CN116026470A - Sea surface temperature measuring method - Google Patents

Sea surface temperature measuring method Download PDF

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CN116026470A
CN116026470A CN202310141384.8A CN202310141384A CN116026470A CN 116026470 A CN116026470 A CN 116026470A CN 202310141384 A CN202310141384 A CN 202310141384A CN 116026470 A CN116026470 A CN 116026470A
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CN116026470B (en
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田斌
察豪
崔萌达
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Naval University of Engineering PLA
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Abstract

本发明提供一种海表面温度测量方法,属于测量技术领域,包括计算得到海面平均辐射率和海水反射的辐射亮度;根据海面平均辐射率和海水反射的辐射亮度,得到传感器轴线方向的等效天空温度和等效海水辐射率;根据史蒂芬‑玻尔兹曼定律,获得真实海温。该海表面温度测量方法能够准确计算海表温度,通过红外传感器测量温度,并计算天空温度和海水辐射率,对测量温度进行修正,得到海表的真实温度,使最终测量的结果具有更高的准确度,通过底部的调节机构能够根据船体的晃动情况对减震效果进行相应调整,达到最优的测量状态。

Figure 202310141384

The invention provides a method for measuring sea surface temperature, which belongs to the field of measurement technology, including calculating the average sea surface emissivity and seawater reflected radiance; according to the sea surface average emissivity and seawater reflected radiance, obtaining the equivalent sky in the sensor axis direction Temperature and equivalent seawater emissivity; according to Stefan‑Boltzmann's law, the true sea temperature is obtained. The sea surface temperature measurement method can accurately calculate the sea surface temperature, measure the temperature through an infrared sensor, calculate the sky temperature and seawater emissivity, and correct the measured temperature to obtain the real temperature of the sea surface, so that the final measurement result has a higher accuracy Accuracy, through the adjustment mechanism at the bottom, the shock absorption effect can be adjusted according to the shaking of the hull to achieve the optimal measurement state.

Figure 202310141384

Description

一种海表面温度测量方法A method for measuring sea surface temperature

技术领域Technical Field

本发明涉及测量技术领域,具体为一种海表面温度测量方法。The invention relates to the field of measurement technology, and in particular to a method for measuring sea surface temperature.

背景技术Background Art

船载蒸发波导监测设备将采集的海上风速、气温、湿度、气压及海表面温度等参数输入到波导模型中计算得到蒸发波导特征量数据,其中,涉及到的海表温度与海水温度不同,需要测量海水与空气接触部分的水温。因蒸发作用和热交换作用的存在,海表温度与海水温度存在一定区别。与其他接触式温度传感器相比,利用红外传感器测量海水温度具有一定优势。但因海表面的红外辐射率小于1,加上天空背景的干扰,红外传感器的测量温度与真实的海温之间存在偏差,会使测量温度低于真实温度,另一方面,现有技术中,通过传感器对海表面温度测量进行测量时,通过减震设备对传感器进行安装后,大风天气导致船体大幅度晃动会影响最终测量结果的精准性,对于减震效果和安装牢固性之间无法自由进行调控。The ship-borne evaporation waveguide monitoring equipment inputs the collected parameters such as offshore wind speed, air temperature, humidity, air pressure and sea surface temperature into the waveguide model to calculate the evaporation waveguide characteristic data. Among them, the sea surface temperature involved is different from the seawater temperature, and it is necessary to measure the water temperature of the part where the seawater contacts the air. Due to the existence of evaporation and heat exchange, there is a certain difference between the sea surface temperature and the seawater temperature. Compared with other contact temperature sensors, the use of infrared sensors to measure seawater temperature has certain advantages. However, because the infrared emissivity of the sea surface is less than 1, coupled with the interference of the sky background, there is a deviation between the measured temperature of the infrared sensor and the actual sea temperature, which will make the measured temperature lower than the actual temperature. On the other hand, in the prior art, when the sea surface temperature is measured by the sensor, after the sensor is installed by the shock absorbing device, the strong wind weather causes the hull to shake significantly, which will affect the accuracy of the final measurement result, and the shock absorption effect and installation firmness cannot be freely adjusted.

发明内容Summary of the invention

针对现有技术存在的不足,本发明目的是提供一种海表面温度测量方法,以解决上述背景技术中提出的问题,本发明可以修正外部干扰,能够准确计算海表面真实温度,能够自由控制减震性能与安装牢固程度之间的关系。In view of the shortcomings of the prior art, the purpose of the present invention is to provide a sea surface temperature measurement method to solve the problems raised in the above-mentioned background technology. The present invention can correct external interference, accurately calculate the true temperature of the sea surface, and freely control the relationship between the shock absorption performance and the installation firmness.

为了实现上述目的,本发明是通过如下的技术方案来实现:一种海表面温度测量方法,包括:In order to achieve the above object, the present invention is implemented through the following technical solutions: a method for measuring sea surface temperature, comprising:

以舰船的舰艏方向为y轴建立空间直角坐标系,获得所述舰船纵摇角度、横摇角度;A spatial rectangular coordinate system is established with the bow direction of the ship as the y-axis to obtain the pitch angle and roll angle of the ship;

获取海上一定高度处的风速以及天空温度,计算得到天空辐射亮度;Obtain the wind speed and sky temperature at a certain height above the sea, and calculate the sky radiation brightness;

将红外传感器组件安装在托架上,并根据红外传感器设置的位置,获得所述红外传感器的安装角、测量倾角以及空间角,其中托架的底部设置有安装杆,且托架通过该安装杆固定在减震器机构的顶部,所述减震器的底端设置有支撑管,所述支撑管的底部连接有调节机构,所述调节机构通过底部的立柱固定在船体上;The infrared sensor assembly is mounted on a bracket, and the mounting angle, the measured inclination angle and the spatial angle of the infrared sensor are obtained according to the position where the infrared sensor is mounted, wherein a mounting rod is arranged at the bottom of the bracket, and the bracket is fixed to the top of the shock absorber mechanism through the mounting rod, and a support tube is arranged at the bottom end of the shock absorber, and an adjustment mechanism is connected to the bottom of the support tube, and the adjustment mechanism is fixed to the hull through a column at the bottom;

根据所述舰船纵摇角度、横摇角度、所述红外传感器的安装角和测量倾角,获得所述红外传感器在辐射方向与Z轴正方向夹角以及所述红外传感器在辐射方向在所述空间直角坐标系中XOY平面的投影与X轴正方向的夹角,所述减震器机构的中心设置有中心杆,所述调节机构配合中心杆对减震器机构的内部进行调控;According to the pitch angle, roll angle, installation angle and measurement inclination angle of the ship, the infrared sensor is installed at an angle of the infrared sensor in the radiation direction and the positive direction of the Z axis, and the infrared sensor is projected in the radiation direction on the XOY plane in the spatial rectangular coordinate system and the positive direction of the X axis. A center rod is provided at the center of the shock absorber mechanism, and the adjustment mechanism cooperates with the center rod to regulate the interior of the shock absorber mechanism;

根据所述海上一定高度处的风速、所述红外传感器在辐射方向与Z轴正方向夹角以及所述红外传感器在辐射方向在所述空间直角坐标系中XOY平面的投影与X轴正方向的夹角,计算得到海面平均辐射率和海水反射的辐射亮度;The average emissivity of the sea surface and the radiation brightness reflected by the sea water are calculated according to the wind speed at a certain height at sea, the angle between the radiation direction of the infrared sensor and the positive direction of the Z axis, and the angle between the projection of the infrared sensor in the radiation direction on the XOY plane in the spatial rectangular coordinate system and the positive direction of the X axis;

根据所述海面平均辐射率和海水反射的辐射亮度,得到传感器轴线方向的等效天空温度和等效海水辐射率;According to the average emissivity of the sea surface and the radiant brightness reflected by the sea water, an equivalent sky temperature and an equivalent sea water emissivity in the direction of the sensor axis are obtained;

根据史蒂芬-玻尔兹曼定律,获得真实海温。According to the Stefan-Boltzmann law, the true sea temperature is obtained.

进一步的,获取海上一定高度上的风速以及天空温度的方法为经验法或测量法。Furthermore, the method for obtaining the wind speed and sky temperature at a certain height above the sea is an empirical method or a measurement method.

进一步的,计算得到天空辐射亮度包括:Furthermore, the sky radiation brightness is calculated including:

根据时间和所述红外传感器的经纬度,得到太阳的辐射方向;Obtaining the solar radiation direction according to the time and the longitude and latitude of the infrared sensor;

当太阳入射方向为

Figure BDA0004087589810000031
时,天空辐射亮度
Figure BDA0004087589810000032
为:When the sun's incident direction is
Figure BDA0004087589810000031
When
Figure BDA0004087589810000032
for:

Figure BDA0004087589810000033
Figure BDA0004087589810000033

其中,Tsky为天空温度;

Figure BDA0004087589810000034
为太阳入射方向为
Figure BDA0004087589810000035
时太阳辐射亮度;θi为太阳入射方向
Figure BDA0004087589810000036
与Z轴正方向夹角;
Figure BDA0004087589810000037
为太阳入射方向在所述空间直角坐标系中XOY平面的投影与X轴正方向的夹角。Wherein, T sky is the sky temperature;
Figure BDA0004087589810000034
The direction of the sun's incidence is
Figure BDA0004087589810000035
The solar radiation brightness at this time; θ i is the incident direction of the sun
Figure BDA0004087589810000036
Angle with the positive direction of Z axis;
Figure BDA0004087589810000037
It is the angle between the projection of the sun's incident direction on the XOY plane in the spatial rectangular coordinate system and the positive direction of the X-axis.

进一步的,根据所述舰船纵摇角度、横摇角度、所述红外传感器的安装角和测量倾角,获得所述红外传感器在辐射方向与Z轴正方向夹角以及所述红外传感器在辐射方向在所述空间直角坐标系中XOY平面的投影与X轴正方向的夹角的计算公式为:Furthermore, according to the pitch angle, roll angle, installation angle and measurement inclination angle of the ship, the calculation formulas for obtaining the angle between the infrared sensor in the radiation direction and the positive direction of the Z axis and the angle between the projection of the infrared sensor in the radiation direction on the XOY plane in the spatial rectangular coordinate system and the positive direction of the X axis are:

Figure BDA0004087589810000038
Figure BDA0004087589810000038

Figure BDA0004087589810000039
Figure BDA0004087589810000039

Figure BDA00040875898100000310
Figure BDA00040875898100000310

其中,θs为测量倾角;

Figure BDA00040875898100000311
为安装角;α1为纵摇角度;α2为横摇角度;θ0为红外传感器在辐射方向与Z轴正方向夹角;
Figure BDA00040875898100000312
为红外传感器在辐射方向在空间直角坐标系中XOY平面的投影与X轴正方向的夹角。Where, θs is the measured inclination angle;
Figure BDA00040875898100000311
is the installation angle; α1 is the pitch angle; α2 is the roll angle; θ0 is the angle between the infrared sensor in the radiation direction and the positive direction of the Z axis;
Figure BDA00040875898100000312
It is the angle between the projection of the infrared sensor in the radiation direction on the XOY plane in the spatial rectangular coordinate system and the positive direction of the X axis.

进一步的,计算得到海面平均辐射率为:Furthermore, the average emissivity of the sea surface is calculated as:

根据Charles Cox及Walter Munk提出的海浪坡度的分布概率为:According to Charles Cox and Walter Munk, the distribution probability of wave slope is:

Figure BDA0004087589810000041
Figure BDA0004087589810000041

其中,sx为X轴方向海浪的坡度分量;sy为Y轴方向海浪的坡度分量;v为海上一定高度处的风速;σ表示史蒂芬-玻尔兹曼常数;Where sx is the slope component of the wave in the X-axis direction; sy is the slope component of the wave in the Y-axis direction; v is the wind speed at a certain height on the sea; σ represents the Stefan-Boltzmann constant;

假设红外传感器辐射方向为

Figure BDA0004087589810000042
海浪的坡度上面元法线方向为
Figure BDA0004087589810000043
则:Assume that the infrared sensor radiation direction is
Figure BDA0004087589810000042
The direction of the normal line of the surface element of the wave slope is
Figure BDA0004087589810000043
but:

Figure BDA0004087589810000044
Figure BDA0004087589810000044

Figure BDA0004087589810000045
Figure BDA0004087589810000045

Figure BDA0004087589810000046
Figure BDA0004087589810000046

其中,x为

Figure BDA0004087589810000047
Figure BDA0004087589810000048
的夹角;θn
Figure BDA0004087589810000049
与Z轴正方向夹角;
Figure BDA00040875898100000410
Figure BDA00040875898100000411
在空间直角坐标系中XOY平面的投影与X轴正方向的夹角;Among them, x is
Figure BDA0004087589810000047
and
Figure BDA0004087589810000048
The angle between
Figure BDA0004087589810000049
Angle with the positive direction of Z axis;
Figure BDA00040875898100000410
for
Figure BDA00040875898100000411
The angle between the projection of the XOY plane and the positive direction of the X axis in the spatial rectangular coordinate system;

则海浪坡度的分布概率为:Then the distribution probability of wave slope is:

Figure BDA00040875898100000412
Figure BDA00040875898100000412

其中,un等于cosθn

Figure BDA00040875898100000413
等于cosθn;Where, u n is equal to cosθ n ;
Figure BDA00040875898100000413
is equal to cosθ n ;

且太阳入射方向

Figure BDA00040875898100000414
与红外传感器在辐射方向为
Figure BDA00040875898100000415
和海浪的坡度上面元法线方向为
Figure BDA00040875898100000416
的关系式为:And the direction of the sun
Figure BDA00040875898100000414
The radiation direction of the infrared sensor is
Figure BDA00040875898100000415
The direction of the normal line of the surface element of the wave slope is
Figure BDA00040875898100000416
The relationship is:

Figure BDA0004087589810000051
Figure BDA0004087589810000051

Figure BDA0004087589810000052
Figure BDA0004087589810000052

则所述海面平均辐射率为:Then the average emissivity of the sea surface is:

Figure BDA0004087589810000053
Figure BDA0004087589810000053

其中,ελ(x)=0.98[1-(1-cosθ0)5],且为海面红外辐射率。Wherein, ε λ (x) = 0.98[1-(1-cosθ 0 ) 5 ], and is the infrared emissivity of the sea surface.

进一步的,计算得到所述海水反射的辐射亮度为:Furthermore, the radiation brightness reflected by the seawater is calculated as:

根据基尔霍夫定律可知,海水的辐射率和反射率相加为1,可知海水反射的辐射亮度为:According to Kirchhoff's law, the sum of the emissivity and reflectivity of seawater is 1, so the radiation brightness reflected by seawater is:

Figure BDA0004087589810000054
Figure BDA0004087589810000054

其中,ρλ为海水反射率。Where ρ λ is the reflectivity of seawater.

进一步的,传感器轴线方向的等效天空温度和等效海水辐射率的公式为:Furthermore, the formulas for the equivalent sky temperature and equivalent seawater emissivity in the sensor axis direction are:

Figure BDA0004087589810000055
Figure BDA0004087589810000055

Figure BDA0004087589810000056
Figure BDA0004087589810000056

其中,α为所述红外传感器的测量半角;Ω为所述红外传感器的空间角;β为在所述空间角为dΩ,所述红外传感器辐射方向

Figure BDA0004087589810000061
与所述红外传感器轴线间的夹角;γ为所述红外传感器辐射方向
Figure BDA0004087589810000062
对应的方位角。Wherein, α is the measurement half angle of the infrared sensor; Ω is the spatial angle of the infrared sensor; β is the radiation direction of the infrared sensor when the spatial angle is dΩ.
Figure BDA0004087589810000061
The angle between the infrared sensor axis and the infrared sensor axis; γ is the radiation direction of the infrared sensor
Figure BDA0004087589810000062
The corresponding azimuth.

进一步的,根据史蒂芬-玻尔兹曼定律,获得真实海温的公式为:Furthermore, according to the Stefan-Boltzmann law, the formula for obtaining the true sea temperature is:

Figure BDA0004087589810000063
Figure BDA0004087589810000063

其中,Tm为所述红外传感器测量温度。Wherein, Tm is the temperature measured by the infrared sensor.

进一步的,所述减震器机构包括密封套筒和弹簧,所述密封套筒的底部安装有顶板,所述弹簧的底端与顶板的表面固定连接,所述顶板的表面贴装有贴合层,所述顶板的中间设置有第一插接套筒,所述中心杆从第一插接套筒的内部穿入到支撑管的内部。Furthermore, the shock absorber mechanism includes a sealing sleeve and a spring, a top plate is installed at the bottom of the sealing sleeve, the bottom end of the spring is fixedly connected to the surface of the top plate, a bonding layer is attached to the surface of the top plate, a first plug-in sleeve is arranged in the middle of the top plate, and the center rod is inserted into the interior of the support tube from the inside of the first plug-in sleeve.

进一步的,所述调节机构包括液压杆和升降通道,中心杆的底端安装有液压杆,所述液压杆的底部设置有增压板,所述升降通道的内部安装有对接板,所述对接板的表面开设有第二插接套筒和定位孔,所述增压板的表面设置有耐磨板,所述耐磨板的顶部安装有定位柱,所述定位柱从定位孔的内部穿过。Furthermore, the adjustment mechanism includes a hydraulic rod and a lifting channel, the hydraulic rod is installed at the bottom end of the center rod, a boosting plate is provided at the bottom of the hydraulic rod, a docking plate is installed inside the lifting channel, a second plug-in sleeve and a positioning hole are provided on the surface of the docking plate, a wear-resistant plate is provided on the surface of the boosting plate, a positioning column is installed on the top of the wear-resistant plate, and the positioning column passes through the inside of the positioning hole.

本发明的有益效果:Beneficial effects of the present invention:

1.该海表面温度测量方法能够准确计算海表温度,通过红外传感器测量温度,并计算天空温度和海水辐射率,对测量温度进行修正,得到海表的真实温度。1. This sea surface temperature measurement method can accurately calculate the sea surface temperature. It measures the temperature through an infrared sensor, calculates the sky temperature and the sea water emissivity, corrects the measured temperature, and obtains the true temperature of the sea surface.

2.该海表面温度测量方法通过底部的调节机构能够将顶部的减震器机构内部的弹簧压缩状态进行调节,因此能够根据船体具体的运行环境对减震器的减震性能进行调控,进而改变顶部红外传感器组件的安装稳定状态,以便于根据船体的晃动情况对减震效果进行相应调整,达到最优的测量状态。2. The sea surface temperature measurement method can adjust the spring compression state inside the top shock absorber mechanism through the adjustment mechanism at the bottom, so that the shock absorption performance of the shock absorber can be adjusted according to the specific operating environment of the hull, thereby changing the installation stability state of the top infrared sensor assembly, so as to adjust the shock absorption effect accordingly according to the shaking of the hull to achieve the optimal measurement state.

附图说明BRIEF DESCRIPTION OF THE DRAWINGS

图1为本发明中海表面温度测量方法的流程框架图;FIG1 is a flow chart of a method for measuring sea surface temperature in the present invention;

图2为本发明中不同倾斜调节下的海表面温度的测量结果;FIG2 is a measurement result of the sea surface temperature under different tilt adjustments in the present invention;

图3为本发明中仿真结果图;FIG3 is a diagram of simulation results in the present invention;

图4为本发明中经验法补偿误差的概率分布图;FIG4 is a probability distribution diagram of the error compensation by the empirical method in the present invention;

图5为本发明红外传感器组件安装结构部分的示意图;FIG5 is a schematic diagram of the mounting structure of the infrared sensor assembly of the present invention;

图6为本发明安装结构中减震器机构部分的示意图;FIG6 is a schematic diagram of the shock absorber mechanism portion of the mounting structure of the present invention;

图7为本发明安装结构中调节机构部分的示意图;FIG7 is a schematic diagram of the adjustment mechanism part of the installation structure of the present invention;

图中:1、红外传感器组件;2、托架;3、安装杆;4、减震器机构;5、支撑管;6、调节机构;7、立柱;8、密封套筒;9、中心杆;10、弹簧;11、顶板;12、贴合层;13、第一插接套筒;14、液压杆;15、增压板;16、耐磨板;17、定位柱;18、升降通道;19、对接板;20、第二插接套筒;21、定位孔。In the figure: 1. infrared sensor assembly; 2. bracket; 3. mounting rod; 4. shock absorber mechanism; 5. support tube; 6. adjustment mechanism; 7. column; 8. sealing sleeve; 9. center rod; 10. spring; 11. top plate; 12. bonding layer; 13. first plug-in sleeve; 14. hydraulic rod; 15. booster plate; 16. wear-resistant plate; 17. positioning column; 18. lifting channel; 19. docking plate; 20. second plug-in sleeve; 21. positioning hole.

具体实施方式DETAILED DESCRIPTION

为使本发明实现的技术手段、创作特征、达成目的与功效易于明白了解,下面结合具体实施方式,进一步阐述本发明。In order to make the technical means, creative features, objectives and effects achieved by the present invention easy to understand, the present invention is further explained below in conjunction with specific implementation methods.

请参阅图1至图7,本发明提供一种技术方案:一种海表面温度测量方法包括:Referring to FIG. 1 to FIG. 7 , the present invention provides a technical solution: a method for measuring sea surface temperature comprises:

对红外传感器组件1进行安装,具体的,将红外传感器组件1安装在托架2上,并根据红外传感器设置的位置,获得红外传感器的安装角、测量倾角以及空间角,其中托架2的底部设置有安装杆3,且托架2通过该安装杆3固定在减震器机构4的顶部,减震器的底端设置有支撑管5,支撑管5的底部连接有调节机构6,调节机构6通过底部的立柱7固定在船体上,通过中心杆9和第一插接套筒13相配合即可限制顶部的红外传感器组件1进能够进行垂直方向上的运动,并通过多组弹簧10连接即可提供稳定的缓冲减震效果。The infrared sensor assembly 1 is installed. Specifically, the infrared sensor assembly 1 is installed on the bracket 2, and the installation angle, measurement inclination angle and spatial angle of the infrared sensor are obtained according to the setting position of the infrared sensor, wherein a mounting rod 3 is provided at the bottom of the bracket 2, and the bracket 2 is fixed to the top of the shock absorber mechanism 4 through the mounting rod 3, and a support tube 5 is provided at the bottom end of the shock absorber, and an adjustment mechanism 6 is connected to the bottom of the support tube 5, and the adjustment mechanism 6 is fixed to the hull through the bottom column 7, and the top infrared sensor assembly 1 can be limited to move in the vertical direction by cooperating with the center rod 9 and the first plug-in sleeve 13, and a stable buffering and shock-absorbing effect can be provided by connecting through multiple groups of springs 10.

根据舰船纵摇角度、横摇角度、红外传感器的安装角和测量倾角,获得红外传感器在辐射方向与Z轴正方向夹角以及红外传感器在辐射方向在空间直角坐标系中XOY平面的投影与X轴正方向的夹角,减震器机构4的中心设置有中心杆9,调节机构6配合中心杆9对减震器机构4的内部进行调控,通过底部的调节机构6能够将顶部的减震器机构4内部的弹簧10压缩状态进行调节,因此能够根据船体具体的运行环境对减震器的减震性能进行调控,进而改变顶部红外传感器组件1的安装稳定状态,以便于根据船体的晃动情况对减震效果进行相应调整,达到最优的测量状态。According to the pitch angle, roll angle, installation angle and measurement inclination angle of the ship, the angle between the infrared sensor in the radiation direction and the positive direction of the Z axis and the angle between the projection of the infrared sensor in the radiation direction on the XOY plane in the spatial rectangular coordinate system and the positive direction of the X axis are obtained. A center rod 9 is arranged at the center of the shock absorber mechanism 4. The adjustment mechanism 6 cooperates with the center rod 9 to regulate the inside of the shock absorber mechanism 4. The compression state of the spring 10 inside the top shock absorber mechanism 4 can be adjusted through the adjustment mechanism 6 at the bottom. Therefore, the shock absorbing performance of the shock absorber can be regulated according to the specific operating environment of the hull, thereby changing the installation stability state of the top infrared sensor assembly 1, so as to adjust the shock absorbing effect accordingly according to the shaking of the hull to achieve the optimal measurement state.

本实施例,减震器机构4包括密封套筒8和弹簧10,密封套筒8的底部安装有顶板11,弹簧10的底端与顶板11的表面固定连接,顶板11的表面贴装有贴合层12,顶板11的中间设置有第一插接套筒13,中心杆9从第一插接套筒13的内部穿入到支撑管5的内部,调节机构6包括液压杆14和升降通道18,中心杆9的底端安装有液压杆14,液压杆14的底部设置有增压板15,升降通道18的内部安装有对接板19,对接板19的表面开设有第二插接套筒20和定位孔21,增压板15的表面设置有耐磨板16,耐磨板16的顶部安装有定位柱17,定位柱17从定位孔21的内部穿过。In this embodiment, the shock absorber mechanism 4 includes a sealing sleeve 8 and a spring 10, a top plate 11 is installed at the bottom of the sealing sleeve 8, the bottom end of the spring 10 is fixedly connected to the surface of the top plate 11, a bonding layer 12 is mounted on the surface of the top plate 11, a first plug-in sleeve 13 is arranged in the middle of the top plate 11, and the center rod 9 penetrates from the inside of the first plug-in sleeve 13 into the inside of the support tube 5, the adjustment mechanism 6 includes a hydraulic rod 14 and a lifting channel 18, a hydraulic rod 14 is installed at the bottom end of the center rod 9, a boosting plate 15 is arranged at the bottom of the hydraulic rod 14, a docking plate 19 is installed inside the lifting channel 18, a second plug-in sleeve 20 and a positioning hole 21 are opened on the surface of the docking plate 19, a wear-resistant plate 16 is arranged on the surface of the boosting plate 15, a positioning column 17 is installed on the top of the wear-resistant plate 16, and the positioning column 17 passes through the inside of the positioning hole 21.

具体的,通过控制液压杆14拉动底部的增压板15上移后,直至耐磨板16与对接板19的底部相接触,即可拉动顶部的中心杆9以及相应的红外传感器组件1等设备下移,同时将弹簧10压缩,密封套筒8按压到贴合层12上,此时弹簧10产生的缓冲减震效果下降,红外传感器组件1相较于最底部的立柱7部分具有更高的牢固性,该状态下能够在降低外部风浪导致红外传感器组件1晃动的程度,从而通过该结构对红外传感器组件1的稳定状态和减震性能之间取得平衡。Specifically, by controlling the hydraulic rod 14 to pull the bottom booster plate 15 upward until the wear-resistant plate 16 contacts the bottom of the docking plate 19, the top center rod 9 and the corresponding infrared sensor assembly 1 and other equipment can be pulled downward, and the spring 10 is compressed and the sealing sleeve 8 is pressed onto the bonding layer 12. At this time, the buffering and shock-absorbing effect of the spring 10 decreases, and the infrared sensor assembly 1 has a higher firmness than the bottom column 7. In this state, the degree of shaking of the infrared sensor assembly 1 caused by external wind and waves can be reduced, thereby achieving a balance between the stability and shock-absorbing performance of the infrared sensor assembly 1 through this structure.

以舰船的舰艏方向为y轴建立空间直角坐标系,获得舰船纵摇角度、横摇角度;该直角坐标系为右手坐标系;A spatial rectangular coordinate system is established with the bow direction of the ship as the y-axis to obtain the pitch angle and roll angle of the ship; the rectangular coordinate system is a right-handed coordinate system;

获取海上一定高度处的风速以及天空温度,计算得到天空辐射亮度;优选的海上高度为12.5米;Obtain the wind speed and sky temperature at a certain height above the sea, and calculate the sky radiation brightness; the preferred height above the sea is 12.5 meters;

具体地,获取海上一定高度上的风速以及天空温度的方法为经验法或测量法,两种方法可通过仿真对比进行择优选择。且根据时间和红外传感器的经纬度,得到太阳的辐射方向;Specifically, the method of obtaining the wind speed and sky temperature at a certain height at sea is the empirical method or the measurement method, and the two methods can be selected through simulation comparison. And according to the time and the longitude and latitude of the infrared sensor, the radiation direction of the sun is obtained;

当太阳入射方向为

Figure BDA0004087589810000091
时,天空辐射亮度
Figure BDA0004087589810000092
为:When the sun's incident direction is
Figure BDA0004087589810000091
When
Figure BDA0004087589810000092
for:

Figure BDA0004087589810000093
Figure BDA0004087589810000093

其中,Tsky为天空温度;

Figure BDA0004087589810000094
为太阳入射方向为
Figure BDA0004087589810000095
时太阳辐射亮度;θi为太阳入射方向
Figure BDA0004087589810000096
与Z轴正方向夹角;
Figure BDA0004087589810000097
为太阳入射方向在空间直角坐标系中XOY平面的投影与X轴正方向的夹角。Wherein, T sky is the sky temperature;
Figure BDA0004087589810000094
The direction of the sun's incidence is
Figure BDA0004087589810000095
The solar radiation brightness at this time; θ i is the incident direction of the sun
Figure BDA0004087589810000096
Angle with the positive direction of Z axis;
Figure BDA0004087589810000097
It is the angle between the projection of the sun's incident direction on the XOY plane in the spatial rectangular coordinate system and the positive direction of the X-axis.

根据红外传感器设置的位置,获得红外传感器的安装角、测量倾角以及空间角;According to the location where the infrared sensor is set, the installation angle, the measurement inclination angle and the space angle of the infrared sensor are obtained;

根据舰船纵摇角度、横摇角度、红外传感器的安装角和测量倾角,获得红外传感器在辐射方向与Z轴正方向夹角以及红外传感器在辐射方向在空间直角坐标系中XOY平面的投影与X轴正方向的夹角;According to the pitch angle, roll angle, installation angle and measurement inclination angle of the ship, the angle between the infrared sensor in the radiation direction and the positive direction of the Z axis and the angle between the projection of the infrared sensor in the radiation direction on the XOY plane in the spatial rectangular coordinate system and the positive direction of the X axis are obtained;

具体地,获得红外传感器在辐射方向与Z轴正方向夹角以及红外传感器在辐射方向在空间直角坐标系中XOY平面的投影与X轴正方向的夹角的计算公式为:Specifically, the calculation formula for obtaining the angle between the infrared sensor in the radiation direction and the positive direction of the Z axis and the angle between the projection of the infrared sensor in the radiation direction on the XOY plane in the spatial rectangular coordinate system and the positive direction of the X axis is:

Figure BDA0004087589810000101
Figure BDA0004087589810000101

Figure BDA0004087589810000102
Figure BDA0004087589810000102

Figure BDA0004087589810000103
Figure BDA0004087589810000103

其中,θs为测量倾角;

Figure BDA0004087589810000104
为安装角;α1为纵摇角度;α2为横摇角度;θ0为红外传感器在辐射方向与Z轴正方向夹角;
Figure BDA0004087589810000105
为红外传感器在辐射方向在空间直角坐标系中XOY平面的投影与X轴正方向的夹角。Where, θ s is the measured inclination angle;
Figure BDA0004087589810000104
is the installation angle; α1 is the pitch angle; α2 is the roll angle; θ0 is the angle between the infrared sensor in the radiation direction and the positive direction of the Z axis;
Figure BDA0004087589810000105
It is the angle between the projection of the infrared sensor in the radiation direction on the XOY plane in the spatial rectangular coordinate system and the positive direction of the X axis.

本实施例,根据海上一定高度处的风速、红外传感器在辐射方向与Z轴正方向夹角以及红外传感器在辐射方向在空间直角坐标系中XOY平面的投影与X轴正方向的夹角,计算得到海面平均辐射率和海水反射的辐射亮度;In this embodiment, the average emissivity of the sea surface and the radiation brightness reflected by the sea water are calculated according to the wind speed at a certain height at sea, the angle between the infrared sensor in the radiation direction and the positive direction of the Z axis, and the angle between the projection of the infrared sensor in the radiation direction on the XOY plane in the spatial rectangular coordinate system and the positive direction of the X axis;

根据海面平均辐射率和海水反射的辐射亮度,得到传感器轴线方向的等效天空温度和等效海水辐射率;According to the average emissivity of the sea surface and the radiation brightness reflected by the sea water, the equivalent sky temperature and equivalent sea water emissivity in the direction of the sensor axis are obtained;

具体地,计算得到海面平均辐射率为:Specifically, the average emissivity of the sea surface is calculated as:

根据Charles Cox及Walter Munk提出的海浪坡度的分布概率为:According to Charles Cox and Walter Munk, the distribution probability of wave slope is:

Figure BDA0004087589810000111
Figure BDA0004087589810000111

其中,sx为X轴方向海浪的坡度分量;sy为Y轴方向海浪的坡度分量;v为海上一定高度处的风速;σ表示史蒂芬-玻尔兹曼常数;Where sx is the slope component of the wave in the X-axis direction; sy is the slope component of the wave in the Y-axis direction; v is the wind speed at a certain height on the sea; σ represents the Stefan-Boltzmann constant;

假设红外传感器辐射方向为

Figure BDA0004087589810000112
海浪的坡度上面元法线方向为
Figure BDA00040875898100001118
则:Assume that the infrared sensor radiation direction is
Figure BDA0004087589810000112
The direction of the normal line of the surface element of the wave slope is
Figure BDA00040875898100001118
but:

Figure BDA0004087589810000113
Figure BDA0004087589810000113

Figure BDA0004087589810000114
Figure BDA0004087589810000114

Figure BDA0004087589810000115
Figure BDA0004087589810000115

其中,x为

Figure BDA0004087589810000116
Figure BDA0004087589810000117
的夹角;θn
Figure BDA0004087589810000118
与Z轴正方向夹角;
Figure BDA0004087589810000119
Figure BDA00040875898100001110
在空间直角坐标系中XOY平面的投影与X轴正方向的夹角;Among them, x is
Figure BDA0004087589810000116
and
Figure BDA0004087589810000117
The angle between
Figure BDA0004087589810000118
Angle with the positive direction of Z axis;
Figure BDA0004087589810000119
for
Figure BDA00040875898100001110
The angle between the projection of the XOY plane and the positive direction of the X axis in the spatial rectangular coordinate system;

则海浪坡度的分布概率为:Then the distribution probability of wave slope is:

Figure BDA00040875898100001111
Figure BDA00040875898100001111

其中,un等于

Figure BDA00040875898100001112
Figure BDA00040875898100001113
等于cosθn;Among them, u n is equal to
Figure BDA00040875898100001112
Figure BDA00040875898100001113
is equal to cosθ n ;

且太阳入射方向

Figure BDA00040875898100001114
与红外传感器在辐射方向为
Figure BDA00040875898100001115
和海浪的坡度上面元法线方向为
Figure BDA00040875898100001116
的关系式为:And the direction of the sun
Figure BDA00040875898100001114
The radiation direction of the infrared sensor is
Figure BDA00040875898100001115
The direction of the normal line of the surface element of the wave slope is
Figure BDA00040875898100001116
The relationship is:

Figure BDA00040875898100001117
Figure BDA00040875898100001117

Figure BDA0004087589810000121
Figure BDA0004087589810000121

则海面平均辐射率为:The average emissivity of the sea surface is:

Figure BDA0004087589810000122
Figure BDA0004087589810000122

其中,ελ(x)=0.98[1-(1-cosθ0)5],且为海面红外辐射率。Wherein, ε λ (x) = 0.98[1-(1-cosθ 0 ) 5 ], and is the infrared emissivity of the sea surface.

计算得到海水反射的辐射亮度为:The calculated radiation brightness reflected by seawater is:

根据基尔霍夫定律可知,海水的辐射率和反射率相加为1,可知海水反射的辐射亮度为:According to Kirchhoff's law, the sum of the emissivity and reflectivity of seawater is 1, so the radiation brightness reflected by seawater is:

Figure BDA0004087589810000123
Figure BDA0004087589810000123

其中,ρλ为海水反射率。Where ρ λ is the reflectivity of seawater.

优选的是,传感器轴线方向的等效天空温度和等效海水辐射率的公式为:Preferably, the formulas for the equivalent sky temperature and equivalent seawater emissivity in the sensor axis direction are:

Figure BDA0004087589810000124
Figure BDA0004087589810000124

Figure BDA0004087589810000125
Figure BDA0004087589810000125

其中,α为红外传感器的测量半角;Ω为红外传感器的空间角;β为在空间角为dΩ,红外传感器辐射方向

Figure BDA0004087589810000126
与红外传感器轴线间的夹角;γ为红外传感器辐射方向
Figure BDA0004087589810000127
对应的方位角,且dΩ=sinβdβdγ。Among them, α is the measurement half angle of the infrared sensor; Ω is the spatial angle of the infrared sensor; β is the radiation direction of the infrared sensor when the spatial angle is dΩ
Figure BDA0004087589810000126
The angle between the infrared sensor axis and the infrared sensor; γ is the radiation direction of the infrared sensor
Figure BDA0004087589810000127
The corresponding azimuth angle, and dΩ=sinβdβdγ.

根据史蒂芬-玻尔兹曼定律,获得真实海温。According to the Stefan-Boltzmann law, the true sea temperature is obtained.

获得真实海温的公式为:The formula for obtaining the true sea temperature is:

Figure BDA0004087589810000131
Figure BDA0004087589810000131

其中,Tm为红外传感器测量温度。Where Tm is the temperature measured by the infrared sensor.

对本发明的算法进行验证,具体为比较倾斜条件下传感器的测量结果和本发明的计算结果。The algorithm of the present invention is verified by comparing the measurement results of the sensor under tilt conditions with the calculation results of the present invention.

本实施例,实验中使用SI-431红外传感器实现温度的测量,传感器测量精度为0.2℃,测量半角为14°。红外传感器固定在倾角可变可支架上,且支架上的刻度可读取倾斜角的大小。实验时天气为多云,测量到的天空温度为12.2℃,图2给出了不同倾斜条件下的海表温度的测量结果,其中蓝色点线为实际的测量结果,红线为仿真的结果。从结果可以看出,受天空背景的影响,随着倾斜角度的增大,传感器的测量结果逐渐降低,这与本发明算法结果的变化趋势相同。实验误差的主要原因包括以下几个方面:一是水表温度不均匀且存在流动,水温存在一定的变化;二是测量过程中需要人工操作,测量结果可能会受人体红外辐射的影响;三是由实验设备造成的误差。In this embodiment, the SI-431 infrared sensor is used in the experiment to measure the temperature. The sensor has a measurement accuracy of 0.2°C and a measurement half angle of 14°. The infrared sensor is fixed on a bracket with a variable inclination angle, and the scale on the bracket can read the size of the inclination angle. The weather was cloudy during the experiment, and the measured sky temperature was 12.2°C. Figure 2 shows the measurement results of the sea surface temperature under different inclination conditions, where the blue dotted line is the actual measurement result and the red line is the simulation result. It can be seen from the results that, affected by the sky background, as the inclination angle increases, the measurement results of the sensor gradually decrease, which is the same as the change trend of the algorithm results of the present invention. The main reasons for the experimental error include the following aspects: First, the water surface temperature is uneven and there is flow, and the water temperature has certain changes; second, manual operation is required during the measurement process, and the measurement results may be affected by human infrared radiation; third, the error is caused by the experimental equipment.

海面辐射率随辐射方向增大而降低,使传感器测量到的海面辐射亮度降低,同时反射率的增大使天空温度对测量结果的影响增大。为验证在不同风速、舰船横纵摇条件下,天空红外辐射的影响,仿真了测量偏差的概率分布函数。在一定范围内随机选取风速、纵横摇角度、天空温度及海表温度,风速选择范围为0~10m/s,纵横摇角度选择范围为对应浪级下的倾角范围,天空温度选择范围为-40℃~20℃,海表温度选择范围为15℃~30℃。仿真结果如图3所示。The sea surface emissivity decreases as the radiation direction increases, which reduces the sea surface radiation brightness measured by the sensor. At the same time, the increase in reflectivity increases the influence of sky temperature on the measurement results. In order to verify the influence of sky infrared radiation under different wind speeds and ship pitch and roll conditions, the probability distribution function of measurement deviation is simulated. The wind speed, pitch and roll angle, sky temperature and sea surface temperature are randomly selected within a certain range. The wind speed selection range is 0 to 10m/s, the pitch and roll angle selection range is the inclination range under the corresponding wave level, the sky temperature selection range is -40℃ to 20℃, and the sea surface temperature selection range is 15℃ to 30℃. The simulation results are shown in Figure 3.

本实施例,从结果看,若不对海水的辐射率和天空温度的干扰进行修正,测量温度与真实海温间,偏差小于1.5℃的概率小于90%,偏差小于1℃的概小于60%,而偏差小于0.3℃小于6%。In this embodiment, from the results, if the interference of the emissivity of the sea water and the sky temperature is not corrected, the probability that the measured temperature and the actual sea temperature will deviate by less than 1.5°C is less than 90%, the probability that the deviation will be less than 1°C is less than 60%, and the probability that the deviation will be less than 0.3°C is less than 6%.

若用于补偿的天空温度分别为20℃、-10℃、0℃和10℃,图4给出了四种天空温度补偿后仍存在的误差的概率分布,从图中可以看出,选用-10℃作为补偿温度误差概率相对较小,小于0.6℃的概率为90%,小于0.3℃的概率为50%。If the sky temperatures used for compensation are 20℃, -10℃, 0℃ and 10℃ respectively, Figure 4 shows the probability distribution of the errors that still exist after compensation for the four sky temperatures. It can be seen from the figure that the error probability of using -10℃ as the compensation temperature is relatively small, with a probability of less than 0.6℃ of 90% and a probability of less than 0.3℃ of 50%.

以上显示和描述了本发明的基本原理和主要特征和本发明的优点,对于本领域技术人员而言,显然本发明不限于上述示范性实施例的细节,而且在不背离本发明的精神或基本特征的情况下,能够以其他的具体形式实现本发明。因此,无论从哪一点来看,均应将实施例看作是示范性的,而且是非限制性的,本发明的范围由所附权利要求而不是上述说明限定,因此旨在将落在权利要求的等同要件的含义和范围内的所有变化囊括在本发明内。不应将权利要求中的任何附图标记视为限制所涉及的权利要求。The above shows and describes the basic principles and main features of the present invention and the advantages of the present invention. It is obvious to those skilled in the art that the present invention is not limited to the details of the above exemplary embodiments, and the present invention can be implemented in other specific forms without departing from the spirit or basic features of the present invention. Therefore, no matter from which point of view, the embodiments should be regarded as exemplary and non-restrictive. The scope of the present invention is defined by the attached claims rather than the above description, and it is intended that all changes falling within the meaning and scope of the equivalent elements of the claims are included in the present invention. Any figure mark in the claims should not be regarded as limiting the claims involved.

此外,应当理解,虽然本说明书按照实施方式加以描述,但并非每个实施方式仅包含一个独立的技术方案,说明书的这种叙述方式仅仅是为清楚起见,本领域技术人员应当将说明书作为一个整体,各实施例中的技术方案也可以经适当组合,形成本领域技术人员可以理解的其他实施方式。In addition, it should be understood that although the present specification is described according to implementation modes, not every implementation mode contains only one independent technical solution. This narrative method of the specification is only for the sake of clarity. Those skilled in the art should regard the specification as a whole. The technical solutions in each embodiment can also be appropriately combined to form other implementation modes that can be understood by those skilled in the art.

Claims (10)

1. A sea surface temperature measuring method is characterized in that: comprising the following steps:
establishing a space rectangular coordinate system by taking the ship bow direction of the ship as a y axis to obtain the ship pitching angle and the ship rolling angle;
acquiring wind speed and sky temperature at a certain height on the sea, and calculating to obtain sky radiation brightness;
the infrared sensor assembly (1) is arranged on the bracket (2), the installation angle, the measurement inclination angle and the space angle of the infrared sensor are obtained according to the position where the infrared sensor is arranged, wherein the bottom of the bracket (2) is provided with a mounting rod (3), the bracket (2) is fixed at the top of the shock absorber mechanism (4) through the mounting rod (3), the bottom end of the shock absorber mechanism (4) is provided with a supporting tube (5), the bottom of the supporting tube (5) is connected with an adjusting mechanism (6), and the adjusting mechanism (6) is fixed on a ship body through a stand column (7) at the bottom;
according to the ship pitching angle, the ship rolling angle, the installation angle and the measurement inclination angle of the infrared sensing device (1), an included angle between the radiation direction and the positive direction of the Z axis of the infrared sensor and an included angle between the projection of the X OY plane and the positive direction of the X axis of the infrared sensor in the space rectangular coordinate system are obtained, a center rod (9) is arranged in the middle of the shock absorber mechanism (4), and the adjusting mechanism (6) is matched with the center rod (9) to adjust and control the inside of the shock absorber mechanism (4);
calculating to obtain the average emissivity of the sea surface and the radiation brightness of seawater reflection according to the wind speed at a certain height on the sea, the included angle between the radiation direction of the infrared sensor and the positive direction of the Z axis and the included angle between the projection of the X OY plane and the positive direction of the X axis of the infrared sensor in the radiation direction in the space rectangular coordinate system;
obtaining the equivalent sky temperature and the equivalent sea water emissivity in the axial direction of the sensor according to the sea surface average emissivity and the sea water reflected radiation brightness;
according to Stefin-Boltzmann's law, the true sea temperature is obtained.
2. A method of sea surface temperature measurement according to claim 1, characterized by: the method for acquiring the wind speed and the sky temperature at a certain altitude at sea is an empirical method or a measurement method.
3. A method of sea surface temperature measurement according to claim 2, characterized by: the calculation of sky radiance comprises the following steps:
obtaining the radiation direction of the sun according to the time and the longitude and latitude of the infrared sensor;
when the incident direction of the sun is
Figure FDA0004087589790000021
When the sky radiation brightness->
Figure FDA0004087589790000022
The method comprises the following steps:
Figure FDA0004087589790000023
wherein T is sky Is sky temperature;
Figure FDA0004087589790000024
is the incident direction of the sun is->
Figure FDA0004087589790000025
Solar radiation brightness at the time; θ i Is the incident direction of the sun->
Figure FDA0004087589790000026
An included angle with the positive direction of the Z axis;
Figure FDA0004087589790000027
Is the included angle between the projection of the sun incidence direction on the XOY plane and the positive X-axis direction in the space rectangular coordinate system.
4. A method of sea surface temperature measurement according to claim 3, characterized by: according to the ship pitching angle, the ship rolling angle, the installation angle and the measurement inclination angle of the infrared sensor, the calculation formulas of the included angle of the infrared sensor in the radiation direction and the positive direction of the Z axis and the included angle of the projection of the infrared sensor in the radiation direction on the XOY plane and the positive direction of the X axis in the space rectangular coordinate system are as follows:
Figure FDA0004087589790000031
Figure FDA0004087589790000032
Figure FDA0004087589790000033
wherein θ s To measure the tilt angle;
Figure FDA0004087589790000034
is the installation angle; alpha 1 Is a pitching angle; alpha 2 Is a roll angle; θ 0 An included angle between the radiation direction of the infrared sensor and the positive direction of the Z axis is formed;
Figure FDA0004087589790000035
Is the included angle between the projection of the infrared sensor on the XOY plane in the space rectangular coordinate system in the radiation direction and the positive X-axis direction.
5. A method of sea surface temperature measurement according to claim 4, wherein: the average emissivity of the sea surface is calculated as follows:
the distribution probability of sea wave gradient according to CharlesCox and WaltermInk is as follows:
Figure FDA0004087589790000036
wherein s is x Is the gradient component of the sea wave in the X-axis direction; s is(s) y Is the gradient component of the sea wave in the Y-axis direction; v is the wind speed at a certain altitude at sea; sigma represents the steven-boltzmann constant;
assume that the radiation direction of the infrared sensor is
Figure FDA0004087589790000037
The normal direction of the element on the gradient of the sea wave is +.>
Figure FDA0004087589790000038
Then:
Figure FDA0004087589790000039
Figure FDA00040875897900000310
Figure FDA00040875897900000414
wherein x is
Figure FDA0004087589790000041
And->
Figure FDA0004087589790000042
Is included in the plane of the first part; θ n Is->
Figure FDA0004087589790000043
An included angle with the positive direction of the Z axis;
Figure FDA0004087589790000044
Is->
Figure FDA0004087589790000045
An included angle between the projection of the XOY plane and the positive direction of the X axis in a space rectangular coordinate system;
the probability of the distribution of sea wave gradients is:
Figure FDA0004087589790000046
wherein u is n Equal to cos theta n
Figure FDA0004087589790000047
Equal to cos theta n
And the incident direction of the sun
Figure FDA0004087589790000048
Is +.>
Figure FDA0004087589790000049
And the normal direction of the element on the gradient of sea wave is +.>
Figure FDA00040875897900000410
The relation of (2) is:
Figure FDA00040875897900000411
Figure FDA00040875897900000412
the average emissivity of the sea surface is:
Figure FDA00040875897900000413
wherein ε λ (x)=0.98[1-(1-cosθ 0 ) 5 ]And is the sea surface infrared emissivity.
6. A method of sea surface temperature measurement according to claim 5, wherein: the radiation brightness of the seawater reflection is calculated as follows:
according to kirchhoff's law, the sum of the emissivity and the reflectivity of seawater is 1, and the radiance of the seawater reflection is:
Figure FDA0004087589790000051
wherein ρ is λ Is the reflectivity of sea water.
7. A method of sea surface temperature measurement according to claim 6, wherein: the formula of equivalent sky temperature and equivalent sea water emissivity in the axial direction of the sensor is:
Figure FDA0004087589790000052
Figure FDA0004087589790000053
wherein alpha is a measurement half angle of the infrared sensor; omega is the spatial angle of the infrared sensor; beta is dΩ in the space angle, and the radiation direction of the infrared sensor
Figure FDA0004087589790000054
An angle with an axis of the infrared sensor; gamma is the radiation direction of the infrared sensor>
Figure FDA0004087589790000055
Corresponding azimuth angles.
8. A method of sea surface temperature measurement according to claim 7, wherein: according to Stefin-Boltzmann's law, the formula for obtaining the true sea temperature is:
Figure FDA0004087589790000056
wherein T is m A temperature is measured for the infrared sensor.
9. A method of sea surface temperature measurement according to claim 1, characterized by: the shock absorber mechanism (4) comprises a sealing sleeve (8) and a spring (10), a top plate (11) is mounted at the bottom of the sealing sleeve (8), the bottom end of the spring (10) is fixedly connected with the surface of the top plate (11), a bonding layer (12) is attached to the surface of the top plate (11), a first plug sleeve (13) is arranged in the middle of the top plate (11), and the center rod (9) penetrates into the support tube (5) from the inside of the first plug sleeve (13).
10. A method of sea surface temperature measurement according to claim 9, wherein: adjustment mechanism (6) are including hydraulic stem (14) and lift passageway (18), and hydraulic stem (14) are installed to the bottom of well core rod (9), the bottom of hydraulic stem (14) is provided with pressure increasing plate (15), the internally mounted of lift passageway (18) has butt plate (19), second grafting sleeve (20) and locating hole (21) have been seted up on the surface of butt plate (19), the surface of pressure increasing plate (15) is provided with antifriction plate (16), reference column (17) are installed at the top of antifriction plate (16), reference column (17) pass from the inside of locating hole (21).
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Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN218094023U (en) * 2022-04-13 2022-12-20 武汉交通职业学院 Self-adaptive automobile suspension shock absorber

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN218094023U (en) * 2022-04-13 2022-12-20 武汉交通职业学院 Self-adaptive automobile suspension shock absorber

Non-Patent Citations (1)

* Cited by examiner, † Cited by third party
Title
崔萌达 等: ""雷达威力预报技术中海表温度测量及修正方法"", 《哈尔滨工业大学学报》, vol. 49, no. 5, pages 116 - 121 *

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