Give step-by-step solution with explanation and final answer: Act like a helpful tutor and exlain me :Problem 3 (5 points): Expand the “mass” equation shown below and what equation will one get if you assume the density is constant. E Op , dpu; 0 Pa —_— = =0 a "oa; (8)
Question:
Give step-by-step solution with explanation and final answer:
Act like a helpful tutor and exlain me :Problem 3 (5 points): Expand the “mass” equation shown below and what equation
will one get if you assume the density is constant.
E Op , dpu;
0 Pa —_— = =0
a "oa;
(8)
This is AI generated Response.
Asked by: manish kumar
Created at: 2025-09-23 09:00:48
Asked by: manish kumar
Created at: 2025-09-23 09:00:48
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# Step-by-Step Solution
Let's break down the problem and answer it step by step.
## Given Equation
The "mass" equation given is:
\[
\frac{\partial \rho}{\partial t} + \frac{\partial (\rho u_j)}{\partial x_j} = 0
\]
where:
- \(\rho\) = density
- \(u_j\) = velocity component in the \(j\)-th direction
- \(x_j\) = spatial coordinate in the \(j\)-th direction
---
## Step 1: **Expand the Second Term**
Use the product rule for differentiation:
\[
\frac{\partial (\rho u_j)}{\partial x_j} = u_j \frac{\partial \rho}{\partial x_j} + \rho \frac{\partial u_j}{\partial x_j}
\]
So the equation becomes:
\[
\frac{\partial \rho}{\partial t}
+ u_j \frac{\partial \rho}{\partial x_j}
+ \rho \frac{\partial u_j}{\partial x_j} = 0
\]
---
## Step 2: **Assume Density is Constant**
If \(\rho\) is **constant**:
- \(\frac{\partial \rho}{\partial t} = 0\)
- \(\frac{\partial \rho}{\partial x_j} = 0\)
Substitute these into the expanded equation:
\[
0 + 0 + \rho \frac{\partial u_j}{\partial x_j} = 0
\]
\[
\rho \frac{\partial u_j}{\partial x_j} = 0
\]
For \(\rho \neq 0\), divide both sides by \(\rho\):
\[
\frac{\partial u_j}{\partial x_j} = 0
\]
---
## Step 3: **Interpretation**
This last equation is the **incompressibility condition** for fluid flow:
\[
\boxed{\nabla \cdot \vec{u} = 0}
\]
where \(\vec{u}\) is the velocity vector.
---
## **Summary Table**
| Step | Equation |
|------------------------|--------------------------------------------------------|
| Original | \(\frac{\partial \rho}{\partial t} + \frac{\partial (\rho u_j)}{\partial x_j} = 0\) |
| Expand | \(\frac{\partial \rho}{\partial t} + u_j \frac{\partial \rho}{\partial x_j} + \rho \frac{\partial u_j}{\partial x_j} = 0\) |
| Density constant | \(\rho \frac{\partial u_j}{\partial x_j} = 0\) |
| Final (Incompressible) | \(\frac{\partial u_j}{\partial x_j} = 0\) |
---
## **Final Answer**
**If density is assumed constant, the mass (continuity) equation simplifies to:**
\[
\boxed{
\frac{\partial u_j}{\partial x_j} = 0
}
\]
This means the flow is incompressible—the divergence of the velocity field is zero.
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