CN103332288B - Edge strip at trailing edge of airplane and design method thereof - Google Patents
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Abstract
一种飞机主翼后缘处的边条及其设计方法。所述边条前缘的侧表面与飞机主翼后缘的侧表面粘接,并且边条的上表面与飞机主翼的上表面光滑过渡,所述边条的下表面与飞机主翼的下表面光滑过渡,以使气流能够平顺地流过边条。当内襟翼收起时,边条的下表面与内襟翼的上表面贴合。本发明中,边条安装在飞机主翼上并与内襟翼对应,以调整后缘襟翼的缝道宽度Gf和缝道重叠量Of,在后缘襟翼大偏度状态下,控制后缘襟翼流动分离,提高飞机起飞/着陆状态的气动性能。
A side bar at the trailing edge of an aircraft main wing and a design method thereof. The side surface of the leading edge of the side strip is bonded to the side surface of the aircraft main wing trailing edge, and the upper surface of the side strip transitions smoothly with the upper surface of the aircraft main wing, and the lower surface of the side strip transitions smoothly with the lower surface of the aircraft main wing , so that the airflow can flow smoothly through the edge strip. When the inner flap is retracted, the lower surface of the side strip is attached to the upper surface of the inner flap. In the present invention, the side strips are installed on the main wing of the aircraft and correspond to the inner flaps to adjust the slot width G f and the overlap O f of the trailing edge flaps. Trailing edge flaps flow separation, improving the aerodynamic performance of the aircraft in takeoff/landing conditions.
Description
技术领域technical field
本发明涉及飞行器设计领域,具体是一种安装在飞机主翼后缘处的边条及其设计方法。The invention relates to the field of aircraft design, in particular to a side strip installed at the trailing edge of an aircraft main wing and a design method thereof.
背景技术Background technique
大型飞机由于翼载大,起飞/着陆时飞行速度低,需要很高的可用升力。现代飞机主要通过以下方法来获取高的可用升力:增加机翼弯度、增加机翼面积、流动控制等。增加机翼弯度为最常用的方法,其主要通过后缘襟翼偏转来实现。后缘襟翼偏转角度越大,机翼弯度改变就越多,飞机可用升力一般也就越高。但是,后缘襟翼可用的偏转角度是有限的。后缘襟翼处于大偏度状态时,后缘襟翼头部的压力系数峰值很高,容易在后缘襟翼上表面诱发流动分离,导致升力损失,降低飞机的起飞/着陆性能,甚至可能出现无法满足飞机起飞/着陆要求的情况。Large aircraft require high available lift due to high wing loads and low flying speeds during takeoff/landing. Modern aircraft obtain high usable lift mainly through the following methods: increasing wing camber, increasing wing area, flow control, etc. Increasing the camber of the wing is the most common method, which is mainly achieved by the deflection of the trailing edge flap. The greater the deflection angle of the trailing edge flaps, the more the wing camber changes and generally the higher the available lift for the aircraft. However, the deflection angle available for trailing edge flaps is limited. When the trailing edge flap is in a state of large deflection, the peak pressure coefficient of the trailing edge flap head is very high, and it is easy to induce flow separation on the upper surface of the trailing edge flap, resulting in loss of lift, reducing the takeoff/landing performance of the aircraft, and even possibly Circumstances arise where the aircraft takeoff/landing requirements cannot be met.
为了控制后缘襟翼大偏度状态出现的流动分离,改善飞机的起飞/着陆性能,国内外开展了大量主动/被动流动控制技术的研究。如在后缘襟翼上表面安装涡流发生器、在后缘襟翼上表面开槽进行吹气/吸气、加装等离子体激励器、铺设MEMS作动器等,均能取得一定的效果。但这些技术普遍存在使用条件苛刻、破坏襟翼原有结构、需要额外能量输入、辅助机构复杂、使用维护成本高等缺点,限制了工程实际应用。In order to control the flow separation in the large deflection state of the trailing edge flap and improve the take-off/landing performance of the aircraft, a large number of active/passive flow control technologies have been researched at home and abroad. For example, installing vortex generators on the upper surface of the trailing edge flap, slotting on the upper surface of the trailing edge flap for blowing/suction, installing plasma actuators, laying MEMS actuators, etc., can all achieve certain results. However, these technologies generally have disadvantages such as harsh conditions of use, damage to the original structure of the flap, need for additional energy input, complex auxiliary mechanisms, and high maintenance costs, which limit the practical application of engineering.
发明内容Contents of the invention
为克服现有技术中存在的使用条件苛刻、破坏襟翼原有结构、需要额外能量输入、辅助机构复杂、使用维护成本高等不足,本发明提出了一种飞机主翼后缘处的边条及其设计方法。In order to overcome the deficiencies in the prior art such as harsh service conditions, damage to the original structure of the flap, need for additional energy input, complex auxiliary mechanisms, and high maintenance costs, the present invention proposes a side strip at the trailing edge of the main wing of the aircraft and its design method.
本发明提出的飞机主翼后缘处的边条,所述边条安装在飞机主翼上并与内襟翼对应,以调整后缘襟翼的缝道宽度Gf和缝道重叠量Of,在后缘襟翼大偏度状态下,控制后缘襟翼流动分离,提高飞机起飞/着陆状态的气动性能。The side bar at the trailing edge of the main wing of the aircraft proposed by the present invention, the side bar is installed on the main wing of the aircraft and corresponds to the inner flap, so as to adjust the slot width G f and the slot overlap O f of the trailing edge flap. When the trailing edge flap is highly deflected, the flow separation of the trailing edge flap is controlled to improve the aerodynamic performance of the aircraft in the takeoff/landing state.
所述边条的后缘为弧形;该边条的展向长度l与飞机内襟翼的展向长度L相同,边条两端的宽度均为边条最大宽度D的25%;边条展向长度方向对称面处的宽度最宽,并且所述边条的最大宽度D为边条展向长度l的0.5%;边条弧形后缘的两端与所述边条最宽处之间用样条插值法光滑连接。所述边条与飞机主翼后缘配合处的厚度与该飞机主翼后缘的厚度相同,并且所述边条的上表面与下表面的型面均与所配合的飞机主翼的型面相同。The trailing edge of the side strip is arc-shaped; the spanwise length l of the side strip is the same as the spanwise length L of the flap in the aircraft, and the width at both ends of the side strip is 25% of the maximum width D of the side strip; The width at the symmetrical plane in the length direction is the widest, and the maximum width D of the side strip is 0.5% of the spanwise length l of the side strip; between the two ends of the arc-shaped trailing edge of the side strip and the widest point of the side strip Smooth connections using spline interpolation. The thickness of the joint between the side strip and the trailing edge of the main wing of the aircraft is the same as that of the trailing edge of the main wing of the aircraft, and the profile of the upper surface and the lower surface of the side strip is the same as that of the matched aircraft main wing.
所述边条前缘的侧表面与飞机主翼后缘的侧表面粘接,并且所述边条的上表面与飞机主翼的上表面光滑过渡,所述边条的下表面与飞机主翼的下表面光滑过渡,以使气流能够平顺地流过边条。当内襟翼收起时,边条的下表面与内襟翼的上表面贴合。The side surface of the leading edge of the side strip is bonded to the side surface of the aircraft main wing trailing edge, and the upper surface of the side strip is smoothly transitioned to the upper surface of the aircraft main wing, and the lower surface of the side strip is connected to the lower surface of the aircraft main wing. Smooth transitions to allow airflow to flow smoothly over the side strips. When the inner flap is retracted, the lower surface of the side strip is attached to the upper surface of the inner flap.
本发明还提出了一种所述飞机主翼后缘处边条的设计方法,其具体过程是:The present invention also proposes a method for designing side strips at the trailing edge of the main wing of the aircraft, the specific process of which is:
步骤1,确定飞机的升力。利用求解雷诺平均N-S方程的数值模拟方法,计算飞行速度V=68m/s,来流攻角a=0°~20°范围内的飞机流场。利用公式(1)得到各个攻角下的飞机升力系数Cl。Step 1, determine the lift of the aircraft. Using the numerical simulation method of solving the Reynolds average N-S equation, calculate the flight speed V=68m/s, and the flow field of the aircraft in the range of a=0°~20°. Use formula (1) to get the aircraft lift coefficient Cl at each angle of attack.
Cl=(Fy*cosa-Fx*sina)/(0.5*ρ*V2*S); (1)Cl=(F y *cosa-F x *sina)/(0.5*ρ*V 2 *S); (1)
其中:Fy是全机总的气动力在y方向的分力;Fx是全机总的气动力在x方向的分力;a为来流攻角;ρ为空气密度;V为飞机的飞行速度;S为飞机的参考面积。Among them: F y is the component force of the total aerodynamic force of the whole aircraft in the y direction; F x is the component force of the total aerodynamic force of the whole aircraft in the x direction; a is the incoming flow angle of attack; ρ is the air density; Flight speed; S is the reference area of the aircraft.
步骤2,确定后缘襟翼发生分离的范围及后缘襟翼的压力系数分布。确定来流攻角a=8°,在内襟翼表面画出表面极限流线;表面极限流线的交汇线即为内襟翼的分离线。在分离线到内襟翼前缘的距离最短位置,作内襟翼的展向剖面,剖面与内襟翼的交线即为该展向位置处的内襟翼型面。取出该型面上的压力系数Cp和型面的几何坐标(x,y),得到压力系数Cp与型面横坐标x的关系图。压力系数Cp的定义为:Step 2, determine the separation range of the trailing edge flap and the pressure coefficient distribution of the trailing edge flap. Determine the incoming flow angle of attack a=8°, draw the surface limit streamline on the surface of the inner flap; the intersection line of the surface limit streamline is the separation line of the inner flap. At the position where the distance from the separation line to the leading edge of the inner flap is the shortest, the spanwise section of the inner flap is made, and the intersection line of the section and the inner flap is the inner flap profile at the spanwise position. Take out the pressure coefficient Cp on the profile surface and the geometric coordinates (x, y) of the profile surface, and obtain the relationship diagram between the pressure coefficient Cp and the profile abscissa x. The pressure coefficient Cp is defined as:
Cp=(Pressure-Preference)/(0.5*ρ*V2); (2)Cp=(Pressure-Preference)/(0.5*ρ*V 2 ); (2)
其中:Pressure为展向剖面处的内襟翼型面各坐标点上的压力;Preference为参考压力,取标准大气压。Among them: Pressure is the pressure on each coordinate point of the inner flap profile at the spanwise section; Preference is the reference pressure, which is the standard atmospheric pressure.
步骤3,确定边条的展向长度。根据步骤2得到内襟翼分离线,在所述内襟翼分离线沿展向的起止范围内,按照边条沿展向的起止位置与内襟翼分离线沿展向的起止位置一致的原则,确定边条的展向长度。Step 3, determine the spanwise length of the side strips. Obtain the inner flap separation line according to step 2, within the spanwise start and end range of the inner flap separation line, follow the principle that the spanwise start and end positions of the side strips are consistent with the spanwise start and end positions of the inner flap separation line , to determine the spanwise length of the strip.
步骤4,确定边条最大宽度的取值范围。将内襟翼分离线与内襟翼前缘距离最短处的展向位置规定为边条最大宽度D的所在位置。Step 4, determine the value range of the maximum width of the side bar. The spanwise position of the shortest distance between the separation line of the inner flap and the leading edge of the inner flap is defined as the position of the maximum width D of the side bar.
步骤5,确定边条两端的宽度。所述边条两端的宽度为边条最大宽度D的20~30%。Step 5, determine the width of both ends of the side strip. The width of both ends of the side strip is 20-30% of the maximum width D of the side strip.
步骤6,校核边条对飞机升力的影响。所述边条的最大宽度D=Dmax。根据步骤4和步骤5确定的边条的最大宽度D和边条两端的宽度,通过样条插值法构造出边条,并将边条加装到飞机的主翼后缘处。利用求解雷诺平均N-S方程的数值模拟方法,计算飞行速度V=68m/s,来流攻角a=0°~20°范围内的飞机流场。利用公式(1)得到各个攻角下的飞机升力系数Cl。Step 6, check the influence of the side strips on the lift of the aircraft. The maximum width D=D max of the strip. According to the maximum width D of the side strip determined in step 4 and step 5 and the widths at both ends of the side strip, the side strip is constructed by the spline interpolation method, and the side strip is added to the trailing edge of the main wing of the aircraft. Using the numerical simulation method of solving the Reynolds average NS equation, calculate the flight speed V=68m/s, and the flow field of the aircraft in the range of a=0°~20°. Use formula (1) to get the aircraft lift coefficient Cl at each angle of attack.
当边条最大宽度D=Dmax,且来流攻角a=0°~20°,若飞机升力系数最大值Clmax≥加装边条前,则边条最大宽度D满足设计要求,结束边条设计;若飞机升力系数最大值Clmax<加装边条前,则边条最大宽度D不满足气动要求,需要减小边条的最大宽度D,继续进行边条设计,进入步骤7。When the maximum width of the side strip D=D max , and the incoming flow angle of attack a=0°~20°, if the maximum lift coefficient Cl max of the aircraft ≥ before the side strip is installed, the maximum width D of the side strip meets the design requirements, and the end side strip design; if the maximum lift coefficient Cl max of the aircraft < before adding the side strips, then the maximum width D of the side strips does not meet the aerodynamic requirements, and it is necessary to reduce the maximum width D of the side strips, continue with the side strip design, and go to step 7.
步骤7,确定目标压力系数。在由步骤2得到的内襟翼型面的压力系数最小值Cpmin1加上一个增量Δ,得到新的压力系数最小值Cpmin2;Cpmin2为目标压力系数。Step 7, determine the target pressure coefficient. Add an increment Δ to the minimum pressure coefficient Cp min1 of the inner flap profile obtained in step 2 to obtain a new minimum pressure coefficient Cp min2 ; Cp min2 is the target pressure coefficient.
步骤8,调整边条的最大宽度。边条最大宽度D的调整量记为ΔD。ΔD的取值范围为[0,Dmax]。边条两端的宽度仍取为边条最大宽度D的20~30%。经过调整后的边条最大宽度D=Dmax-ΔD。通过样条插值法构造出边条,并将边条加装到飞机的主翼后缘处。利用求解雷诺平均N-S方程的数值模拟方法,计算飞行速度V=68m/s,来流攻角a=8°的飞机流场。采用与步骤2相同的方法,得到边条最大宽度D所在展向位置处的内襟翼型面的压力系数最小值Cpmin_ΔD。其与目标压力系数的差值ΔCp=Cpmin2-Cpmin_ΔD。Step 8, adjust the maximum width of the side bar. The adjustment amount of the maximum width D of the side bar is recorded as ΔD. The value range of ΔD is [0, D max ]. The width at both ends of the side strip is still taken as 20-30% of the maximum width D of the side strip. The adjusted maximum width of the side bar D=D max -ΔD. The side strips are constructed by the spline interpolation method, and the side strips are added to the trailing edge of the main wing of the aircraft. Using the numerical simulation method of solving the Reynolds average NS equation, the flow field of the aircraft with the flight speed V=68m/s and the incoming flow angle of attack a=8° is calculated. Using the same method as step 2, obtain the minimum pressure coefficient Cp min_ΔD of the inner flap profile at the spanwise position where the maximum width D of the side strip is located. The difference between it and the target pressure coefficient ΔCp=Cp min2 −Cp min_ΔD .
步骤9,确定目标压力系数对应的边条最大宽度。根据由步骤8得到的ΔCp的大小,利用公式(3)确定边条最大宽度D的调整量ΔD的新值。然后,重复步骤8的构造边条、流场求解和获得ΔCp过程,直至|ΔCpi+1/Cpmin2|≤0.05。Step 9, determine the maximum width of the side bar corresponding to the target pressure coefficient. According to the size of ΔCp obtained in step 8, use the formula (3) to determine the new value of the adjustment amount ΔD of the maximum width D of the side bar. Then, repeat step 8 of constructing side strips, solving flow field and obtaining ΔCp until |ΔCp i+1 /Cp min2 |≤0.05.
公式(3)为:Formula (3) is:
ΔDi+1=ΔDi/(1-k*ΔCpi/Dmax); (3)ΔD i+1 =ΔD i /(1-k*ΔCp i /D max ); (3)
其中:ΔDi为第i次的边条最大宽度的调整量;ΔDi+1为第i+1次的边条最大宽度的调整量;ΔCpi为目标压力系数Cpmin2与第i次边条最大宽度调整量对应的内襟翼型面压力系数最小值Cpmin_ΔDi的差值;Dmax为由结构约束确定的边条的最大宽度的上限;k为松弛因子,用于控制调整量ΔDi+1的大小。所述的i为边条最大宽度的调整次数。Among them: ΔD i is the adjustment amount of the maximum width of the i-th side strip; ΔD i+1 is the adjustment amount of the maximum width of the i+1-th side strip; ΔCp i is the target pressure coefficient Cp min2 and the i-th side strip The difference between the minimum pressure coefficient Cp min_ΔDi of the inner flap profile corresponding to the maximum width adjustment; D max is the upper limit of the maximum width of the side strip determined by structural constraints; k is the relaxation factor, which is used to control the adjustment ΔD i+ 1 size. The said i is the number of adjustments of the maximum width of the side bar.
经过第i+1次调整后,有如下关系式:After the i+1th adjustment, the relationship is as follows:
ΔCpi+1=Cpmin2-Cpmin_ΔDi+1; (4)ΔCp i+1 =Cp min2 -Cp min_ΔDi+1 ; (4)
公式(4)中:Cpmin_ΔDi+1为第i+1次的边条最大宽度的调整量对应的内襟翼型面压力系数最小值;ΔCpi+1为目标压力系数与第i+1次的边条最大宽度的调整量对应的内襟翼型面压力系数最小值的差值。In the formula (4): Cp min_ΔDi+1 is the minimum value of the pressure coefficient of the inner flap profile corresponding to the adjustment of the maximum width of the side bar for the i+1th time; ΔCp i+1 is the target pressure coefficient and the i+1th time The adjustment amount of the maximum width of the side strip corresponds to the difference of the minimum pressure coefficient of the inner flap profile.
当|ΔCpi+1/Cpmin2|≤0.05时,结束调整,进入步骤10。When |ΔCp i+1 /Cp min2 |≤0.05, end the adjustment and go to step 10.
步骤10,校核边条对飞机升力的影响。利用求解雷诺平均N-S方程的数值模拟方法,计算飞行速度V=68m/s,来流攻角a=0°~20°范围内的飞机流场。利用公式(1)得到各个攻角下的飞机升力系数Cl。Step 10, check the influence of the side strips on the lift of the aircraft. Using the numerical simulation method of solving the Reynolds average N-S equation, calculate the flight speed V=68m/s, and the flow field of the aircraft in the range of a=0°~20°. Use formula (1) to get the aircraft lift coefficient Cl at each angle of attack.
若飞机升力系数最大值Clmax≥加装边条前,则边条最大宽度D满足设计要求,结束边条设计;若飞机升力系数最大值Clmax<加装边条前,说明目标压力系数Cpmin2 不合理,增量Δ取值偏大,将增量Δ调整至原增量的90%,然后重新进入步骤7,继续进行边条的设计。所述的增量Δ为内襟翼型面的压力系数最小值Cpmin1的增量。If the maximum value of the aircraft lift coefficient Cl max ≥ before the addition of side strips, then the maximum width D of the side strips meets the design requirements, and the design of the side strips ends; if the maximum value of the aircraft lift coefficient Cl max < before the addition of side strips, the target pressure coefficient Cp min2 Unreasonable, the value of the increment Δ is too large, adjust the increment Δ to 90% of the original increment, and then re-enter step 7 to continue the design of the side strips. The increment Δ is the pressure coefficient of the inner flap profile Increment of minimum value Cp min1 .
本发明中,通过在某飞机的主翼后缘处加装边条,后缘襟翼的缝道参数发生了明显改变。将使用边条前的后缘襟翼缝道重叠量O1修补为使用边条后的后缘襟翼缝道重叠量O2;且O1为负值,O2为正值。随着使用边条后的后缘襟翼缝道重叠量O2修补为正值,变使用边条前的后缘襟翼缝道宽度G1为使用边条后的后缘襟翼缝道宽度G2,且G2<G1。缝道参数的这种变化产生的效果是:飞机主翼对后缘襟翼上表面流动的抑制作用加强,后缘襟翼的压力系数峰值下降,逆压梯度降低,从而原先存在于后缘襟翼上表面的流动分离得到有效控制,襟翼流动品质改善,升力增加,飞机起飞/着陆状态的气动性能提升。In the present invention, by installing side strips at the trailing edge of the main wing of an aircraft, the seam parameters of the trailing edge flaps are significantly changed. Repair the overlapping amount O1 of the trailing edge flap slot before using the side strip to the overlapping amount O2 of the trailing edge flap slot after using the side strip; and O1 is a negative value, and O2 is a positive value. As the overlapping amount O2 of the trailing edge flap slot after using the strip is repaired to a positive value, the width G1 of the trailing edge flap slot before using the strip is changed to the width G2 of the trailing edge flap slot after using the strip, And G2<G1. The effect of this change in the slot parameters is that the main wing of the aircraft suppresses the flow on the upper surface of the trailing edge flap, the peak value of the pressure coefficient of the trailing edge flap decreases, and the reverse pressure gradient decreases. The flow separation on the upper surface is effectively controlled, the flow quality of the flap is improved, the lift force is increased, and the aerodynamic performance of the aircraft in the takeoff/landing state is improved.
与现有技术相比,本发明所取得的效果表现在以下方面:Compared with prior art, the effect that the present invention obtains shows in the following aspects:
1.边条能够有效提高飞机起飞/着陆状态的气动性能。仅在某飞机的主翼后缘处加装一根边条,即可有效控制内襟翼上的流动分离,使各攻角下的升力均明显提升,尤其是攻角α=8°~12°的飞机起飞/着陆最常用状态,升力增加约4%,有效改善了飞机的起飞/着陆性能。1. The side strips can effectively improve the aerodynamic performance of the aircraft in the takeoff/landing state. Only one side strip is added to the trailing edge of the main wing of an aircraft to effectively control the flow separation on the inner flap, so that the lift force at each angle of attack is significantly improved, especially the angle of attack α=8°~12° In the most common state of aircraft takeoff/landing, the lift force is increased by about 4%, which effectively improves the takeoff/landing performance of the aircraft.
2.边条通过粘接方式安装于飞机的主翼后缘处,避免了破坏飞机原有结构的问题,特别适用于现有飞机的改进设计,且安装维护方便,工程实用性强。2. The side strips are installed on the rear edge of the main wing of the aircraft by bonding, which avoids the problem of destroying the original structure of the aircraft. It is especially suitable for the improved design of existing aircraft, and it is easy to install and maintain, and has strong engineering practicability.
3.边条有效缓和了最大升力与起飞/着陆最常用状态可用升力的矛盾。由于后缘襟翼的偏度是以保证最大升力为主要目的设计的,容易造成攻角α=8°~12°的飞机起飞/着陆最常用状态,后缘襟翼出现流动分离。使用边条可以在保证最大升力的前提下,治愈飞机起飞/着陆最常用攻角下的后缘襟翼流动分离,避免为了防止后缘襟翼分离而减小后缘襟翼偏度,导致最大升力损失的问题。3. The side strips effectively alleviate the contradiction between the maximum lift and the available lift in the most common state of takeoff/landing. Since the deflection of the trailing edge flap is mainly designed to ensure the maximum lift force, it is easy to cause the most common state of takeoff/landing of the aircraft with an angle of attack α=8°~12°, and the trailing edge flap will appear flow separation. The use of side strips can cure the flow separation of the trailing edge flaps at the most commonly used angles of attack for aircraft takeoff/landing under the premise of ensuring the maximum lift, and avoid reducing the trailing edge flap deflection in order to prevent the separation of the trailing edge flaps, resulting in maximum The issue of lift loss.
4.大型飞机的主翼后缘一般设计成为扰流板形式,因此,边条安装于主翼后缘处,一方面,可用于控制后缘襟翼流动分离,改善飞机起飞/着陆状态的气动性能;另一方面,又能增加扰流板的面积,提高扰流板的效率。4. The trailing edge of the main wing of a large aircraft is generally designed in the form of a spoiler. Therefore, the side strip is installed at the trailing edge of the main wing. On the one hand, it can be used to control the flow separation of the trailing edge flap and improve the aerodynamic performance of the aircraft in the takeoff/landing state; On the other hand, it can increase the area of the spoiler and improve the efficiency of the spoiler.
附图说明Description of drawings
附图1是边条在某飞机主翼上的应用示意图;Accompanying drawing 1 is the application schematic diagram of side bar on the main wing of certain aircraft;
附图2是加装了边条的飞机机翼局部放大图;Accompanying drawing 2 is the partially enlarged view of the aircraft wing with additional side strips;
附图3是边条与飞机主翼及后缘襟翼的位置关系示意图;Accompanying drawing 3 is a schematic diagram of the positional relationship between the side bar and the main wing of the aircraft and the trailing edge flap;
附图4是边条调整后缘襟翼缝道参数示意图;Accompanying drawing 4 is a schematic diagram of the parameters of the trailing edge flap slot for side strip adjustment;
附图5是边条的增升效果示意图;Accompanying drawing 5 is the schematic diagram of the increasing effect of the side bar;
附图6是本发明的边条设计流程图;Accompanying drawing 6 is the flow chart of side bar design of the present invention;
附图7是全机气动力分解示意图;其中:Fx是全机总的气动力在x方向的分力,Fy是全机总的气动力在y方向的分力,Flift是全机升力,Fdrag是全机阻力。Accompanying drawing 7 is a schematic diagram of the aerodynamic decomposition of the whole machine; wherein: F x is the component force of the total aerodynamic force of the whole machine in the x direction, F y is the component force of the total aerodynamic force of the whole machine in the y direction, and F lift is the component force of the total aerodynamic force of the whole machine in the y direction. Lift, F drag is the overall drag.
附图8是加装边条前的内襟翼流动特性;Accompanying drawing 8 is the flow characteristics of the inner flap before installing side strips;
附图9是内襟翼型面压力系数最小值调整示意图;Accompanying drawing 9 is a schematic diagram of adjusting the minimum value of the pressure coefficient of the inner flap profile;
附图10是加装边条后的内襟翼流动特性;Accompanying drawing 10 is the flow characteristics of the inner flap after adding the edge strip;
附图11是加装边条前/后的内襟翼型面压力系数分布对比。其中:Accompanying drawing 11 is the comparison of the pressure coefficient distribution of the inner flap profile before/after the side strip is added. in:
1.前缘缝翼;2.飞机主翼;3.后缘襟翼;4.边条;5.内襟翼;6.外襟翼;7.内襟翼表面极限流线;8.内襟翼分离线;9.加装边条前的压力系数分布;10.加装边条后的压力系数分布。1. Leading edge slat; 2. Aircraft main wing; 3. Trailing edge flap; 4. Side strip; 5. Inner flap; 6. Outer flap; 7. Limit streamline of inner flap surface; 8. Inner flap Wing separation line; 9. Pressure coefficient distribution before adding side strips; 10. Pressure coefficient distribution after adding side strips.
具体实施方式Detailed ways
如附图1,附图2所示。本实施例是一种安装在飞机主翼后缘处的边条,并且所述边条4位于该飞机主翼2与内襟翼5对应处。通过在飞机主翼2的后缘加装边条4,以调整后缘襟翼的缝道宽度Gf和缝道重叠量Of,在后缘襟翼大偏度状态下,控制后缘襟翼流动分离,提高飞机起飞/着陆状态的气动性能。As shown in accompanying drawing 1, accompanying drawing 2. This embodiment is a side strip installed at the trailing edge of the main wing of the aircraft, and the side strip 4 is located at the position corresponding to the main wing 2 and the inner flap 5 of the aircraft. By installing side strips 4 on the trailing edge of the main wing 2 of the aircraft, the slot width G f and slot overlap O f of the trailing edge flap can be adjusted, and the trailing edge flap can be controlled under the state of large deflection of the trailing edge flap. Flow separation for improved aerodynamic performance in takeoff/landing conditions.
如附图3所示。所述用于某飞机的边条4为用铝合金制成的条形板,并且所述边条4的一个侧表面为弧形,并以该弧形侧表面为所述边条4的后缘。边条4的展向长度l与飞机内襟翼5的展向长度L相同,边条4两端的宽度均为边条4最大宽度D的25%;边条4的展向长度方向对称面处的宽度最宽,并且所述边条4的最大宽度D为边条4展向长度l的0.5%;边条4弧形侧表面的两端与所述边条4最宽处之间用样条插值法光滑连接。所述边条4与飞机主翼2后缘配合处的厚度与该飞机主翼2后缘的厚度相同,并且所述边条4的上表面与下表面的型面均与所配合的飞机主翼2的型面相同。As shown in Figure 3. The side strip 4 used for a certain aircraft is a strip plate made of aluminum alloy, and one side surface of the side strip 4 is arc-shaped, and the arc-shaped side surface is used as the back of the side strip 4 edge. The spanwise length l of the side strip 4 is the same as the spanwise length L of the aircraft inner flap 5, and the width at both ends of the side strip 4 is 25% of the maximum width D of the side strip 4; The width of the side strip 4 is the widest, and the maximum width D of the side strip 4 is 0.5% of the spanwise length l of the side strip 4; Smooth connection by strip interpolation. The thickness of the place where the side strip 4 is matched with the rear edge of the aircraft main wing 2 is the same as the thickness of the aircraft main wing 2 trailing edge, and the profile of the upper surface and the lower surface of the side strip 4 is consistent with that of the matched aircraft main wing 2. The profile is the same.
将所述边条4安装在飞机主翼2后缘处,并使边条4的位置与内襟翼5的位置对应。所述边条4前缘的侧表面与飞机主翼2后缘的侧表面通过粘接的方式连接,并且所述边条4的上表面与飞机主翼2的上表面光滑过渡,所述边条4的下表面与飞机主翼2的下表面光滑过渡,以使气流能够平顺地流过边条4。当内襟翼5收起时,边条4的下表面与内襟翼5的上表面贴合。The edge strip 4 is installed at the rear edge of the main wing 2 of the aircraft, and the position of the edge strip 4 corresponds to the position of the inner flap 5 . The side surface of the front edge of the side strip 4 is connected with the side surface of the aircraft main wing 2 trailing edge by bonding, and the upper surface of the side strip 4 and the upper surface of the aircraft main wing 2 are smoothly transitioned, and the side strip 4 The lower surface of the lower surface and the lower surface of the main wing 2 of the aircraft transition smoothly, so that the airflow can flow through the side strips 4 smoothly. When the inner flap 5 is retracted, the lower surface of the edge strip 4 is attached to the upper surface of the inner flap 5 .
附图4给出了本实施例的边条用于调整后缘襟翼缝道参数的原理。从附图4中可以看到,通过在某飞机的主翼后缘加装边条,后缘襟翼的缝道参数发生了明显改变,将使用边条前的后缘襟翼缝道重叠量O1修补为使用边条后的后缘襟翼缝道重叠量O2;所述使用边条前的后缘襟翼缝道重叠量O1为负值,使用边条后的后缘襟翼缝道重叠量O2为正值。随着使用边条后的后缘襟翼缝道重叠量O2修补为正值,变使用边条前的后缘襟翼缝道宽度G1为使用边条后的后缘襟翼缝道宽度G2,且G2<G1。Accompanying drawing 4 has provided the principle that the side bar of this embodiment is used to adjust the slot parameter of trailing edge flap. It can be seen from attached drawing 4 that by installing side strips on the trailing edge of the main wing of an aircraft, the seam parameters of the trailing edge flaps have changed significantly, and the seam overlap O1 of the trailing edge flaps before the strips will be used The repair is the overlapping amount O2 of the trailing edge flap slot after using the side strip; the overlapping amount O1 of the trailing edge flap slot before using the side strip is a negative value, and the overlapping amount of the trailing edge flap slot after using the side strip O2 is a positive value. As the overlapping amount O2 of the trailing edge flap slot after using the strip is repaired to a positive value, the width G1 of the trailing edge flap slot before using the strip is changed to the width G2 of the trailing edge flap slot after using the strip, And G2<G1.
从附图5的边条增升效果示意图可以看出,在某飞机的主翼后缘加装边条以后,各攻角下的升力均有明显增加。特别是飞机起飞/着陆状态最常用攻角α=8°~12°,升力增加约4%,将有效改善飞机的起飞/着陆性能。It can be seen from the schematic diagram of the lift-increasing effect of the side strips in Figure 5 that after the side strips are installed on the trailing edge of the main wing of an aircraft, the lift force at each angle of attack is significantly increased. Especially the most commonly used angle of attack α=8°~12° in the takeoff/landing state of the aircraft, and the lift force increases by about 4%, which will effectively improve the takeoff/landing performance of the aircraft.
附图8、附图10和附图11揭示了本实施例的主翼后缘边条提高飞机起飞/着陆状态气动性能的物理机制。Accompanying drawing 8, accompanying drawing 10 and accompanying drawing 11 disclose the physical mechanism that the main wing trailing edge strip of this embodiment improves the aerodynamic performance of aircraft take-off/landing state.
从附图11给出的压力系数分布可以看到,在马赫数Ma=0.20,攻角α=8°时,某飞机在使用边条前,内襟翼型面的压力系数Cp的峰值达到了-3.4。内襟翼压力系数峰值高,会在压力系数峰值附近形成强逆压梯度,增加内襟翼发生分离的危险,这点从附图8的内襟翼流动特性上也能得到印证。From the pressure coefficient distribution given in Figure 11, it can be seen that when the Mach number Ma=0.20 and the angle of attack α=8°, the peak value of the pressure coefficient Cp of the inner flap profile reaches -3.4. The high peak pressure coefficient of the inner flap will form a strong reverse pressure gradient near the peak pressure coefficient, increasing the risk of separation of the inner flap, which can also be confirmed from the flow characteristics of the inner flap in Figure 8.
后缘襟翼的压力系数峰值高,根源在于飞机的主翼与后缘襟翼之间的缝道参数不合理,飞机的主翼对后缘襟翼上表面流动的抑制能力弱,后缘襟翼头部气流的上洗效应太强。而在飞机的主翼后缘加装了边条之后,后缘襟翼缝道重叠量Of增加,后缘襟翼缝道宽度Gf减小,飞机主翼对后缘襟翼的抑制作用明显加强。The peak value of the pressure coefficient of the trailing edge flap is high, which is rooted in the unreasonable seam parameters between the main wing and the trailing edge flap. The upwash effect of the external airflow is too strong. However, after the side strips are installed on the trailing edge of the main wing of the aircraft, the overlapping amount O f of the slots of the trailing edge flaps increases, the width G f of the slots of the trailing edge flaps decreases, and the restraining effect of the main wing on the trailing edge flaps is obviously strengthened .
附图11的压力系数分布则显示,在飞机的主翼后缘加装边条之后,内襟翼型面的压力系数峰值明显下降,从原先的-3.4降低为-2.5,有效减弱了逆压梯度,内襟翼的流动特性也因此得以改善,内襟翼上表面的分离消失,重新获得了理想的附着流动特性,如附图10所示。The distribution of the pressure coefficient in Figure 11 shows that after the side strips are installed on the trailing edge of the main wing of the aircraft, the peak value of the pressure coefficient of the inner flap profile drops significantly from the original -3.4 to -2.5, which effectively weakens the reverse pressure gradient , the flow characteristics of the inner flap are also improved, the separation of the upper surface of the inner flap disappears, and the ideal adhesion flow characteristics are regained, as shown in Figure 10.
内襟翼流动特性改善,使得绕飞机机翼的气流流速加快,反映到附图11的压力系数分布上就是飞机的主翼和前缘缝翼的压力系数峰值提高,环量增加,从而有效弥补了内襟翼的升力损失,增加了总升力,提高了飞机起飞/着陆状态的气动性能。The improvement of the flow characteristics of the inner flaps makes the air flow velocity around the wings of the aircraft faster, which is reflected in the distribution of the pressure coefficients in Figure 11, which means that the peak pressure coefficients of the main wings and leading edge slats of the aircraft increase, and the circulation increases, thus effectively making up for the The lift loss of the inner flaps increases the total lift and improves the aerodynamic performance of the aircraft in takeoff/landing conditions.
本实施例还提出了一种所述边条的设计方法,具体过程是:Present embodiment also proposes a kind of design method of described side bar, concrete process is:
步骤1,确定飞机的升力。利用求解雷诺平均N-S方程的数值模拟方法,计算飞行速度V=68m/s,来流攻角a=0°~20°范围内的飞机流场。利用公式(1),得到各个攻角下的飞机升力系数Cl。Step 1, determine the lift of the aircraft. Using the numerical simulation method of solving the Reynolds average N-S equation, calculate the flight speed V=68m/s, and the flow field of the aircraft in the range of a=0°~20°. Using formula (1), the lift coefficient Cl of the aircraft at each angle of attack is obtained.
Cl=(Fy*cosa-Fx*sina)/(0.5*ρ*V2*S); (1)Cl=(F y *cosa-F x *sina)/(0.5*ρ*V 2 *S); (1)
其中:Fy是全机总的气动力在y方向的分力;Fx是全机总的气动力在x方向的分力;a为来流攻角;ρ为空气密度;V为飞机的飞行速度;S为飞机的参考面积。全机气动力分解参见附图7。Among them: F y is the component force of the total aerodynamic force of the whole aircraft in the y direction; F x is the component force of the total aerodynamic force of the whole aircraft in the x direction; a is the incoming flow angle of attack; ρ is the air density; Flight speed; S is the reference area of the aircraft. See accompanying drawing 7 for the aerodynamic decomposition of the whole machine.
步骤2,确定后缘襟翼发生分离的范围及后缘襟翼的压力系数分布。由于飞机起飞/着陆状态最常用的来流攻角在a=8°左右。因此,确定来流攻角a=8°,利用Tecplot图形处理软件,导入由步骤1计算得到的流场结果,在内襟翼5的表面画出表面极限流线7,如附图8所示。表面极限流线7的交汇线即为内襟翼5的分离线8。得到内襟翼分离线8后,在分离线8到内襟翼5前缘的距离最短位置,作内襟翼5的展向剖面,剖面与内襟翼5的交线即为该展向位置处的内襟翼型面。取出该型面上的压力系数Cp和型面的几何坐标(x,y),得到压力系数Cp与型面横坐标x的关系图,如附图9所示。本实施例中,内襟翼分离线8到内襟翼5前缘的距离最短位置在内襟翼5展向长度方向对称面处。压力系数Cp的定义为:Step 2, determine the separation range of the trailing edge flap and the pressure coefficient distribution of the trailing edge flap. Due to the takeoff/landing status of the aircraft, the most commonly used angle of attack is around a=8°. Therefore, determine the incoming flow angle of attack a=8°, use the Tecplot graphics processing software to import the flow field results calculated in step 1, and draw the surface limit streamline 7 on the surface of the inner flap 5, as shown in Figure 8 . The intersection line of the surface limiting streamlines 7 is the separation line 8 of the inner flap 5 . After the inner flap separation line 8 is obtained, the spanwise section of the inner flap 5 is made at the shortest distance from the separation line 8 to the leading edge of the inner flap 5, and the intersection line of the section and the inner flap 5 is the spanwise position The inner flap profile at . Take out the pressure coefficient Cp on the profile surface and the geometric coordinates (x, y) of the profile surface to obtain the relationship diagram between the pressure coefficient Cp and the abscissa x coordinate of the profile surface, as shown in Figure 9. In this embodiment, the shortest distance from the inner flap separation line 8 to the leading edge of the inner flap 5 is at the symmetrical plane of the inner flap 5 in the spanwise longitudinal direction. The pressure coefficient Cp is defined as:
Cp=(Pressure-Preference)/(0.5*ρ*V2); (2)Cp=(Pressure-Preference)/(0.5*ρ*V 2 ); (2)
其中:Pressure为展向剖面处的内襟翼型面各坐标点上的压力;Preference为参考压力,取标准大气压。Among them: Pressure is the pressure on each coordinate point of the inner flap profile at the spanwise section; Preference is the reference pressure, which is the standard atmospheric pressure.
步骤3,确定边条的展向长度。根据步骤2得到内襟翼分离线8,在所述内襟翼分离线8沿展向的起止范围内,按照边条沿展向的起止位置与内襟翼分离线沿展向的起止位置一致的原则,确定边条4的展向长度。本实施例中,由于分离线8贯穿内襟翼5的整个展向方向,如附图8所示,所以边条4的展向长度l与内襟翼5的展向长度L相同。Step 3, determine the spanwise length of the side strips. According to step 2, the inner flap separation line 8 is obtained. Within the start and end range of the inner flap separation line 8 along the span direction, the start and end positions of the side strips along the span direction are consistent with the start and end positions of the inner flap separation line along the span direction. Based on the principle, determine the spanwise length of the side strip 4. In this embodiment, since the separation line 8 runs through the entire spanwise direction of the inner flap 5 , as shown in FIG. 8 , the spanwise length l of the edge strip 4 is the same as the spanwise length L of the inner flap 5 .
步骤4,确定边条最大宽度的取值范围。将内襟翼分离线8与内襟翼5前缘距离最短处的展向位置,规定为边条最大宽度D所在的位置。由于本实施例的边条4的上表面与下表面的型面均与所配合的飞机主翼2的型面相同。而在真实飞机上,主翼型面的最小厚度不应小于4mm,这就确定了边条的最大宽度D的取值上限Dmax。本实施例中,由结构约束确定的边条的最大宽度D的上限Dmax=0.8%l。因此,本实施例的边条4的最大宽度D的取值范围为[0,Dmax]。Step 4, determine the value range of the maximum width of the side bar. The spanwise position of the shortest distance between the inner flap separation line 8 and the leading edge of the inner flap 5 is defined as the position where the maximum width D of the side bar is located. Because the profiles of the upper surface and the lower surface of the side bar 4 in this embodiment are the same as the profile of the matched aircraft main wing 2 . On a real aircraft, the minimum thickness of the main airfoil should not be less than 4 mm, which determines the upper limit D max of the maximum width D of the side strip. In this embodiment, the upper limit D max of the maximum width D of the side bars determined by structural constraints is 0.8%l. Therefore, the value range of the maximum width D of the side bar 4 in this embodiment is [0, D max ].
步骤5,确定边条两端的宽度。所述边条4两端的宽度为边条最大宽度D的20~30%,以便于边条4与主翼2后缘粘接及确保粘接强度。本实施例中,取边条4两端的宽度为边条最大宽度D的25%。Step 5, determine the width of both ends of the side strip. The width of both ends of the side strip 4 is 20-30% of the maximum width D of the side strip, so as to facilitate the bonding of the side strip 4 and the rear edge of the main wing 2 and ensure the bonding strength. In this embodiment, the width at both ends of the side strip 4 is taken as 25% of the maximum width D of the side strip.
步骤6,校核边条对飞机升力的影响。所述边条的最大宽度D=Dmax。根据步骤4和步骤5确定的边条4的最大宽度D和边条4两端的宽度,通过样条插值法构造出边条4,并将边条4加装到飞机的主翼后缘2处。利用求解雷诺平均N-S方程的数值模拟方法,计算飞行速度V=68m/s,来流攻角a=0°~20°范围内的飞机流场。利用公式(1)得到各个攻角下的飞机升力系数Cl。Step 6, check the influence of the side strips on the lift of the aircraft. The maximum width D=D max of the strip. According to the maximum width D of the side bar 4 determined in step 4 and step 5 and the width at both ends of the side bar 4, the side bar 4 is constructed by the spline interpolation method, and the side bar 4 is added to the main wing trailing edge 2 of the aircraft. Using the numerical simulation method of solving the Reynolds average NS equation, calculate the flight speed V=68m/s, and the flow field of the aircraft in the range of a=0°~20°. Use formula (1) to get the aircraft lift coefficient Cl at each angle of attack.
当边条最大宽度D=Dmax,且来流攻角a=0°~20°,若飞机升力系数最大值Clmax≥加装边条前,则边条最大宽度D满足设计要求,结束边条设计;若飞机升力系数最大值Clmax<加装边条前,则边条最大宽度D不满足气动要求,需要减小边条的最大宽度D,继续进行边条设计,进入步骤7。When the maximum width of the side strip D=D max , and the incoming flow angle of attack a=0°~20°, if the maximum lift coefficient Cl max of the aircraft ≥ before the side strip is installed, the maximum width D of the side strip meets the design requirements, and the end side strip design; if the maximum lift coefficient Cl max of the aircraft < before adding the side strips, then the maximum width D of the side strips does not meet the aerodynamic requirements, and it is necessary to reduce the maximum width D of the side strips, continue with the side strip design, and go to step 7.
步骤7,确定目标压力系数。将由步骤2得到的内襟翼型面的压力系数最小值Cpmin1加上一个增量Δ,从而得到一个新的压力系数最小值Cpmin2,如附图9所示。Cpmin2称为目标压力系数。本实施例中,没有加装边条时,由步骤2得到的内襟翼5的型面压力系数最小值Cpmin1=-3.4,取增量Δ=0.9,得到目标压力系数Cpmin2=-2.5。Step 7, determine the target pressure coefficient. Add an increment Δ to the minimum pressure coefficient Cp min1 of the inner flap profile obtained in step 2 to obtain a new minimum pressure coefficient Cp min2 , as shown in Fig. 9 . Cp min2 is called the target pressure coefficient. In this embodiment, when no side strips are installed, the minimum value of the profile pressure coefficient Cp min1 of the inner flap 5 obtained in step 2 =-3.4, and the increment Δ=0.9 is taken to obtain the target pressure coefficient Cp min2 =-2.5 .
步骤8,调整边条的最大宽度。边条最大宽度D的调整量记为ΔD。ΔD的取值范围为[0,Dmax]。本实施例中,第一次调整时,取ΔD=0.2Dmax,边条两端的宽度仍取为边条最大宽度D的25%。经过调整后的边条最大宽度D=Dmax-ΔD。通过样条插值法构造出边条,并将边条加装到飞机的主翼后缘处。利用求解雷诺平均N-S方程的数值模拟方法,计算飞行速度V=68m/s,来流攻角a=8°的飞机流场。利用与步骤2相同的方法,得到边条最大宽度D所在展向位置处的内襟翼5的型面压力系数最小值Cpmin_ΔD。其与目标压力系数的差值ΔCp=Cpmin2-Cpmin_ΔD。Step 8, adjust the maximum width of the side bar. The adjustment amount of the maximum width D of the side bar is recorded as ΔD. The value range of ΔD is [0, D max ]. In this embodiment, when adjusting for the first time, ΔD=0.2D max is taken, and the width at both ends of the side bar is still taken as 25% of the maximum width D of the side bar. The adjusted maximum width of the side bar D=D max -ΔD. The side strips are constructed by the spline interpolation method, and the side strips are added to the trailing edge of the main wing of the aircraft. Using the numerical simulation method of solving the Reynolds average NS equation, the flow field of the aircraft with the flight speed V=68m/s and the incoming flow angle of attack a=8° is calculated. Using the same method as step 2, the minimum value Cp min_ΔD of the profile pressure coefficient of the inner flap 5 at the spanwise position where the maximum width D of the side strip is located is obtained. The difference between it and the target pressure coefficient ΔCp=Cp min2 −Cp min_ΔD .
步骤9,确定目标压力系数对应的边条最大宽度。根据由步骤8得到的ΔCp的大小,利用公式(3)确定边条最大宽度D的调整量ΔD的新值。然后,重复步骤8的构造边条、流场求解和获得ΔCp过程,直至|ΔCpi+1/Cpmin2|≤0.05。Step 9, determine the maximum width of the side bar corresponding to the target pressure coefficient. According to the size of ΔCp obtained in step 8, use the formula (3) to determine the new value of the adjustment amount ΔD of the maximum width D of the side bar. Then, repeat step 8 of constructing side strips, solving flow field and obtaining ΔCp until |ΔCp i+1 /Cp min2 |≤0.05.
公式(3)为:Formula (3) is:
ΔDi+1=ΔDi/(1-k*ΔCpi/Dmax); (3)ΔD i+1 =ΔD i /(1-k*ΔCp i /D max ); (3)
其中:ΔDi为第i次的边条最大宽度的调整量;ΔDi+1为第i+1次的边条最大宽度的调整量;ΔCpi为目标压力系数Cpmin2与第i次边条最大宽度调整量对应的内襟翼型面压力系数最小值Cpmin_ΔDi的差值;Dmax为由结构约束确定的边条的最大宽度的上限;k为松弛因子,用于控制调整量ΔDi+1的大小,本实施例取k=0.005。所述的i为边条最大宽度的调整次数。Among them: ΔD i is the adjustment amount of the maximum width of the i-th side strip; ΔD i+1 is the adjustment amount of the maximum width of the i+1-th side strip; ΔCp i is the target pressure coefficient Cp min2 and the i-th side strip The difference between the minimum pressure coefficient Cp min_ΔDi of the inner flap profile corresponding to the maximum width adjustment; D max is the upper limit of the maximum width of the side strip determined by structural constraints; k is the relaxation factor, which is used to control the adjustment ΔD i+ 1 , this embodiment takes k=0.005. The said i is the number of adjustments of the maximum width of the side bar.
经过第i+1次调整后,有如下关系式:After the i+1th adjustment, the relationship is as follows:
ΔCpi+1=Cpmin2-Cpmin_ΔDi+1; (4)ΔCp i+1 =Cp min2 -Cp min_ΔDi+1 ; (4)
公式(4)中:Cpmin_ΔDi+1为第i+1次的边条最大宽度的调整量对应的内襟翼型面压力系数最小值;ΔCpi+1为目标压力系数与第i+1次的边条最大宽度的调整量对应的内襟翼型面压力系数最小值的差值。In the formula (4): Cp min_ΔDi+1 is the minimum value of the pressure coefficient of the inner flap profile corresponding to the adjustment of the maximum width of the side bar for the i+1th time; ΔCp i+1 is the target pressure coefficient and the i+1th time The adjustment amount of the maximum width of the side strip corresponds to the difference of the minimum pressure coefficient of the inner flap profile.
当|ΔCpi+1/Cpmin2|≤0.05时,结束调整,进入步骤10。When |ΔCp i+1 /Cp min2 |≤0.05, end the adjustment and go to step 10.
步骤10,校核边条对飞机升力的影响。利用求解雷诺平均N-S方程的数值模拟方法,计算飞行速度V=68m/s,来流攻角a=0°~20°范围内的飞机流场。利用公式(1),得到各个攻角下飞机升力系数Cl。Step 10, check the influence of the side strips on the lift of the aircraft. Using the numerical simulation method of solving the Reynolds average N-S equation, calculate the flight speed V=68m/s, and the flow field of the aircraft in the range of a=0°~20°. Using formula (1), the lift coefficient Cl of the aircraft at each angle of attack is obtained.
若飞机升力系数最大值Clmax≥加装边条前,则边条满足设计要求,结束边条设计;若飞机升力系数最大值Clmax<加装边条前,说明目标压力系数Cpmin2不合理,增量Δ取值偏大,将增量Δ调整至原增量的90%,然后重新进入步骤7,继续进行边条的设计。所述的增量Δ为内襟翼型面的压力系数最小值Cpmin1的增量。If the maximum value of the aircraft lift coefficient Cl max ≥ before the installation of the side strips, the side strips meet the design requirements, and the design of the side strips is completed; if the maximum value of the aircraft lift coefficient Cl max < before the installation of the side strips, it means that the target pressure coefficient Cp min2 is unreasonable , the value of the increment Δ is too large, adjust the increment Δ to 90% of the original increment, and then re-enter step 7 to continue the design of the side strips. The increment Δ is the increment of the minimum pressure coefficient Cp min1 of the inner flap profile.
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US11014649B2 (en) * | 2016-06-29 | 2021-05-25 | Bombardier Inc. | Methods and systems for deploying adjacent trailing edge flaps |
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