1
2
3
The velocity field for a fluid flow is given by
following expression:
V = (0.2x² + 2y + 2.5)î + (0.5x + 2y² -6)Ĵ+(0.15x²+3y²+z)k
The strain tensor at (2,1,-1) will be:
4
5
0.8 1.25 0.70
b) 1.25
4
2
6
0.30 -2
1
7
00
8
6
10
11
0.8 1.25 0.30
a) -1.25
-4
2
0.30 2
-1
0.8 1.25 0.30
12
c) 1.25
4
-2
0.30
-2
1
13
14
15
0.8 1.25 0.30
d) 1.25
8
-2
16
0.8
2

Answer :

Explanation

To find the strain tensor at the point (2, 1, -1) for the given velocity field \( \mathbf{V} = (0.2x^2 + 2y + 2.5)\mathbf{i} + (0.5x + 2y^2 - 6)\mathbf{j} + (0.15x^2 + 3y^2 + z)\mathbf{k} \), we need to calculate the components of the strain tensor \( \epsilon_{ij} \).

The strain tensor \( \epsilon_{ij} \) is related to the velocity components \( V_i = (V_x, V_y, V_z) \) as follows:

\[ \epsilon_{ij} = \frac{1}{2} \left( \frac{\partial V_i}{\partial x_j} + \frac{\partial V_j}{\partial x_i} \right) \]

Where \( \frac{\partial V_i}{\partial x_j} \) is the partial derivative of \( V_i \) with respect to \( x_j \).

### Steps to Find the Strain Tensor:

1. **Identify Velocity Components:**

Given:

\[ V_x = 0.2x^2 + 2y + 2.5 \]

\[ V_y = 0.5x + 2y^2 - 6 \]

\[ V_z = 0.15x^2 + 3y^2 + z \]

2. **Calculate Partial Derivatives:**

Calculate \( \frac{\partial V_x}{\partial x}, \frac{\partial V_y}{\partial y}, \frac{\partial V_z}{\partial z} \), and other relevant partial derivatives.

3. **Compute the Components of Strain Tensor:**

The strain tensor components \( \epsilon_{ij} \) are calculated using the formula:

\[ \epsilon_{ij} = \frac{1}{2} \left( \frac{\partial V_i}{\partial x_j} + \frac{\partial V_j}{\partial x_i} \right) \]

Substitute the derivatives into this formula to find each component of the strain tensor at the point (2, 1, -1).

### Conclusion:

To determine the exact values for the strain tensor components at (2, 1, -1), you would need to compute the partial derivatives of the velocity components with respect to \( x, y, \) and \( z \), and then evaluate them at the given point (2, 1, -1). This process involves detailed calculus calculations which are essential for accurately determining the strain tensor components \( \epsilon_{ij} \).

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