Calibration and verification of streaked optical pyrometer system used for laser-induced shock experiments

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

doi:10.1017/hpl.2019.27

Journals >High Power Laser Science and Engineering >Volume 7 >Issue 3 >Page 03000e49 > Article

High Power Laser Science and Engineering
Vol. 7, Issue 3, 03000e49 (2019)

Calibration and verification of streaked optical pyrometer system used for laser-induced shock experiments

Zhiyu He¹, Guo Jia^1、†, Fan Zhang¹, Xiuguang Huang^1、2, Zhiheng Fang¹, Jiaqing Dong¹, Hua Shu¹, Junjian Ye¹, Zhiyong Xie¹, Yuchun Tu¹, Qili Zhang³, Erfu Guo¹, Wenbing Pei^1、2, and Sizu Fu^1、2

Author Affiliations

¹Shanghai Institute of Laser Plasma, CAEP, Shanghai 201800, China

²IFSA Collaborative Innovation Center, Shanghai Jiao Tong University, Shanghai 200240, China

³Institute of Applied Physics and Computational Mathematics, Beijing 100094, China

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DOI: 10.1017/hpl.2019.27 Cite this Article Set citation alerts

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 Copy Citation Text

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$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).$

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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$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)).$

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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No.	MCP	Channel	Standard: Lamp A		Standard: Lamp B
			$T_{B}$ (K)	$\unicode[STIX]{x1D702}_{B}$ (%)	$T_{A}$ (K)	$\unicode[STIX]{x1D702}_{A}$ (%)
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

Table 1. 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.

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No.	Sample
				(nm)	(nm)			(K)	(K)
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

Table 2. 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.