Potamias Dimitrios, Alxneit Ivo, Wokaun Alexander
Solar Technology Laboratory, Paul Scherrer Institute, CH-5232 Villigen PSI, Switzerland.
Department Energy and Environment, Paul Scherrer Institute, CH-5232 Villigen PSI, Switzerland.
Rev Sci Instrum. 2017 Sep;88(9):095112. doi: 10.1063/1.4987129.
The design, implementation, calibration, and assessment of double modulation pyrometry to measure surface temperatures of radiatively heated samples in our 1 kW imaging furnace is presented. The method requires that the intensity of the external radiation can be modulated. This was achieved by a rotating blade mounted parallel to the optical axis of the imaging furnace. Double modulation pyrometry independently measures the external radiation reflected by the sample as well as the sum of thermal and reflected radiation and extracts the thermal emission as the difference of these signals. Thus a two-step calibration is required: First, the relative gains of the measured signals are equalized and then a temperature calibration is performed. For the latter, we transfer the calibration from a calibrated solar blind pyrometer that operates at a different wavelength. We demonstrate that the worst case systematic error associated with this procedure is about 300 K but becomes negligible if a reasonable estimate of the sample's emissivity is used. An analysis of the influence of the uncertainties in the calibration coefficients reveals that one (out of the five) coefficient contributes almost 50% to the final temperature error. On a low emission sample like platinum, the lower detection limit is around 1700 K and the accuracy typically about 20 K. Note that these moderate specifications are specific for the use of double modulation pyrometry at the imaging furnace. It is mainly caused by the difficulty to achieve and maintain good overlap of the hot zone with a diameter of about 3 mm Full Width at Half Height and the measurement spot both of which are of similar size.
本文介绍了在我们的1千瓦成像炉中用于测量辐射加热样品表面温度的双调制高温测定法的设计、实施、校准和评估。该方法要求外部辐射强度能够被调制。这通过平行于成像炉光轴安装的旋转叶片来实现。双调制高温测定法独立测量样品反射的外部辐射以及热辐射和反射辐射的总和,并提取热发射作为这些信号的差值。因此需要进行两步校准:首先,均衡测量信号的相对增益,然后进行温度校准。对于后者,我们从工作在不同波长的校准过的日盲高温计进行校准传递。我们证明与该程序相关的最坏情况系统误差约为300K,但如果使用样品发射率的合理估计值,该误差可忽略不计。对校准系数不确定性影响的分析表明,五个系数中的一个对最终温度误差的贡献几乎达到50%。在像铂这样的低发射率样品上,检测下限约为1700K,精度通常约为20K。请注意,这些适度的规格是成像炉中使用双调制高温测定法所特有的。这主要是由于难以实现并保持直径约3毫米半高全宽的热区与测量点的良好重叠,两者尺寸相似。