Math Problem Statement

can i use this approach for this question? Consider steady, incompressible, axisymmetric flow (r, z) and (ur, uz) for which the stream function is defined as ur = βˆ’(1/r)(βˆ‚πœ“/βˆ‚z) and uz = (1/r)(βˆ‚πœ“/βˆ‚r). Verify that πœ“ so defined satisfies the continuity equation. What conditions or restrictions are required on πœ“?

Solution

Yes, you can use this approach to verify that the stream function ψ\psi satisfies the continuity equation for the given steady, incompressible, axisymmetric flow.

Steps to Verify

  1. Continuity Equation for Axisymmetric Flow: The continuity equation for steady, incompressible, axisymmetric flow can be expressed as: 1rβˆ‚(rur)βˆ‚r+βˆ‚uzβˆ‚z=0\frac{1}{r} \frac{\partial (r u_r)}{\partial r} + \frac{\partial u_z}{\partial z} = 0

  2. Substituting the Stream Function: Given: ur=βˆ’1rβˆ‚Οˆβˆ‚z,uz=1rβˆ‚Οˆβˆ‚ru_r = -\frac{1}{r} \frac{\partial \psi}{\partial z}, \quad u_z = \frac{1}{r} \frac{\partial \psi}{\partial r}

    We first compute rurr u_r: rur=βˆ’βˆ‚Οˆβˆ‚zr u_r = -\frac{\partial \psi}{\partial z} Then differentiate with respect to rr: βˆ‚(rur)βˆ‚r=βˆ’βˆ‚2Οˆβˆ‚zβˆ‚r\frac{\partial (r u_r)}{\partial r} = -\frac{\partial^2 \psi}{\partial z \partial r}

    Next, we compute βˆ‚uzβˆ‚z\frac{\partial u_z}{\partial z}: βˆ‚uzβˆ‚z=1rβˆ‚2Οˆβˆ‚rβˆ‚z\frac{\partial u_z}{\partial z} = \frac{1}{r} \frac{\partial^2 \psi}{\partial r \partial z}

  3. Substituting Back into the Continuity Equation: Plugging these into the continuity equation gives: 1r(βˆ’βˆ‚2Οˆβˆ‚zβˆ‚r)+1rβˆ‚2Οˆβˆ‚rβˆ‚z=0\frac{1}{r} \left(-\frac{\partial^2 \psi}{\partial z \partial r}\right) + \frac{1}{r} \frac{\partial^2 \psi}{\partial r \partial z} = 0

    Since mixed partial derivatives are equal (assuming ψ\psi is sufficiently smooth): βˆ’βˆ‚2Οˆβˆ‚zβˆ‚r+βˆ‚2Οˆβˆ‚rβˆ‚z=0-\frac{\partial^2 \psi}{\partial z \partial r} + \frac{\partial^2 \psi}{\partial r \partial z} = 0

    This confirms that the continuity equation is satisfied.

Conditions/Restrictions on ψ\psi

To ensure the validity of this approach, ψ\psi must satisfy the following conditions:

  1. Smoothness: ψ\psi should be continuously differentiable in the domain of interest, allowing for the interchange of partial derivatives.
  2. Boundary Conditions: Appropriate boundary conditions should be defined for the physical problem to ensure uniqueness of the solution.
  3. Non-singularity: The stream function should not be singular in the flow domain, particularly as rr approaches zero to avoid undefined behavior.

Would you like more details or clarification on any part of this? Here are some related questions you might consider:

  1. How do boundary conditions affect the solution for ψ\psi?
  2. Can you provide a specific example of a flow that uses this stream function?
  3. What are the implications of axisymmetry on the flow field?
  4. How does the incompressibility assumption simplify the analysis?
  5. What techniques can be used to solve for ψ\psi in practice?

Tip: Always check the physical significance of your derived equations in the context of fluid dynamics.

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Math Problem Analysis

Mathematical Concepts

Fluid Dynamics
Continuity Equation
Partial Differential Equations

Formulas

Continuity equation: (1/r)(βˆ‚(ru_r)/βˆ‚r) + (βˆ‚u_z/βˆ‚z) = 0
Stream function definitions: ur = -(1/r)(βˆ‚Οˆ/βˆ‚z), uz = (1/r)(βˆ‚Οˆ/βˆ‚r)

Theorems

Existence of stream functions in fluid dynamics
Equality of mixed partial derivatives

Suitable Grade Level

Graduate Level