Show that the Stokes equation: ∇ = ( ∂/∂x,∂/∂y,∂/∂z) ρv ̇=-∇p+η∇^2 v can be written as: ρv ̇= - ∂ p / ∂x_1 + η ∂^2 v_1 / ∂x^2 whch is the fluid motion equation. η∇^2 v = ∇p ∇ . v = 0 (dot product is zero) Ω = ∇ ⋀ v (curl of velocity vector) can be written as follows for an incompressible fluid, where Ω is vorticity. ρv ̇=-∇p-η∇ ⋀ Ω -∇p=-∂p/∂x_i ⋀ is the cross product η is the dynamic of shear viscosity, viscosity is a measure of a fluid's resistance to shear deformation. [Newtonian fluids] where v is velocity vector, where v = (v_i , v_j , v_k) where i is in the x direction, j in the y direction and k in the z direction. ρ is mass density p is pressure incompressibility is when: ∂v_i/∂x_i + ∂v_j/∂x_j + ∂v_k/∂x_k = 0
Question
Show that the Stokes equation:
∇ = ( ∂/∂x,∂/∂y,∂/∂z)
ρv ̇=-∇p+η∇^2 v
can be written as:
ρv ̇= - ∂ p / ∂x_1 + η ∂^2 v_1 / ∂x^2 whch is the fluid motion equation.
η∇^2 v = ∇p ∇ . v = 0 (dot product is zero) Ω = ∇ ⋀ v (curl of velocity vector)
can be written as follows for an incompressible fluid, where Ω is vorticity.
ρv ̇=-∇p-η∇ ⋀ Ω
-∇p=-∂p/∂x_i
⋀ is the cross product η is the dynamic of shear viscosity, viscosity is a measure of a fluid's resistance to shear deformation. [Newtonian fluids]
where v is velocity vector, where v = (v_i , v_j , v_k) where i is in the x direction, j in the y direction and k in the z direction.
ρ is mass density p is pressure
incompressibility is when: ∂v_i/∂x_i + ∂v_j/∂x_j + ∂v_k/∂x_k = 0
Solution
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