Gas injection device
11002663 · 2021-05-11
Assignee
Inventors
Cpc classification
G01N21/01
PHYSICS
G01N15/0806
PHYSICS
G01N15/088
PHYSICS
International classification
Abstract
A gas injection device, wherein comprising: a gas channel including an air inlet provided at a upper portion therein and a gas outlet provided at a lower portion therein; and a light channel including an incident light channel and a reflected light channel provided at each side of the gas channel separately, wherein gases arrives at a surface of a sample to be tested via said gas channel and flows out from a slit between said light channel, the gas outlet of gas channel, and the surface of the sample to be tested, and gases flow in a manner of laminar flow with the Peclet number of an air flow being larger than 1. The gas injection device can effectively prevent air from returning back to the measurement system.
Claims
1. A gas injection device, wherein comprising: a gas channel including an air inlet provided at an upper portion therein and a gas outlet provided at a lower portion therein; and a light channel including an incident light channel and a reflected light channel provided at each side of the gas channel separately, wherein gases arrives at a surface of a sample to be tested via said gas channel and flows out from said light channel and a slit between the gas outlet of said gas channel and a surface of the sample to be tested, and gases flow in a manner of laminar flow with the Peclet number of an air flow being larger than 1.
2. The gas injection device according to claim 1 wherein, an inner diameter of the gas outlet of the gas channel, an inner diameter of said light channel, and a height from said gas channel to the surface of said sample to be tested meet the next formula:
Fd/π(d.sup.2/2+Dh)μ<200, wherein, F is a volume of gas flow; d is an inner diameter of the light channel; D is an inner diameter of the gas outlet of the gas channel, h is a height from the gas outlet of said gas channel to the surface of said sample to be tested, and μ is dynamic viscosity.
3. The gas injection device according to claim 1 wherein, an inner diameter of said gas outlet is greater than that of said air inlet.
4. The gas injection device according to claim 1 wherein, an inner diameter for the gas outlet of said gas channel is 0.1-250 mm.
5. The gas injection device according to claim 1 wherein, an inner diameter of said light channel is 0.5-20 mm.
6. The gas injection device according to claim 1, wherein, a height from the gas outlet of said gas channel to the surface of said sample to be tested is 0.1-10 mm.
7. The gas injection device according to claim 1, wherein, a length of said gas channel is 0.1-10 cm.
8. The gas injection device according to claim 1, wherein, an inner diameter for the air inlet of said air channel is 0.1-20 mm.
9. The gas injection device according to claim 1 wherein, a diameter for the surface where the gas outlet of the gas channel being formed is 1-300 mm.
Description
BRIEF DESCRIPTION OF THE SEVERAL VIEWS OF THE DRAWINGS
(1)
(2)
(3)
DETAILED DESCRIPTION
(4) In order to make the intention, technical solutions and advantages of the present invention more explicit, a clear and complete description of the technical solutions in embodiments of the present invention will be made on the basis of embodiment drawings of the present invention. It should be understood that preferred embodiments described here is used only to explain the present invention, not to limit the present invention. Described embodiments are only a portion but not all embodiments of the present invention. All other embodiments without inventive work obtained by the people skilled in the art on basis of the embodiment of present invention will fall in the protection scope thereof.
(5)
(6) Specific parameters of the light channel and the gas channel are set to ensure that solvent vapor can flow in a manner of laminar flow in the process of testing.
(7) First, we need to define the airflow and calculate the flow rate. The flow rate can be obtained via V=F/S. Wherein, V is the flow rate, F is the air flow volume. Assuming that the sum of the cross-sectional area S1 of the light channel 12 and the side surface area S2 of the slit 14 which is between the gas outlet 112 of the gas channel 11 and the surface 13 of the sample to be tested is taken as the airflow cross-sectional area S,
i.e. S=S.sub.1+S.sub.2,
wherein, the cross-sectional area 51 of the light channel 12 is the sum of the cross-sectional area of the incident light channel 121 and that of the reflected light channel 122. Further assuming that both the cross-sections of the incident light channel 121 and that of the reflected light channel 122 are circles, and diameters of them are d, then
S.sub.1=πd.sup.2/2,
(8) assuming that the side superficial area S2 of the slit 14 from gas outlet 112 of gas channel 11 to surface of the sample to be tested 13 is the superficial area of a cylindrical and that the diameter of the gas outlet 112 is D, the height of the slit 14 is h, then
S.sub.2=πDh,
(9) so we can obtain the cross-sectional area of the air flow as S=πd.sup.2/2+πDh.
(10) Next, we need to calculate Reynolds number R, which is the basis for discriminating flow characteristics,
R=Vd/μ,
(11) wherein, μ is dynamic viscosity. If the used gas is air, then μ=2.2×10.sup.−5 m.sup.2/s.
(12) In the present invention, the gas flows in a manner of laminar flow when Reynolds number is less than 200. In that case, the inner diameter D of the gas outlet 112 of the gas channel 11, the inner diameter d of the light channel 12, and the height h of the slit 14 i.e. the height from gas outlet 112 of gas channel 11 to a surface of the sample to be tested 13 meet the relational expression below, so that the gas can flow in a manner of laminar flow:
Fd/π(d.sup.2/2+Dh)μ<200,
(13) wherein F is gas flow, d is the inner diameter of the light channel, D is the inner diameter of the gas outlet of the gas channel, h is the height from the gas outlet of said gas channel to the surface of the sample to be tested, μ is dynamic viscosity.
(14) Preferably, the inner diameter of the gas outlet 112 is 0.1-250 mm and that of the light channel 12 is 0.5-20 mm. Preferably, the height from the gas outlet 112 of the gas channel 11 to the surface of the sample to be tested 13 is 0.1-10 mm. The length of the inner diameter of the air inlet 111 of the gas channel is 0.1-20 mm. Preferably, the diameter of the cross-sectional area in the gas injection device where air channel outlet being formed is 1-300 mm.
(15) In a more specific embodiment, the inner diameter d of the light channel 12 of the gas injection device is 3 mm, the inner diameter D of gas outlet 112 of gas channel 11 is 5 mm and the height h of a slit 14 between gas outlet 112 and the surface of sample to be tested 13 is 0.4 mm. Assuming that the range of change of air flow is 2-20 L/h, then the airflow cross-sectional area based upon the formula above can be obtained as S=0.2 cm.sup.2. When the gas flow is 2 L/h, the flow rate V is 2.8 cm/s, and when the gas flow is 20 L/h, the flow rate V is 28 cm/s. When the gas flow is 2 L/h, R is 6.4, and when the gas flow is 20 L/h, R is 64. It means that the airflow in the gas injection device with the parameters listed above flows in a manner of laminar flow.
(16) In addition, it is necessary for the gas channel 11 to be designed with a sufficient length so as to prevent atmosphere air from returning back to the measurement area. We may use Peclet number Pe to estimate the diffusion and convection of the airflow in the gas injection device of present invention. In the present invention, Pe may be described as Pe=VL/D.sub.a, wherein, V denotes flow rate, L denotes length of the gas channel 11, D.sub.a denotes diffusion coefficient of the air in Argon, which approximates as 0.2 cm.sup.2/s. When Pe is less than 1, diffusion dominates; and when Pe is larger than 1, the impact of diffusion can be ignored.
(17) Therefore, in this embodiment the gas channel 11 is designed with a sufficient length so as to prevent atmosphere air from returning back to the measurement area. Further preferably, the length L of the gas channel is 0.1-10 cm. Therefore, when the air flow is 2 L/h, Peclet number Pe is 10.5; when the air flow is 20 L/h, Pe is 105. When Pe is greater than 10, the impact of diffusion may be ignored. It shows that gas injection device disclosed in the present invention can effectively prevent backflow of air, in particular when the flow rate is quite low.
(18) It should be noted that structure of the gas injection device shown in
(19) In addition, in the above-described embodiments, the circle shape is taken as an example to calculate the cross-sectional area of the light channel. However, the light channel is not limited to the circular shape. For example, the light channel can be of any shape, such as an ellipse or a rectangle. Size of the inner diameter of incident light channel and reflected light channel can also be different. In addition, the light path may also be non-cylindrical, i.e., the apertures of light incident and exiting through the light path may vary in size. The angle to set light channel and gas channel may be adjusted according to the actual situation.
(20) The above is only a specific embodiment of the present invention, but the scope of the present invention is not limited thereto, and any person skilled in the art can easily think of changes or substitutions within the technical scope of the present invention, all of which should be covered by the scope of the present invention.