Author Affiliations
1Key Laboratory of Pulsed Power Laser Technology, National University of Defense Technology, Hefei, Anhui 230037, China2Troops 32256, Chinese People's Liberation Army, Guilin, Guangxi 541000, Chinashow less
Fig. 1. CGI system for penetrating scattering media
Fig. 2. Experimental results of CGI penetrating scattering medium
[10,12]. (a)
Ni≈0; (b)
Ni≠0; (c) degraded patterns; (d) undegraded patterns
Fig. 3. Transmission path of photon in cylindrical scattering medium
Fig. 4. Schematic diagram of CGI combined with Monte Carlo model
Fig. 5. Lena simulation results at different uniform mass concentrations of smoke (0.1, 0.2, 0.3, 0.4, 0.5 g·m-3). (a) PSF of smoke at different concentrations; (b) results of TI; (c) reconstruction images of CGI
Fig. 6. Relationship between reconstruction image quality and smoke mass concentration in three cases
Fig. 7. Smoke with uneven concentration distribution at some heights. (a) z=2.5 m; (b) z=5 m; (c) z=10 m;(d) z=20 m
Fig. 8. Lena simulation results at different uneven mass concentrations of smoke(20, 30, 50, 100 g·s-1). (a) PSF of smoke; (b) TI results; (c) CGI results
Fig. 9. Results of CGI at time-varying concentrations. (a) Random variation range (0.9,1); (b) random variation range (0.99,1); (c) random variation range (0.999,1); (d) random variation range (0.9999,1)
Parameter | Value | Parameter | Value |
---|
Target plane z /m | 20 | Particle radius r /μm | 0.4 | Anisotropic factor g | 0.8 | Scattering coefficient us / (cm2·g-1) | 1.2 | Wavelength λ/m | 532 | Absorption coefficient ua / (cm2·g-1) | 0.25 | Tracking photon number N | 107 | Energy decay threshold T | 10-5 |
|
Table 1. Some parameters used in simulation