新型非朱尔加热技术:外部激光加热的钻石天细胞
Yoshiyuki Okuda1, Kenta Oka1, Koutaro Hikosaka1
1Department of Earth and Planetary Science, The University of Tokyo, 7-3-1 Hongo, Bunkyo-ku, Tokyo 113-0033, Japan.
The Review of scientific instruments
|December 11, 2023
概括
本研究介绍了一种使用激光加热进行高压和高温实验的简化外加热钻石天电池 (EHDAC). 这种新的技术可以实现高效的加热和更容易的物理性能测量,而无需复杂的布线.
科学领域:
- 高压和温度物理学的高压和温度物理.
- 材料科学是一种材料科学.
- 地质物理学 地质物理学
背景情况:
- 外部加热的钻石天电池 (EHDAC) 对于高压/高温研究至关重要,通常使用朱尔加热.
- 在EHDAC设置中,焦力加热需要复杂的电线和加热器,使实验和物理属性测量变得复杂.
- 现有的EHDAC方法面临着设置复杂性和各种测量的可访问性方面的挑战.
研究的目的:
- 开发一种简化的EHDAC技术,使用激光加热代替传统的焦尔加热.
- 为了证明激光加热在达到高温和实现各种物理性质测量的有效性.
- 为了克服与传统的EHDAC方法相关的复杂设置和布线的局限性.
主要方法:
- 提出了一种EHDAC技术,使用激光加热带有热绝缘座的密封件.
- 通过将激光热向钻石,达到高达900K的温度.
- 通过测量H2O冰VII的融化温度和高压/温度阻抗来验证设置.
主要成果:
- 在EHDAC设置中使用激光加热成功达到900K.
- 对H2O冰VII的融化温度测量与之前的研究一致.
- 通过对H2O的阻抗分析证明了电阻测量的能力.
结论:
- 激光加热的EHDAC为朱尔加热系统提供了一个简化,更高效的替代方案.
- 消除了对加热器和布线的需求,使DAC体保持室温.
- 在高压/高温研究中更容易获得更广泛的物理性质测量.
更多相关视频
06:04Simulation of the Planetary Interior Differentiation Processes in the Laboratory
Published on: November 15, 2013
11.6K
07:48An Externally-Heated Diamond Anvil Cell for Synthesis and Single-Crystal Elasticity Determination of Ice-VII at High Pressure-Temperature Conditions
Published on: June 18, 2020
6.8K
相关概念视频
Joule-Thomson Effect
The Joule-Thomson effect, also known as the Joule-Kelvin effect, describes the temperature change of a fluid when it is forced through a valve or porous plug while keeping it in a thermally insulated environment. This experiment is called a throttling process. This is an important effect widely used in refrigeration and the liquefaction of gases.
This experiment forces high-pressure gas through a throttle valve or a porous plug to a lower-pressure region. The gas expands as it passes through to...
This experiment forces high-pressure gas through a throttle valve or a porous plug to a lower-pressure region. The gas expands as it passes through to...
The Joule and Joule–Thomson Experiments
Consider an adiabatic system composed of two chambers, A and B, designed such that no heat flows into or out of the system. Initially, chamber A is filled with a gas at a fixed temperature T1, pressure p1, and volume V1, while chamber B is evacuated. The gas is then gradually forced through a rigid, porous barrier to chamber B, ultimately reaching temperature T2, pressure p2, and volume V2. A piston on the right side maintains a constant pressure (p2), which is lower than p1. The significant...
