Preliminary Questions
Indicate with an arrow the boundary orientation of the boundary curves of the surfaces in Figure 17.44, oriented by the outward-pointing normal vectors.
Let \({\bf F} = {\bf curl}({\bf A})\). Which of the following are related by Stokes’ Theorem?
What is the definition of a vector potential?
Which of the following statements is correct?
Which condition on \({\bf F}\) guarantees that the flux through \(S_1\) is equal to the flux through \(S_2\) for any two oriented surfaces \(S_1\) and \(S_2\) with the same oriented boundary?
Exercises
In Exercises 1–4, calculate \({\bf curl}({\bf F})\).
\({\bf F}=\langle z - y^2, x + z^3, y + x^2\rangle\)
\(\displaystyle{{\bf F}=\langle \frac{y}x, \frac{y}z, \frac{z}x \rangle}\)
\({\bf F}=\langle e^y,\sin x, \cos x\rangle\)
\(\displaystyle{{\bf F}=\langle \frac{x}{x^2+y^2}, \frac{y}{x^2+y^2},0 \rangle}\)
In Exercises 5–8, verify Stokes’ Theorem for the given vector field and surface, oriented with an upward-pointing normal.
\({\bf F}=\langle 2xy, x, y+z\rangle,\quad\) the surface \(z=1-x^2-y^2\) for \(x^2+ y^2\le 1\)
\({\bf F} = \langle y z,0,x\rangle,\quad\) the portion of the plane \(\displaystyle{\frac{x}2 +\frac{y}3+z=1}\) where \(x, y, z \ge 0 \)
\({\bf F} = \langle e^{y-z}, 0,0\rangle,\quad\) the square with vertices \((1,0,1)\), \((1,1,1)\), \((0,1,1)\), and \((0,0,1)\)
\({\bf F} = \langle y, x, x^2+y^2\rangle,\quad\) the upper hemisphere \(x^2+y^2+z^2=1\), \(z\ge 0\)
In Exercises 9 and 10, calculate \({\bf curl}({\bf F})\) and then use Stokes’ Theorem to compute the flux of \({\bf curl}({\bf F})\) through the given surface as a line integral.
\({\bf F} = \langle e^{z^2}-y,e^{z^3}+x,\cos(xz)\rangle,\quad\) the upper hemisphere \(x^2+y^2+z^2=1\), \(z\ge 0\) with outward-pointing normal
\({\bf F} = \langle x+y,z^2-4,x\sqrt{y^2+1})\rangle,\quad\) surface of the wedge-shaped box in Figure 17.45 (bottom included, top excluded) with outward-point-ing normal
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Let \(S\) be the surface of the cylinder (not including the top and bottom) of radius 2 for \(1\le z \le 6\), oriented with outward-pointing normal (Figure 17.46).
Let \(S\) be the portion of the plane \(z=x\) contained in the half-cylinder of radius \(R\) depicted in Figure 17.47. Use Stokes’ Theorem to calculate the circulation of \({\bf F}=\langle z, x, y + 2z\rangle\) around the boundary of \(S\) (a half-ellipse) in the counterclockwise direction when viewed from above. Hint: Show that \({\bf curl}({\bf F})\) is orthogonal to the normal vector to the plane.
Let \(I\) be the flux of \({\bf F} = \langle e^y,2xe^{x^2}, z^2 \rangle\) through the upper hemisphere \(S\) of the unit sphere.
Let \({\bf F} = \langle 0, -z, 1\rangle\). Let \(S\) be the spherical cap \(x^2+y^2+z^2\le 1\), where \(z\ge\tfrac12\). Evaluate \(\displaystyle{\iint_{S\,} {\bf F}\cdot d{\bf S}}\) directly as a surface integral. Then verify that \({\bf F}={\bf curl}({\bf A})\), where \({\bf A}=(0,x,xz)\) and evaluate the surface integral again using Stokes’ Theorem.
Let \({\bf A}\) be the vector potential and \({\bf B}\) the magnetic field of the infinite solenoid of radius \(R\) in Example 6. Use Stokes’ Theorem to compute:
The magnetic field \({\bf B}\) due to a small current loop (which we place at the origin) is called a magnetic dipole (Figure 17.48). Let \(\rho=(x^2+y^2+z^2)^{1/2}\). For \(\rho\) large, \({\bf B}={\bf curl}({\bf A})\), where \[ {\bf A}=\langle -\frac{y}{\rho^3}, \frac{x}{\rho^3},0\rangle \]
A uniform magnetic field \({\bf B}\) has constant strength \(b\) in the \(z\)-direction [that is, \({\bf B} = \langle 0,0,b\rangle\)].
Let \({\bf F} = \langle -x^2y, x, 0\rangle\). Referring to Figure 17.49, let \(C\) be the closed path \(ABCD\). Use Stokes’ Theorem to evaluate \(\displaystyle{\int_{C}{\bf F}\cdot d{\bf s}}\) in two ways. First, regard \(C\) as the boundary of the rectangle with vertices \(A\), \(B\), \(C\), and \(D\). Then treat \(C\) as the boundary of the wedge-shaped box with open top.
Let \({\bf F} = \langle y^2, 2z + x, 2y^2 \rangle\). Use Stokes’ Theorem to find a plane with equation \(\displaystyle{ax+by+cz=0}\) (where \(a,b,c\) are not all zero) such that \(\displaystyle{\oint_C\,{\bf F}\cdot\,d{\bf s}=0}\) for every closed \(C\) lying in the plane. Hint: Choose \(a,b,c\) so that \({\bf curl}({\bf F})\) lies in the plane.
Let \({\bf F}=\langle -z^2, 2zx, 4y - x^2\rangle\) and let \(C\) be a simple closed curve in the plane \(x+y+z=4\) that encloses a region of area \(16\) (Figure 17.50). Calculate \(\displaystyle{\oint_C{\bf F}\cdot d{\bf s}}\), where \(C\) is oriented in the counterclockwise direction (when viewed from above the plane).
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Let \({\bf F} = \langle y^2, x^2, z^2\rangle\). Show that \[ \int_{C_1} {\bf F} \cdot d{\bf s} = \int_{C_2} {\bf F} \cdot d{\bf s} \] for any two closed curves lying on a cylinder whose central axis is the \(z\)-axis (Figure 17.51).
The curl of a vector field \({\bf F}\) at the origin is \({\bf v}_0 = \langle 3,1,4\rangle\). Estimate the circulation around the small parallelogram spanned by the vectors \({\bf A}=\langle 0,\tfrac12,\tfrac12\rangle\) and \({\bf B}=\langle 0,0,\tfrac13\rangle\).
You know two things about a vector field \({\bf F}\):
Determine the flux of \({\bf F}\) through the surface \(S\) in Figure 17.52, oriented with upward pointing normal.
Suppose that \({\bf F}\) has a vector potential and that \({\bf F}(x, y, 0) = {\bf k}\). Find the flux of \({\bf F}\) through the surface \(S\) in Figure 17.38, oriented with upward pointing normal.
Prove that \(\displaystyle{{\bf curl}(f{\bf A}) = \nabla f\times{\bf A}}\), where \(f\) is a differentiable function and \({\bf A}\) is a constant vector.
Show that \({\bf curl}({\bf F})=\mathbf{0}\) if \({\bf F}\) is radial, meaning that \({\bf F}=f(\rho)\langle x, y, z\rangle\) for some function \(f(\rho)\), where \(\rho=\sqrt{x^2+y^2+z^2}\). Hint: It is enough to show that one component of \({\bf curl}({\bf F})\) is zero, because it will then follow for the other two components by symmetry.
Prove the following Product Rule: \begin{equation*} {\bf curl}(f{\bf F}) = f{\bf curl}({\bf F}) + \nabla f\times{\bf F} \end{equation*}
Assume that \(f\) and \(g\) have continuous partial derivatives of order 2. Prove that \[ \oint_{\partial S} f\nabla(g)\cdot d{\bf s} = \iint_{S} \nabla(f)\times\nabla(g)\cdot d{\bf s} \]
Verify that \({\bf B}={\bf curl}({\bf A})\) for \(r>R\) in the setting of Example 6.
Explain carefully why Green’s Theorem is a special case of Stokes’ Theorem.
Further Insights and Challenges
In this exercise, we use the notation of the proof of Theorem 1 and prove \begin{equation} \oint_C F_3(x,y,z){\bf k} \cdot d{\bf s} = \iint_{S} {\bf curl}(F_3(x,y,z){\bf k})\cdot d{\bf S}\tag{11} \end{equation}
In particular, \(S\) is the graph of \(z=f(x,y)\) over a domain \(D\), and \(C\) is the boundary of \(S\) with parametrization \((x(t),y(t),f(x(t),y(t)))\).
Let \({\bf F}\) be a continuously differentiable vector field in \({\bf R}^3\), \(Q\) a point, and \(S\) a plane containing \(Q\) with unit normal vector \({\bf e}\). Let \(C_r\) be a circle of radius \(r\) centered at \(Q\) in \(S\), and let \(S_r\) be the disk enclosed by \(C_r\). Assume \(S_r\) is oriented with unit normal vector \({\bf e}\).
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