在高温和磁场下测量Nernst和Seebeck效应的测量设置,对元素斯木和全Heusler化合物进行了测试
M Parzer1, T Schmid1, F Garmroudi1
1Institute of Solid State Physics, Technische Universität Wien, 1040 Vienna, Austria.
The Review of scientific instruments
|April 23, 2024
概括
一个新的设置允许在高温 (700 K) 和磁场 (12 T) 中同时测量Seebeck和Nernst效应. 这一进步允许在高达560K的高温物质中进行准确的热电和热磁性质分析,例如斯木和海斯勒化合物.
科学领域:
- 凝聚物质物理学 凝聚物质物理学
- 材料科学是一种材料科学.
- 热力学是一种热力学.
背景情况:
- 热电和热磁效应对于能量转换和传感至关重要.
- 之前的研究受到较低的温度和磁场范围的限制.
- 准确的测量对于理解材料特性至关重要.
研究的目的:
- 引入和验证一个新的测量设置,用于Seebeck和Nernst效应.
- 为了使高温和高磁场的同时测量.
- 扩大热电和热磁研究可访问的温度和场范围.
主要方法:
- 为同时进行Seebeck和Nernst效应研究开发测量系统.
- 导出测量方程以纠正虚假的偏移电压和系统错误.
- 实验验证使用多晶斯木和全Heusler材料.
主要成果:
- 该设置可以成功执行高达700K和12T的同时测量.
- 测量方程有效抵消偏移电压,确保准确性.
- 测试材料的热电和热磁性质与报告的值保持一致.
- 首次报告特定材料的特性,最高可达560K.
结论:
- 开发的设置可用于高温和高磁场研究.
- 该系统克服了以前在温度和场间隔方面的限制.
- 这促进了热电和热磁材料的先进研究.
更多相关视频
12:02Determination of Thermodynamic Properties of Alkaline Earth-liquid Metal Alloys Using the Electromotive Force Technique
Published on: November 3, 2017
13.1K
04:22Author Spotlight: Advancements in High-Performance Thermoelectric Thin Films Through Radio Frequency Magnetron Sputtering
Published on: May 17, 2024
2.8K
相关概念视频
Diamagnetism
2.4K
Materials consisting of paired electrons have zero net magnetic moments. However, when these materials are placed under an external magnetic field, the moments opposite to the field are induced. Such materials are called diamagnets. Diamagnetism is the response of the diamagnets when placed in an external magnetic field.
Diamagnetism was discovered by Anton Brugmans in 1778 when he observed that bismuth gets repelled by magnetic fields, thus theorizing that diamagnets get repelled by magnets....
Diamagnetism was discovered by Anton Brugmans in 1778 when he observed that bismuth gets repelled by magnetic fields, thus theorizing that diamagnets get repelled by magnets....
2.4K
Ferromagnetism
2.4K
Materials like iron, nickel, and cobalt consist of magnetic domains, within which the magnetic dipoles are arranged parallel to each other. The magnetic dipoles are rigidly aligned in the same direction within a domain by quantum mechanical coupling among the atoms. This coupling is so strong that even thermal agitation at room temperature cannot break it. The result is that each domain has a net dipole moment. However, some materials have weaker coupling, and are ferromagnetic at lower...
2.4K
Superconductor
1.1K
A substance that reaches superconductivity, a state in which magnetic fields cannot penetrate, and there is no electrical resistance, is referred to as a superconductor. In 1911, Heike Kamerlingh Onnes of Leiden University, a Dutch physicist, observed a relation between the temperature and the resistance of the element mercury. The mercury sample was then cooled in liquid helium to study the linear dependence of resistance on temperature. It was observed that, as the temperature decreased, the...
1.1K
Magnetic Susceptibility and Permeability
1.1K
In linear magnetic materials, like paramagnets and diamagnets, magnetization is proportional to the magnetic field intensity. The constant of proportionality, a dimensionless number, is called magnetic susceptibility. The value of the susceptibility depends on the type of material.
When diamagnetic materials are placed under an external magnetic field, the moments opposite to the field are induced. Hence, the susceptibility for diamagnets has a minimal negative value of 10-5–10-6. Since...
When diamagnetic materials are placed under an external magnetic field, the moments opposite to the field are induced. Hence, the susceptibility for diamagnets has a minimal negative value of 10-5–10-6. Since...
1.1K
The Hall Effect
2.4K
Edwin H. Hall, in the year 1879, devised an experiment that could be used to identify the polarity of the predominant charge carriers in a conducting material. From a historical perspective, this experiment was the first to demonstrate that the charge carriers in most metals are negative.
2.4K
Types Of Superconductors
974
A superconductor is a substance that offers zero resistance to the electric current when it drops below a critical temperature. Zero resistance is not the only interesting phenomenon as materials reach their transition temperatures. A second effect is the exclusion of magnetic fields. This is known as the Meissner effect. A light, permanent magnet placed over a superconducting sample will levitate in a stable position above the superconductor. High-speed trains that levitate on strong...
974
