← 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 13 yrs · Read the full method →

Question

For a two-dimensional potential flow, the velocity potential is given by ϕ=x2yxy2+13(x3y3)\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 q=ϕ\vec q=\nabla\phi, the velocity components are u=ϕx, v=ϕyu=\dfrac{\partial\phi}{\partial x},\ v=\dfrac{\partial\phi}{\partial y}. The stream function ψ\psi satisfies the Cauchy–Riemann relations u=ψy, v=ψxu=\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=ϕx=2xyy2+x2,u=x2+2xyy2.u=\frac{\partial\phi}{\partial x}=2xy-y^2+x^2,\qquad\boxed{u=x^2+2xy-y^2.} v=ϕy=x22xyy2,v=x22xyy2.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)

2ϕx2=ux=2x+2y,2ϕy2=vy=2x2y.\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=2ϕx2+2ϕy2=(2x+2y)+(2x2y)=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 ux+vy=0\dfrac{\partial u}{\partial x}+\dfrac{\partial v}{\partial y}=0 is satisfied:

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

Step 3 — Stream function

Integrate ψy=u=x2+2xyy2\dfrac{\partial\psi}{\partial y}=u=x^2+2xy-y^2 with respect to yy:

ψ=x2y+xy2y33+f(x).\psi=x^2y+xy^2-\frac{y^3}{3}+f(x).

Differentiate and match ψx=v\dfrac{\partial\psi}{\partial x}=-v:

ψx=2xy+y2+f(x)=!v=(x22xyy2)=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+xy213(x3+y3).  \boxed{\;\psi=x^2y+xy^2-\frac13\big(x^3+y^3\big).\;}
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