Chapter 15: Problem 21
Calculate the divergence and curl of the given vector field \(\mathbf{F}\). \(\mathbf{F}(x, y, z)=\left(y^{2}+z^{2}\right) \mathbf{i}+\left(x^{2}+z^{2}\right) \mathbf{j}+\left(x^{2}+y^{2}\right) \mathbf{k}\)
Short Answer
Expert verified
The divergence of \( \mathbf{F} \) is 0. The curl of \( \mathbf{F} \) is \((2y - 2z)\mathbf{i} + (2z - 2x)\mathbf{j} + (2x - 2y)\mathbf{k}\)."
Step by step solution
01
Find the Divergence of \( \mathbf{F} \)
To calculate the divergence of a vector field \( \mathbf{F}(x, y, z) = F_1 \mathbf{i} + F_2 \mathbf{j} + F_3 \mathbf{k} \), use the formula: \( abla \cdot \mathbf{F} = \frac{\partial F_1}{\partial x} + \frac{\partial F_2}{\partial y} + \frac{\partial F_3}{\partial z} \). Here, \( F_1 = y^2 + z^2 \), \( F_2 = x^2 + z^2 \), and \( F_3 = x^2 + y^2 \).
02
Compute Partial Derivatives for Divergence
Compute \( \frac{\partial F_1}{\partial x} = 0 \) (since \( F_1 \) doesn't depend on \( x \)), \( \frac{\partial F_2}{\partial y} = 0 \) (since \( F_2 \) doesn't depend on \( y \)), and \( \frac{\partial F_3}{\partial z} = 0 \) (since \( F_3 \) doesn't depend on \( z \)).
03
Calculate the Divergence Result
Substitute the derivatives into the formula for divergence: \( abla \cdot \mathbf{F} = 0 + 0 + 0 = 0 \). Thus, the divergence of the vector field \( \mathbf{F} \) is 0.
04
Find the Curl of \( \mathbf{F} \)
To calculate the curl, use the formula: \( abla \times \mathbf{F} = \left( \frac{\partial F_3}{\partial y} - \frac{\partial F_2}{\partial z} \right) \mathbf{i} + \left( \frac{\partial F_1}{\partial z} - \frac{\partial F_3}{\partial x} \right) \mathbf{j} + \left( \frac{\partial F_2}{\partial x} - \frac{\partial F_1}{\partial y} \right) \mathbf{k} \).
05
Compute Partial Derivatives for Curl
Evaluate each component: \( \frac{\partial F_3}{\partial y} = 2y \), \( \frac{\partial F_2}{\partial z} = 2z \), \( \frac{\partial F_1}{\partial z} = 2z \), \( \frac{\partial F_3}{\partial x} = 2x \), \( \frac{\partial F_2}{\partial x} = 2x \), and \( \frac{\partial F_1}{\partial y} = 2y \).
06
Calculate the Curl Result
Substitute the derivatives into the formula for the curl: \( abla \times \mathbf{F} = (2y - 2z) \mathbf{i} + (2z - 2x) \mathbf{j} + (2x - 2y) \mathbf{k} \). Thus, the curl of the vector field \( \mathbf{F} \) is \((2y - 2z)\mathbf{i} + (2z - 2x)\mathbf{j} + (2x - 2y)\mathbf{k}\).
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Key Concepts
These are the key concepts you need to understand to accurately answer the question.
Divergence
Divergence is a fundamental concept in vector calculus. It tells us how much a vector field spreads out from a point. For any given vector field \( \mathbf{F}(x, y, z) = F_1 \mathbf{i} + F_2 \mathbf{j} + F_3 \mathbf{k} \), the divergence is represented by the dot product of the del operator and the vector field.
This can be expressed as: \[ abla \cdot \mathbf{F} = \frac{\partial F_1}{\partial x} + \frac{\partial F_2}{\partial y} + \frac{\partial F_3}{\partial z}. \]To understand divergence intuitively:
This can be expressed as: \[ abla \cdot \mathbf{F} = \frac{\partial F_1}{\partial x} + \frac{\partial F_2}{\partial y} + \frac{\partial F_3}{\partial z}. \]To understand divergence intuitively:
- Imagine water flowing out of a point source.
- Divergence measures the tendency of this flow to spread out or converge at a point.
Curl
Curl is another key concept in vector calculus, and it focuses on the rotation of the vector field. In simple terms, the curl of a vector field provides a measurement of the field's tendency to rotate around a point.
For a vector field \( \mathbf{F}(x, y, z) = F_1 \mathbf{i} + F_2 \mathbf{j} + F_3 \mathbf{k} \), the curl is calculated using the cross product with the del operator, given by:\[ abla \times \mathbf{F} = \left( \frac{\partial F_3}{\partial y} - \frac{\partial F_2}{\partial z} \right) \mathbf{i} + \left( \frac{\partial F_1}{\partial z} - \frac{\partial F_3}{\partial x} \right) \mathbf{j} + \left( \frac{\partial F_2}{\partial x} - \frac{\partial F_1}{\partial y} \right) \mathbf{k}. \]Think of it in terms of fluid flow:
For a vector field \( \mathbf{F}(x, y, z) = F_1 \mathbf{i} + F_2 \mathbf{j} + F_3 \mathbf{k} \), the curl is calculated using the cross product with the del operator, given by:\[ abla \times \mathbf{F} = \left( \frac{\partial F_3}{\partial y} - \frac{\partial F_2}{\partial z} \right) \mathbf{i} + \left( \frac{\partial F_1}{\partial z} - \frac{\partial F_3}{\partial x} \right) \mathbf{j} + \left( \frac{\partial F_2}{\partial x} - \frac{\partial F_1}{\partial y} \right) \mathbf{k}. \]Think of it in terms of fluid flow:
- If you imagine the vector field as a fluid flow, the curl at a point gives the axis around which the flow tends to rotate.
- A higher curl magnitude signifies stronger rotation around that axis.
Vector Field
A vector field assigns a vector to every point in a region of space. It can be thought of as a way to visualize physical phenomena that have direction and magnitude at every point. The vector field \( \mathbf{F}(x, y, z) = (y^2 + z^2)\mathbf{i} + (x^2 + z^2)\mathbf{j} + (x^2 + y^2)\mathbf{k} \) we used in the exercise is an example of a 3D vector field.
Key features of vector fields include:
Key features of vector fields include:
- Magnitude: The length of the vector at a point indicates the field's strength at that point.
- Direction: The orientation of the vector provides insight into the direction of the effect, such as force or fluid flow, at that location.