• Infrared and Laser Engineering
  • Vol. 50, Issue 5, 20210147 (2021)
Juan Li1、2, Hao Yu1、2, Tiancheng Yu1、2, Yudan Gou1、2, Huomu Yang1, and Jun Wang1、2
Author Affiliations
  • 1College of Electronic Information, Sichuan University, Chengdu 610065, China
  • 2Suzhou Everbright Photonics Co., Ltd., Suzhou 215163, China
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    DOI: 10.3788/IRLA20210147 Cite this Article
    Juan Li, Hao Yu, Tiancheng Yu, Yudan Gou, Huomu Yang, Jun Wang. Design of high efficiency diode laser module for wireless power transmission[J]. Infrared and Laser Engineering, 2021, 50(5): 20210147 Copy Citation Text show less
    The far-field spots and intensity distribution curve of Gaussian beam. (a) The far-field intensity distribution curve of Gaussian beam; (b) The far-field spots of Gaussian beam
    Fig. 1. The far-field spots and intensity distribution curve of Gaussian beam. (a) The far-field intensity distribution curve of Gaussian beam; (b) The far-field spots of Gaussian beam
    Optical simulation of laser system
    Fig. 2. Optical simulation of laser system
    Optical simulation at the receiver. (a) Optical field distribution of output beams from eight modules respectiveliy; (b) Optical field distribution of laser system in different sizes
    Fig. 3. Optical simulation at the receiver. (a) Optical field distribution of output beams from eight modules respectiveliy; (b) Optical field distribution of laser system in different sizes
    The effect of angle deflection on the optical field distribution at the receiver. (a) The unevenness distribution was obtained by optimizing the combination of 8 modules with deflection angles respectively; (b) Optical field distribution when the spot unevenness reaches the minimum; (c) Optical field distribution when the spot unevenness reaches the maximum
    Fig. 4. The effect of angle deflection on the optical field distribution at the receiver. (a) The unevenness distribution was obtained by optimizing the combination of 8 modules with deflection angles respectively; (b) Optical field distribution when the spot unevenness reaches the minimum; (c) Optical field distribution when the spot unevenness reaches the maximum
    The effect of defocusing of FA cylindrical lens on optical field distribution at receiver. (a) The relationship between the unevenness and the moving distance of lens; (b) The optical field distribution when the lens moves in the opposite direction of beam propagation to the beam outlet (−0.08 m), and the unevenness is 0.227; (c) The unevenness reaches the minimum which is 0.218; (d) The optical field distribution of the lens with a distance of 0.08 m in the direction of beam transmission, and the unevenness is 0.237
    Fig. 5. The effect of defocusing of FA cylindrical lens on optical field distribution at receiver. (a) The relationship between the unevenness and the moving distance of lens; (b) The optical field distribution when the lens moves in the opposite direction of beam propagation to the beam outlet (−0.08 m), and the unevenness is 0.227; (c) The unevenness reaches the minimum which is 0.218; (d) The optical field distribution of the lens with a distance of 0.08 m in the direction of beam transmission, and the unevenness is 0.237
    The influence of the power variation of each module on the optical field distribution of the receiver. (a) The unevenness distribution was obtained by optimizing the combination of 8 modules with different output power respectively; (b) Optical field distribution when the spot unevenness reaches the minimum; (c) Optical field distribution when the spot unevenness reaches the maximum
    Fig. 6. The influence of the power variation of each module on the optical field distribution of the receiver. (a) The unevenness distribution was obtained by optimizing the combination of 8 modules with different output power respectively; (b) Optical field distribution when the spot unevenness reaches the minimum; (c) Optical field distribution when the spot unevenness reaches the maximum
    The far-field spots and intensity distribution curve of different beams. (a) The far-field intensity distribution curve of the output beam from diode laser system for short distance LWPT at the receiver; (b) The far-field spots of the output beam from diode laser system for short distance LWPT at the receiver
    Fig. 7. The far-field spots and intensity distribution curve of different beams. (a) The far-field intensity distribution curve of the output beam from diode laser system for short distance LWPT at the receiver; (b) The far-field spots of the output beam from diode laser system for short distance LWPT at the receiver
    Laser system output characteristics. (a) LIV curve of laser system; (b) The spectral characteristics of the laser system vs the operating current
    Fig. 8. Laser system output characteristics. (a) LIV curve of laser system; (b) The spectral characteristics of the laser system vs the operating current
    Measure of optical field distribution which is transmitted beyond 20 m under working current. (a) Optical field distribution of 20 m transmitted by 8 sub-beams; (b) The optical field distribution of laser system, which is transmitted beyond 20 m, and the spot size is 0.44 m×0.49 m
    Fig. 9. Measure of optical field distribution which is transmitted beyond 20 m under working current. (a) Optical field distribution of 20 m transmitted by 8 sub-beams; (b) The optical field distribution of laser system, which is transmitted beyond 20 m, and the spot size is 0.44 m×0.49 m
    The optical field distribution of laser system after optimizing, which is transmitted beyond 20 m
    Fig. 10. The optical field distribution of laser system after optimizing, which is transmitted beyond 20 m
    Juan Li, Hao Yu, Tiancheng Yu, Yudan Gou, Huomu Yang, Jun Wang. Design of high efficiency diode laser module for wireless power transmission[J]. Infrared and Laser Engineering, 2021, 50(5): 20210147
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