Calibration and verification of streaked optical pyrometer system used for laser-induced shock experiments Download: 833次
1 Shanghai Institute of Laser Plasma, CAEP, Shanghai 201800, China
2 IFSA Collaborative Innovation Center, Shanghai Jiao Tong University, Shanghai 200240, China
3 Institute of Applied Physics and Computational Mathematics, Beijing 100094, China
Figures & Tables
Fig. 1. Spectral radiance and Planck fit of the lower-color-temperature $({\sim}3000~\text{K})$ halogen tungsten lamp (thick orange line and thin red line) and the higher-color-temperature $({\sim}5000~\text{K})$ specially designed lamp (thick blue line and thin purple line).
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Fig. 2. Calibration and verification configuration of the SOP system (top view).
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Fig. 3. (a) LSF FWHM and (b) spectral response of the SC-10 streak camera.
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Fig. 4. Schematic of the four-channel filter.
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Fig. 5. Spectral radiance data and theoretical Planck fit curve for conditions using (a) Lamp A as the standard or (b) Lamp B as the standard. Spatial chromaticity maps representing the measured temperature using (c) Lamp A as the standard or (d) Lamp B as the standard.
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Fig. 6. Relationship between $\unicode[STIX]{x0394}T/T$ and $\unicode[STIX]{x0394}X/X$ and the sensitivity curve of the calibration (No. S003B, (a) and (b)) and shock-wave experiment (No. D0211, (c) and (d)).
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Fig. 7. (a) Schematic of the target; (b) VISAR line-image record; (c) SOP image record; (d) a comparison of the reflectivity as a function of shock velocity in quartz and fused silica by Hicks et al.[2, 6]; and (e) a comparison of the measured temperature as a function of shock velocity in quartz by Hicks et al. (solid pink diamonds), the Sesame model (solid cyan line), and this work (solid blue circles for fused silica and solid red circles for quartz).
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Table1. Calibration and verification results (measured temperature $T$, deviation between the measured temperature and the standard value $\unicode[STIX]{x1D702}$) of the SOP system using a single-channel (No. S001–S0024) or multi-channel (No. M001–M002) method are listed in addition to the MCP of the streak camera for each experiment.
No. | MCP | Channel | Standard: Lamp A | Standard: Lamp B |
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| | | $T_{B}$ (K) | $\unicode[STIX]{x1D702}_{B}$ (%) | $T_{A}$ (K) | $\unicode[STIX]{x1D702}_{A}$ (%) |
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M001 | 850 V | Four-channel | 4893 | 1.3 | 2904 | 1.7 | M002 | 800 V | Four-channel | 4870 | 1.8 | 2924 | 0.99 | S001 | 750 V | Single-channel: 442 nm | 4801 | 3.2 | 2981 | 0.94 | S002 | 800 V | Single-channel: 442 nm | 4818 | 2.9 | 2975 | 0.74 | S003 | 850 V | Single-channel: 442 nm | 4839 | 2.4 | 2966 | 0.44 | S0011 | 850 V | Single-channel: 410 nm | 4711 | 5.2 | 2981 | 0.94 | S0012 | 850 V | Single-channel: 450 nm | 4844 | 2.3 | 2967 | 0.47 | S0013 | 850 V | Single-channel: 490 nm | 4857 | 2.0 | 2978 | 0.84 | S0014 | 850 V | Single-channel: 590 nm | 4749 | 4.3 | 3041 | 2.9 | S0021 | 800 V | Single-channel: 410 nm | 4752 | 4.3 | 2990 | 1.2 | S0022 | 800 V | Single-channel: 450 nm | 4879 | 1.6 | 2977 | 0.81 | S0023 | 800 V | Single-channel: 490 nm | 4894 | 1.3 | 2983 | 1.0 | S0024 | 800 V | Single-channel: 590 nm | 4782 | 3.6 | 3057 | 3.4 |
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Table2. Variables and their uncertainties in the calibrations and shock-wave experiments. Samples for the calibrations using a single-channel begin with an S; samples for calibrations using a multi-channel begin with an M; and samples for the shock-wave experiments begin with a D. In particular, the $L_{m}$, $\unicode[STIX]{x1D700}$, and $T$ of the shock-wave experiments refer to values at the interface of the sample and base material.
No. | Sample | | | | | | | | |
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| | | | (nm) | (nm) | | | (K) | (K) |
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M001B | Lamp B | Four-channel | $2.2\times 10^{-4}$ | $6.0\times 10^{-5}$ | 4893 | 226 | M002B | Lamp B | Four-channel | $2.3\times 10^{-4}$ | $9.8\times 10^{-5}$ | 4870 | 217 | S001B | Lamp B | $1.99\times 10^{9}$ | $2.99\times 10^{8}$ | 442 | 20 | $2.5\times 10^{-4}$ | $2.7\times 10^{-6}$ | 4799 | 121 | S002B | Lamp B | $2.04\times 10^{9}$ | $3.06\times 10^{8}$ | 442 | 20 | $2.5\times 10^{-4}$ | $2.7\times 10^{-6}$ | 4817 | 121 | S003B | Lamp B | $2.10\times 10^{9}$ | $3.15\times 10^{8}$ | 442 | 20 | $2.5\times 10^{-4}$ | $2.7\times 10^{-6}$ | 4838 | 122 | S0011B | Lamp B | $1.49\times 10^{9}$ | $2.23\times 10^{8}$ | 410 | 10 | $2.5\times 10^{-4}$ | $2.7\times 10^{-6}$ | 4711 | 102 | S0012B | Lamp B | $2.18\times 10^{9}$ | $3.27\times 10^{8}$ | 450 | 10 | $2.5\times 10^{-4}$ | $2.7\times 10^{-6}$ | 4843 | 113 | S0013B | Lamp B | $2.48\times 10^{9}$ | $3.72\times 10^{8}$ | 490 | 15 | $2.5\times 10^{-4}$ | $2.7\times 10^{-6}$ | 4854 | 123 | S0014B | Lamp B | $2.45\times 10^{9}$ | $3.68\times 10^{8}$ | 590 | 15 | $2.5\times 10^{-4}$ | $2.7\times 10^{-6}$ | 4747 | 138 | S0021B | Lamp B | $1.52\times 10^{9}$ | $2.28\times 10^{8}$ | 410 | 10 | $2.5\times 10^{-4}$ | $2.7\times 10^{-6}$ | 4725 | 103 | S0022B | Lamp B | $2.26\times 10^{9}$ | $3.39\times 10^{8}$ | 450 | 10 | $2.5\times 10^{-4}$ | $2.7\times 10^{-6}$ | 4869 | 114 | S0023B | Lamp B | $2.56\times 10^{9}$ | $3.84\times 10^{8}$ | 490 | 15 | $2.5\times 10^{-4}$ | $2.7\times 10^{-6}$ | 4880 | 124 | S0024B | Lamp B | $2.49\times 10^{9}$ | $3.73\times 10^{8}$ | 590 | 15 | $2.5\times 10^{-4}$ | $2.7\times 10^{-6}$ | 4762 | 139 | M001A | Lamp A | Four-channel | $7.0\times 10^{-3}$ | $3.0\times 10^{-3}$ | 2904 | 140 | M002A | Lamp A | Four-channel | $7.3\times 10^{-3}$ | $2.5\times 10^{-3}$ | 2924 | 50 | S001A | Lamp A | $7.68\times 10^{8}$ | $1.15\times 10^{8}$ | 442 | 20 | $6.1\times 10^{-3}$ | $3.9\times 10^{-5}$ | 2981 | 84 | S002A | Lamp A | $7.52\times 10^{8}$ | $1.13\times 10^{8}$ | 442 | 20 | $6.1\times 10^{-3}$ | $3.9\times 10^{-5}$ | 2975 | 84 | S003A | Lamp A | $7.29\times 10^{8}$ | $1.09\times 10^{8}$ | 442 | 20 | $6.1\times 10^{-3}$ | $3.9\times 10^{-5}$ | 2967 | 84 | S0011A | Lamp A | $4.78\times 10^{8}$ | $7.17\times 10^{7}$ | 410 | 10 | $6.1\times 10^{-3}$ | $3.9\times 10^{-5}$ | 2982 | 56 | S0012A | Lamp A | $8.12\times 10^{8}$ | $1.22\times 10^{8}$ | 450 | 10 | $6.1\times 10^{-3}$ | $3.9\times 10^{-5}$ | 2968 | 54 | S0013A | Lamp A | $1.32\times 10^{9}$ | $1.98\times 10^{8}$ | 490 | 15 | $6.1\times 10^{-3}$ | $3.9\times 10^{-5}$ | 2977 | 64 | S0014A | Lamp A | $3.30\times 10^{9}$ | $4.95\times 10^{8}$ | 590 | 15 | $6.1\times 10^{-3}$ | $3.9\times 10^{-5}$ | 3040 | 64 | S0021A | Lamp A | $4.81\times 10^{8}$ | $7.21\times 10^{7}$ | 410 | 10 | $6.1\times 10^{-3}$ | $3.9\times 10^{-5}$ | 2983 | 57 | S0022A | Lamp A | $8.38\times 10^{8}$ | $1.26\times 10^{8}$ | 450 | 10 | $6.1\times 10^{-3}$ | $3.9\times 10^{-5}$ | 2976 | 54 | S0023A | Lamp A | $1.36\times 10^{9}$ | $2.04\times 10^{8}$ | 490 | 15 | $6.1\times 10^{-3}$ | $3.9\times 10^{-5}$ | 2986 | 64 | S0024A | Lamp A | $3.50\times 10^{9}$ | $5.25\times 10^{8}$ | 590 | 15 | $6.1\times 10^{-3}$ | $3.9\times 10^{-5}$ | 3062 | 65 | D0211 | Quartz | $4.61\times 10^{15}$ | $6.91\times 10^{14}$ | 450 | 10 | 0.707 | 0.109 | 46498 | 7727 | D0212 | Quartz | $1.80\times 10^{15}$ | $2.70\times 10^{14}$ | 590 | 15 | 0.720 | 0.111 | 47710 | 8787 | D0213 | Fused silica | $4.37\times 10^{15}$ | $6.55\times 10^{14}$ | 410 | 10 | 0.534 | 0.082 | 43134 | 6847 | D0214 | Fused silica | $3.65\times 10^{15}$ | $5.47\times 10^{14}$ | 490 | 15 | 0.534 | 0.082 | 61117 | 11836 |
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Zhiyu He, Guo Jia, Fan Zhang, Xiuguang Huang, Zhiheng Fang, Jiaqing Dong, Hua Shu, Junjian Ye, Zhiyong Xie, Yuchun Tu, Qili Zhang, Erfu Guo, Wenbing Pei, Sizu Fu. Calibration and verification of streaked optical pyrometer system used for laser-induced shock experiments[J]. High Power Laser Science and Engineering, 2019, 7(3): 03000e49.