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pinn_granular_segregation's Introduction

Overview

Understand the granular segregation and the transport equation
PINN implementation

1. Introduction

An advection-diffusion transport equation has been successfully used to model the segregation. Within this continuum framework, the concentration of species $i$ can be expressed as

$$\frac{\partial c_i}{\partial t} + {\nabla \cdot (\pmb u c_i)}={\nabla \cdot (D\nabla c_i)}.$$

With assumption of incompressible flow and negligible vertical acceleration, the above equation in the $z$ direction can be written as

$$\frac{\partial c_i}{\partial t} +\frac{\partial (w+w_{i})c_i}{\partial z}=\frac{\partial}{\partial z} \Big( D\frac{\partial c_i}{\partial z} \Big),$$

or, rearranging, as

$$ w_{i}c_i-D\frac{\partial c_i}{\partial z}=0, $$

where $w_{i}$ is the segregation velocity relative to the bulk velocity $w$.

full model simplified model
intruder scaled segregation force $$F_{i,0}$$ $$-f^g(R)\frac{\partial{p}}{\partial{z}}V_i+f^k(R)\frac{p}{\dot\gamma}\frac{\partial\dot\gamma}{\partial{z}}V_i $$
Mixture scaled segregation force $$\hat F_{l}$$
$$\hat{F}_{s}$$
$$(\hat{F}{l,0}-\cos{\theta})\textrm{tanh}\Big( \frac{\cos{\theta}-\hat{F}{s,0}}{\hat{F}{l,0}-\cos{\theta}}\frac{c_s}{c_l} \Big)$$
$$-(\hat{F}
{l,0}-\cos{\theta}){\frac{c_l}{c_s}}\textrm{tanh}\Big( \frac{\cos{\theta}-\hat{F}{s,0}}{\hat{F}{l,0}-\cos{\theta}}\frac{c_s}{c_l} \Big)$$
effective friction $$\mu_{eff}$$ $$\mu_s+\frac{\mu_2-\mu_s}{I_c/I+1}$$
viscosity $$\eta$$ $$\mu_{eff} \frac{P}{\dot\gamma}$$
drag coefficient $$c_{d,l}$$
$$c_{d,s}$$
$$[k_1-k_2\exp(-k_3 R)]+s_1 I R +s_2 I (R_\rho-1)$$
$$c_{d,l}/R^2$$
segregation velocity $$w_l$$
$$w_s$$
$$\frac{ \hat F_{l} m_l g_0}{c_{d,l} \pi \eta d_l}$$
$$-\frac{ \hat F_s m_s g_0}{c_{d,s} \pi \eta d_s}$$
$$0.26 d_s \ln R \dot\gamma (1-c_i)$$
diffusion coefficient $$D$$ $$0.042 \dot \gamma (c_ld_l+c_sd_s)^2$$ $$0.042 \dot \gamma {\bar d}^2$$

The full model prediction is compared to the previous model by Schlick et al. 2015 with different values of $\lambda$.

$$\frac{d_c}{d_z}=\frac{1}{\lambda}c_l(1-c_l)$$

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