The condition for irrotational motion
∂y∂u−∂x∂v=0
From the definition of stream function ψ, we get u=∂x∂ϕ,v=∂y∂ϕ
Thus, the velocity components become
u=∂x∂ϕ=2x,v=∂y∂ϕ=−2y+1
∂y∂u=0,∂x∂v=0
Since
∂y∂u−∂x∂v=0−0=0then ϕ=x2–y2+y represents the velocity potential for 2 dimensional Irrotational flow.
∂y∂ψ=u=2x,−∂x∂ψ=v=−2y+1Then
ψ=2xy+g(x)
∂x∂ψ=2y+g′(x)=−v=2y−1
g′(x)=−1
g(x)=−x+CStream function is
ψ=2xy−x+C
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