• Chinese Optics Letters
  • Vol. 19, Issue 10, 102601 (2021)
Zixiao Miao and Qican Zhang*
Author Affiliations
  • Department of Opto-Electronics, Sichuan University, Chengdu 610065, China
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    DOI: 10.3788/COL202119.102601 Cite this Article Set citation alerts
    Zixiao Miao, Qican Zhang. Dual-frequency fringe for improving measurement accuracy of three-dimensional shape measurement[J]. Chinese Optics Letters, 2021, 19(10): 102601 Copy Citation Text show less
    Principle of the proposed dual-frequency method: (a) four phase-shifting patterns of fh; (b) four phase-shifting patterns of fl; (c) wrapped phase ϕh; (d) wrapped phase ϕl; (e) phase difference ϕd; (f) phase sum ϕs; (g) one cross section of the unwrapped phase difference Φd, fringe order kl, and wrapped phase ϕl; (h) one cross section of the phase sum ϕs, fringe order ks, and unwrapped phase Φl.
    Fig. 1. Principle of the proposed dual-frequency method: (a) four phase-shifting patterns of fh; (b) four phase-shifting patterns of fl; (c) wrapped phase ϕh; (d) wrapped phase ϕl; (e) phase difference ϕd; (f) phase sum ϕs; (g) one cross section of the unwrapped phase difference Φd, fringe order kl, and wrapped phase ϕl; (h) one cross section of the phase sum ϕs, fringe order ks, and unwrapped phase Φl.
    Chart of the computer simulation process of the proposed dual-frequency by FPP.
    Fig. 2. Chart of the computer simulation process of the proposed dual-frequency by FPP.
    Computer simulation results of the proposed dual-frequency in 3D shape measurement. (a), (b) One cross section of wrapped phases (Tl = 170 pixels, Th = 150 pixels) and synthetic phases (Td = 1275 pixels, Ts = 79.7 pixels); (c) one cross section of wrapped phase ϕl, phase difference ϕd, and fringe order kl; (d) one cross section of wrapped phase ϕs, unwrapped phase Φl, and fringe order ks; (e) one cross section of the restored object’s height; (f) one cross section of the restored height error.
    Fig. 3. Computer simulation results of the proposed dual-frequency in 3D shape measurement. (a), (b) One cross section of wrapped phases (Tl = 170 pixels, Th = 150 pixels) and synthetic phases (Td = 1275 pixels, Ts = 79.7 pixels); (c) one cross section of wrapped phase ϕl, phase difference ϕd, and fringe order kl; (d) one cross section of wrapped phase ϕs, unwrapped phase Φl, and fringe order ks; (e) one cross section of the restored object’s height; (f) one cross section of the restored height error.
    Trend chart of measurement accuracy with the high frequency of 1/30 and changing low frequency.
    Fig. 4. Trend chart of measurement accuracy with the high frequency of 1/30 and changing low frequency.
    Reconstruction phase error of reference plane (a) by the conventional dual-frequency method and (b)–(f) by the proposed dual-frequency method with different low frequencies (fh = 1/45, and fl = 1/50, 1/70, 1/90, 1/120, 1/140).
    Fig. 5. Reconstruction phase error of reference plane (a) by the conventional dual-frequency method and (b)–(f) by the proposed dual-frequency method with different low frequencies (fh = 1/45, and fl = 1/50, 1/70, 1/90, 1/120, 1/140).
    Experimental results of measuring a simple object: (a), (b) one of the captured fringe patterns of fh and fl (Th = 80 pixels, Tl = 85 pixels); (c), (d) wrapped phases ϕh and ϕl; (e) phase difference (Td = 1360 pixels); (f) wrapped phase sum (Ts = 41.2 pixels); (g) fringe order kl; (h) unwrapped phase Φl; (i) fringe order ks; (j) unwrapped phase sum Φs.
    Fig. 6. Experimental results of measuring a simple object: (a), (b) one of the captured fringe patterns of fh and fl (Th = 80 pixels, Tl = 85 pixels); (c), (d) wrapped phases ϕh and ϕl; (e) phase difference (Td = 1360 pixels); (f) wrapped phase sum (Ts = 41.2 pixels); (g) fringe order kl; (h) unwrapped phase Φl; (i) fringe order ks; (j) unwrapped phase sum Φs.
    Reconstruction of the object’s absolute phase (a) by the conventional dual-frequency method and (b)–(f) by the proposed dual-frequency method with different low frequencies (fh = 1/45, and fl = 1/50, 1/70, 1/90, 1/120, 1/140).
    Fig. 7. Reconstruction of the object’s absolute phase (a) by the conventional dual-frequency method and (b)–(f) by the proposed dual-frequency method with different low frequencies (fh = 1/45, and fl = 1/50, 1/70, 1/90, 1/120, 1/140).
    Reconstruction phase errors with different low frequencies corresponding to Fig. 7.
    Fig. 8. Reconstruction phase errors with different low frequencies corresponding to Fig. 7.
    Trend chart of measurement accuracy of actual experiments with a fixed high frequency and various low frequencies in measuring (a) the foam heart and (b) the petal.
    Fig. 9. Trend chart of measurement accuracy of actual experiments with a fixed high frequency and various low frequencies in measuring (a) the foam heart and (b) the petal.
    Zixiao Miao, Qican Zhang. Dual-frequency fringe for improving measurement accuracy of three-dimensional shape measurement[J]. Chinese Optics Letters, 2021, 19(10): 102601
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