← 2018 Paper 2

UPSC 2018 Maths Optional Paper 2 Q8b — Step-by-Step Solution

15 marks · Section B

Potential flow · Mechanics & Fluid Dynamics · asked 10× in 14 yrs · Read the full method →

Question

For a two-dimensional potential flow, the velocity potential is given by ϕ=x2y−xy2+13(x3−y3)\phi=x^2y-xy^2+\tfrac13(x^3-y^3). Determine the velocity components along the directions xx and yy. Also, determine the stream function ψ\psi and check whether ϕ\phi represents a possible case of flow or not.

Technique

u=ϕx, v=ϕyu=\phi_x,\,v=\phi_y; possibility test ∇2ϕ=0\nabla^2\phi=0; stream function by integrating the Cauchy–Riemann relations u=ψy, v=−ψxu=\psi_y,\ v=-\psi_x.

Solution

Setup. With the convention q⃗=∇ϕ\vec q=\nabla\phi, the velocity components are u=∂ϕ∂x, v=∂ϕ∂yu=\dfrac{\partial\phi}{\partial x},\ v=\dfrac{\partial\phi}{\partial y}. The stream function ψ\psi satisfies the Cauchy–Riemann relations u=∂ψ∂y, v=−∂ψ∂xu=\dfrac{\partial\psi}{\partial y},\ v=-\dfrac{\partial\psi}{\partial x}. The flow is “possible” (incompressible) iff ϕ\phi is harmonic, ∇2ϕ=0\nabla^2\phi=0.

Step 1 — Velocity components

u=∂ϕ∂x=2xy−y2+x2,u=x2+2xy−y2.u=\frac{\partial\phi}{\partial x}=2xy-y^2+x^2,\qquad\boxed{u=x^2+2xy-y^2.} v=∂ϕ∂y=x2−2xy−y2,v=x2−2xy−y2.v=\frac{\partial\phi}{\partial y}=x^2-2xy-y^2,\qquad\boxed{v=x^2-2xy-y^2.}

Step 2 — Check whether the flow is possible (harmonic ϕ\phi)

∂2ϕ∂x2=∂u∂x=2x+2y,∂2ϕ∂y2=∂v∂y=−2x−2y.\frac{\partial^2\phi}{\partial x^2}=\frac{\partial u}{\partial x}=2x+2y,\qquad \frac{\partial^2\phi}{\partial y^2}=\frac{\partial v}{\partial y}=-2x-2y. ∇2ϕ=∂2ϕ∂x2+∂2ϕ∂y2=(2x+2y)+(−2x−2y)=0.\nabla^2\phi=\frac{\partial^2\phi}{\partial x^2}+\frac{\partial^2\phi}{\partial y^2}=(2x+2y)+(-2x-2y)=0.

Since ∇2ϕ=0\nabla^2\phi=0, the continuity equation ∂u∂x+∂v∂y=0\dfrac{\partial u}{\partial x}+\dfrac{\partial v}{\partial y}=0 is satisfied:

  ϕ is harmonic⇒ϕ represents a possible (incompressible) flow.  \boxed{\;\phi\text{ is harmonic} \Rightarrow \phi\text{ represents a possible (incompressible) flow.}\;}

Step 3 — Stream function

Integrate ∂ψ∂y=u=x2+2xy−y2\dfrac{\partial\psi}{\partial y}=u=x^2+2xy-y^2 with respect to yy:

ψ=x2y+xy2−y33+f(x).\psi=x^2y+xy^2-\frac{y^3}{3}+f(x).

Differentiate and match ∂ψ∂x=−v\dfrac{\partial\psi}{\partial x}=-v:

∂ψ∂x=2xy+y2+f′(x)=!−v=−(x2−2xy−y2)=−x2+2xy+y2.\frac{\partial\psi}{\partial x}=2xy+y^2+f'(x)\stackrel{!}{=}-v=-(x^2-2xy-y^2)=-x^2+2xy+y^2.

Comparing: f′(x)=−x2f'(x)=-x^2, so f(x)=−x33f(x)=-\dfrac{x^3}{3} (constant absorbed). Hence

Answer

  ψ=x2y+xy2−13(x3+y3).  \boxed{\;\psi=x^2y+xy^2-\frac13\big(x^3+y^3\big).\;}
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