单绍琪, 伍锦鸣, 文雅欣, 李汴生, 郭晓雪, 黎玉茗, 阮征, 李丹丹, 吴子东. 点状远红外发射源及其组合的辐照特性[J]. 红外技术, 2021, 43(1): 79-88.
引用本文: 单绍琪, 伍锦鸣, 文雅欣, 李汴生, 郭晓雪, 黎玉茗, 阮征, 李丹丹, 吴子东. 点状远红外发射源及其组合的辐照特性[J]. 红外技术, 2021, 43(1): 79-88.
SHAN Shaoqi, WU Jinmin, WEN Yaxin, LI Biansheng, GUO Xiaoxue, LI Yuming, RUAN Zheng, LI Dandan, WU Zidong. Irradiation Characteristics of Point-shaped Far-Infrared Emission Source and Combination[J]. Infrared Technology , 2021, 43(1): 79-88.
Citation: SHAN Shaoqi, WU Jinmin, WEN Yaxin, LI Biansheng, GUO Xiaoxue, LI Yuming, RUAN Zheng, LI Dandan, WU Zidong. Irradiation Characteristics of Point-shaped Far-Infrared Emission Source and Combination[J]. Infrared Technology , 2021, 43(1): 79-88.

点状远红外发射源及其组合的辐照特性

Irradiation Characteristics of Point-shaped Far-Infrared Emission Source and Combination

  • 摘要: 本文先探究3种材料的远红外辐照特性以及质量、辐照面积以及金属对远红外辐照的影响,再以点状远红外发射源为研究对象,研究了点状远红外发射源的不同影响因素及其功率密度分布规律。结果表明:远红外烧结材料的功率密度最高,陶瓷材料次之,玻璃材料最低,并确定了远红外材料功率密度的影响因素有质量、辐照面积以及金属外罩;点状远红外发射源的功率密度随着温度的升高而升高,其功率密度峰值对应的波长主要在λ=6, 10 mm附近。点状远红外发射源其功率密度呈放射状分布,在法向距离L=0~3 cm、平面内半径r=0~1 cm范围内,远红外功率密度衰减率较低,并建立了功率密度E与法向距离L的数学模型。最后据此设计了一种均匀场能的远红外发射源组合模型,验证实验表明该模型场能分布均匀,达到预期。

     

    Abstract: In this study, the far-infrared radiation characteristics of three materials and the effects of different metals on far-infrared radiation were explored. The study used the point-shaped far-infrared emission source as a research object to examine the different influencing factors and power density distribution regulation of the point-shaped far-infrared source. Results indicated that the far-infrared sintered material exhibited the highest power density, followed by the ceramic and glass materials. Factors that affected the power density of far-infrared materials were identified as the quality, irradiated area, and metal cover. The power density of the point-shaped far-infrared source increased with temperature, and the wavelength corresponding to the maximum power density was approximately λ=6-10 μm. The power density of the point-shaped far-infrared emission source was distributed in a radial manner. In the range of the vertical distance L=0-3 cm and radius r=0-1 cm, the far-infrared power density attenuation rate was low and was designed accordingly. In addition, a mathematical model of power density E and normal distance L was established. Based on these factors, we designed a far-infrared emitter combination model with a uniform field energy. Results revealed that the field energy of this model was evenly distributed to achieve the desired effect.

     

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