BIOS said:
I don't understand your question, you use many symbols without explaining them.
I don't have a question, maybe you mean something else? I'm sorry, I assumed you were already familiar with the usual notation: m=mass,g=gravity,V (and U)=velocity,d=diameter,\mu=viscosity,\rho=density. The subscript 'p' stands for particle, 'g' for gas. The index 'i' means the component in direction 'i'.
Could you answer my following questions please?
1) The drag force is calculated by either Stoke's law or Drag Force equation, depending on the particles and Re. Because we are talking about small particles in low velocities, we only apply Stokes law and NOT Drag Force equation (with the Drag Coefficient in it). Right?
You always use a drag force equation, it is just that the drag force equation is Stokes drag when the Reynolds number is smaller than 1. If your Reynolds number is smaller than 1, then C=1 in the equation above.
2) The equation of Stoke's Drag Force shows that Force is proportional to the relative velocity of the fluid to the particle. Is this a vector equation?? Ie. what if the particle moves down and the fluid moves horizontally?
The equation of motion is a vector equation, you need an equation for each of the directions. In 3-D, you need an equation for the x,y, and z-direction. If a particle moves down and the fluid moves horizontally, then it can move in at least 2 directions, so you need at least 2 equations of motion.
3) What is the point to calculate terminal velocity? How is terminal velocity and horizontal displacement relate?
What do you mean with 'what is the point'? Terminal velocity says that the net forces on the particle are zero, so in your example, assuming your particle is much heavier than air and there are no pressure gradients, the gravitational force balances the drag force in the vertical direction. In horizontal direction, the only force (in my equation at least) is the drag force, and the drag force is zero when the particle moves with the local gas velocity. The local gas velocity is therefore the terminal velocity in the horizontal direction.