CN105572051A - Polarized water turbidity measurement device, system and method - Google Patents

Polarized water turbidity measurement device, system and method Download PDF

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CN105572051A
CN105572051A CN201510944841.2A CN201510944841A CN105572051A CN 105572051 A CN105572051 A CN 105572051A CN 201510944841 A CN201510944841 A CN 201510944841A CN 105572051 A CN105572051 A CN 105572051A
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water turbidity
formula
light
turbidity
light intensity
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CN105572051B (en
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常建华
伍煜
陈程
黄刚
李慧凝
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Nanjing University of Information Science and Technology
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Abstract

本发明公开了一种偏振式水浊度的测量装置、测量系统及测量方法,其特征在于,包括:用于向第一透镜(2)发射一束单色光I的光源(1),所述单色光I依次穿过所述第一透镜(2)、和第一偏振片(5)后由分光镜(8)分光成呈90°夹角的入射光Ia和散射光Ib,所述散射光Ib进入第一光电探测器(7),所述入射光Ia进入测量槽(3)后的90°表面散射光Ia1依次通过第二偏振片(6)和第二透镜(4)后进入第二光电探测器(9);所述测量槽(3)内设置有温度测量传感器。本发明提供的一种偏振式水浊度的测量装置、测量系统及测量方法,采用最小二乘支持向量机的数据处理方式,对温度进行补偿,消除测量误差,提高测量精度。

The invention discloses a polarized water turbidity measuring device, measuring system and measuring method, which is characterized in that it comprises: a light source (1) for emitting a beam of monochromatic light I to a first lens (2), the The monochromatic light I sequentially passes through the first lens (2) and the first polarizer (5) and is split into incident light I a and scattered light I b at an angle of 90° by the beam splitter (8), The scattered light I b enters the first photodetector (7), and the 90° surface scattered light I a1 after the incident light I a enters the measuring groove (3) passes through the second polarizer (6) and the second lens in sequence After (4), it enters the second photodetector (9); a temperature measuring sensor is arranged in the measuring tank (3). The invention provides a polarized water turbidity measurement device, measurement system and measurement method, which adopts the data processing mode of the least squares support vector machine to compensate the temperature, eliminate the measurement error, and improve the measurement accuracy.

Description

一种偏振式水浊度的测量装置、测量系统及测量方法A polarized water turbidity measuring device, measuring system and measuring method

技术领域technical field

本发明涉及一种偏振式水浊度的测量装置、测量系统及测量方法,属于液体浊度测量技术领域。The invention relates to a polarized water turbidity measuring device, a measuring system and a measuring method, belonging to the technical field of liquid turbidity measurement.

背景技术Background technique

水的浊度是水样中的一种光学效应,是指水样中悬浮的固体颗粒物以及杂质对光的散射及吸收所引起的水样透明度变化的程度。其浊度大小与杂质的浓度大小、光学性质等都有关系。近年来,水体污染事件时有发生,威胁着广大人民群众的生命健康,引起了大众对水质监测的关心。光电测量法由于其快速、准确的特性被广泛地使用在浊度的测量领域之中。The turbidity of water is an optical effect in water samples, which refers to the degree of transparency of water samples caused by the scattering and absorption of light by suspended solid particles and impurities in water samples. The turbidity is related to the concentration of impurities and optical properties. In recent years, water pollution incidents have occurred from time to time, threatening the lives and health of the general public, and arousing the public's concern about water quality monitoring. Photoelectric measurement is widely used in the field of turbidity measurement due to its fast and accurate characteristics.

根据浊度测量国际标准ISO7027,浊度的测量是在90°方向上测量散射光,该测量方法在低浊度区域具有良好的线性关系,但由于散射光在高浊度区域产生了多次散射导致了测量误差,其测量量程受到了巨大的限制,无法广泛的应用于化工浊度的检测之中。而在另一方面,在实际测量中,由于背景光以及入射液体中的杂散光不可避免地进入探测器之中,影响整个浊度仪的测量精度。According to the international standard ISO7027 for turbidity measurement, the measurement of turbidity is to measure the scattered light in the direction of 90°. This measurement method has a good linear relationship in the low turbidity area, but due to the multiple scattering of scattered light in the high turbidity area It leads to measurement errors, and its measurement range is greatly limited, so it cannot be widely used in the detection of chemical turbidity. On the other hand, in actual measurement, background light and stray light in the incident liquid inevitably enter the detector, affecting the measurement accuracy of the entire turbidimeter.

在已经公开的中国发明(CN1087425)中,发明人采用了单光源入射液面,接受90°的表面散射光通过透镜汇聚之后入射探测器,虽然发明人采用了自动清洗的装置,以解决由于污损而造成的误差。但由于该测量方法采用了一个探测器,故无法解决因光源抖动所造成的测量误差。同时其选择的无偏振的光进行测量,探测器对各种光源没有选择性,无法去除背景光以及多次散射光的影响。针对以上的两种问题,本发专利设计的浊度仪测量仪,通过利用偏振光的特性,消除大部分背景光和杂散光干扰的影响。同时双光路的设计可以极大地去除光源老化造成的光强抖动的影响。同透射法以及90°散射法相比,光程更短,多次散射较少,故测量量程较大。同时放置温度传感器,测量装置内的温度。本装置采用最小二乘支持向量机(LS-SVM)的数据回归处理方法,同时对温度、散射光强、原光强、光强比值进行数据拟合,相比于普通的最小二乘法的拟合方法,该方法在少样本、非线性、高维度的问题上具有更好的线性,解决了温度对浊度的影响,提高了精度。In the disclosed Chinese invention (CN1087425), the inventor has adopted a single light source to enter the liquid surface, accepting 90° surface scattered light to be incident on the detector after being converged by the lens, although the inventor has adopted an automatic cleaning device to solve the problem caused by contamination. errors caused by damage. However, since this measurement method uses a detector, it cannot solve the measurement error caused by the shaking of the light source. At the same time, it selects non-polarized light for measurement, and the detector has no selectivity for various light sources, and cannot remove the influence of background light and multiple scattered light. In view of the above two problems, the turbidimeter measuring instrument designed by the patent of this invention eliminates most of the influence of background light and stray light interference by utilizing the characteristics of polarized light. At the same time, the design of dual optical paths can greatly eliminate the influence of light intensity jitter caused by the aging of the light source. Compared with the transmission method and the 90°scattering method, the optical path is shorter and the multiple scattering is less, so the measurement range is larger. A temperature sensor is also placed to measure the temperature inside the device. This device adopts the least squares support vector machine (LS-SVM) data regression processing method, and at the same time performs data fitting on temperature, scattered light intensity, original light intensity, and light intensity ratio. The combination method has better linearity on the problems of few samples, nonlinearity and high dimensionality, and solves the influence of temperature on turbidity, improving the accuracy.

发明内容Contents of the invention

本发明所要解决的技术问题是,提供一种单光源双光路偏振光的偏振式水浊度的测量装置及测量系统;进一步地,本发明提供一种解决由于光源不稳导致的浊度测量的误差,以及消除背景光和多次散射杂散光造成的影响,同时采用最小二乘支持向量机的数据处理方式,对温度进行补偿,消除测量误差,提高测量精度的偏振式水浊度的测量方法。The technical problem to be solved by the present invention is to provide a polarized water turbidity measurement device and measurement system with a single light source and dual optical path polarized light; further, the present invention provides a method for solving turbidity measurement caused by unstable light source error, and eliminate the influence of background light and multiple scattered stray light, and at the same time adopt the least squares support vector machine data processing method to compensate the temperature, eliminate the measurement error, and improve the measurement accuracy of the polarized water turbidity measurement method .

为解决上述技术问题,本发明采用的技术方案为:In order to solve the problems of the technologies described above, the technical solution adopted in the present invention is:

一种偏振式水浊度的测量装置,其特征在于,包括:用于向第一透镜发射一束单色光I的光源,所述单色光I依次穿过所述第一透镜、和第一偏振片后由分光镜分光成呈90°夹角的入射光Ia和散射光Ib,所述散射光Ib进入第一光电探测器,所述入射光Ia进入测量槽后的90°表面散射光Ia1依次通过第二偏振片和第二透镜后进入第二光电探测器;所述测量槽内设置有温度测量传感器。A polarized water turbidity measurement device, characterized in that it includes: a light source for emitting a beam of monochromatic light I to the first lens, and the monochromatic light I passes through the first lens and the second lens in sequence. After a polarizer, the light is split into incident light I a and scattered light I b at an angle of 90° by a spectroscopic mirror, and the scattered light I b enters the first photodetector, and the incident light I a enters the 90° behind the measuring groove. ° The surface scattered light I a1 enters the second photodetector after passing through the second polarizer and the second lens in sequence; a temperature measuring sensor is arranged in the measuring groove.

所述测量槽包括U型槽,所述U型槽包括两垂直设置的进水槽和出水槽,所述进水槽和出水槽的底端由横向槽连通,所述进水槽和出水槽的四周均设置有溢流槽,位于所述进水槽和出水槽相对侧的两所述溢流槽底部相连通;所述进水槽的顶端高于所述出水槽的顶端;所述进水槽的内壁上设置有至少一对折流板。The measuring tank comprises a U-shaped tank, and the U-shaped tank comprises two vertically arranged water inlet tanks and water outlet tanks, the bottom ends of the water inlet tanks and the water outlet tanks are connected by transverse grooves, and the surroundings of the water inlet tanks and the water outlet tanks are all An overflow tank is provided, and the bottoms of the two overflow tanks located on opposite sides of the water inlet tank and the water outlet tank are connected; the top of the water inlet tank is higher than the top of the water outlet tank; the inner wall of the water inlet tank is set There is at least one pair of baffles.

所述折流板与进水槽内壁的夹角为45~75°。The included angle between the baffle plate and the inner wall of the water inlet tank is 45° to 75°.

所述进水槽的顶端高出所述出水槽的顶端至少2厘米,所述进水槽的横截面面积大于所述出水槽的横截面面积。The top of the water inlet groove is at least 2 cm higher than the top of the water outlet groove, and the cross-sectional area of the water inlet groove is larger than that of the water outlet groove.

所述光源为860nm的近红外光;所述分光镜为光栅式分光镜;所述第一光电探测器和第二光电探测器均为光电三极管;所述温度测量传感器为DHT22传感器。The light source is 860nm near-infrared light; the spectroscope is a grating spectroscope; both the first photodetector and the second photodetector are phototransistors; the temperature measuring sensor is a DHT22 sensor.

一种偏振式水浊度的测量系统,其特征在于:包括上述的测量装置、信号处理模块、显示模块和挡板控制电路;所述信号处理模块包括依次连接的放大电路、滤波电路、AD转换电路;所述放大电路分别与所述第一光电探测器和第二光电探测器连接,所述显示模块与挡板控制电路连接;所述信号处理模块与所述显示模块相连接。A measurement system for polarized water turbidity, characterized in that: it includes the above-mentioned measuring device, a signal processing module, a display module and a baffle control circuit; the signal processing module includes sequentially connected amplifier circuits, filter circuits, AD conversion circuit; the amplifying circuit is respectively connected with the first photodetector and the second photodetector, and the display module is connected with the baffle control circuit; the signal processing module is connected with the display module.

一种偏振式水浊度的测量装置的测量方法,其特征在于:包括以下步骤:A measuring method of a polarized water turbidity measuring device, characterized in that: comprising the following steps:

利用最小二乘向量支持机的线性回归方程组:A system of linear regression equations using a least squares vector support machine:

y=WTΦ(x)+b(1)y=W T Φ(x)+b(1)

minmin JJ (( WW ,, ee )) == 11 22 WW TT WW ++ CC ΣΣ kk == 11 nno ee kk 22 -- -- -- (( 22 ))

s.t.y(xk)=WTΦ(xk)+b+ek,k=1,....n(3)sty(x k )=W T Φ(x k )+b+e k ,k=1,....n(3)

式(1)中,Φ(x)代表各个输入的水浊度影响因子对浊度值的影响函数;W代表各个水浊度影响因子的函数系数矩阵;y代表水浊度;In formula (1), Φ(x) represents the influence function of each input water turbidity influencing factor on the turbidity value; W represents the function coefficient matrix of each water turbidity influencing factor; y represents water turbidity;

式(2)是对式(1)进行最小二乘向量拟合,式(2)中的e代表误差;ek代表各个水浊度影响因子的误差;T代表矩阵的运算方式;C代表用于控制误差比重的调节因子;J(W,e)代表约束条件,选择W和e的最小值;Equation (2) is the least squares vector fitting of Equation (1), e in Equation (2) represents the error; e k represents the error of each water turbidity influencing factor; T represents the operation mode of the matrix; Adjustment factor for the proportion of control error; J(W,e) represents the constraint condition, choose the minimum value of W and e;

对式(1)、(2)进行约束化得式(3),s.t.是受约束的意思;式(2)和式(3)组成一个方程组;Formula (1), (2) is constrained to get formula (3), s.t. is the meaning of being constrained; formula (2) and formula (3) form a group of equations;

由式(3)建立拉格朗日等式:The Lagrangian equation is established by formula (3):

LL (( WW ,, bb ,, ee ,, αα )) == JJ (( WW ,, ee )) -- ΣΣ ii NN αα ii (( WW TT ΦΦ (( xx ii )) ++ bb -- ythe y (( xx ii )) )) -- -- -- (( 44 ))

式(4)中,α代表拉格朗日乘子;αi代表各个水浊度影响因子的拉格朗日乘子;i=1~N;In formula (4), α represents the Lagrangian multiplier; α i represents the Lagrangian multiplier of each water turbidity influencing factor; i=1~N;

根据KKT条件,对式(4)中的W,e,α,b求偏导得:According to the KKT condition, partial derivatives are obtained for W, e, α, b in formula (4):

∂∂ LL ∂∂ WW == 00 →&Right Arrow; ΣΣ ii == 11 NN αα ii ΦΦ (( xx ii )) -- -- -- (( 55 ))

∂∂ LL ∂∂ bb == 00 →&Right Arrow; ΣΣ ii == 11 NN αα ii == 00 -- -- -- (( 66 ))

∂∂ LL ∂∂ ee == 00 →&Right Arrow; αα ii == CeCe kk -- -- -- (( 77 ))

∂∂ LL ∂∂ αα ii == 00 →&Right Arrow; WW TT ΦΦ (( xx ii )) ++ bb ++ ee kk -- ythe y (( xx ii )) -- -- -- (( 88 ))

由式(5)~式(8)求解b和α,得最小二乘支持向量机模型:Solve b and α from equations (5) to (8) to get the least squares support vector machine model:

ff (( xx )) == ΣΣ ii == 11 NN αα ii kk (( xx ,, xx ii )) ++ bb -- -- -- (( 99 ))

式(9)中,f(x)代表水浊度;k(x,xi)代表各个水浊度影响因子的径向基函数;In formula (9), f(x) represents water turbidity; k(x, x i ) represents the radial basis function of each water turbidity influencing factor;

kk (( xx ,, xx ii )) == expexp {{ -- || || xx -- xx ii || || 22 σσ 22 }} -- -- -- (( 1010 ))

式(10)中,x代表各个水浊度影响因子的当前测量的值;xi代表之前各个水浊度影响因子的训练值;σ代表核函数宽度;In formula (10), x represents the current measured value of each water turbidity influencing factor; x i represents the previous training value of each water turbidity influencing factor; σ represents the width of the kernel function;

将式(10)带入式(9),得:Put formula (10) into formula (9), get:

ff (( xx )) == ΣΣ ii == 11 NN αα ii expexp {{ -- || || xx -- xx ii || || 22 σσ 22 }} ++ bb -- -- -- (( 1111 ))

将各个水浊度影响因子分别作为输入值带入式(11)中,调节调节因子C和核函数宽度σ,输出值f(x)为浊度值;输出值f(x)与标准浊度液进行标定。Bring each water turbidity influence factor into the formula (11) as input value, adjust the adjustment factor C and the kernel function width σ, the output value f(x) is the turbidity value; the output value f(x) and the standard turbidity liquid for calibration.

所述水浊度影响因子包括温度、散射光强、参考光强和光强比值;所述散射光强为散射光Ib的光强,所述参考光强为Ia1的光强,所述光强比值为Ib/Ia1Described water turbidity influence factor comprises temperature, scattered light intensity, reference light intensity and light intensity ratio; Described scattered light intensity is the light intensity of scattered light Ib , and described reference light intensity is the light intensity of Ia1, and described The light intensity ratio is I b /I a1 .

所述标准浊度液的制备方法为:将几种不同水浊度的福尔马肼溶液依次充入所述测量槽中,分别测得其相应的电压值,所述电压值包括Ib和Ia1The preparation method of described standard turbidity liquid is: the formazin solution of several different water turbidities is filled in described measuring tank successively, records its corresponding voltage value respectively, and described voltage value comprises I b and I a1 .

所述标准浊度液的水浊度计算方法为:根据电压值计算光强比值Ib/Ia1,将标准浊度液的水浊度y和光强比值x分别作为横、纵坐标,线性拟合,得线性方程,y=k1x+b1,k1和b1为定值,将测量并计算得到的光强比值代入y=k1x+b1方程中就得到水浊度的大小。The water turbidity calculation method of the standard turbidity liquid is: calculate the light intensity ratio I b /I a1 according to the voltage value, and use the water turbidity y and the light intensity ratio x of the standard turbidity liquid as the horizontal and vertical coordinates respectively, linear Fitting to get a linear equation, y=k 1 x+b 1 , k 1 and b 1 are fixed values, the measured and calculated light intensity ratio is substituted into the y=k 1 x+b 1 equation to get the water turbidity the size of.

本发明专用以上技术方案与现有技术相比,具有以下技术效果:Compared with the prior art, the above technical scheme dedicated to the present invention has the following technical effects:

1、本发明的测量装置及测量系统,提出了一种单光源双光路的浊度测量方案,测量散射光以及参考光,能有效地减小光源不稳以及探测器的污损导致的测量误差。1. The measurement device and measurement system of the present invention proposes a turbidity measurement scheme with a single light source and two light paths to measure scattered light and reference light, which can effectively reduce the measurement error caused by the instability of the light source and the contamination of the detector .

2、本发明的测量装置及测量系统,采用起偏器产生、检偏器检测偏振光,可以极大地减小背景光和杂散光的影响,提高精度。2. The measuring device and measuring system of the present invention adopt polarizers to generate polarized light and analyzers to detect polarized light, which can greatly reduce the influence of background light and stray light and improve precision.

3、本发明的测量装置及测量系统,所设计的测量槽,利用重力差注水,液体经过折流板,保证水流缓慢且被测液面水平。3. In the measuring device and measuring system of the present invention, the designed measuring tank utilizes the gravity difference to inject water, and the liquid passes through the baffle to ensure that the water flow is slow and the liquid level to be measured is level.

4、本发明的测量装置及测量系统,提高了系统检测灵敏度,简化了整个测量系统,且具有更高的系统集成度,结构更紧凑,实现在复杂环境条件下水体浊度的在线快速检测。4. The measuring device and measuring system of the present invention improve the detection sensitivity of the system, simplify the entire measuring system, have a higher system integration degree, and have a more compact structure, and realize online rapid detection of water body turbidity under complex environmental conditions.

5、本发明采用最小二乘支持向量机的数据处理方式,对温度进行了补偿,消除测量误差,提高了测量精度。5. The present invention adopts the data processing method of the least squares support vector machine, compensates the temperature, eliminates the measurement error, and improves the measurement accuracy.

本发明提供的一种偏振式水浊度的测量装置、测量系统及测量方法,提出了一种单光源双探测器的双光路的浊度测量方案,测量90°散射光以及光源本身的光信号,有效地减小光源不稳导致的测量误差。由于采用了偏振光探测,可以极大地减少背景杂散光以及经过多次散射误入探测器的光所造成的误差,精度较高,抗干扰能力强。同时,利用表面散射的原理与传统的透射法以及90°散射法相比,光程更短,多次散射较少,故测量量程较大。同时放置温度传感器,测量装置内的温度。本装置采用最小二乘支持向量机(LS-SVM)的数据回归处理方法,同时对温度、散射光强、原光强、光强比值进行数据拟合,相比于普通的最小二乘法的拟合方法,该方法在少样本、非线性、高维度的问题上具有更好的线性,解决了温度对浊度的影响,提高了精度。The present invention provides a polarized water turbidity measurement device, measurement system and measurement method, and proposes a turbidity measurement scheme with a single light source and dual detectors and a dual optical path to measure 90° scattered light and the light signal of the light source itself , effectively reducing the measurement error caused by the instability of the light source. Due to the use of polarized light detection, it can greatly reduce the error caused by background stray light and light that has been scattered into the detector by multiple scattering, with high precision and strong anti-interference ability. At the same time, compared with the traditional transmission method and 90°scattering method, using the principle of surface scattering has a shorter optical path and less multiple scattering, so the measurement range is larger. A temperature sensor is also placed to measure the temperature inside the device. This device adopts the least squares support vector machine (LS-SVM) data regression processing method, and at the same time performs data fitting on temperature, scattered light intensity, original light intensity, and light intensity ratio. The combination method has better linearity on the problems of few samples, nonlinearity and high dimensionality, and solves the influence of temperature on turbidity, improving the accuracy.

说明书附图Instructions attached

图1为本发明的流程图;Fig. 1 is a flowchart of the present invention;

图2为本发明中测量槽的结构示意图。Fig. 2 is a schematic diagram of the structure of the measuring tank in the present invention.

具体实施方式detailed description

下面结合附图对本发明作更进一步的说明。The present invention will be further described below in conjunction with the accompanying drawings.

如图1~图2所示,一种偏振式水浊度的测量装置,其特征在于,包括:用于向第一透镜2发射一束单色光I的光源1,所述单色光I依次穿过所述第一透镜2、和第一偏振片5后由分光镜8分光成呈90°夹角的入射光Ia和散射光Ib,所述散射光Ib进入第一光电探测器7,所述入射光Ia进入测量槽3后的90°表面散射光Ia1依次通过第二偏振片6和第二透镜4后进入第二光电探测器9;所述测量槽3内设置有温度测量传感器。As shown in Figures 1 to 2, a polarized water turbidity measurement device is characterized in that it includes: a light source 1 for emitting a beam of monochromatic light I to the first lens 2, and the monochromatic light I After passing through the first lens 2 and the first polarizer 5 in turn, the light is split into incident light I a and scattered light I b at an angle of 90° by the beam splitter 8, and the scattered light I b enters the first photodetector device 7, the 90° surface scattered light I a1 after the incident light Ia enters the measurement groove 3 passes through the second polarizer 6 and the second lens 4 in sequence and then enters the second photodetector 9; set in the measurement groove 3 There is a temperature measuring sensor.

所述测量槽3包括U型槽,所述U型槽包括两垂直设置的进水槽12和出水槽10,所述进水槽12和出水槽10的底端由横向槽13连通,所述进水槽12和出水槽10的四周均设置有溢流槽14,位于所述进水槽12和出水槽10相对侧的两所述溢流槽14底部相连通;所述进水槽12的顶端高于所述出水槽10的顶端;所述进水槽12的内壁上设置有至少一对折流板11。Described measuring groove 3 comprises U-shaped groove, and described U-shaped groove comprises two vertically arranged water inlet grooves 12 and water outlet groove 10, and the bottom end of described water inlet groove 12 and water outlet groove 10 is communicated by transverse groove 13, and described water inlet groove 12 and the water outlet tank 10 are all provided with overflow tanks 14 around, and the bottoms of the two overflow tanks 14 located on the opposite sides of the water inlet tank 12 and the water outlet tank 10 are connected; the top of the water inlet tank 12 is higher than the At the top of the water outlet tank 10 ; at least one pair of baffles 11 are arranged on the inner wall of the water inlet tank 12 .

溢出水体经过收集装置流入回收池,以便后续利用。The overflow water flows into the recovery tank through the collection device for subsequent use.

所述折流板11与进水槽12内壁的夹角为45~75°。The included angle between the baffle plate 11 and the inner wall of the water inlet tank 12 is 45° to 75°.

所述进水槽12的顶端高出所述出水槽10的顶端至少2厘米,所述进水槽12的横截面面积大于所述出水槽10的横截面面积。The top of the water inlet groove 12 is at least 2 cm higher than the top of the water outlet groove 10 , and the cross-sectional area of the water inlet groove 12 is larger than that of the water outlet groove 10 .

所述光源1为860nm的近红外光;所述分光镜8为光栅式分光镜;所述第一光电探测器7和第二光电探测器9均为光电三极管;所述温度测量传感器为DHT22传感器。The light source 1 is near-infrared light of 860nm; the spectroscope 8 is a grating spectroscope; the first photodetector 7 and the second photodetector 9 are phototransistors; the temperature measuring sensor is a DHT22 sensor .

一种偏振式水浊度的测量系统,其特征在于:包括上述的测量装置、信号处理模块、显示模块和挡板控制电路;所述信号处理模块包括依次连接的放大电路、滤波电路、AD转换电路;所述放大电路分别与所述第一光电探测器7和第二光电探测器9连接,所述显示模块与挡板控制电路连接;所述信号处理模块与所述显示模块相连接。A measurement system for polarized water turbidity, characterized in that: it includes the above-mentioned measuring device, a signal processing module, a display module and a baffle control circuit; the signal processing module includes sequentially connected amplifier circuits, filter circuits, AD conversion circuit; the amplifying circuit is connected to the first photodetector 7 and the second photodetector 9 respectively, and the display module is connected to the baffle control circuit; the signal processing module is connected to the display module.

光源1采用860nm的近红外光,可以最大限度的减小水样的色度对于浊度测量的影响;分光镜8采用光栅式分光镜,将光源发出的单色光分成已知光强比例关系的两束同频率的光,光栅式分光镜产生光谱各色区大致相等,红光区分辨率比棱镜式要高;光电探测器为一光电三极管,光电三极管灵敏度较高,体积小;测量槽3入水口在左,出水口在右,利用两者的高度差进行注水操作,以减小水的流速,避免气泡的产生,并保持被测液面的水平且槽内壁采用折流板11的设计,使水体中的气泡附着,避免气泡对浊度测量的影响。The light source 1 uses 860nm near-infrared light, which can minimize the influence of the chromaticity of the water sample on the turbidity measurement; the beam splitter 8 uses a grating type beam splitter to divide the monochromatic light emitted by the light source into a known light intensity ratio relationship For two beams of light with the same frequency, the grating-type beam splitter produces roughly the same color regions of the spectrum, and the resolution of the red light region is higher than that of the prism type; the photodetector is a phototransistor, which has high sensitivity and small size; the measurement tank 3 The water inlet is on the left, and the water outlet is on the right. The height difference between the two is used for water injection operation to reduce the water flow rate, avoid the generation of air bubbles, and maintain the level of the measured liquid level. The inner wall of the tank adopts the design of baffle plate 11. , so that the air bubbles in the water body can attach to avoid the influence of air bubbles on turbidity measurement.

本发明的光路详细路径如下:光束I由光源1产生,经过第一透镜2以及起偏器5(即第一偏振片)之后,以与被测液面成30°入射,通过分光镜8产生了光束Ia与光束Ib,光束Ib直接入射第一光电检测器7。光束Ia入射测量槽3,后散射光Ia1入射至第二偏振片6,后经过第二透镜4的汇聚作用入射至第二光电检测器9,测量时需要保证上述所有器件均在同一平面上,以及偏振片的偏振方向与光线的入射方向以及震动方向的平面相垂直。The detailed path of the optical path of the present invention is as follows: the light beam I is produced by the light source 1, after passing through the first lens 2 and the polarizer 5 (i.e. the first polarizer), to be incident at 30° with the liquid surface to be measured, and generated by the beam splitter 8 The light beam I a and the light beam I b are separated, and the light beam I b directly enters the first photodetector 7 . The light beam I a is incident on the measurement groove 3, and the scattered light I a1 is incident on the second polarizer 6, and then incident on the second photodetector 9 through the converging effect of the second lens 4. It is necessary to ensure that all the above-mentioned devices are on the same plane during measurement. , and the polarization direction of the polarizer is perpendicular to the plane of the incident direction of the light and the vibration direction.

本发明利用光的透射法方式测量待测液体的浊度,其原理如下:The present invention utilizes the transmission method of light to measure the turbidity of the liquid to be measured, and its principle is as follows:

本发明专光源发出的光I经过起偏器之后,根据马吕斯定律衰减为原来的一半I′后入射至分光镜8,Ia1是Ia经过分光镜8的光。Ib1是Ib经过表面散射与入射光方向成90°的光。两者之商d与当前待测样液的浊度具有一定的函数关系,推导如下:After passing through the polarizer, the light I emitted by the special light source of the present invention is attenuated to half of the original I′ according to the Malus law and then enters the beam splitter 8. I a1 is the light of I a passing through the beam splitter 8. I b1 is the light that is scattered by the surface of I b at 90° to the direction of the incident light. The quotient d of the two has a certain functional relationship with the turbidity of the current sample liquid to be tested, and the derivation is as follows:

dd == II bb 11 II aa 11

其中:Ia1和Ib1经过第一光电探测器和第二光电探测器进行光电转换过后的电压值,Ib1=IbWherein: the voltage values of I a1 and I b1 after photoelectric conversion by the first photodetector and the second photodetector, I b1 =I b ;

根据比尔朗伯定律以及mile散射定理,将Ib1=β1IbKT,Ia1=β2Ia带入可以得到:According to Bill Lambert's law and mile scattering theorem, taking I b1 = β 1 I b KT, I a1 = β 2 I a into it can be obtained:

dd == ββ 11 II bb KK TT ββ 22 II aa

其中:β1与β2是分光系数,K与待测液体的成分、性质有关,T为待测液体的浊度值;β1、β2和K均为常数,用β1*K/β2=D来表示,Among them: β 1 and β 2 are spectral coefficients, K is related to the composition and properties of the liquid to be measured, T is the turbidity value of the liquid to be measured; β 1 , β 2 and K are all constants, and β 1* K/β 2 = D to represent,

可得, d = β 1 I b K T β 2 I b = β 1 K T β 2 Available, d = β 1 I b K T β 2 I b = β 1 K T β 2

将上式化简可得, d = β 1 K T β 2 = D T Simplify the above formula to get, d = β 1 K T β 2 = D. T

由上式可知d与T成正比,则可以通过Ia1与Ib1之比d求得待测液体的浊度值T。由于在低浊度时,表面散射光光强较小,很难被探测误差较大。同时在不同的温度下,液体布朗运动会有所不同,散射光光强也会不同,故下面对测量温度等进行补偿计算。It can be seen from the above formula that d is directly proportional to T, and the turbidity value T of the liquid to be tested can be obtained through the ratio d of I a1 to I b1 . Since the intensity of scattered light on the surface is small at low turbidity, it is difficult to be detected and the error is large. At the same time, at different temperatures, the Brownian motion of the liquid will be different, and the intensity of the scattered light will also be different, so the compensation calculation for the measurement temperature will be performed below.

一种偏振式水浊度的测量装置的测量方法,其特征在于:包括以下步骤:A measuring method of a polarized water turbidity measuring device, characterized in that: comprising the following steps:

利用最小二乘向量支持机的线性回归方程组:A system of linear regression equations using a least squares vector support machine:

y=WTΦ(x)+b(1)y=W T Φ(x)+b(1)

minmin JJ (( WW ,, ee )) == 11 22 WW TT WW ++ CC ΣΣ kk == 11 nno ee kk 22 -- -- -- (( 22 ))

s.t.y(xk)=WTΦ(xk)+b+ek,k=1,....n(3)sty(x k )=W T Φ(x k )+b+e k ,k=1,....n(3)

式(1)中,Φ(x)代表各个输入的水浊度影响因子对浊度值的影响函数;W代表各个水浊度影响因子的函数系数矩阵;y代表水浊度;In formula (1), Φ(x) represents the influence function of each input water turbidity influencing factor on the turbidity value; W represents the function coefficient matrix of each water turbidity influencing factor; y represents water turbidity;

式(2)是对式(1)进行最小二乘向量拟合,式(2)中的e代表误差;ek代表各个水浊度影响因子的误差;T代表矩阵的运算方式;C代表用于控制误差比重的调节因子;J(W,e)代表约束条件,选择W和e的最小值;Equation (2) is the least squares vector fitting of Equation (1), e in Equation (2) represents the error; e k represents the error of each water turbidity influencing factor; T represents the operation mode of the matrix; Adjustment factor for the proportion of control error; J(W,e) represents the constraint condition, choose the minimum value of W and e;

W=[W1,W2,W3,W4]是温度、散射光强、参考光强和光强比值对浊度影响函数的四个系数的集合,也就是一个系数矩阵;W=[W1, W2, W3, W4] is a set of four coefficients of the influence function of temperature, scattered light intensity, reference light intensity and light intensity ratio on turbidity, that is, a coefficient matrix;

对式(1)、(2)进行约束化得式(3),s.t.是subjectto的缩写,是受约束的意思;式(2)和式(3)组成一个方程组;Formula (1), (2) is constrained to get formula (3), s.t. is the abbreviation of subjectto, which means constrained; formula (2) and formula (3) form a group of equations;

式(2)与传统的线性回归方法相比,增加了误差的平方和项,要求误差平方和最小,防止极端值占据主导地位。同时,最小二乘支持向量机与传统的方法相比,将线性规划问题改进为求解线性方程组的问题,从而提高计算精度,并且对异常值敏感。由于该问题是无约束问题,难以处理。建立拉格朗日等式,将其变为有约束的问题。Compared with the traditional linear regression method, formula (2) increases the sum of squares of the errors, and requires the minimum sum of squares of errors to prevent extreme values from dominating. At the same time, compared with the traditional method, the least squares support vector machine improves the linear programming problem to solve the problem of linear equations, thereby improving the calculation accuracy, and is sensitive to outliers. Since this problem is an unconstrained problem, it is difficult to handle. Establish the Lagrangian equation and turn it into a constrained problem.

由式(3)建立拉格朗日等式:The Lagrangian equation is established by formula (3):

LL (( WW ,, bb ,, ee ,, αα )) == JJ (( WW ,, ee )) -- ΣΣ ii NN αα ii (( WW TT ΦΦ (( xx ii )) ++ bb -- ythe y (( xx ii )) )) -- -- -- (( 44 ))

式(4)中,α代表拉格朗日乘子;αi代表各个水浊度影响因子的拉格朗日乘子;i=1~N;In formula (4), α represents the Lagrangian multiplier; α i represents the Lagrangian multiplier of each water turbidity influencing factor; i=1~N;

根据KKT条件,对式(4)中的W,e,α,b求偏导得:According to the KKT condition, partial derivatives are obtained for W, e, α, b in formula (4):

∂∂ LL ∂∂ WW == 00 →&Right Arrow; ΣΣ ii == 11 NN αα ii ΦΦ (( xx ii )) -- -- -- (( 55 ))

∂∂ LL ∂∂ bb == 00 →&Right Arrow; ΣΣ ii == 11 NN αα ii == 00 -- -- -- (( 66 ))

∂∂ LL ∂∂ ee == 00 →&Right Arrow; αα ii == CeCe kk -- -- -- (( 77 ))

∂∂ LL ∂∂ αα ii == 00 →&Right Arrow; WW TT ΦΦ (( xx ii )) ++ bb ++ ee kk -- ythe y (( xx ii )) -- -- -- (( 88 ))

由式(5)~式(8)求解b和α,得最小二乘支持向量机模型:Solve b and α from equations (5) to (8) to get the least squares support vector machine model:

ff (( xx )) == ΣΣ ii == 11 NN αα ii kk (( xx ,, xx ii )) ++ bb -- -- -- (( 99 ))

式(9)中,f(x)代表水浊度;k(x,xi)代表各个水浊度影响因子的径向基函数;其中k(x,xi)为径向基函数,有线性核函数,S型核函数、多项式型核函数,一般取高斯核函数;In formula (9), f(x) represents water turbidity; k(x, x i ) represents the radial basis function of each water turbidity influencing factor; where k(x, x i ) is a radial basis function, Linear kernel function, S-type kernel function, polynomial kernel function, generally take Gaussian kernel function;

kk (( xx ,, xx ii )) == expexp {{ -- || || xx -- xx ii || || 22 σσ 22 }} -- -- -- (( 1010 ))

式(10)中,x代表各个水浊度影响因子的当前测量的值;xi代表之前各个水浊度影响因子的训练值;σ代表核函数宽度;In formula (10), x represents the current measured value of each water turbidity influencing factor; x i represents the previous training value of each water turbidity influencing factor; σ represents the width of the kernel function;

将式(10)带入式(9),得:Put formula (10) into formula (9), get:

ff (( xx )) == ΣΣ ii == 11 NN αα ii expexp {{ -- || || xx -- xx ii || || 22 σσ 22 }} ++ bb -- -- -- (( 1111 ))

将各个水浊度影响因子分别作为输入值带入式(11)中,调节调节因子C和核函数宽度σ,输出值f(x)为浊度值;输出值f(x)与标准浊度液进行标定。Bring each water turbidity influence factor into the formula (11) as input value, adjust the adjustment factor C and the kernel function width σ, the output value f(x) is the turbidity value; the output value f(x) and the standard turbidity liquid for calibration.

所述水浊度影响因子包括温度、散射光强、参考光强和光强比值;所述散射光强为散射光Ib的光强,所述参考光强为Ia1的光强,所述光强比值为Ib/Ia1Described water turbidity influence factor comprises temperature, scattered light intensity, reference light intensity and light intensity ratio; Described scattered light intensity is the light intensity of scattered light Ib , and described reference light intensity is the light intensity of Ia1, and described The light intensity ratio is I b /I a1 .

所述标准浊度液的制备方法为:将几种不同水浊度的福尔马肼溶液依次充入所述测量槽3中,分别测得其相应的电压值,所述电压值包括Ib和Ia1The preparation method of described standard turbidity liquid is: the formazin solution of several different water turbidities is filled in the described measuring tank 3 successively, respectively measure its corresponding voltage value, and described voltage value comprises I b and I a1 .

所述标准浊度液的水浊度计算方法为:根据电压值计算光强比值Ib/Ia1,将标准浊度液的水浊度y和光强比值x分别作为横、纵坐标,线性拟合,得线性方程,y=k1x+b1,k1和b1为定值,将测量并计算得到的光强比值代入y=k1x+b1方程中就得到水浊度的大小。The water turbidity calculation method of the standard turbidity liquid is as follows: calculate the light intensity ratio I b /I a1 according to the voltage value, and use the water turbidity y and the light intensity ratio x of the standard turbidity liquid as the horizontal and vertical coordinates respectively, linear Fitting to get a linear equation, y=k 1 x+b 1 , k 1 and b 1 are fixed values, and substituting the measured and calculated light intensity ratio into the y=k 1 x+b 1 equation to get the water turbidity the size of.

本发明的实施步骤如下:Implementation steps of the present invention are as follows:

1、打开入水口阀与出水口阀,在测量槽3中缓慢充进待测液体。多余的液体从入水口溢出。1. Open the water inlet valve and the water outlet valve, and slowly fill the measuring tank 3 with the liquid to be tested. Excess liquid overflows from the water inlet.

2、控制电路通过向光电探测器发送指令,使得光电探测器在测量前先进行预热,在光电探测器的温度稳定后,进行测量。2. The control circuit sends an instruction to the photodetector, so that the photodetector is preheated before the measurement, and the measurement is performed after the temperature of the photodetector is stable.

3、光源输出相应频率光束经过起偏器之后,经过分光镜8后产生了两束光,进入测量系统,散射光经过检偏器之后,透镜将接收到的光进行汇聚并传送给光电探测器,光电探测器将各自接收到的光信号转换为电信号并传送给信号处理模块。可以调节检偏器的检偏方向,以保证第二光电探测器所得到的光强最大。3. After the light source outputs the corresponding frequency light beam through the polarizer, two beams of light are generated after passing through the beam splitter 8, and enter the measurement system. After the scattered light passes through the analyzer, the lens gathers the received light and transmits it to the photodetector , the photodetectors convert the received optical signals into electrical signals and transmit them to the signal processing module. The polarization analysis direction of the polarization analyzer can be adjusted to ensure the maximum light intensity obtained by the second photodetector.

4、信号处理模块中的放大电路、滤波电路及AD转换电路依次对电信号进行放大、滤波、AD转换,生成数字信号并传送给控制电路进行处理,由控制电路得到解调后的电压值,并由公式得到比值d,将比值d,参考光强度Ib,散射光强度Ia1,以及温度值T作为输入变量Xi带入最小二乘支持向量机中,得到的结果y经过MatLab工具箱进行数据训练后得到b与α,进行数据拟合、标定后,最后传送给显示模块显示。4. The amplification circuit, filter circuit and AD conversion circuit in the signal processing module sequentially amplify, filter and AD convert the electrical signal, generate a digital signal and send it to the control circuit for processing, and the control circuit obtains the demodulated voltage value, And the ratio d is obtained from the formula, and the ratio d, the reference light intensity I b , the scattered light intensity Ia 1 , and the temperature value T are brought into the least squares support vector machine as the input variable Xi, and the obtained result y is processed by the MatLab toolbox After data training, b and α are obtained, after data fitting and calibration, they are finally sent to the display module for display.

以上所述仅是本发明的优选实施方式,应当指出:对于本技术领域的普通技术人员来说,在不脱离本发明原理的前提下,还可以做出若干改进和润饰,这些改进和润饰也应视为本发明的保护范围。The above is only a preferred embodiment of the present invention, it should be pointed out that for those of ordinary skill in the art, without departing from the principle of the present invention, some improvements and modifications can also be made. It should be regarded as the protection scope of the present invention.

Claims (10)

1. the measurement mechanism of a polarization type water turbidity, it is characterized in that, comprise: for launching the light source (1) of a monochromic beam I to the first lens (2), described monochromatic light I becomes incident light I in 90 ° angles with after the first polaroid (5) by spectroscope (8) light splitting through described first lens (2) successively awith scattered light I b, described scattered light I benter the first photodetector (7), described incident light I aenter 90 ° of surface scattering light I after measuring flume (3) a1successively by entering the second photodetector (9) after the second polaroid (6) and the second lens (4); Described measuring flume is provided with sensor for measuring temperature in (3).
2. the measurement mechanism of a kind of polarization type water turbidity according to claim 1, it is characterized in that: described measuring flume (3) comprises U-type groove, described U-type groove comprises two vertically disposed intake chambers (12) and effluent trough (10), described intake chamber (12) is communicated with by transverse groove (13) with the bottom of effluent trough (10), the surrounding of described intake chamber (12) and effluent trough (10) is provided with overflow groove (14), be positioned at described intake chamber (12) and effluent trough (10) opposite side two described in overflow groove (14) bottom be connected, the top of described intake chamber (12) is higher than the top of described effluent trough (10), the inwall of described intake chamber (12) is provided with at least one pair of baffle (11).
3. the measurement mechanism of a kind of polarization type water turbidity according to claim 2, is characterized in that: described baffle (11) is 45 ~ 75 ° with the angle of intake chamber (12) inwall.
4. the measurement mechanism of a kind of polarization type water turbidity according to claim 2, it is characterized in that: the top of described intake chamber (12) exceeds at least 2 centimetres, the top of described effluent trough (10), the cross-sectional area of described intake chamber (12) is greater than the cross-sectional area of described effluent trough (10).
5. the measurement mechanism of a kind of polarization type water turbidity according to claim 1, is characterized in that: the near infrared light that described light source (1) is 860nm; Described spectroscope (8) is raster pattern spectroscope; Described first photodetector (7) and the second photodetector (9) are phototriode; Described sensor for measuring temperature is DHT22 sensor.
6. a measuring system for polarization type water turbidity, is characterized in that: comprise the measurement mechanism as described in any one of Claims 1 to 5, signal processing module, display module and baffle controls circuit; Described signal processing module comprises the amplifying circuit, filtering circuit, the A/D convertor circuit that connect successively; Described amplifying circuit is connected with described first photodetector (7) and the second photodetector (9) respectively, and described display module is connected with baffle controls circuit; Described signal processing module is connected with described display module.
7. the measuring method of the measurement mechanism of a kind of polarization type water turbidity according to any one of Claims 1 to 5, is characterized in that: comprise the following steps:
Utilize the equation of linear regression group of least square vector support machine:
y=W TΦ(x)+b(1)
min J ( W , e ) = 1 2 W T W + C Σ k = 1 n e k 2 - - - ( 2 )
s.t.y(x k)=W TΦ(x k)+b+e k,k=1,....n(3)
In formula (1), Φ (x) represents the water turbidity factor of influence of each input to the influence function of turbidity value; W represents the function coefficients matrix of each water turbidity factor of influence; Y represents water turbidity;
Formula (2) carries out the matching of least square vector, the e Representative errors in formula (2) to formula (1); e krepresent the error of each water turbidity factor of influence; T represents the compute mode of matrix; C representative is used for the regulatory factor of departure proportion; J (W, e) represents constraint condition, selects the minimum value of W and e;
Formula (1), (2) are carried out to about fasciculation and obtained formula (3), and s.t. is the affined meaning; Formula (2) and formula (3) composition system of equations;
Lagrange's equation is set up by formula (3):
L ( W , b , e , α ) = J ( W , e ) - Σ i N α i ( W T Φ ( x i ) + b - y ( x i ) ) - - - ( 4 )
In formula (4), α represents Lagrange multiplier; α irepresent the Lagrange multiplier of each water turbidity factor of influence; I=1 ~ N;
According to KKT condition, to the W in formula (4), e, α, b ask local derviation to obtain:
∂ L ∂ W = 0 → Σ i = 1 N α i Φ ( x i ) - - - ( 5 )
∂ L ∂ b = 0 → Σ i = 1 N α i = 0 - - - ( 6 )
∂ L ∂ e = 0 → α i = Ce k - - - ( 7 )
∂ L ∂ α i = 0 → W T Φ ( x i ) + b + e k - y ( x i ) - - - ( 8 )
Solved b and α by formula (5) ~ formula (8), obtained least square method supporting vector machine model:
f ( x ) = Σ i = 1 N α i k ( x , x i ) + b - - - ( 9 )
In formula (9), f (x) represents water turbidity; K (x, x i) represent the radial basis function of each water turbidity factor of influence;
k ( x , x i ) = exp { - | | x - x i | | 2 σ 2 } - - - ( 10 )
In formula (10), x represents the value when pre-test of each water turbidity factor of influence; x ithe trained values of each water turbidity factor of influence before representative; σ represents kernel function width;
Bring formula (10) into formula (9):
f ( x ) = Σ j = 1 N α i exp { - | | x - x i | | 2 σ 2 } + b - - - ( 11 )
Bring in formula (11) using each water turbidity factor of influence as input value, regulate regulatory factor C and kernel function width cs, output valve f (x) is turbidity value; Output valve f (x) and standard turbidity solution are demarcated.
8. the measuring method of a kind of polarization type water turbidity according to claim 7, is characterized in that: described water turbidity factor of influence comprises temperature, scattered light intensity, reference light intensity and light intensity ratio; Described scattered light intensity is scattered light I blight intensity, described with reference to light intensity be Ia 1light intensity, described light intensity ratio is I b/ I a1.
9. the measuring method of a kind of polarization type water turbidity according to claim 7, it is characterized in that: the preparation method of described standard turbidity solution is: the formal hydrazine solution of several different water turbidity is filled with successively in described measuring flume (3), record its corresponding magnitude of voltage respectively, described magnitude of voltage comprises I band I a1.
10. the measuring method of a kind of polarization type water turbidity according to claim 8, is characterized in that: the water turbidity computing method of described standard turbidity solution are: calculate light intensity ratio I according to magnitude of voltage b/ I a1, using the water turbidity y of standard turbidity solution and light intensity ratio x as horizontal, ordinate, linear fit, obtains linear equation, y=k 1x+b 1, k 1and b 1for definite value, will measure and the light intensity ratio calculated substitution y=k 1x+b 1the size of water turbidity is just obtained in equation.
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