首页> 外国专利> MEASUREMENT OF THERMAL DIFFUSION RATE BY LASER FLASH METHOD

MEASUREMENT OF THERMAL DIFFUSION RATE BY LASER FLASH METHOD

机译:激光闪光法测量热扩散率

摘要

PURPOSE: To improve the analysis speed by establishing a theoretical formula for temperature rise by using the dimensionless time difined by a specific formula, obtaining the dimensionless time required until the temperature rises by a specific ratio of a maximum temperature rise value, and finding out the thermal diffusion rate of a specimen based on both the obtained dimensionless time and the time obtained from actually measured temperature rise curve. ;CONSTITUTION: The thickness of a specimen is represented by b, the inner and outer radiuses in a surface irradiation area by r1 and r2, the inner and outer radiuses in a rear surface heat radiation area by r3 and r4, the thermal diffusion rate by α, respectively. Then, a representative time tc1 is defined by the effective distance 1 defined by the formula, and further the actual time t is divided by the time tc1 to define the dimensionless time. Since a theoretical response formula for temperature rise may be calculated unless the heat loss is taken into account, various data of the specimen are substituted into it to obtain a temperature rise curve. The curve is used to calculate the time t1/2* required until the temperature rises a half of a maximum temperature rise value. On the other hand, a laser is actually cast on the specimen and the time t1/2 required until the temperature rises a half of the maximum temperature rise value is measured actually. The thermal diffusion rate α can be obtained from a formula, α=t1/2*12/t1/2.;COPYRIGHT: (C)1995,JPO
机译:目的:通过使用由特定公式定义的无因次时间建立温升的理论公式,获得直到温度以最大温升值的特定比例上升直到温度上升所需的无量纲时间,从而提高分析速度,从而提高分析速度。样品的热扩散率基于获得的无量纲时间和从实际测量的温度上升曲线获得的时间。 ;组成:样品的厚度用b表示,表面照射区域的内半径和外半径用r 1 和r 2 表示,内半径和半径用背面散热面积分别为r 3 和r 4 ,热扩散速率为α。然后,用公式定义的有效距离1定义代表时间t c1 ,然后将实际时间t除以时间t c1 来定义无量纲时间。由于除非考虑热损失,否则可以计算出温度上升的理论响应公式,因此将样品的各种数据代入其中以获得温度上升曲线。该曲线用于计算直到温度升高到最大温度升高值的一半所需的时间t 1/2 *。另一方面,实际上是将激光投射在样品上,并且实际上测量了直到温度升高到最大温度升高值的一半所需的时间t 1/2 。热扩散率α可以通过公式α= t 1/2 * 1 2 / t 1/2 获得。COPYRIGHT :(C)1995,日本特许厅

著录项

  • 公开/公告号JPH07159357A

    专利类型

  • 公开/公告日1995-06-23

    原文格式PDF

  • 申请/专利权人 RIGAKU CORP;

    申请/专利号JP19930339813

  • 发明设计人 ARII TADASHI;

    申请日1993-12-07

  • 分类号G01N25/18;

  • 国家 JP

  • 入库时间 2022-08-22 04:23:27

相似文献

  • 专利
  • 外文文献
  • 中文文献
获取专利

客服邮箱:kefu@zhangqiaokeyan.com

京公网安备:11010802029741号 ICP备案号:京ICP备15016152号-6 六维联合信息科技 (北京) 有限公司©版权所有
  • 客服微信

  • 服务号