Chapter 16: Problem 14
Verify that Stokes' Theorem is true for the given vector field \(\mathbf{F}\) and surface \(S .\) \(\mathbf{F}(x, y, z)=-2 y z \mathbf{i}+y \mathbf{j}+3 x \mathbf{k}\) \(S\) is the part of the paraboloid \(z=5-x^{2}-y^{2}\) that lies above the plane \(z=1,\) oriented upward
Short Answer
Expert verified
Stokes' Theorem holds for \(\mathbf{F}\) and \(S\); both integrals equal 6\pi.
Step by step solution
01
Understand Stokes' Theorem
Stokes' Theorem relates the surface integral of the curl of a vector field over a surface \( S \) to the line integral of the vector field along the boundary \( C \) of the surface. Mathematically, it is expressed as: \( \int_{S} (abla \times \mathbf{F}) \cdot \mathbf{n} \, dS = \oint_{C} \mathbf{F} \cdot d\mathbf{r} \). Here, \( \mathbf{n} \) is the outward-pointing unit normal vector to the surface \( S \). We need to verify this theorem for the given vector field \( \mathbf{F} \) and surface \( S \).
02
Compute the Surface Description
The surface \( S \) is a part of the paraboloid \( z = 5 - x^2 - y^2 \) which is above the plane \( z = 1 \). This means \( 1 \leq z \leq 5 - x^2 - y^2 \), so we have \( x^2 + y^2 \leq 4 \). The boundary \( C \) of \( S \) is the circle \( x^2 + y^2 = 4 \) in the plane \( z = 1 \). The surface is oriented upward.
03
Compute \( \nabla \times \mathbf{F} \)
First, compute the curl of \( \mathbf{F} \). Given \( \mathbf{F} = -2yz \mathbf{i} + y \mathbf{j} + 3x \mathbf{k} \), we find \( abla \times \mathbf{F} = \left( \frac{\partial}{\partial y}(3x) - \frac{\partial}{\partial z}(y) \right) \mathbf{i} - \left( \frac{\partial}{\partial x}(3x) - \frac{\partial}{\partial z}(-2yz) \right) \mathbf{j} + \left( \frac{\partial}{\partial x}(y) - \frac{\partial}{\partial y}(-2yz) \right) \mathbf{k} \). This simplifies to \( abla \times \mathbf{F} = 0 \mathbf{i} + 2z \mathbf{j} + 1 \mathbf{k} \).
04
Set up the Surface Integral
The surface integral is \( \int_{S} (abla \times \mathbf{F}) \cdot \mathbf{n} \, dS = \int_{S} (0 \mathbf{i} + 2z \mathbf{j} + 1 \mathbf{k}) \cdot \mathbf{n} \, dS \). Since \( S \) is oriented upward, \( \mathbf{n} \) is the unit vector pointing upward. We set up \( \int_{S} (2z \cdot n_j + n_k) \ dS \). The unit normal to the surface is derived from the gradient of the surface equation. As the surface is \( z = 5 - x^2 - y^2 \), \( \mathbf{n} \) pointing upward is indeed \( \langle -2x, -2y, 1 \rangle/\sqrt{4x^2 + 4y^2 + 1} \). The upward unit normal simplifies to approximately align with \( \mathbf{k} \).
05
Parameterize and Compute the Surface Integral
Parameterize \( S \) using polar coordinates, \( x = r \cos \theta \), \( y = r \sin \theta \), with \( 0 \leq r \leq 2 \) and \( 0 \leq \theta < 2\pi \). Substitute into the surface integral: \( \int_{0}^{2\pi} \int_{0}^{2} (2 - r^2) \, r \, dr \, d\theta \). Calculate the inner integral: \( \int_{0}^{2} (2r - r^3) \, dr = [r^2 - \frac{r^4}{4}]_{0}^{2} = 4 - 4/4 = 3 \). The outer integral becomes \( 3 \int_{0}^{2\pi} d\theta = 6\pi \).
06
Compute the Line Integral Around C
The boundary \( C \) is the circle \( x^2 + y^2 = 4 \) at \( z = 1 \). In polar coordinates, \( x = 2\cos \theta \), \( y = 2\sin \theta \), \( z = 1 \). \( \mathbf{F} = -4\sin \theta \mathbf{i} + 2 \sin \theta \mathbf{j} + 6 \cos \theta \mathbf{k} \). On \( C \), \( d\mathbf{r} = -2\sin \theta \mathbf{i} \, d\theta + 2\cos \theta \mathbf{j} \, d\theta \). Evaluate the line integral \( \oint_{C} \mathbf{F} \cdot d\mathbf{r} = \int_{0}^{2\pi} (-4\sin \theta)(-2\sin \theta) + 2\sin \theta (2\cos \theta) \, d\theta \). Simplifying, integrate \( \int_{0}^{2\pi} (8\sin^2 \theta + 4\sin \theta \cos \theta) \, d\theta = 6\pi \).
07
Verify Stokes' Theorem
The surface integral \( \int_{S} (abla \times \mathbf{F}) \cdot d\mathbf{S} = 6\pi \). The line integral \( \oint_{C} \mathbf{F} \cdot d\mathbf{r} = 6\pi \). Both integrals yield the same value, verifying Stokes' Theorem for the given vector field and surface.
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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 space. Imagine a vector, which has both direction and magnitude, attached to each point within a region. This way, you can visualize how vectors behave at different locations.
In the context of the given problem, the vector field is described by the expression \( \mathbf{F}(x, y, z) = -2yz \mathbf{i} + y \mathbf{j} + 3x \mathbf{k} \). Here are a few points about this vector field:
In the context of the given problem, the vector field is described by the expression \( \mathbf{F}(x, y, z) = -2yz \mathbf{i} + y \mathbf{j} + 3x \mathbf{k} \). Here are a few points about this vector field:
- Each variable \( x, y, \) and \( z \) contributes differently to the vector's components.
- As \( y \) and \( z \) change, they affect the \( i \)-component by \( -2yz \).
- The \( j \)-component is purely from \( y \), showing a simpler relationship.
- The \( k \)-component depends only on \( x \), depicted by \( 3x \).
Surface integral
A surface integral helps to generalize the concept of integrating over a surface in three-dimensional space. It is especially useful in physics and engineering to measure quantities, such as flux, over a surface.
For our problem, Stokes' Theorem involves the surface integral of the curl of the vector field \( \mathbf{F} \) over the surface \( S \). Here, the surface \( S \) is part of a paraboloid and is defined by \( z = 5 - x^2 - y^2 \) above the plane \( z = 1 \).
Key points regarding surface integral:
For our problem, Stokes' Theorem involves the surface integral of the curl of the vector field \( \mathbf{F} \) over the surface \( S \). Here, the surface \( S \) is part of a paraboloid and is defined by \( z = 5 - x^2 - y^2 \) above the plane \( z = 1 \).
Key points regarding surface integral:
- It consists of adding up contributions from tiny surface patches for the whole surface.
- The vector field is evaluated on these surface patches.
- Orientation is crucial: the surface is oriented with its normal vector pointing upward.
Line integral
A line integral calculates the work done by a vector field along a curve. Imagine it as summing the field's influence along a specific path or boundary.
In this exercise, we look at the boundary \( C \) of the surface \( S \), which is a circle given by \( x^2 + y^2 = 4 \) in the plane \( z = 1 \). We compute how \( \mathbf{F} \) behaves along this boundary.
Here are important aspects concerning line integrals:
In this exercise, we look at the boundary \( C \) of the surface \( S \), which is a circle given by \( x^2 + y^2 = 4 \) in the plane \( z = 1 \). We compute how \( \mathbf{F} \) behaves along this boundary.
Here are important aspects concerning line integrals:
- Determine the parametric equations for \( C \); here \( x = 2\cos \theta \) and \( y = 2\sin \theta \).
- The differential path length element is \( d\mathbf{r} = -2\sin \theta \mathbf{i} \, d\theta + 2\cos \theta \mathbf{j} \, d\theta \).
- Calculate the influence by evaluating the integral of \( \mathbf{F} \cdot d\mathbf{r} \).
Curl of a vector field
The curl of a vector field is a measure of its tendency to rotate around a point. Think of it as capturing the rotational effect of the vectors around a point in space.
The curl is fundamental to Stokes' Theorem as it links line integrals to surface integrals. For \( \mathbf{F} \), we compute the curl as \( abla \times \mathbf{F} = 0 \mathbf{i} + 2z \mathbf{j} + 1 \mathbf{k} \).
Important points about the curl of a vector field:
The curl is fundamental to Stokes' Theorem as it links line integrals to surface integrals. For \( \mathbf{F} \), we compute the curl as \( abla \times \mathbf{F} = 0 \mathbf{i} + 2z \mathbf{j} + 1 \mathbf{k} \).
Important points about the curl of a vector field:
- It's a vector resulting from the cross-product of the del operator \( abla \) and \( \mathbf{F} \).
- Indicates how much and in which way vectors rotate around a given point.
- A non-zero curl implies a more pronounced rotational effect.