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CN111351609A - Method for measuring wall shear stress vector - Google Patents

Method for measuring wall shear stress vector Download PDF

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CN111351609A
CN111351609A CN202010180082.8A CN202010180082A CN111351609A CN 111351609 A CN111351609 A CN 111351609A CN 202010180082 A CN202010180082 A CN 202010180082A CN 111351609 A CN111351609 A CN 111351609A
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shear stress
wall
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wall shear
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高南
刘玄鹤
王昊
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Dalian University of Technology
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    • GPHYSICS
    • G01MEASURING; TESTING
    • G01LMEASURING FORCE, STRESS, TORQUE, WORK, MECHANICAL POWER, MECHANICAL EFFICIENCY, OR FLUID PRESSURE
    • G01L11/00Measuring steady or quasi-steady pressure of a fluid or a fluent solid material by means not provided for in group G01L7/00 or G01L9/00
    • G01L11/002Measuring steady or quasi-steady pressure of a fluid or a fluent solid material by means not provided for in group G01L7/00 or G01L9/00 by thermal means, e.g. hypsometer
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01MTESTING STATIC OR DYNAMIC BALANCE OF MACHINES OR STRUCTURES; TESTING OF STRUCTURES OR APPARATUS, NOT OTHERWISE PROVIDED FOR
    • G01M10/00Hydrodynamic testing; Arrangements in or on ship-testing tanks or water tunnels
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N11/00Investigating flow properties of materials, e.g. viscosity, plasticity; Analysing materials by determining flow properties

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Abstract

本发明提供了一种壁面切应力矢量的测量方法,属于流体力学实验技术领域。本发明的壁面切应力矢量测量方法使用的测量结构由两个安装在壁面上的相互垂直的免标定热膜传感器构成。这两个传感器的尺寸和结构完全相同。传感器的免标定原理采用双层镍箔来阻隔作为敏感元件的热膜向壁面的热传递的方法实现。采集这两个传感器的电压电流并对两个传感器的发热功率加以计算,结合两个传感器安装的位置关系,可以推算出壁面切应力的大小和方向。该方法无需标定即可测量壁面切应力的大小和方向。

Figure 202010180082

The invention provides a method for measuring wall shear stress vector, which belongs to the technical field of fluid mechanics experiment. The measurement structure used in the method for measuring the wall shear stress vector of the present invention is composed of two calibration-free hot film sensors installed on the wall surface perpendicular to each other. The two sensors are identical in size and construction. The principle of free calibration of the sensor is realized by using double-layer nickel foil to block the heat transfer from the thermal film as the sensitive element to the wall. Collect the voltage and current of the two sensors and calculate the heating power of the two sensors. Combined with the positional relationship between the two sensors, the magnitude and direction of the wall shear stress can be calculated. This method can measure the magnitude and direction of wall shear stress without calibration.

Figure 202010180082

Description

一种壁面切应力矢量的测量方法A Measurement Method of Wall Shear Stress Vector

技术领域technical field

本发明属于流体力学实验技术领域,涉及一种壁面切应力的矢量测量方法,用于测量流场中壁面的切应力的大小和方向。The invention belongs to the technical field of fluid mechanics experiments, and relates to a vector measurement method of wall shear stress, which is used to measure the magnitude and direction of wall shear stress in a flow field.

背景技术Background technique

壁面切应力是流场中壁面的重要参数,它能确定壁面粘性力和壁面附近速度的分布,测量壁面切应力的方法有在壁面上直接测量方法和测量与壁面切应力相关的物理量的间接测量方法。其中,采用热交换原理的微机电传感器在测量领域得到了广泛的应用。在热交换原理的传感器中,一种无需标定的壁面切应力传感器可以对壁面切应力的大小进行测量,但该传感器无法识别壁面切应力的方向。The wall shear stress is an important parameter of the wall in the flow field. It can determine the distribution of the viscous force on the wall and the velocity near the wall. The methods of measuring the wall shear stress include direct measurement on the wall and indirect measurement of physical quantities related to the wall shear stress. method. Among them, the microelectromechanical sensor using the principle of heat exchange has been widely used in the field of measurement. In the heat exchange principle sensor, a non-calibrated wall shear stress sensor can measure the magnitude of the wall shear stress, but the sensor cannot identify the direction of the wall shear stress.

发明内容SUMMARY OF THE INVENTION

本发明提出一种壁面切应力矢量的测量方法,可以测量流场中壁面切应力的大小和方向。The invention provides a method for measuring the wall shear stress vector, which can measure the magnitude and direction of the wall shear stress in the flow field.

本发明的技术方案:Technical scheme of the present invention:

一种壁面切应力矢量的测量方法:所述的测量方法由两个尺寸和结构均相同的安装在壁面上的相互垂直的免标定热膜传感器构成的测量结构组成。方向范围在两个传感器之间的待测壁面切应力作用在这种测量结构上,此时组成这个测量结构的每个免标定热膜传感器的电压和电流与两个因素相关:一是壁面切应力的大小,二是壁面切应力的方向与免标定热膜传感器安装方向的夹角。结合两个免标定热膜传感器的电压和电流,得出两个传感器的加热功率,可以计算出壁面切应力的大小和方向。A method for measuring the shear stress vector of a wall surface: the measuring method consists of two measuring structures consisting of two perpendicular calibration-free hot film sensors installed on the wall surface with the same size and structure. The wall shear stress to be measured between the two sensors in the direction range acts on this measurement structure. At this time, the voltage and current of each calibration-free hot film sensor composing this measurement structure are related to two factors: one is the wall shear stress. The size of the stress, the second is the angle between the direction of the wall shear stress and the installation direction of the calibration-free thermal film sensor. Combining the voltage and current of the two calibration-free hot film sensors, the heating power of the two sensors is obtained, and the magnitude and direction of the wall shear stress can be calculated.

本发明的有益效果:本发明通过构建两个安装在壁面上的相互垂直的免标定热膜传感器组成的测量结构,结合这两个传感器的加热功率,即可计算出测量结构位置处的壁面切应力的大小和方向,仅靠对测量结构中传感器电压和电流的测量即可实现测量,在使用中不需要对测量结构进行标定,适用于需要测量壁面切应力的大小和方向但又不方便进行标定的场合。Beneficial effects of the present invention: The present invention constructs a measurement structure composed of two calibration-free thermal film sensors installed on the wall surface perpendicular to each other, and combines the heating power of the two sensors to calculate the wall surface cut at the position of the measurement structure. The magnitude and direction of the stress can be measured only by measuring the voltage and current of the sensor in the measuring structure. It is not necessary to calibrate the measuring structure in use. It is suitable for measuring the magnitude and direction of the wall shear stress but it is not convenient to carry out the case of calibration.

附图说明Description of drawings

图1是免标定热膜传感器的结构原理图。Figure 1 is a schematic diagram of the structure of a calibration-free hot film sensor.

图2是两个免标定热膜传感器的安装位置图。Figure 2 is the installation position diagram of two calibration-free hot film sensors.

具体实施方式Detailed ways

以下结合附图及技术方案,进一步说明本发明的具体实施方式。The specific embodiments of the present invention will be further described below with reference to the accompanying drawings and technical solutions.

热交换原理的免标定热膜切应力传感器的示意图如图1所示。传感器由两片镍箔和一层聚酰亚胺薄膜构成,将两片镍箔通电加热至同一温度,其中一片镍箔与流场中的流体直接接触,与流体热交换,作为敏感元件。另一片镍箔安装在聚酰亚胺薄膜另一侧的对应位置,作为敏感元件的衬底,并使两片镍箔工作在同一温度下。这样敏感元件向壁面传导的热量就可以减小至几乎为零。这时热膜的发热功率Q与壁面切应力存在以下关系:The schematic diagram of the calibration-free thermal film shear stress sensor based on the principle of heat exchange is shown in Figure 1. The sensor consists of two nickel foils and a layer of polyimide film. The two nickel foils are energized and heated to the same temperature. One of the nickel foils is in direct contact with the fluid in the flow field and exchanges heat with the fluid as a sensitive element. Another piece of nickel foil is installed at the corresponding position on the other side of the polyimide film, as the substrate of the sensitive element, and makes the two pieces of nickel foil work at the same temperature. In this way, the heat conducted by the sensitive element to the wall can be reduced to almost zero. At this time, the heating power Q of the thermal film has the following relationship with the wall shear stress:

Figure BDA0002412202560000021
Figure BDA0002412202560000021

其中根据换热理论推导:Which is derived from the heat transfer theory:

Figure BDA0002412202560000022
Figure BDA0002412202560000022

其中,Tf是镍箔温度,Ta是流体温度,w是镍箔宽度,l是镍箔长度,k、ρ、Cp、μ分别是流体的导热系数、密度、比热容和粘度;where Tf is the temperature of the nickel foil, Ta is the temperature of the fluid, w is the width of the nickel foil, l is the length of the nickel foil, and k, ρ, Cp, and μ are the thermal conductivity, density, specific heat capacity and viscosity of the fluid, respectively;

根据电阻温度系数公式,镍箔的温度Tf使用以下公式推算出来:According to the formula for the temperature coefficient of resistance, the temperature Tf of the nickel foil is calculated using the following formula:

Figure BDA0002412202560000023
Figure BDA0002412202560000023

其中,Tf是镍箔温度,T0是镍箔在室温下的温度,α是镍的电阻温度系数,R0是镍箔在常温下的电阻,R是镍箔在工作状态下的电阻。通过对电流的控制和电阻的测量可以把两片镍箔加热至同一温度,作为敏感元件的热膜与壁面的热传递即可忽略。Among them, T f is the temperature of the nickel foil, T 0 is the temperature of the nickel foil at room temperature, α is the temperature coefficient of resistance of nickel, R 0 is the resistance of the nickel foil at room temperature, and R is the resistance of the nickel foil in the working state. By controlling the current and measuring the resistance, the two pieces of nickel foil can be heated to the same temperature, and the heat transfer between the thermal film and the wall as a sensitive element can be ignored.

上述分析是建立在来流方向与传感器法向夹角为零的情况下的结论,当来流方向与传感器法向方向夹角为α时,根据换热理论,可以得出:The above analysis is based on the conclusion that the angle between the incoming flow direction and the normal direction of the sensor is zero. When the angle between the incoming flow direction and the normal direction of the sensor is α, according to the heat transfer theory, it can be concluded that:

Figure BDA0002412202560000031
Figure BDA0002412202560000031

可见,当来流方向与传感器法线方向有夹角时,热膜的加热功率与夹角为零的情况相比,乘以夹角余弦值的三分之一次方即为此时的加热功率。It can be seen that when there is an angle between the incoming flow direction and the normal direction of the sensor, the heating power of the thermal film is compared with the case where the angle is zero, and the heating power is multiplied by the third power of the cosine value of the angle at this time. power.

本发明提出的测量结构由两个贴装在壁面上的免标定热膜传感器组成,这两个热膜传感器对称安装,相互垂直,如图2所示。其中,两个热膜传感器的法向与来流方向的夹角分别为α1和α2,壁面切应力与两个传感器对称轴的夹角为β,两个传感器的工作温度相同,均为Tf,则根据公式(4),两个热膜传感器的发热功率Q1和Q2可以表示为以下形式The measurement structure proposed by the present invention is composed of two calibration-free thermal film sensors mounted on the wall surface. The two thermal film sensors are installed symmetrically and perpendicular to each other, as shown in FIG. 2 . Among them, the angle between the normal direction and the incoming flow direction of the two hot film sensors is α 1 and α 2 respectively, the angle between the wall shear stress and the symmetry axis of the two sensors is β, and the working temperature of the two sensors is the same, both T f , then according to formula (4), the heating powers Q 1 and Q 2 of the two thermal film sensors can be expressed in the following form

Figure BDA0002412202560000032
Figure BDA0002412202560000032

Figure BDA0002412202560000033
Figure BDA0002412202560000033

在实际应用中,Q1和Q2是通过热膜的电压和电流可以直接测量和计算,公式(5)和(6)中的未知量为切应力和夹角,由示意图中的几何关系, In practical applications, Q1 and Q2 are the voltages and currents through the hot film that can be directly measured and calculated. The unknowns in equations (5) and (6) are the shear stress and the included angle. From the geometric relationship in the schematic diagram,

α1=β-45° (7)α 1 =β-45° (7)

α2=β+45° (8)α 2 =β+45° (8)

将该角度关系代入,得到Substitute this angle relationship into the

Figure BDA0002412202560000034
Figure BDA0002412202560000034

Figure BDA0002412202560000041
Figure BDA0002412202560000041

即通过测量两个传感器的发热功率,可得到壁面切应力的大小和方向。That is, by measuring the heating power of the two sensors, the magnitude and direction of the wall shear stress can be obtained.

Claims (1)

1.一种壁面切应力矢量的测量方法,其特征在于,该测量方法使用两个安装在壁面上的相互垂直的热膜传感器进行测量;两个热膜传感器的尺寸和结构完全相同;热膜传感器根据加热功率与壁面切应力的关系来测量壁面切应力的大小;热膜传感器使用工作在同一温度下的双层镍箔实现,以阻隔作为敏感元件的镍箔与壁面之间的热传递,以实现传感器的免标定测量;通过对两个热膜传感器的加热功率的换算,得出壁面切应力的大小和方向;两个热膜传感器的加热功率分别为Q1和Q2,壁面切应力的方向β和大小τw分别为:1. a method for measuring wall shear stress vector, characterized in that the measuring method uses two mutually perpendicular hot film sensors installed on the wall surface to measure; the size and structure of the two hot film sensors are exactly the same; the hot film The sensor measures the shear stress of the wall according to the relationship between the heating power and the shear stress of the wall; the hot film sensor is realized by double-layer nickel foil working at the same temperature to block the heat transfer between the nickel foil as a sensitive element and the wall, In order to realize the calibration-free measurement of the sensor; through the conversion of the heating power of the two hot film sensors, the magnitude and direction of the wall shear stress are obtained; the heating power of the two hot film sensors are Q 1 and Q 2 respectively, and the wall shear stress The direction β and size τ w are respectively:
Figure FDA0002412202550000011
Figure FDA0002412202550000011
Figure FDA0002412202550000012
Figure FDA0002412202550000012
式中:Q1和Q2表示热膜传感器的发热功率;A为根据传感器尺寸和工作温差通过换热理论推导出的常数。In the formula: Q 1 and Q 2 represent the heating power of the hot film sensor; A is a constant derived from the heat transfer theory according to the sensor size and the working temperature difference.
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