论文标题

无悬崖车身的亚音线管流中的不稳定动力学

Unsteady dynamics in a subsonic duct flow with a bluff body

论文作者

George, Luckachan. K., Karthick, S. K., Srikrishnan, A. R., Kannan, R.

论文摘要

在亚音速导管流中进行了一系列对特定悬崖体型(V-GUTTER)的降低数值模拟,以评估不稳定的尾流动力学。 V-Gutter的两个几何参数有不同:V-Gutter的基本角度($θ$)和在V-Gutter的前沿处的缝隙($ξ$)的大小($ξ$)。分析了湍流运动学和压力场,以评估$ m_ \ infty = 0.25 $的自由式马赫数和基于虚张声势的横向长度(L)$ re_l = 0.1 \ 0.1 \ 0.1 \ times 10^6 $的自由式马赫数和一个自由式雷诺数。考虑了五个V-Gutter角度($θ$,$^\ circ =π/6,π/4,π/3,5π/12,π/2 $)和三个缝隙尺寸($ξ$,mm = 0,0.25,0.5)仅被视为特定$θ= [π/6] $。通常,在考虑到较高的阻力($ C_D $)和总压力损失($ΔP_0$)的最大速度和压力上的高波动。另一方面,流线型的身体($θ=π/6 $)的存在倾向于有效地稳定尾流,因此几乎产生了较低$ C_D $和$ΔP_0$的周期性脱落结构。对于$θ= [π/6] $,可以看到涡流脱落的宽光谱,峰值为$ [fl/u_ \ infty] \ sim 0.08 $。对于$θ\ geq [π/4] $,可以看到逐渐衰减的显着离散脱落频率。同样,如前所述,$ξ$对$θ= [π/6] $ case的影响会产生离散的脱落频率,而不是扩大的频率。脱落频率最大增加到$ [fl/u_ \ infty] \ sim 0.26 $,最大缝隙尺寸为$ξ= 0.5 $。还提供了更多关于脱落涡流,尾流的动量不足,流场中的能量含量以及主要时空结构的见解。

A series of reduced-order numerical simulations on a specific bluff body type (v-gutters) in a subsonic duct flow is done to assess the unsteady wake dynamics. Two of the v-gutter's geometrical parameters are varied: the v-gutter's base angle ($θ$) and the size of a slit ($ξ$) at the leading-edge of the v-gutter. Turbulent flow kinematics and pressure field are analyzed to evaluate the unsteadiness at a freestream Mach number of $M_\infty = 0.25$ and a freestream Reynolds number based on bluff body's transverse length (L) of $Re_L=0.1 \times 10^6$. Five v-gutter angles are considered ($θ$, $^\circ = π/6, π/4, π/3, 5π/12, π/2$) and three slit sizes ($ξ$, mm =0,0.25,0.5) are considered only for a particular $θ= [π/6]$. In general, high fluctuations in velocity and pressure are seen for the bluffest body in consideration ($θ= π/2$) with higher drag ($c_d$) and total pressure loss ($Δp_0$). On the other hand, the presence of a slit on a streamlined body ($θ= π/6$) tends to efficiently stabilize the wake and thus, producing almost a periodic shedding structure with lower $c_d$ and $Δp_0$. For $θ= [π/6]$, broadened spectra in vortex shedding is seen with a peak at $[fL/u_\infty] \sim 0.08$. For $θ\geq [π/4]$, a dominant discrete shedding frequency is seen with a gradual spectral decay. Similarly, the effects of $ξ$ on the $θ= [π/6]$ case produce a discrete shedding frequency instead of a broadened one, as told before. The shedding frequency increases to a maximum of $[fL/u_\infty] \sim 0.26$ for the maximum slit size of $ξ= 0.5$. More insights on the shedding vortices, momentum deficit in the wake, varying energy contents in the flow field, and the dominant spatiotemporal structures are also provided.

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