In Exercises 1 to 4, find an appropriate parametrization for the given piecewise-smooth curve in \(\mathbb {R}^2\), with the implied orientation.
The curve \(C\), which goes along the circle of radius 3, from the point \((3,0)\) to the point \((-3,0)\), and then in a straight line along the \(x\)-axis back to \((3,0)\)
The curve \(C\), which goes along \(y=x^2\) from the point \((0,0)\) to the point \((2,4)\), then in a straight line from \((2,4)\) to \((0,4)\), and then along the \(y\)-axis back to \((0,0)\)
The curve \(C\), which goes along \(y= \sin x\) from the point \((0,0)\) to the point \((\pi, 0)\), and then along the \(x\)-axis back to \((0,0)\)
The closed curve \(C\) described by the ellipse \[ \frac{(x-2)^{2}}{4} + \frac{(y-3)^{2}}{9} = 1 \] oriented counterclockwise
In Exercises 5 to 8, find an appropriate parametrization for the given piecewise-smooth curve in \(\mathbb{R}^3\).
The intersection of the plane \(z=3\) with the elliptical cylinder \[ \frac{x^2}{9} + \frac{y^2}{16} = 1 \]
The triangle formed by traveling from the point \((1,2,3)\) to \((0,-2,1)\), to \((6,4,2)\), and back to \((1,2,3)\)
The intersection of the surfaces \(y=x\) and \(z=x^3\), from the point \((-3,-3,9)\) to \((2,2,4)\)
The intersection of the cylinder \(y^2 + z^2 = 1\) and the plane \(z=x\)
Let \(f(x,y,z) = y\) and \({\bf c}(t) = (0,0,t), 0 \leq t \leq 1\). Prove that \(\int_{\bf c}f \,{\it ds} = 0\).
Evaluate the following path integrals \(\int_{\bf c}f(x,y,z) \ {\it ds}\), where
Evaluate the following path integrals \(\int_{\bf c} f(x,y,z) \,{\it ds}\), where
Evaluate the integral of \(f(x,y,z)\) along the path \({\bf c}\), where
Let \(f\colon\, {\mathbb R}^3\backslash \{ xz \hbox{ plane} \}\rightarrow {\mathbb R}\) be defined by \(f(x,y,z)=1/y^3\). Evaluate \(\int_{\bf c}f(x,y,z)\,{\it ds}\), where \({\bf c}\colon [1,e] \rightarrow {\mathbb R}^3\) is given by \({\bf c}(t) =(\log t) {\bf i} + t{\bf j} + 2 {\bf k}\).
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Let \(f(x,y) = 2x - y\), and consider the path \(x = t^4, y = t^4, -1 \leq t \leq 1\).
Exercises 16 to 19 are concerned with the application of the path integral to the problem of defining the average value of a scalar function along a path. Define the number \[ \frac{\int_{\bf c}f(x,y,z)\,{\it ds} }{l({\bf c})} \] to be the average value of f along \({\bf c}\). Here \(l({\bf c})\) is the length of the path: \[ l({\bf c}) = \int_{\bf c}\|{\bf c}'(t) \| \,{\it dt} . \] (This is analogous to the average of a function over a region defined in Section 6.3.)
Find the average \(y\) coordinate of the points on the semicircle parametrized by \({\bf c}\colon\,[0,\pi]\rightarrow {\mathbb R}^3, \theta \mapsto (0 , a \sin \theta, a \cos \theta); a> 0\).
Suppose the semicircle in Exercise 17 is made of a wire with a uniform density of 2 grams per unit length.
Let \({\bf c}\) be the path given by \({\bf c}(t)= (t^2, t, 3)\) for \(t \in [0,1]\).
Show that the path integral of a function \(f(x,y)\) over a path \(C\) given by the graph of \(y=g(x)\), \(a \leq x \leq b\) is given by: \[ \int_{C} f \,{\it ds} = \int_{a}^{b} f(x,g(x)) \sqrt{1 + [g'(x)]^2} \,{\it dx} \]
Conclude that if \(g:[a,b] \rightarrow \mathbb R\) is piecewise continuously differentiable, then the length of the graph of \(g\) on \([a,b]\) is given by: \[ \int_{C} f \,{\it ds} = \int_{a}^{b} \sqrt{1 + g'(x)^2} \,{\it dx}. \]
If \(g\colon\, [a,b]\rightarrow {\mathbb R}\) is piecewise continuously differentiable, let the length of the graph of \(g\) on \([a, b]\) be defined as the length of the path \(t \mapsto (t,g(t))\) for \(t \in [a,b]\).
Show that the length of the graph of \(g\) on \([a, b]\) is \[ \int^b_a \sqrt{1 + [g'(x)]^2} \,{\it dx}. \]
Use Exercise \(21\) to find the length of the graph of \(y = \log x\) from \(x=1\) to \(x=2\).
Use Exercise \(20\) to evaluate the path integral of \(f(x,y)=y\) over the graph of the semicircle \(y = \sqrt{1-x^2}\), \(-1 \leq x \leq 1\).
Compute the path integral of \(f(x,y)=y^2\) over the graph \(y = e^x\), \(0 \leq x \leq 1\).
Compute the path integral of \(f(x,y,z)={\it xyz}\) over the path \(c(t) = (\cos t, \sin t, t)\), \(0 \leq t \leq \frac{\pi}{2}\).
Find the mass of a wire formed by the intersection of the sphere \(x^2 + y^2 + z^2 =1\) and the plane \(x + y + z = 0\) if the density at \((x,y,z)\) is given by \(\rho(x,y,z) = x^2\) grams per unit length of wire.
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Evaluate \(\int_{\bf c}f \,{\it ds}\), where \(f(x,y,z) = z \) and \({\bf c}(t)=(t \cos t, t \sin t, t)\) for \(0 \leq t \leq t_0\).
Write the following limit as a path integral of \(f(x,y, z) = {\it xy}\) over some path \({\bf c}\) on [0, 1] and evaluate: \[ {\displaystyle \mathop {\rm limit}_{N \rightarrow \infty}} \sum_{i=1}^{N-1} t_i^2 \big(t^2_{i+1} \,{-}\, t^2_i\big), \] where \(t_1,\ldots, t_N\) is a partition of \([0, 1]\).
Consider paths that connect the points \(A = (0, 1)\) and \(B = (1, 0)\) in the xy plane, as in Figure 7.5.footnote #
Galileo contemplated the following question: Does a bead falling under the influence of gravity from a point \(A\) to a point \(B\) along a curve do so in the least possible time if that curve is a circular arc? For any given path, the time of transit \(T\) is a path integral \[ T=\int\frac{{\it dt}}{v}, \] where the bead’s velocity is \(v=\sqrt{2{\it gy}}\), where \(g\) is the gravitational constant. In 1697, Johann Bernoulli challenged the mathematical world to find the path in which the bead would roll from \(A\) to \(B\) in the least time. This solution would determine whether Galileo’s considerations had been correct.
Incidentally, Newton was the first to send his solution [which turned out to be a cycloid—the same curve (inverted) that we studied in Section 2.4, Example 4], but he did so anonymously. Bernoulli was not fooled, however. When he received the solution, he immediately knew its author, exclaiming, “I know the Lion from his paw.” While the solution of this problem is a cycloid, it is known in the literature as the brachistrochrone. This was the beginning of the important field called the calculus of variations.