ব্যাখ্যা
For 2D flow, Ψ is constant along a streamline.
The curves Ψ = constant represent streamlines.
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For 2D flow, Ψ is constant along a streamline.
The curves Ψ = constant represent streamlines.
Definition of stream function ensures incompressibility: ∇·q = 0.
Relation: u = ∂Ψ∂y, v = −∂Ψ/∂x
u = ∂Ψ/∂y = ∂(xy)/∂y = x, v= −∂Ψ/∂x = −∂(xy)/∂x = −y
Stream function is constant along stream line.
Ψ = constant → x² + y² = constant → circles around origin
A stream function ensures continuity in 2D incompressible flow, but irrotationality requires ∇ × q = 0.
Ψ = const is always a streamline.
Stream function Ψ → continuity satisfied (incompressible)
Velocity potential φ → irrotational condition satisfied.
So both together ⇒ incompressible & irrotational.
These are the Cauchy–Riemann equations in fluid flow form.
ক) Yes, because continuity holds → Continuity is necessary but not sufficient.×
খ) Yes, because Cauchy–Riemann equations are satisfied → Correct √
গ) No, because ∇×q≠0 → vorticity is 0 ×
ঘ) No, because flow is compressible → the flow is incompressible ×
w(z) is the complex potential, widely used in potential flow theory.
qr = -cosθ, qθ = sinθ.
Check with Ψ =-rsinθ:
qr = (1/r) ∂Ψ/∂θ = (1/r)(-rcosθ) = -cosθ,
qθ = -∂Ψ /∂r = sinθ
Matches the velocity field.
Flow is irrotational but velocities vary with position → this is a pure extensional (strain) flow.
Flow is irrotational → velocity potential exists.
In 2D incompressible flow, Δψ=flow rate per unit depthΔΨ = flow rate per unit depth between two streamlines.
Continuity condition for incompressible flow.
At (x,y)=(2,1): u=−3, v=−6