Chapter 15: Problem 10
Use the Divergence Theorem to find the flux of F across the surface ? with outward orientation. $$ \begin{array}{l}{\mathbf{F}(x, y, z)=z^{3} \mathbf{i}-x^{3} \mathbf{j}+y^{3} \mathbf{k}, \quad \text { where } \sigma \text { is the sphere }} \\\ {x^{2}+y^{2}+z^{2}=a^{2}}\end{array} $$
Short Answer
Expert verified
The flux of \( \mathbf{F} \) across the sphere is 0.
Step by step solution
01
Understand the Divergence Theorem
The Divergence Theorem relates the flux of a vector field \( \mathbf{F} \) through a closed surface \( \sigma \) to the integral of the divergence of \( \mathbf{F} \) over the volume \( V \) inside \( \sigma \). It is given by \( \iint_{\sigma} \mathbf{F} \cdot \mathbf{n} \,d\sigma = \iiint_{V} abla \cdot \mathbf{F} \,dV \). Here, \( \mathbf{n} \) is the outward normal to the surface.
02
Compute the Divergence of F
For the vector field \( \mathbf{F}(x, y, z) = z^3 \mathbf{i} - x^3 \mathbf{j} + y^3 \mathbf{k} \), the divergence \( abla \cdot \mathbf{F} \) is calculated by taking the partial derivatives: \( \frac{\partial}{\partial x}(z^3) + \frac{\partial}{\partial y}(-x^3) + \frac{\partial}{\partial z}(y^3) = 0 + 0 + 0 = 0 \). Thus, \( abla \cdot \mathbf{F} = 0 \).
03
Apply the Divergence Theorem
Since \( abla \cdot \mathbf{F} = 0 \), we have \( \iiint_{V} abla \cdot \mathbf{F} \,dV = \iiint_{V} 0 \,dV = 0 \). By the Divergence Theorem, \( \iint_{\sigma} \mathbf{F} \cdot \mathbf{n} \,d\sigma = \iiint_{V} 0 \,dV = 0 \).
04
Conclude the Flux Calculation
Because the integral over the volume is zero, the flux of \( \mathbf{F} \) across the surface \( \sigma \) with the outward orientation is also zero. Therefore, the given vector field \( \mathbf{F} \) has no net outward flux through the sphere.
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Key Concepts
These are the key concepts you need to understand to accurately answer the question.
Vector Field
A vector field is a function that assigns a vector to every point in a space. The vector field given in this exercise is \( \mathbf{F}(x, y, z) = z^3 \mathbf{i} - x^3 \mathbf{j} + y^3 \mathbf{k} \). Here, \( \mathbf{i}, \mathbf{j}, \mathbf{k} \) represent the unit vectors along the x, y, and z axes respectively.
Understanding a vector field is crucial in visualizing how vectors vary and are distributed throughout space. Each vector within \( \mathbf{F} \) gives us the direction and magnitude at a specific point \((x, y, z)\).
- The \( z^3 \mathbf{i} \) component means that the influence in the x-direction increases with the cube of the z-coordinate.- The term \(-x^3 \mathbf{j} \) implies a similar cubic influence in the negative y-direction.- Finally, the \( y^3 \mathbf{k} \) indicates a positive z-direction influence, also increasing cubically with y.
These components together define how the vector field vicariously moves around a spherical region, which in our case is the sphere \( x^2 + y^2 + z^2 = a^2 \). Understanding this vector function is the first step in applying concepts like the Divergence Theorem.
Understanding a vector field is crucial in visualizing how vectors vary and are distributed throughout space. Each vector within \( \mathbf{F} \) gives us the direction and magnitude at a specific point \((x, y, z)\).
- The \( z^3 \mathbf{i} \) component means that the influence in the x-direction increases with the cube of the z-coordinate.- The term \(-x^3 \mathbf{j} \) implies a similar cubic influence in the negative y-direction.- Finally, the \( y^3 \mathbf{k} \) indicates a positive z-direction influence, also increasing cubically with y.
These components together define how the vector field vicariously moves around a spherical region, which in our case is the sphere \( x^2 + y^2 + z^2 = a^2 \). Understanding this vector function is the first step in applying concepts like the Divergence Theorem.
Flux Calculation
Calculating the flux involves determining how much of the vector field penetrates through a given surface. For a closed surface like a sphere, it can be described using the Divergence Theorem. The theorem connects the flux through the surface to the divergence over the volume it encloses.
Here's how it generally works:
Here's how it generally works:
- Calculate the divergence of the vector field \( \mathbf{F} \) using \( abla \cdot \mathbf{F} \).
- If \( abla \cdot \mathbf{F} = 0 \), as it does here, it signals that there are no sources or sinks inside the volume, leading to zero net flux.
- Evaluate the integral over the volume, which equals zero, thereby confirming zero flux.
Surface Integration
Surface integration is a method used to evaluate the flow or flux across a surface. It consists of finding how a vector field interacts with the surface's normal vectors. When the surface is closed, the integration helps in understanding the net flow through the surface.
Given a surface like the sphere \( x^2 + y^2 + z^2 = a^2 \), the outward orientation implies considering the outward normal vector \( \mathbf{n} \) when performing the surface integral.
In our case, surface integration of a vector field through this sphere determines how \( \mathbf{F} \) moves in and out of the spherical boundary. However, since the divergence calculated was zero, surface integration becomes straightforward – the net movement across the surface is zero. That means no portion of \( \mathbf{F} \) flows out or into the sphere in a net sense.
- Surface integration checks local interactions of the field with the surface normals along the entire boundary.- Typically, each bit of surface is considered with the dot product \( \mathbf{F} \cdot \mathbf{n} \), and integrating this over the whole surface gives us the flux measure.
Thus, by surface integration, the conclusion is reinforced: there is zero net flux, illustrating a harmonious no-net-flow field across the closed spherical surface.
Given a surface like the sphere \( x^2 + y^2 + z^2 = a^2 \), the outward orientation implies considering the outward normal vector \( \mathbf{n} \) when performing the surface integral.
In our case, surface integration of a vector field through this sphere determines how \( \mathbf{F} \) moves in and out of the spherical boundary. However, since the divergence calculated was zero, surface integration becomes straightforward – the net movement across the surface is zero. That means no portion of \( \mathbf{F} \) flows out or into the sphere in a net sense.
- Surface integration checks local interactions of the field with the surface normals along the entire boundary.- Typically, each bit of surface is considered with the dot product \( \mathbf{F} \cdot \mathbf{n} \), and integrating this over the whole surface gives us the flux measure.
Thus, by surface integration, the conclusion is reinforced: there is zero net flux, illustrating a harmonious no-net-flow field across the closed spherical surface.