Etalon effect suppression method and device for detection of residual oxygen in glass medicine bottles
A technology for suppressing devices and residual oxygen, which is applied in measuring devices, transmittance measurement, instruments, etc., can solve the problems of low detection accuracy of residual oxygen, improve the detection accuracy of oxygen concentration and the stability of the system, and suppress the etalon effect of effect
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Embodiment 1
[0050] refer to figure 1 The etalon effect suppression method for the detection of residual oxygen in glass vials provided by Embodiment 1 of the present invention includes:
[0051] Step S101, obtaining the main transmitted light intensity after the laser penetrates the glass medicine bottle and the transmitted light intensity after two reflections, and converting them into a first current signal;
[0052] Step S102, acquiring the transmitted light intensity after one reflection and the transmitted light intensity after three reflections when the laser penetrates the glass medicine bottle, and converting them into a second current signal;
[0053] Step S103, obtaining an output current according to the first current signal and the second current signal;
[0054] Step S104, extracting the second harmonic current signal of the output current;
[0055] Step S105, obtaining the oxygen concentration according to the second harmonic current signal.
[0056]The etalon effect supp...
Embodiment 2
[0058] refer to figure 2 The etalon effect suppression method for the detection of residual oxygen in glass vials provided by Embodiment 2 of the present invention includes:
[0059] Step S201, adjust the incident angle of the laser so that the incident angle satisfies L / λ∈M, where M is a positive integer, where L is the optical path of the laser penetrating the glass vial, λ is the wavelength of the laser, and L=d / cosθ 2 , d is the diameter and length of the glass vial, θ 2 is the angle of refraction.
[0060] Specifically, the schematic diagram of the glass vial etalon effect generation in this embodiment is shown in image 3 . Since by changing the angle θ of the incident light 1 , can change the refraction angle θ 2 , then the optical path L=d / cosθ 2 also changes accordingly, when the incident angle θ 1 Adjust to an appropriate value, and when the central wavelength emitted by the laser is the central wavelength absorbed by oxygen, L / λ is a positive integer M.
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