CN116227176A - Combined structure and design method of square column vortex induced oscillation suppression with flexible plate behind - Google Patents
Combined structure and design method of square column vortex induced oscillation suppression with flexible plate behind Download PDFInfo
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Abstract
Description
技术领域technical field
本发明涉及海洋工程技术领域,具体涉及一种后置柔性板的方柱涡激振荡抑制组合结构及其设计方法。The invention relates to the technical field of marine engineering, in particular to a square column vortex-induced oscillation suppression combined structure with a rear flexible plate and a design method thereof.
背景技术Background technique
方柱的涡激振荡是方柱绕流过程中两侧及尾部产生交替脱落的涡旋,涡脱落产生的周期性力使弹性或弹性支撑的方柱受迫振动,方柱的振动又会影响尾流场特性,形成复杂的含被动运动的流固耦合问题。当共振现象发生时,即方柱振动频率与涡脱频率相近时,结构发生大幅振荡,严重影响结构的稳定性和安全性。The vortex-induced oscillation of the square column is the vortex that alternately falls off on both sides and the tail during the flow around the square column. The periodic force generated by the vortex shedding makes the elastic or elastically supported square column forced to vibrate, and the vibration of the square column will affect the flow rate of the square column. The characteristics of the wake field form a complex fluid-solid coupling problem with passive motion. When the resonance phenomenon occurs, that is, when the vibration frequency of the square column is close to the frequency of the vortex shedding, the structure will vibrate greatly, seriously affecting the stability and safety of the structure.
方柱的涡激振荡研究表明,流体流过方柱时,方柱会受到流向的阻力和与流向垂直的升力作用,其中升力是涡脱落产生的脉动引起的,而阻力分为涡脱落使方柱前后出现压力差导致的压差阻力和粘性作用产生的粘性阻力。在涡激振荡中,振动主要表现为方柱在升力方向的振荡。工程中,海洋平台支架、桥梁由于长期的涡激振荡,不仅可能破坏结构稳定性,如果发生共振将造成结构损坏,因此涡激振荡抑制具有重要的应用价值和研究意义。The research on the vortex-induced oscillation of the square column shows that when the fluid flows through the square column, the square column will be subjected to the resistance of the flow direction and the lift force perpendicular to the flow direction. The lift force is caused by the pulsation generated by vortex shedding, and the resistance is divided into square Pressure difference resistance caused by pressure difference before and after the column and viscous resistance caused by viscous action. In vortex-induced oscillation, the vibration is mainly manifested as the oscillation of the square column in the direction of lift force. In engineering, the long-term vortex-induced oscillation of offshore platform supports and bridges may not only damage the structural stability, but also cause structural damage if resonance occurs. Therefore, vortex-induced oscillation suppression has important application value and research significance.
在研究流场中柔性板与圆柱的耦合运动时发现,柔性结构在来流作用下被动变形,其尾部流场形成复杂多频率涡旋,与柔性结构相互作用后,对结构的动力学特性有显著影响,处于涡街中的柔性结构可以从涡街中汲取能量,在一定程度上可以减小系统受到的作用力。所以方柱若能基于柔性结构特征进行相应改进,以减小流场作用于结构上的交变力,将对理论研究和工程应用有很大助益。When studying the coupling motion of the flexible plate and the cylinder in the flow field, it is found that the flexible structure is passively deformed under the action of the incoming flow, and the flow field at the tail forms a complex multi-frequency vortex, which interacts with the flexible structure and has a significant impact on the dynamic characteristics of the structure. Significantly, the flexible structure in the vortex street can absorb energy from the vortex street, which can reduce the force on the system to a certain extent. Therefore, if the square column can be improved based on the characteristics of the flexible structure to reduce the alternating force of the flow field on the structure, it will be of great benefit to theoretical research and engineering applications.
发明内容Contents of the invention
本发明要解决的技术问题在于针对方柱涡激振荡共振时所产生的大幅振动的问题,提供一种后置柔性板的方柱涡激振荡抑制组合结构及其设计方法,从而有效抑制组合结构振荡。The technical problem to be solved by the present invention is to provide a square column vortex induced oscillation suppression combination structure and its design method with a rear flexible plate for the large vibration generated during the vortex induced oscillation resonance of the square column, so as to effectively suppress the combined structure oscillation.
本发明为解决上述提出的技术问题所采用的技术方案为:The technical scheme that the present invention adopts for solving the technical problem of above-mentioned proposal is:
一种后置柔性板的方柱涡激振荡抑制组合结构,包括方柱和设置于所述方柱后部的一柔性板,所述柔性板垂直于方柱表面设置,并置于方柱横截面边长的中点位置。A combined structure for suppressing vortex-induced oscillations of a square column with a rear flexible plate, comprising a square column and a flexible plate arranged at the rear of the square column, the flexible plate is arranged perpendicular to the surface of the square column, and placed on the side of the square column The location of the midpoint of the side length of the section.
上述方案中,所述柔性板与方柱铰链连接。In the above solution, the flexible board is hinged to the square column.
上述方案中,所述柔性板采用轻质、耐腐蚀材料。In the above solution, the flexible board is made of lightweight and corrosion-resistant materials.
相应的,本发明还提出上述后置柔性板的方柱涡激振荡抑制组合结构的设计方法,包括以下步骤:Correspondingly, the present invention also proposes a design method of the above-mentioned square column vortex induced oscillation suppression combined structure with a rear flexible plate, including the following steps:
S1、绕流中单个方柱涡激振荡数值模拟,具体包括以下步骤:S1. Numerical simulation of vortex-induced oscillation of a single square column in the flow around it, specifically including the following steps:
S1.1、建立方柱的结构与流场分析模型;S1.1. Establish the structure and flow field analysis model of the square column;
S1.2、对于方柱的纵向运动建立结构-弹簧-阻尼模型,通过计算流体力学方法对设定雷诺数Re下单个方柱绕流涡激振荡特性开展数值实验,计算方柱涡激振荡过程中受到的升力系数、阻力系数、方柱振荡无量纲幅度;S1.2. Establish a structure-spring-damping model for the longitudinal motion of the square column, and carry out numerical experiments on the vortex-induced oscillation characteristics of a single square column at a set Reynolds number Re by means of computational fluid dynamics, and calculate the vortex-induced oscillation process of the square column The lift coefficient, drag coefficient and dimensionless amplitude of square column oscillation received in
S2、绕流中方柱后置柔性板组合结构的涡激振荡数值模拟,具体包括以下步骤:S2. Numerical simulation of the vortex-induced oscillation of the composite structure with a flexible plate behind the square column in the flow, including the following steps:
S2.1、选取不同长度、不同柔度的柔性板建立方柱后置柔性板组合结构的结构与流场分析模型;S2.1. Select flexible plates with different lengths and different degrees of flexibility to establish a structural and flow field analysis model for the combined structure of the square column with flexible plates behind it;
S2.2、计算方柱后置柔性板组合结构模型在相同雷诺数Re下的涡激振荡运动,经数值实验得到后置不同长度、不同柔度的柔性板下的升力系数、阻力系数、组合结构振荡无量纲幅度;S2.2. Calculate the vortex-induced oscillation motion of the combined structure model of the square column rear flexible plate at the same Reynolds number Re. Through numerical experiments, the lift coefficient, drag coefficient, and combination of the flexible plate with different lengths and different flexibility can be obtained. Dimensionless magnitude of structural oscillations;
S3、对比单个方柱与方柱后置柔性板组合结构涡激振荡运动学及动力学响应:S3. Comparing the vortex-induced oscillation kinematics and dynamic response of a single square column and a square column rear-mounted flexible plate composite structure:
根据步骤S1和S2的计算结果,对单个方柱和不同长度、不同柔度下方柱后置柔性板组合结构的升力系数、阻力系数、振荡无量纲幅度进行对比,分析后置柔性板组合结构的减振、减阻效果;According to the calculation results of steps S1 and S2, compare the lift coefficient, drag coefficient, and dimensionless amplitude of oscillation of the single square column and the rear flexible plate composite structure of the lower column with different lengths and different flexibility, and analyze the performance of the rear flexible plate composite structure Vibration reduction and drag reduction effect;
S4、得到减振、减阻效果最好的方柱后置柔性板组合结构的模型参数。S4. Obtaining the model parameters of the combined structure with the square column and rear flexible plate with the best vibration reduction and drag reduction effects.
上述方法中,步骤S1.2中,方柱的结构-弹簧-阻尼模型在流场中的运动由纵向运动方程式(1)控制In the above method, in step S1.2, the movement of the structure-spring-damper model of the square column in the flow field is controlled by the longitudinal motion equation (1)
式中:Y为方柱振荡无量纲幅度,Y=y/D,y为方柱的纵向位移,D为方柱边长,分别表示方柱无量纲速度、方柱无量纲加速度;In the formula: Y is the dimensionless amplitude of the vibration of the square column, Y=y/D, y is the longitudinal displacement of the square column, D is the side length of the square column, Respectively represent the dimensionless velocity of the square column and the dimensionless acceleration of the square column;
ξ为阻尼比;ξ is the damping ratio;
U*为折减速度,U*=U∞/fnD,fn为方柱的固有频率,U∞为流体流速;U * is the reduction speed, U * = U ∞ /f n D, f n is the natural frequency of the square column, U ∞ is the fluid flow rate;
CL为升力系数,FL为方柱受到的升力,ρf为流体密度;C L is the lift coefficient, F L is the lift force on the square column, ρ f is the fluid density;
m*=m/ρfD2为方柱与流体的质量比,m为方柱的质量;m * =m/ρ f D 2 is the mass ratio of square column and fluid, m is the quality of square column;
流体运动通过N-S方程的求解或通过格子玻尔兹曼方法进行求解;其中,粘性不可压缩流场运动采用N-S方程:The fluid motion is solved by solving the N-S equation or by the lattice Boltzmann method; among them, the viscous incompressible flow field motion uses the N-S equation:
式中:ρf为流体密度,p为流体压力,u为速度矢量,t为时间,μ为流体动力粘度系数,f为力密度;In the formula: ρ f is fluid density, p is fluid pressure, u is velocity vector, t is time, μ is fluid dynamic viscosity coefficient, f is force density;
格子玻尔兹曼方法即,离散求解格子玻尔兹曼方程,控制方程如下:The lattice Boltzmann method is to discretely solve the lattice Boltzmann equation, and the governing equation is as follows:
fα(x+eαδt,t+δt)=fα(x,t)+Φα (4)f α (x+e α δ t ,t+δ t )=f α (x,t)+Φ α (4)
式中:δt为时间步长,α代表离散晶格方向,eα为晶格速度向量,Φα表示碰撞项与外力项,fα为密度分布函数,x为欧拉点位置坐标,t为时间;In the formula: δ t is the time step, α represents the discrete lattice direction, e α is the lattice velocity vector, Φ α represents the collision term and external force term, f α is the density distribution function, x is the position coordinate of the Euler point, t for time;
方柱与流场的耦合选用浸入边界法,使用欧拉网格描述流场,拉格朗日网格描述结构边界,通过将复杂边界的作用转化为欧拉网格上的力源项,并用式(5)、式(6)中的Delta函数δ(x-X(s,t))将拉格朗日点与欧拉点间的力和速度进行转换:The coupling between the square column and the flow field adopts the immersed boundary method, using the Euler grid to describe the flow field, and the Lagrangian grid to describe the structural boundary. By converting the effect of the complex boundary into the force source item on the Euler grid, and using The Delta function δ(x-X(s,t)) in formula (5) and formula (6) converts the force and velocity between Lagrangian point and Euler point:
式中:x为欧拉点位置坐标,X为拉格朗日点位置坐标,s为拉格朗日点坐标标号,ds为拉格朗日边界的线段长度,u为速度矢量,f(x,t)为对应时刻位置的力密度,F(s,t)为固体边界点上所受的力;In the formula: x is the position coordinate of Euler point, X is the position coordinate of Lagrangian point, s is the coordinate label of Lagrangian point, ds is the line segment length of Lagrangian boundary, u is the velocity vector, f(x ,t) is the force density at the corresponding time position, F(s,t) is the force on the solid boundary point;
通过耦合求解方柱振荡方程如式(1)、流场方程如式(2)-(3)或(4),计算得到方柱的升力系数CL、阻力系数CD,方柱振荡无量纲幅度Y。By coupling and solving the square column oscillation equation such as formula (1) and the flow field equation such as formula (2)-(3) or (4), the lift coefficient C L and drag coefficient C D of the square column are calculated, and the square column oscillation is dimensionless Amplitude Y.
上述方法中,步骤S2.2中,方柱后置柔性板组合结构中对于方柱的振荡及流场的求解与S1.2中单个方柱绕流涡激振荡的数值求解方法相同,方柱振荡方程如式(1)所示,流场方程如式(2)-(3)或(4);柔性板被动运动通过柔性板运动方程求解,柔性板运动方程如式(7)所示,式(8)表示柔性板的不可伸缩条件:In the above method, in step S2.2, the solution to the oscillation and flow field of the square column in the composite structure with a flexible plate behind the square column is the same as the numerical solution method for the vortex induced oscillation around a single square column in S1.2. The oscillation equation is shown in formula (1), and the flow field equation is shown in formula (2)-(3) or (4); the passive motion of the flexible plate is solved by the flexible plate motion equation, and the flexible plate motion equation is shown in formula (7), Equation (8) expresses the non-stretch condition of the flexible board:
式中:ρs为柔性板的线性密度,Xs为柔性板的位置坐标,表示物理量沿板切线方向的导数,t为时间,T为拉伸张力,Kb为弯曲刚度,Ff为流体流对板施加的力;In the formula: ρ s is the linear density of the flexible board, X s is the position coordinate of the flexible board, Indicates the derivative of the physical quantity along the tangential direction of the plate, t is the time, T is the tensile tension, K b is the bending stiffness, F f is the force exerted by the fluid flow on the plate;
方柱后置柔性板组合结构与流场的耦合选用浸入边界法,并通过如式(5)、式(6)中的Delta函数δ(x-X(s,t))进行拉格朗日点与欧拉点间的力和速度的转换;The coupling of the combined structure with the flexible plate behind the square column and the flow field adopts the immersed boundary method, and the Lagrangian point and Transformation of forces and velocities between Euler points;
通过耦合求解方柱振荡方程如式(1)所示、流场方程如式(2)-(3)或(4)所示、柔性板运动方程如式(7)所示,计算得到方柱后置柔性板组合结构的升力系数C′L、阻力系数C′D,组合结构振荡无量纲振幅Y′。Solve the oscillation equation of the square column by coupling as shown in equation (1), the flow field equation is shown in equation (2)-(3) or (4), and the motion equation of the flexible plate is shown in equation (7). The lift coefficient C′ L and the drag coefficient C′ D of the rear flexible plate composite structure, and the dimensionless amplitude Y′ of the composite structure oscillation.
上述方法中,步骤S3中,采用平均流场来分析流场特性,所述平均流场为将一个振荡周期内的流场平均。In the above method, in step S3, an average flow field is used to analyze flow field characteristics, and the average flow field is an average of the flow field within one oscillation cycle.
本发明的有益效果在于:The beneficial effects of the present invention are:
1、本发明所设计的方柱后置柔性板的涡激振荡抑制组合结构能够大幅降低结构涡激振荡幅度及时均阻力,进而有效地提高结构的稳定性和安全性。本发明提出的针对方柱后置柔性板参数设计及优化的数值分析方法可以更经济、高效、精确地设计结构形状、尺寸,不限柔性平板材料参数、尺寸、变形形状、具体安置位置,及流场环境的复杂性。1. The vortex-induced oscillation suppression combined structure of the square column rear flexible plate designed by the present invention can greatly reduce the amplitude and average resistance of the vortex-induced oscillation of the structure, thereby effectively improving the stability and safety of the structure. The numerical analysis method for the design and optimization of the parameters of the rear flexible plate of the square column proposed by the present invention can design the structural shape and size more economically, efficiently and accurately, and is not limited to the material parameters, size, deformation shape, and specific placement position of the flexible plate, and The complexity of the flow field environment.
2、根据本发明设计的最优方案中,方柱后置柔性板涡激振荡抑制结构方柱无量纲振荡幅度最多可降低76.83%,升力系数振荡幅值降低85.90%,阻力系数均值降低33.31%。在使用过程中,该方柱后置柔性板的涡激振荡抑制结构的具体参数可根据本发明所用的CFD设计方法调整至最优的状态,能够对方柱涡激振荡产生有效抑制。2. In the optimal solution designed according to the present invention, the dimensionless oscillation amplitude of the square column can be reduced by up to 76.83%, the vibration amplitude of the lift coefficient can be reduced by 85.90%, and the average value of the drag coefficient can be reduced by 33.31%. . During use, the specific parameters of the vortex-induced oscillation suppression structure with the flexible plate behind the square column can be adjusted to the optimal state according to the CFD design method used in the present invention, which can effectively suppress the vortex-induced oscillation of the square column.
3、根据本发明所设计结构适用范围广泛,可用于海洋工程、建筑等领域。3. The structure designed according to the present invention has a wide range of applications and can be used in ocean engineering, construction and other fields.
附图说明Description of drawings
下面将结合附图及实施例对本发明作进一步说明,附图中:The present invention will be further described below in conjunction with accompanying drawing and embodiment, in the accompanying drawing:
图1是本发明后置柔性板的方柱涡激振荡抑制组合结构的结构示意图;Fig. 1 is a structural schematic diagram of a square column vortex-induced oscillation suppression combined structure with a rear flexible plate of the present invention;
图2是本发明设计方法中建立的方柱的结构与流场分析模型;Fig. 2 is the structure and the flow field analysis model of the square column set up in the design method of the present invention;
图3是本发明设计方法中建立的方柱的结构-弹簧-阻尼模型;Fig. 3 is the structure-spring-damping model of the square column set up in the design method of the present invention;
图4是本发明设计方法中建立的方柱后置柔性板组合结构的结构与流场分析模型;Fig. 4 is the structure and the flow field analysis model of the square post rear flexible plate combination structure that is set up in the design method of the present invention;
图5是本发明实施例中单个方柱的平均流场涡量图;Fig. 5 is the average flow field vorticity diagram of a single square column in the embodiment of the present invention;
图6是本发明实施例中方柱后置L=1.5D,w*=1.5柔性板组合结构的平均流场涡量云图;Fig. 6 is the average flow field vorticity nephogram of the combined structure of the square column rear L=1.5D, w * =1.5 in the embodiment of the present invention;
图7是本发明实施例中单个方柱的平均流场压力云图;Fig. 7 is the average flow field pressure nephogram of a single square column in the embodiment of the present invention;
图8是本发明实施例中方柱后置L=1.5D,w*=1.5柔性板组合结构的平均流场压力云图。Fig. 8 is a cloud diagram of the average flow field pressure of the combined structure of the square column rear L = 1.5D, w * = 1.5 flexible plate in the embodiment of the present invention.
具体实施方式Detailed ways
为了对本发明的技术特征、目的和效果有更加清楚的理解,现对照附图详细说明本发明的具体实施方式。In order to have a clearer understanding of the technical features, purposes and effects of the present invention, the specific implementation manners of the present invention will now be described in detail with reference to the accompanying drawings.
如图1所示,本发明提出一种后置柔性板的方柱涡激振荡抑制组合结构,包括方柱和设置于方柱后部的一轻质、耐腐蚀柔性板,方柱与柔性板铰链连接,柔性板垂直于方柱表面设置,并置于方柱横截面边长的中点位置。方柱与柔性板为一个组合结构;其中,方柱横截面为正方形,其边长为D,方柱的质量比m*=2;柔性板的长度用L表示,柔性板的厚度相较于其长度很小,可忽略不计,在涡激振荡抑制组合结构设计中选取不同长度及不同柔度的平板进行数值实验及对比分析,从而确定其结构参数。As shown in Figure 1, the present invention proposes a square column vortex-induced oscillation suppression combined structure with a rear flexible plate, including a square column and a lightweight, corrosion-resistant flexible plate arranged at the rear of the square column, the square column and the flexible plate The hinge connection, the flexible plate is arranged perpendicular to the surface of the square column, and placed at the midpoint of the side length of the cross section of the square column. The square column and the flexible plate are a combined structure; wherein, the cross section of the square column is a square, its side length is D, and the mass ratio of the square column is m * =2; the length of the flexible plate is represented by L, and the thickness of the flexible plate is compared to Its length is very small and can be ignored. In the design of combined structure for vortex-induced oscillation suppression, plates with different lengths and different flexibility are selected for numerical experiments and comparative analysis, so as to determine its structural parameters.
相应的,本发明还提出上述后置柔性板的方柱涡激振荡抑制组合结构的设计方法,为确定该组合结构的涡激振荡抑制效果,先对单个方柱涡激振荡进行计算流体力学(CFD)数值实验,再对所设计的方柱后置柔性板组合结构进行高保真数值模拟,对比结构的升力系数、阻力系数、振荡幅度并选出涡激振荡抑制效果最优的方柱后置柔性板组合结构的结构参数。该设计方法具体包括以下步骤:Correspondingly, the present invention also proposes a design method for the above-mentioned square column vortex-induced oscillation suppression combined structure with a flexible plate at the rear. In order to determine the vortex-induced oscillation suppression effect of the combined structure, first perform computational fluid dynamics ( CFD) numerical experiments, and then carry out high-fidelity numerical simulation on the designed square column rear flexible plate composite structure, compare the lift coefficient, drag coefficient, and oscillation amplitude of the structure, and select the square column rear with the best vortex induced oscillation suppression effect. Structural parameters of flexible board composite structure. The design method specifically includes the following steps:
S1、绕流中单个方柱涡激振荡数值模拟,具体包括以下步骤:S1. Numerical simulation of vortex-induced oscillation of a single square column in the flow around it, specifically including the following steps:
S1.1、建立方柱的结构与流场分析模型。如图2所示,对流场中振荡方柱问题进行方柱的几何建模,并根据方柱的尺寸确定计算域的尺寸,在此基础上,建立振荡方柱的结构与流场分析模型。需要说明的是,图2中U∞表示流体速度,D表示方柱的边长,左侧y表示方柱y方向的位移。S1.1. Establish the structure and flow field analysis model of the square column. As shown in Figure 2, the geometric modeling of the square column is carried out for the problem of the oscillating square column in the flow field, and the size of the calculation domain is determined according to the size of the square column. On this basis, the structure and flow field analysis model of the oscillating square column is established . It should be noted that U ∞ in Figure 2 represents the fluid velocity, D represents the side length of the square column, and y on the left represents the displacement in the y direction of the square column.
S1.2、由于方柱的涡激振荡以纵向(垂直于流向,即图中所示的y方向)运动为主,故仅考虑纵向运动,对于方柱的纵向运动建立结构-弹簧-阻尼模型,通过计算流体力学(CFD)方法对设定雷诺数Re下单个方柱绕流涡激振荡特性开展数值实验,计算方柱涡激振荡过程中受到的升力系数、阻力系数、方柱振荡无量纲幅度。其中,升力系数CL=2FL/(ρfU∞ 2D),阻力系数CD=2FD/(ρfU∞ 2D),FL为方柱涡激振荡过程中受到的升力,FD为方柱涡激振荡过程中受到的阻力,U∞为流体速度,ρf为流体密度。方柱振荡无量纲幅度Y=y/D,即振幅y与方柱边长D之比。S1.2. Since the vortex-induced oscillation of the square column is mainly longitudinal (perpendicular to the flow direction, that is, the y direction shown in the figure), only the longitudinal motion is considered, and a structure-spring-damping model is established for the longitudinal motion of the square column , through computational fluid dynamics (CFD) method to carry out numerical experiments on the vortex-induced oscillation characteristics of a single square column at a set Reynolds number Re, and calculate the lift coefficient, drag coefficient, and dimensionless vibration of the square column during the vortex-induced oscillation process magnitude. Among them, the lift coefficient C L =2F L /(ρ f U ∞ 2 D), the drag coefficient C D =2F D /(ρ f U ∞ 2 D), and F L is the lift force received during the vortex induced oscillation of the square column, F D is the resistance suffered by the square column during vortex-induced oscillation, U ∞ is the fluid velocity, and ρ f is the fluid density. The dimensionless amplitude of the vibration of the square column Y=y/D, that is, the ratio of the amplitude y to the side length D of the square column.
建立的弹簧-阻尼模型如图3所示,其在流场中的运动由纵向运动方程式(1)控制The established spring-damper model is shown in Figure 3, and its motion in the flow field is controlled by the longitudinal motion equation (1)
式中:Y为方柱振荡无量纲幅度,Y=y/D,y为方柱的纵向位移,D为方柱边长,分别表示方柱无量纲速度、方柱无量纲加速度;In the formula: Y is the dimensionless amplitude of the vibration of the square column, Y=y/D, y is the longitudinal displacement of the square column, D is the side length of the square column, Respectively represent the dimensionless velocity of the square column and the dimensionless acceleration of the square column;
ξ为阻尼比;ξ is the damping ratio;
U*为折减速度,U*=U∞/fnD,fn为方柱的固有频率,U∞为流体流速;U * is the reduction speed, U * = U ∞ /f n D, f n is the natural frequency of the square column, U ∞ is the fluid flow rate;
CL为升力系数,FL为方柱受到的升力,ρf为流体密度;C L is the lift coefficient, F L is the lift force on the square column, ρ f is the fluid density;
m*=m/ρfD2为方柱与流体的质量比,m为方柱的质量。m * =m/ρ f D 2 is the mass ratio of the square column to the fluid, and m is the mass of the square column.
流体运动通过N-S方程的求解或通过格子玻尔兹曼方法进行求解。其中,粘性不可压缩流场运动采用N-S方程:The fluid motion is solved by the solution of the N-S equations or by the lattice Boltzmann method. Among them, the viscous incompressible flow field motion adopts the N-S equation:
式中:ρf为流体密度,p为流体压力,u为速度矢量,t为时间,μ为流体动力粘度系数,f为力密度。In the formula: ρ f is fluid density, p is fluid pressure, u is velocity vector, t is time, μ is fluid dynamic viscosity coefficient, f is force density.
格子玻尔兹曼方法即,离散求解格子玻尔兹曼方程,控制方程如下:The lattice Boltzmann method is to discretely solve the lattice Boltzmann equation, and the governing equation is as follows:
fα(x+eαδt,t+δt)=fα(x,t)+Φα (4)f α (x+e α δ t ,t+δ t )=f α (x,t)+Φ α (4)
式中:δt为时间步长,α代表离散晶格方向,eα为晶格速度向量,Φα表示碰撞项与外力项,fα为密度分布函数,x为欧拉点位置坐标,t为时间。In the formula: δ t is the time step, α represents the discrete lattice direction, e α is the lattice velocity vector, Φ α represents the collision term and external force term, f α is the density distribution function, x is the position coordinate of the Euler point, t for time.
方柱与流场的耦合选用浸入边界法,使用欧拉网格描述流场,拉格朗日网格描述结构边界,通过将复杂边界的作用转化为欧拉网格上的力源项,并用式(5)、式(6)中的Delta函数δ(x-X(s,t))将拉格朗日点与欧拉点间的力和速度进行转换:The coupling between the square column and the flow field adopts the immersed boundary method, using the Euler grid to describe the flow field, and the Lagrangian grid to describe the structural boundary. By converting the effect of the complex boundary into the force source item on the Euler grid, and using The Delta function δ(x-X(s,t)) in formula (5) and formula (6) converts the force and velocity between Lagrangian point and Euler point:
式中:x为欧拉点位置坐标,X为拉格朗日点位置坐标,s为拉格朗日点坐标标号,ds为拉格朗日边界的线段长度,u为速度矢量,f(x,t)为对应时刻位置的力密度,F(,t)为固体边界点上所受的力。In the formula: x is the position coordinate of Euler point, X is the position coordinate of Lagrangian point, s is the coordinate label of Lagrangian point, ds is the line segment length of Lagrangian boundary, u is the velocity vector, f(x ,t) is the force density at the corresponding time position, and F(,t) is the force on the solid boundary point.
通过耦合求解方柱振荡方程如式(1)、流场方程如式(2)-(3)或(4),计算得到方柱的升力系数CL、阻力系数CD,方柱振荡无量纲幅度Y。By coupling and solving the square column oscillation equation such as formula (1) and the flow field equation such as formula (2)-(3) or (4), the lift coefficient C L and drag coefficient C D of the square column are calculated, and the square column oscillation is dimensionless Amplitude Y.
由于方柱受到的作用力具有周期性,综合考虑后,以方柱无量纲振幅来分析方柱的振荡幅度,以升力系数振荡幅度,阻力系数均值来分析作用于方柱的水动力。Due to the periodicity of the force on the square column, after comprehensive consideration, the vibration amplitude of the square column is analyzed by the dimensionless amplitude of the square column, and the hydrodynamic force acting on the square column is analyzed by the oscillation amplitude of the lift coefficient and the mean value of the drag coefficient.
本实施例中,对于Re=150下,质量比m*=2,折减速度U*=5下的方柱绕流,单个方柱振荡无量纲幅度Y为0.46,升力系数振荡幅度为1.963,阻力系数均值为2.338。In this embodiment, for the flow around a square column under Re=150, mass ratio m * =2, and reduction velocity U * =5, the dimensionless oscillation amplitude Y of a single square column is 0.46, and the oscillation amplitude of the lift coefficient is 1.963. The average resistance coefficient is 2.338.
S2、绕流中方柱后置柔性板组合结构的涡激振荡数值模拟,具体包括以下步骤:S2. Numerical simulation of the vortex-induced oscillation of the composite structure with a flexible plate behind the square column in the flow, including the following steps:
S2.1、选取不同长度、不同柔度的柔性板建立方柱后置柔性板组合结构的结构与流场分析模型。如图4所示,基于步骤S1中方柱及计算域的尺寸,设计不同长度、不同柔度的柔性板,并将柔性板后置于方柱,在此基础上,建立流场中方柱后置柔性板组合结构的结构流场分析模型。S2.1. Select flexible plates with different lengths and different degrees of flexibility to establish a structural and flow field analysis model for the combined structure of the square column with flexible plates behind. As shown in Figure 4, based on the size of the square column and the calculation domain in step S1, design flexible plates of different lengths and different degrees of flexibility, and place the flexible plate behind the square column. On this basis, the square column in the flow field is established Structural flow field analysis model of flexible plate composite structure.
S2.2、计算方柱后置柔性板组合结构模型在相同雷诺数Re下的涡激振荡运动,经数值实验得到后置不同参数柔性板下的升力系数、阻力系数、组合结构振荡无量纲幅度。S2.2. Calculate the vortex-induced oscillation motion of the combined structure model of the square column rear flexible plate under the same Reynolds number Re. Through numerical experiments, the lift coefficient, drag coefficient, and dimensionless amplitude of the combined structure oscillation under the flexible plate with different parameters are obtained .
方柱后置柔性板组合结构中对于方柱的振荡及流场的求解与S1.2中单个方柱绕流涡激振荡的数值求解方法相同,方柱振荡方程如式(1)所示,流场方程如式(2)-(3)或(4);柔性板被动运动通过柔性板运动方程求解,柔性板运动方程如式(7)所示,式(8)表示柔性板的不可伸缩条件:The solution to the oscillation and flow field of the square column in the composite structure with a flexible plate behind the square column is the same as the numerical solution of the vortex induced oscillation around a single square column in S1.2. The oscillation equation of the square column is shown in equation (1), The flow field equation is shown in formula (2)-(3) or (4); the passive motion of the flexible plate is solved through the equation of motion of the flexible plate, the equation of motion of the flexible plate is shown in formula (7), and the formula (8) expresses the non-stretch of the flexible plate condition:
式中:ρs为柔性板的线性密度,Xs为柔性板的位置坐标,表示物理量沿板切线方向的导数,t为时间,T为拉伸张力,Kb为弯曲刚度,Ff为流体流对板施加的力;In the formula: ρ s is the linear density of the flexible board, X s is the position coordinate of the flexible board, Indicates the derivative of the physical quantity along the tangential direction of the plate, t is the time, T is the tensile tension, K b is the bending stiffness, F f is the force exerted by the fluid flow on the plate;
方柱后置柔性板组合结构与流场的耦合选用浸入边界法,并通过如式(5)、式(6)中的Delta函数δ(x-X(s,t))进行拉格朗日点与欧拉点间的力和速度的转换;The coupling of the combined structure with the flexible plate behind the square column and the flow field adopts the immersed boundary method, and the Lagrangian point and Transformation of forces and velocities between Euler points;
通过耦合求解方柱振荡方程如式(1)所示、流场方程如式(2)-(3)或(4)所示、柔性板运动方程如式(7)所示,计算得到方柱后置柔性板组合结构的升力系数C′L、阻力系数C′D,组合结构振荡无量纲幅度Y′。Solve the oscillation equation of the square column by coupling as shown in equation (1), the flow field equation is shown in equation (2)-(3) or (4), and the motion equation of the flexible plate is shown in equation (7). The lift coefficient C′ L and the drag coefficient C′ D of the combined structure of the rear flexible plate, and the dimensionless amplitude Y′ of the combined structure oscillation.
由于方柱受到的作用力具有周期性,综合考虑后,以组合结构振荡无量纲幅度来分析方柱后置柔性板组合结构中方柱振荡幅度,以升力系数振荡幅度、阻力系数均值来分析方柱后置柔性板组合结构的运动学及动力学特性。Due to the periodicity of the force on the square column, after comprehensive consideration, the vibration amplitude of the square column in the composite structure with a flexible plate behind the square column is analyzed by the dimensionless amplitude of the combined structure oscillation, and the square column is analyzed by the oscillation amplitude of the lift coefficient and the mean value of the drag coefficient. Kinematics and dynamics characteristics of rear flexible plate composite structure.
本实施例中,设计不同长度、不同柔度的柔性板。按照上述步骤S2的方法对所设计的多个方柱后置柔性板组合结构的模型进行高保真数值模拟。然后统计分析后置不同长度L、不同柔度w*的柔性板下的升力系数振荡幅度、阻力系数均值及组合机构振荡无量纲幅度。In this embodiment, flexible boards of different lengths and flexibility are designed. Perform high-fidelity numerical simulation on the designed composite structure model of multiple square columns with rear flexible plates according to the method of step S2 above. Then statistically analyze the lift coefficient oscillation amplitude, the drag coefficient average value and the dimensionless amplitude of the combined mechanism oscillation under the flexible plates with different length L and different flexibility w * .
板的柔度w*=2πfvωn,其中Kb为弯曲系数,fv为单个固定方柱的旋涡脱落频率。The flexibility of the plate w * = 2πf v ω n , where K b is the bending coefficient, and f v is the vortex shedding frequency of a single fixed square column.
柔性板设计参数中,长度L取:1.2D、1.5D、3D;柔度w*取:1、1.5、2。Among the design parameters of the flexible board, the length L is taken as: 1.2D, 1.5D, 3D; the flexibility w * is taken as: 1, 1.5, 2.
本实施例中,在相同雷诺数下,设计不同长度、不同柔度的柔性板的组合结构振荡无量纲振幅、升力系数振荡幅度、阻力系数均值如下结果如下表1:In this embodiment, under the same Reynolds number, the combined structure of flexible plates with different lengths and different pliability is designed.
表1不同方案组合结构Table 1 Combination structure of different schemes
S3、对比单个方柱与方柱后置柔性板组合结构涡激振荡运动学及动力学响应。S3. Comparing the kinematics and dynamic response of the vortex-induced oscillation between a single square column and a combined structure with a flexible plate behind the square column.
根据步骤S1和S2的计算结果,对单个方柱和不同长度、不同柔度下方柱后置柔性板组合结构的升力系数、阻力系数、振荡无量纲幅度进行对比,分析后置柔性板组合结构的减振、减阻效果。According to the calculation results of steps S1 and S2, compare the lift coefficient, drag coefficient, and dimensionless amplitude of oscillation of the single square column and the rear flexible plate composite structure of the lower column with different lengths and different flexibility, and analyze the performance of the rear flexible plate composite structure Vibration reduction and drag reduction effect.
采用平均流场来分析流场特性,其中平均流场为将一个振荡周期内的流场平均。流体流过单个方柱时,从平均流场压力云图(图7)中可见方柱前后压差较大且垂向压力作用范围较大,使得方柱周围产生较大压差阻力,从单个方柱的平均流场涡量图(图5)中可见,方柱两侧及尾部脱落的涡的区域较大,故方柱垂向振动幅值及受力较大。而从方柱后置柔性板组合结构的平均流场压力云图(图8)中可见,方柱前后压差较小且垂向压力分布范围较小,从其对应的平均流场涡量云图(图6)中可见,方柱两侧及尾部脱落的涡的范围也显著减小,从而使得方柱垂向振动幅度减小。从运动学、动力学角度分析,由步骤S1、步骤S2的结果可见,相对于单个方柱的涡激振荡,方柱后置柔性板后,方柱无量纲振荡幅度、升力系数振荡幅度、阻力系数均值均有显著降低。可见,方柱后置柔性板有优良的减振、减阻效果。The average flow field is used to analyze the flow field characteristics, where the average flow field is the average of the flow field within one oscillation period. When the fluid flows through a single square column, it can be seen from the average flow field pressure cloud diagram (Fig. 7) that the pressure difference between the front and rear of the square column is large and the vertical pressure range is large, resulting in a large pressure differential resistance around the square column. From the vorticity diagram of the average flow field of the column (Fig. 5), it can be seen that the area of the shedding vortex on both sides and the tail of the square column is relatively large, so the vertical vibration amplitude and force of the square column are relatively large. However, it can be seen from the average flow field pressure cloud diagram (Fig. 8) of the square column rear flexible plate composite structure that the pressure difference between the front and back of the square column is small and the vertical pressure distribution range is small. From the corresponding average flow field vorticity cloud diagram ( It can be seen from Fig. 6) that the scope of the shedding vortex on both sides and tail of the square column is also significantly reduced, so that the vertical vibration amplitude of the square column is reduced. From the perspective of kinematics and dynamics, it can be seen from the results of steps S1 and S2 that, compared with the vortex-induced oscillation of a single square column, the square column is placed behind the flexible plate, and the dimensionless oscillation amplitude, lift coefficient oscillation amplitude, and resistance of the square column The mean values of the coefficients were significantly reduced. It can be seen that the flexible plate behind the square column has excellent vibration and drag reduction effects.
S4、得到涡激振荡抑制结构的减振、减阻效果最好的方柱后置柔性板组合结构的模型参数。S4. Obtaining the model parameters of the combined structure with flexible plate behind the square column, which has the best vibration reduction and drag reduction effect of the vortex-induced oscillation suppression structure.
方柱后置柔性板后,方柱振荡无量纲幅度、升力系数振荡幅度、阻力系数均值相较于单个方柱均有明显降低。不同柔度的柔性平板的减振、减阻效果有所不同。数值实验结果表明,现考虑设计参数范围中,方柱后置柔性平板w*=1.5,L=1.5D下的减振、减阻效果最优。最优方案中,方柱后置柔性板涡激振荡抑制结构方柱无量纲振荡幅度最多可降低76.83%,升力系数振荡幅值降低85.90%,阻力系数均值降低33.31%。After the square column is equipped with a flexible plate, the dimensionless amplitude of vibration of the square column, the oscillation amplitude of the lift coefficient, and the mean value of the drag coefficient are all significantly lower than those of a single square column. The vibration reduction and drag reduction effects of flexible plates with different flexibility are different. Numerical experiment results show that, considering the range of design parameters now, the vibration reduction and drag reduction effects are the best under the condition of w * = 1.5, L = 1.5D and the rear flexible plate of the square column. In the optimal scheme, the vortex-induced oscillation suppression structure with the flexible plate behind the square column can reduce the dimensionless oscillation amplitude of the square column by 76.83%, the amplitude of the lift coefficient oscillation by 85.90%, and the average value of the drag coefficient by 33.31%.
因此,根据本发明设计方法所设计的方柱后置柔性板的涡激振荡抑制组合结构的具体参数结合图1如下所示:方柱边长为D,柔性平板长度L=1.5D,柔度w*=1.5。Therefore, according to the design method of the present invention, the specific parameters of the vortex-induced oscillation suppression combined structure of the square column rear flexible plate designed in conjunction with Figure 1 are as follows: the side length of the square column is D, the length of the flexible plate is L=1.5D, and the flexibility w * = 1.5.
在使用过程中,该方柱后置柔性板的涡激振荡抑制结构的具体参数可根据图1及本发明所用的CFD设计方法调整至最优的状态,能够对方柱涡激振荡产生有效抑制。During use, the specific parameters of the vortex-induced oscillation suppression structure with the flexible plate behind the square column can be adjusted to the optimal state according to Fig. 1 and the CFD design method used in the present invention, which can effectively suppress the vortex-induced oscillation of the square column.
上面结合附图对本发明的实施例进行了描述,但是本发明并不局限于上述的具体实施方式,上述的具体实施方式仅仅是示意性的,而不是限制性的,本领域的普通技术人员在本发明的启示下,在不脱离本发明宗旨和权利要求所保护的范围情况下,还可做出很多形式,这些均属于本发明的保护之内。Embodiments of the present invention have been described above in conjunction with the accompanying drawings, but the present invention is not limited to the above-mentioned specific implementations, and the above-mentioned specific implementations are only illustrative, rather than restrictive, and those of ordinary skill in the art will Under the enlightenment of the present invention, many forms can also be made without departing from the gist of the present invention and the protection scope of the claims, and these all belong to the protection of the present invention.
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| CN109799049A (en) * | 2019-03-06 | 2019-05-24 | 北京理工大学 | A kind of elastic cylinder vortex-induced vibration rule and coupling mechanism measuring method |
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| US20060089803A1 (en) * | 2002-12-27 | 2006-04-27 | Riken | Method and device for numberical analysis of flow field of non-compressive viscous fluid, directly using v-cad data |
| CN109799049A (en) * | 2019-03-06 | 2019-05-24 | 北京理工大学 | A kind of elastic cylinder vortex-induced vibration rule and coupling mechanism measuring method |
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