solve completely with complete elaboration , For a certain incompressible flow field, it is suggested that the velocity components are given by the equations u = 2xy , v = -x^2y, w = 0 Is this a physicatly possible flow field? Fxplain Hint Any plysically possible incompressible flow field must satisty conservation of mass
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solve completely with complete elaboration , For a certain incompressible flow field, it is suggested that the velocity components are given by the equations u = 2xy , v = -x^2y, w = 0 Is this a physicatly possible flow field? Fxplain Hint Any plysically possible incompressible flow field must satisty conservation of mass
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Asked by: manish kumar
Created at: 2025-12-18 10:40:30
Asked by: manish kumar
Created at: 2025-12-18 10:40:30
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# Problem Statement
Given velocity components for a flow field:
- \( u = 2xy \)
- v = -x^2y)
- \( w = \)
We are asked:
**Is this a physically possible incompressible flow field?**
*Hint: Any physically possible incompressible flow field must satisfy conservation of mass.*
---
# Step 1: Conservation of Mass for Incompressible Flow
The conservation of mass (continuity equation) for an incompressible fluid is:
\[
\frac{\partial u}{\partial x} + \frac{\partial v}{\partial y} + \frac{\partial w}{\partial z} =
\]
---
# Step 2: Calculate the Partial Derivatives
Given:
- \( u = 2xy \)
- \( v = -x^2y \)
- \( w = \)
Let's compute the required partial derivatives:
## \( \frac{\partial u}{\partial x} \)
\[
\frac{\partial u}{\partial x} = \frac{\partial (2xy)}{\partial x} = 2y
\]
## \( \frac{\partial v}{\partial y} \)
\[
\frac{\partial v}{\partial y} = \frac{\partial (-x^2y)}{\partial y} = -x^2
\]
## \( \frac{\partial w}{\partial z} \)
\[
\frac{\partial w}{\partial z} = \frac{\partial ()}{\partial z} =
\]
---
# Step 3: Substitute into the Continuity Equation
\[
\frac{\partial u}{\partial x} + \frac{\partial v}{\partial y} + \frac{\partial w}{\partial z} = 2y + (-x^2) + = 2y - x^2
\]
For incompressible flow, this sum **must be zero everywhere**:
\[
2y - x^2 =
\implies 2y = x^2
\]
---
# Step 4: Interpretation
- The equation \( 2y - x^2 = \) is **not true for all (x, y, z)** in the flow field.
- It is only satisfied on the curve \( y = \frac{x^2}{2} \), not everywhere.
---
# Step 5: Conclusion
## Is this a physically possible incompressible flow field?
**No**, this velocity field does **not** represent a physically possible incompressible flow field everywhere, because the continuity equation is not satisfied for arbitrary \((x, y, z)\).
---
## Summary Table
| Term | Value |
|-------------|------------------|
| \( u \) | \( 2xy \) |
| \( v \) | \( -x^2y \) |
| \( w \) | \( \) |
| Continuity | \( 2y - x^2 \) |
| Incompressible? | **NO** |
---
## Final Statement
**The flow field is not physically possible for an incompressible fluid because it does not satisfy the continuity equation everywhere in the domain.**
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