Chapter 15: Problem 7
In Problems 6 through 10, use Stokes' theorem to evaluate $$\oint_{C} \mathbf{F} \cdot \mathbf{T} d s.$$ \(\mathbf{F}=2 z \mathbf{i}+x \mathbf{j}+3 y \mathbf{k} ; \quad C\) is the ellipse in which the plane \(z=x\) meets the cylinder \(x^{2}+y^{2}=4\), oriented counterclockwise as viewed from above.
Short Answer
Expert verified
The value is \(8\pi\).
Step by step solution
01
Understand Stokes' Theorem
Stokes' Theorem relates a surface integral over a surface \(S\) to a line integral around the boundary \(C\) of \(S\). It is given by \( \oint_{C} \mathbf{F} \cdot \mathbf{T} \, ds = \iint_{S} (abla \times \mathbf{F}) \cdot \mathbf{n} \, dS \), where \( abla \times \mathbf{F} \) is the curl of \( \mathbf{F} \) and \( \mathbf{n} \) is the unit normal to \(S\).
02
Compute the Curl of F
First, find the curl of \(\mathbf{F}\). Given \( \mathbf{F} = 2z\mathbf{i} + x \mathbf{j} + 3y \mathbf{k} \), the curl \( abla \times \mathbf{F} \) is computed using the determinant:\[abla \times \mathbf{F} = \begin{vmatrix}\mathbf{i} & \mathbf{j} & \mathbf{k} \\frac{\partial}{\partial x} & \frac{\partial}{\partial y} & \frac{\partial}{\partial z} \2z & x & 3y\end{vmatrix}.\]After expansion, \( abla \times \mathbf{F} = (3 - 0)\mathbf{i} - (0 - 2)\mathbf{j} + (1 - 0)\mathbf{k} = 3\mathbf{i} + 2\mathbf{j} + \mathbf{k}.\)
03
Describe the Surface S
The surface \( S \) is part of the plane \( z = x \) within the cylinder \( x^2 + y^2 = 4 \). Thus \( z \) can be expressed as \( z = x \) for the points on the surface. The boundary of this surface is the curve \( C \), which is an ellipse.
04
Determine the Normal Vector for the Surface
The plane \( z = x \) has a normal vector \( \mathbf{n} = \langle 1, 0, -1 \rangle \) because it is oriented with respect to \( z - x = 0 \). However, since our surface is part of this plane within a cylinder, we ensure it's outward oriented with \( \mathbf{n} = \langle 1, 0, -1 \rangle \).
05
Evaluate the Surface Integral
The integral becomes \( \iint_{S} (abla \times \mathbf{F}) \cdot \mathbf{n} \, dS \). Substitute \( abla \times \mathbf{F} = \langle 3, 2, 1 \rangle \) and \( \mathbf{n} = \langle 1, 0, -1 \rangle \), so the dot product is:\[\langle 3, 2, 1 \rangle \cdot \langle 1, 0, -1 \rangle = 3\cdot1 + 2\cdot0 + 1\cdot(-1) = 2.\]Now evaluate \( \iint_{S} 2 \, dS \), where the area of \( S \) is the area of the elliptical region \( x^2 + y^2 \leq 4 \). The area of this circle is \( \pi \times 4 = 4\pi \). Hence the integral is \( 2 \times 4\pi = 8\pi \).
06
Final Result
By Stokes’ theorem, \( \oint_{C} \mathbf{F} \cdot \mathbf{T} \, ds = 8\pi \). Therefore, the value of the line integral around curve \( C \) is \( 8\pi \).
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Key Concepts
These are the key concepts you need to understand to accurately answer the question.
Line Integral
A line integral helps determine the work done by a force field along a curve. The concept involves tracing out a path and summing contributions from every tiny segment of this path. In mathematical terms, the line integral of a vector field \( \mathbf{F} \) along a curve \( C \) is denoted as \( \oint_{C} \mathbf{F} \cdot \mathbf{T} \, ds \). This requires:
- Understanding \( \mathbf{F} \), the vector field.
- \( \mathbf{T} \), the unit tangent vector at each point on the curve.
- \( ds \), the differential element of the curve, representing a miniature piece of the path.
Curl of a Vector Field
The curl of a vector field is a measure of the field's rotation or swirling behavior at a given point. It can be thought of as how much the field spins around the point. For a vector field \( \mathbf{F} = 2z\mathbf{i} + x \mathbf{j} + 3y \mathbf{k} \), the curl is calculated using a cross product of the del operator \( abla \) and the vector field \( \mathbf{F} \):
- Visualize \( abla \times \mathbf{F} \) as the 3D rotation of the field.
- The resulting vector, \( \mathbf{curl} \), represents the axis of rotation and magnitude.
- The specific steps involve setting up and evaluating a determinant which captures partial derivatives with respect to each coordinate direction.
Surface Integral
A surface integral extends line integrals to two dimensions, integrating over a surface instead of a curve. For vector fields, the surface integral is used to measure the flux - or total flow - across the surface. The expression \( \iint_{S} (abla \times \mathbf{F}) \cdot \mathbf{n} \, dS \) tells you:
- The curl of the field \( abla \times \mathbf{F} \), an indicator of how the field rotates around the surface.
- \( \mathbf{n} \), the normal vector, which provides the maximum point of surface for considering the flow direction.
- \( dS \), an area element of the surface \( S \), comparable to \( ds \) in line integrals.
Normal Vector
The normal vector is essential for understanding the orientation of a surface in space. It is a vector perpendicular to the surface at any given point, and it plays a crucial role in surface integrals. Here’s what to remember about normal vectors:
- The normal vector \( \mathbf{n} \) determines the direction "outwards" from a surface.
- It interacts with other vectors through dot products to convey the extent to which fields pierce the surface.
- In our problem, since the plane is defined by \( z = x \), the normal vector is \( \langle 1, 0, -1 \rangle \), ensuring we regarded the orientation correctly for Stokes' Theorem.
- The chosen normal vector ensures that our calculations account for the surface's correct side which affects how we analyze the surface integral.