移动性与格子导热率 (μW/κL) 的比率达到了5.2 × 103 cm3 K J-1 V-1.1.
- 在 (Sr0.2Ba0.2Ca0.2Pb0.2La0.2) TiO3薄膜中,最大测量zT为0.24在488K,估计zT为~0.8在1173K.
结论:
- 在基于SrTiO3的热电学中,透工程有效地解了载体和声子运输.
- 这种方法显著提高了热电性能.
- 开发的材料显示出作为高性能n型热电氧化物具有有前途的潜力.
相关概念视频
Carrier Generation and Recombination
548
Carrier generation is the process by which electron-hole pairs (EHPs) are created within the semiconductor. In direct-bandgap semiconductors, such as gallium arsenide (GaAs), this occurs efficiently when energy absorption prompts valence electrons to leap into the conduction band, leaving behind holes.
This process is given by the generation rate G and is efficient due to the conservation of momentum between the valence band maximum and conduction band minimum.
Indirect generation involves an...
This process is given by the generation rate G and is efficient due to the conservation of momentum between the valence band maximum and conduction band minimum.
Indirect generation involves an...
548
Entropy and the Second Law of Thermodynamics
2.8K
The second law of thermodynamics can be stated quantitatively using the concept of entropy. Entropy is the measure of disorder of the system.
The relation between entropy and disorder can be illustrated with the example of the phase change of ice to water. In ice, the molecules are located at specific sites giving a solid state, whereas, in a liquid form, these molecules are much freer to move. The molecular arrangement has therefore become more randomized. Although the change in average...
The relation between entropy and disorder can be illustrated with the example of the phase change of ice to water. In ice, the molecules are located at specific sites giving a solid state, whereas, in a liquid form, these molecules are much freer to move. The molecular arrangement has therefore become more randomized. Although the change in average...
2.8K
Entropy Change in Reversible Processes
2.5K
In the Carnot engine, which achieves the maximum efficiency between two reservoirs of fixed temperatures, the total change in entropy is zero. The observation can be generalized by considering any reversible cyclic process consisting of many Carnot cycles. Thus, it can be stated that the total entropy change of any ideal reversible cycle is zero.
The statement can be further generalized to prove that entropy is a state function. Take a cyclic process between any two points on a p-V diagram.
The statement can be further generalized to prove that entropy is a state function. Take a cyclic process between any two points on a p-V diagram.
2.5K
Types of Semiconductors
562
Intrinsic semiconductors are highly pure materials with no impurities. At absolute zero, these semiconductors behave as perfect insulators because all the valence electrons are bound, and the conduction band is empty, disallowing electrical conduction. The Fermi level is a concept used to describe the probability of occupancy of energy levels by electrons at thermal equilibrium. In intrinsic semiconductors, the Fermi level is positioned at the midpoint of the energy gap at absolute zero. When...
562
Thermodynamic Potentials
788
Thermodynamic potentials are state functions that are extremely useful in analyzing a thermodynamic system. They have dimensions of energy. The four important thermodynamic potentials are internal energy, enthalpy, Helmholtz free energy, and Gibbs free energy. These thermodynamic potentials can be expressed using two of the following variables: pressure, volume, temperature, and entropy. These two variables are expressed as the rate of change of the thermodynamic potential with respect to other...
788
Third Law of Thermodynamics
18.5K
A pure, perfectly crystalline solid possessing no kinetic energy (that is, at a temperature of absolute zero, 0 K) may be described by a single microstate, as its purity, perfect crystallinity,and complete lack of motion means there is but one possible location for each identical atom or molecule comprising the crystal (W = 1). According to the Boltzmann equation, the entropy of this system is zero.
18.5K


