WO2018068249A1 - Algorithms of resonance wave reflectivity through interface of the transition zone - Google Patents
Algorithms of resonance wave reflectivity through interface of the transition zone Download PDFInfo
- Publication number
- WO2018068249A1 WO2018068249A1 PCT/CN2016/101951 CN2016101951W WO2018068249A1 WO 2018068249 A1 WO2018068249 A1 WO 2018068249A1 CN 2016101951 W CN2016101951 W CN 2016101951W WO 2018068249 A1 WO2018068249 A1 WO 2018068249A1
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- interface
- wave
- angle
- reflectivity
- incident
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- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N21/00—Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
- G01N21/17—Systems in which incident light is modified in accordance with the properties of the material investigated
- G01N21/55—Specular reflectivity
Definitions
- the invention is related to Classics wave theory for calculation the reflectivity of the interface of resonance wave when wave through the interface or the interface of the transition zone.
- the methods of this invention will be widely used that wave spread through the interface in various fields such as light, electromagnetic waves, sound wave, water wave and so on for resonance wave that have both refractive wave energy and reflective wave energy.
- This theory solving the problem method is first to find out the interface area of resonance wave as inner the boundary; second to calculate the ratio of both transmission (refraction) and reflection wave energy, and to calculate the angle of separately wave travel direction; and then third as the inner boundary refractive wave as new incident wave go to refractive area, and reflective wave as new incident wave go to the area of incident wave with initial value to calculate.
- the formulas are derived by ratio of both incident normal component and refractive wavelength for the resonance reflectivity.
- reflection wave energy is begin to emerge when the normal component of incident wavelength through the interface is compressed to the resonance wavelength near three quarters of wavelength of the refraction wave. Following Angle of incidence wave change and the ratio of the wavelength gradually being compressed, it is increase gradually for reflection wave energy.
- the reflection wave energy is half value of incident wave energy when the ratio of the normal component of incident wavelength being compressed to a half wavelength of the refraction wave.
- the incident wave energy could all be reflected when the normal component of incident wavelength is compressed to a quarter wavelength of the refraction wave.
- the angle of incident wave is less than or equal to the angle of resonant reflection critical means ⁇ 0 ⁇ R , or the coefficient of compressibility is m ⁇ m R ,
- the transition zone biggest role is set Mutation interface up soft and smooth, it is slow for wave travelling that the interface of mutation could block and produce to reflected wave energy, and even can eliminate the reflected wave energy, the incident wave go into pure transmission or refraction wave.
- a steep cliff On the other side is a gentle slope, It is easily for the people that go to the top of the mountain by other side of a gentle slope, and it is difficulty to climb the steep cliff.
- the first step to calculate the interface reflectivity and transmission rate as shown in Fig 8. And then we may calculate the transmission rate of the refraction wave energy after the first step. Among various order no reflection wave energy, only the last order have the reflection wave energy.
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- Physics & Mathematics (AREA)
- Health & Medical Sciences (AREA)
- Life Sciences & Earth Sciences (AREA)
- Chemical & Material Sciences (AREA)
- Analytical Chemistry (AREA)
- Biochemistry (AREA)
- General Health & Medical Sciences (AREA)
- General Physics & Mathematics (AREA)
- Immunology (AREA)
- Pathology (AREA)
- Investigating Or Analysing Materials By Optical Means (AREA)
Priority Applications (2)
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PCT/CN2016/101951 WO2018068249A1 (en) | 2016-10-13 | 2016-10-13 | Algorithms of resonance wave reflectivity through interface of the transition zone |
CN201680087961.8A CN109844501A (zh) | 2016-10-13 | 2016-10-13 | 通过过渡区界面共振波反射率计算方法 |
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PCT/CN2016/101951 WO2018068249A1 (en) | 2016-10-13 | 2016-10-13 | Algorithms of resonance wave reflectivity through interface of the transition zone |
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WO2018068249A1 true WO2018068249A1 (en) | 2018-04-19 |
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WO (1) | WO2018068249A1 (zh) |
Cited By (1)
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CN109948266A (zh) * | 2019-03-25 | 2019-06-28 | 杭州电子科技大学 | 基于陈绝缘体-手征介质界面的Kerr极化偏转分析方法 |
Citations (5)
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WO2017041243A1 (en) * | 2015-09-09 | 2017-03-16 | Yonggang Zhang | The calculation method of wave reflective index on interface |
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CN2732203Y (zh) * | 2004-10-11 | 2005-10-12 | 李治军 | 弧轨型多方向多角度体外冲击波碎石超声定位器 |
US9658353B2 (en) * | 2010-06-17 | 2017-05-23 | Westerngeco L.L.C. | Regulating coherent boundary reflections during generation of a modeled wavefield |
CN102175652B (zh) * | 2011-01-28 | 2015-03-04 | 华中科技大学 | 二阶微扰法随机粗糙面透射特性计算方法 |
CN102230986B (zh) * | 2011-05-20 | 2013-10-09 | 北京航空航天大学 | 一种光学相位器件及其应用方法和系统 |
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- 2016-10-13 CN CN201680087961.8A patent/CN109844501A/zh active Pending
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Patent Citations (5)
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CN102183435A (zh) * | 2011-01-25 | 2011-09-14 | 中国船舶重工集团公司第七一五研究所 | 一种基于多路径反射理论的海底密度和声速测量方法 |
CN102353515A (zh) * | 2011-06-22 | 2012-02-15 | 中国海洋大学 | 一种浅海非线性内波声学监测方法及系统 |
CN104880426A (zh) * | 2015-05-21 | 2015-09-02 | 江苏大学 | 液体光谱透过率的测量方法 |
CN105241843A (zh) * | 2015-09-02 | 2016-01-13 | 大连天岛海洋科技有限公司 | 一种波导界面反射波临界角的近似计算方法 |
WO2017041243A1 (en) * | 2015-09-09 | 2017-03-16 | Yonggang Zhang | The calculation method of wave reflective index on interface |
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Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN109948266A (zh) * | 2019-03-25 | 2019-06-28 | 杭州电子科技大学 | 基于陈绝缘体-手征介质界面的Kerr极化偏转分析方法 |
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