The angle between viscous force and direction of flow of liquid
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The Navier-Stokes equations then become:
ρ[∂v⃗ ∂t+(v⃗ ∇⃗ )v⃗ ]=−∇⃗ p+ηΔv⃗ +f⃗
and are simplified to:
0=η∂2v∂y2+ρgx
where gx=ρgsinθ with g the gravitational constant.
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