Determine which of the following vector fields \({\bf F}\) in the plane is the gradient of a scalar function \(f\). If such an \(f\) exists, find it.
Repeat Exercise 1 for the following vector fields:
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For each of the following vector fields \(\textbf{F}\), determine (i) if there exists a function \(g\) such that \(\nabla g = \textbf{F}\), and (ii) if there exists a vector field \(\textbf{G}\) such that \(\hbox{curl } \textbf{G} = \textbf{F}\). (It is not necessary to find \(g\) or \(\textbf{G}\).)
For each of the following vector fields \(\textbf{F}\), determine (i) if there exists a function \(g\) such that \(\nabla g = \textbf{F}\), and (ii) if there exists a vector field \(\textbf{G}\) such that \(\hbox{curl } \textbf{G} = \textbf{F}\). (It is not necessary to find \(g\) or \(\textbf{G}\).)
Show that any two potential functions for a vector field on \({\mathbb R}^3\) differ at most by a constant.
Let \({\bf F} (x,y,z) = (2xyz + \sin x) {\bf i} + x^2 z {\bf j} + x^2 y {\bf k}\). Find a function \(f\) such that \({\bf F} = {\nabla}\! f\).
Evaluate \(\int_{\bf c} {\bf F} \,{\cdot}\, d {\bf s}\), where \({\bf c} (t) = (\cos^5 t, \sin^3 t, t^4), 0 \le t \le \pi\), and \({\bf F}\) is as in Exercise 7.
If \(f(x)\) is a smooth function of one variable, must \({\bf F}(x,y)=f(x){\bf i}+f(y){\bf j}\) be a gradient?
Let \({\bf F} (x,y,z) = xy {\bf i}+ y {\bf j} + z {\bf k}\). Can there exist a function \(f\) such that \({\bf F} = {\nabla}\! f\)?
Let \({\bf F} = F_1 {\bf i} + F_2 {\bf j} + F_3 {\bf k}\) and suppose each \(F_k\) satisfies the homogeneity condition \[ F_k (tx, ty,tz) = t F_k (x,y,z), \qquad k=1,2,3. \]
Suppose also \({\nabla} \times {\bf F} ={\bf 0}\). Prove that \({\bf F} = {\nabla}\! f\), where \[ 2f (x,y,z) = x F_1 (x,y,z) + y F_2 (x,y,z) +z F_3 (x,y,z). \] [HINT: Use Review Exercise 31, Chapter 2.]
Let \({\bf F} (x,y,z) = (e^x \sin y) {\bf i} + ( e^x \cos y) {\bf j} + z^2 {\bf k}\). Evaluate the integral \(\int_{\bf c} {\bf F} \,{\cdot}\, d {\bf s}\), where \({\bf c} (t) = ( \sqrt{t}, t^3, \exp \sqrt{t}), 0 \le t \le 1\).
Let a fluid have the velocity field \({\bf F} (x,y,z) = xy {\bf i} + yz {\bf j} + xz {\bf k}\). What is the circulation around the unit circle in the \(xy\) plane? Interpret your answer.
The mass of the earth is approximately \(6 \times 10^{27}\) g and that of the sun is 330,000 times as much. The gravitational constant is \(6.7 \times 10^{-8} {\rm cm}^3/{\rm s}^2\,{\cdot}\,\)g. The distance of the earth from the sun is about \(1.5 \times 10^{12}\) cm. Compute, approximately, the work necessary to increase the distance of the earth from the sun by 1 cm.
Determine if the following vector fields \(\textbf{F}\) are gradient fields. If there exists a fuction \(f\) such that \(\nabla f = \textbf{F}\), find \(f\).
Determine if the following vector fields \(\textbf{F}\) are gradient fields. If there exists a function \(f\) such that \(\nabla f = \textbf{F}\), find \(f\).
Show that the following vector fields are conservative. Calculate \(\int_C {\bf F} \,{\cdot}\, d {\bf s}\) for the given curve.
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Prove Theorem 8. [HINT: Define \({\bf G} = G_1 {\bf i} + G_2 {\bf j} + G_3 {\bf k}\) by \begin{eqnarray*} G_1 (x,y,z) & = & \int_0^z F_2 (x,y,t) \,{\it {\,d} t} - \int_0^y F_3 (x,t,0) \,{\it {\,d} t} \\[2pt] G_2 (x,y,z) & = & - \int_0^z F_1 (x,y,t) \,{\it {\,d} t}\\[-10pt] \end{eqnarray*} and \(G_3 (x,y,z)=0\).]
Is each of the following vector fields the curl of some other vector field? If so, find the vector field.
Let \({\bf F} = xz {\bf i} - yz {\bf j} + y {\bf k}\). Verify that \({\nabla} \,{\cdot}\, {\bf F} =0\). Find a \({\bf G}\) such that \({\bf F} = {\nabla} \times {\bf G}\).
Repeat Exercise 22 for \({\bf F} = y^2 {\bf i} + z^2 {\bf j} + x^2 {\bf k}\).
Let \({\bf F} = xe^y {\bf i} - (x \cos z) {\bf j} - z e^y {\bf k}\). Find a \({\bf G}\) such that \({\bf F} = {\nabla} \times {\bf G}\).
Let \({\bf F} = (x \cos y) {\bf i} - (\sin y) {\bf j} + (\sin x) {\bf k}\). Find a \({\bf G}\) such that \({\bf F} = {\nabla} \times {\bf G}\).
By using different paths from \((0, 0, 0)\) to \((x,y,z)\), show that the function \(f\) defined in the proof of Theorem 7 for “condition (ii) implies condition (iii)” satisfies \(\partial\! f / \partial x = F_1\) and \(\partial\! f/ \partial y = F_2\).
Let \({\bf F}\) be the vector field on \({\mathbb R}^3\) given by \({\bf F} = - y {\bf i} + x {\bf j}\).
Let \({\bf G}\) be the vector field on \({\mathbb R}^3\backslash \{z \hbox{ axis}\}\) defined by \[ {\bf G} = \frac{-y}{x^2 + y^2}\, {\bf i} + \frac{x}{x^2 + y^2}\, {\bf j}. \]
Let \({\bf F} = - ({\it GmM} {\bf r} / r^3)\) be the gravitational force field defined on \({\mathbb R}^3 \backslash \{{\bf 0}\}\).