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Non-Newtonian stress, collisional dissipation and heat flux in the shear flow of inelastic disks: a reduction via Grad's moment method

机译:非弹性圆盘剪切流中的非牛顿应力,碰撞耗散和热通量:通过格雷德矩方法的降低

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The non-Newtonian stress tensor, collisional dissipation rate and heat flux in the plane shear flow of smooth inelastic disks are analysed from the Grad-level moment equations using the anisotropic Gaussian as a reference. For steady uniform shear flow, the balance equation for the second moment of velocity fluctuations is solved semi-analytically, yielding closed-form expressions for the shear viscosity μ, pressure p, first normal stress difference N_1 and dissipation rate D as functions of (i) density or area fraction v, (ii) restitution coefficient e, (iii) dimensionless shear rate R, (iv) temperature anisotropy η (the difference between the principal eigenvalues of the second-moment tensor) and (v) angle between the principal directions of the shear tensor and the second-moment tensor. The last two parameters are zero at the Navier-Stokes order, recovering the known exact transport coefficients from the present analysis in the limit η ?→ 0, and are therefore measures of the non-Newtonian rheology of the medium. An exact analytical solution for leading-order moment equations is given, which helped to determine the scaling relations of R, η and with inelasticity. We show that the terms at super-Burnett order must be retained for a quantitative prediction of transport coefficients, especially at moderate to large densities for small values of the restitution coefficient (e-1). Particle simulation data for a sheared inelastic hard-disk system are compared with theoretical results, with good agreement for p, μ and N_1 over a range of densities spanning from the dilute to close to the freezing point. In contrast, the predictions from a constitutive model at Navier-Stokes order are found to deviate significantly from both the simulation and the moment theory even at moderate values of the restitution coefficient (e~0.9). Lastly, a generalized Fourier law for the granular heat flux, which vanishes identically in the uniform shear state, is derived for a dilute granular gas by analysing the non-uniform shear flow via an expansion around the anisotropic Gaussian state. We show that the gradient of the deviatoric part of the kinetic stress drives a heat current and the thermal conductivity is characterized by an anisotropic second-rank tensor, for which explicit analytical expressions are given.
机译:以各向异性高斯为基准,从Grad级矩方程分析了光滑非弹性圆盘平面剪切流中的非牛顿应力张量,碰撞耗散率和热通量。对于稳定的均匀剪切流,半解析求解速度波动的第二阶矩的平衡方程,得出剪切粘度μ,压力p,第一法向应力差N_1和耗散率D作为(i的函数)的闭合表达式。 )密度或面积分数v,(ii)恢复系数e,(iii)无因次剪切速率R,(iv)温度各向异性η(第二矩张量的主特征值之差)和(v)主角之间的夹角张量和第二矩张量的方向。最后两个参数在Navier-Stokes阶上为零,从当前分析中以ηπ→0为极限恢复了已知的精确传输系数,因此是介质的非牛顿流变学的量度。给出了矩矩方程的精确解析解,这有助于确定R,η的比例关系并具有非弹性。我们表明,对于运输系数的定量预测,必须保留超伯奈特级的术语,尤其是对于恢复系数的小值(e -1),在中等到大密度下尤其如此。将剪切的非弹性硬盘系统的粒子模拟数据与理论结果进行了比较,在从稀度到接近冰点的一系列密度范围内,p,μ和N_1的一致性良好。相反,即使在恢复系数为中等值(e〜0.9)时,也发现本构模型在Navier-Stokes阶上的预测与模拟和力矩理论均存在显着偏差。最后,通过分析各向异性高斯状态附近的膨胀的非均匀剪切流,推导了稀颗粒气体的颗粒热通量的通用傅里叶定律,在均匀剪切状态下消失。我们表明,动应力的偏斜部分的梯度驱动热电流,并且热导率的特征是各向异性的二阶张量,对此给出了明确的解析表达式。

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