Problem 246
Question
Find the divergence of \(\mathbf{F}\) at the given point. $$ \mathbf{F}(x, y, z)=x y z \mathbf{i}+y \mathbf{j}+z \mathbf{k} \text { at }(1,2,3) $$
Step-by-Step Solution
Verified Answer
The divergence at the point (1, 2, 3) is 8.
1Step 1: Understand the Problem
We need to find the divergence of the vector field \( \mathbf{F}(x, y, z) = x y z \mathbf{i} + y \mathbf{j} + z \mathbf{k} \) at the point \( (1, 2, 3) \).
2Step 2: Recall the Formula for Divergence
The divergence of a vector field \( \mathbf{F}(x, y, z) = P \mathbf{i} + Q \mathbf{j} + R \mathbf{k} \) is given by the formula \( abla \cdot \mathbf{F} = \frac{\partial P}{\partial x} + \frac{\partial Q}{\partial y} + \frac{\partial R}{\partial z} \).
3Step 3: Identify Components of \( \mathbf{F} \)
In the vector field \( \mathbf{F}(x, y, z) = x y z \mathbf{i} + y \mathbf{j} + z \mathbf{k} \), the components are \( P = xyz \), \( Q = y \), and \( R = z \).
4Step 4: Compute Partial Derivative with respect to \( x \)
Find \( \frac{\partial P}{\partial x} \). Since \( P = xyz \), we treat \( y \) and \( z \) as constants, giving \( \frac{\partial (xyz)}{\partial x} = yz \).
5Step 5: Compute Partial Derivative with respect to \( y \)
Find \( \frac{\partial Q}{\partial y} \). Since \( Q = y \), this gives us \( \frac{\partial y}{\partial y} = 1 \).
6Step 6: Compute Partial Derivative with respect to \( z \)
Find \( \frac{\partial R}{\partial z} \). Since \( R = z \), we have \( \frac{\partial z}{\partial z} = 1 \).
7Step 7: Sum the Partial Derivatives
Add the partial derivatives: \( abla \cdot \mathbf{F} = yz + 1 + 1 \).
8Step 8: Evaluate at the Given Point \( (1, 2, 3) \)
Substitute \( y = 2 \) and \( z = 3 \) into the expression obtained in Step 7: \( abla \cdot \mathbf{F} = 2 \cdot 3 + 1 + 1 = 6 + 1 + 1 = 8 \).
Key Concepts
Vector FieldsPartial DerivativesCalculus
Vector Fields
A vector field is a mathematical construction representing a function that provides a vector for each point in space. This can be visualized as an array of arrows where each arrow has a direction and magnitude specific to that location. In physics, vector fields often represent quantities like velocity or force fields, indicating how these quantities vary over space.
In the context of the original exercise, the vector field \( \mathbf{F}(x, y, z) = x y z \mathbf{i} + y \mathbf{j} + z \mathbf{k} \) is a function of three variables (\( x, y, z \)), where each point in the space has an associated vector.
In the context of the original exercise, the vector field \( \mathbf{F}(x, y, z) = x y z \mathbf{i} + y \mathbf{j} + z \mathbf{k} \) is a function of three variables (\( x, y, z \)), where each point in the space has an associated vector.
- \( \mathbf{i} \), \( \mathbf{j} \), and \( \mathbf{k} \) represent the unit vectors in the direction of the x, y, and z axes, respectively.
- The components of the vector field are not constant; they depend on the position \((x, y, z)\).
Partial Derivatives
Partial derivatives are an essential part of multivariable calculus. They measure the rate at which a function changes with respect to one of its variables while keeping the other variables constant. This concept is fundamental when dealing with fields or functions of multiple variables.
In our original exercise, each component of the vector field \( \mathbf{F} \) is differentiated partially:
In our original exercise, each component of the vector field \( \mathbf{F} \) is differentiated partially:
- For \( P = xyz \), the partial derivative with respect to \( x \) is \( \frac{\partial (xyz)}{\partial x} = yz \), treating \( y \) and \( z \) as constants.
- For \( Q = y \), the partial derivative with respect to \( y \) is \( \frac{\partial y}{\partial y} = 1 \), an indication that \( Q \) changes linearly.
- For \( R = z \), \( \frac{\partial z}{\partial z} = 1 \), as it also changes linearly in the direction of \( z \).
Calculus
Calculus is the branch of mathematics dealing with the study of change and motion. It includes techniques like differentiation and integration. In the realm of vector fields and physics, calculus provides us with tools like divergence, curl, and various integral theorems which help in understanding and quantifying spatial phenomena.
In this exercise, we used calculus to find the divergence of a given vector field. Divergence is a scalar value that gives the magnitude of a field's source at a given point, influencing how much the field is emanating from or converging at that point.
The divergence for the vector field \( \mathbf{F}(x, y, z) = x y z \mathbf{i} + y \mathbf{j} + z \mathbf{k} \) was computed as:
In this exercise, we used calculus to find the divergence of a given vector field. Divergence is a scalar value that gives the magnitude of a field's source at a given point, influencing how much the field is emanating from or converging at that point.
The divergence for the vector field \( \mathbf{F}(x, y, z) = x y z \mathbf{i} + y \mathbf{j} + z \mathbf{k} \) was computed as:
- Calculate partial derivatives for each component.
- Sum these to find \( abla \cdot \mathbf{F} = yz + 1 + 1 \).
Other exercises in this chapter
Problem 244
Use a computer algebra system to find the curl of the given vector fields. $$ \mathbf{F}(x, y, z)=\sin (x-y) \mathbf{i}+\sin (y-z) \mathbf{j}+\sin (z-x) \mathbf
View solution Problem 245
Find the divergence of \(\mathbf{F}\) at the given point. $$ \mathbf{F}(x, y, z)=\mathbf{i}+\mathbf{j}+\mathbf{k} \text { at }(2,-1,3) $$
View solution Problem 247
Find the divergence of \(\mathbf{F}\) at the given point. $$ \mathbf{F}(x, y, z)=e^{-x y} \mathbf{i}+e^{x z} \mathbf{j}+e^{y z} \mathbf{k} \text { at }(3,2,0) $
View solution Problem 248
Find the divergence of \(\mathbf{F}\) at the given point. $$ \mathbf{F}(x, y, z)=x y z \mathbf{i}+y \mathbf{j}+z \mathbf{k} \text { at }(1,2,1) $$
View solution