5.2: Exercises
- Page ID
- 92321
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\(\newcommand{\avec}{\mathbf a}\) \(\newcommand{\bvec}{\mathbf b}\) \(\newcommand{\cvec}{\mathbf c}\) \(\newcommand{\dvec}{\mathbf d}\) \(\newcommand{\dtil}{\widetilde{\mathbf d}}\) \(\newcommand{\evec}{\mathbf e}\) \(\newcommand{\fvec}{\mathbf f}\) \(\newcommand{\nvec}{\mathbf n}\) \(\newcommand{\pvec}{\mathbf p}\) \(\newcommand{\qvec}{\mathbf q}\) \(\newcommand{\svec}{\mathbf s}\) \(\newcommand{\tvec}{\mathbf t}\) \(\newcommand{\uvec}{\mathbf u}\) \(\newcommand{\vvec}{\mathbf v}\) \(\newcommand{\wvec}{\mathbf w}\) \(\newcommand{\xvec}{\mathbf x}\) \(\newcommand{\yvec}{\mathbf y}\) \(\newcommand{\zvec}{\mathbf z}\) \(\newcommand{\rvec}{\mathbf r}\) \(\newcommand{\mvec}{\mathbf m}\) \(\newcommand{\zerovec}{\mathbf 0}\) \(\newcommand{\onevec}{\mathbf 1}\) \(\newcommand{\real}{\mathbb R}\) \(\newcommand{\twovec}[2]{\left[\begin{array}{r}#1 \\ #2 \end{array}\right]}\) \(\newcommand{\ctwovec}[2]{\left[\begin{array}{c}#1 \\ #2 \end{array}\right]}\) \(\newcommand{\threevec}[3]{\left[\begin{array}{r}#1 \\ #2 \\ #3 \end{array}\right]}\) \(\newcommand{\cthreevec}[3]{\left[\begin{array}{c}#1 \\ #2 \\ #3 \end{array}\right]}\) \(\newcommand{\fourvec}[4]{\left[\begin{array}{r}#1 \\ #2 \\ #3 \\ #4 \end{array}\right]}\) \(\newcommand{\cfourvec}[4]{\left[\begin{array}{c}#1 \\ #2 \\ #3 \\ #4 \end{array}\right]}\) \(\newcommand{\fivevec}[5]{\left[\begin{array}{r}#1 \\ #2 \\ #3 \\ #4 \\ #5 \\ \end{array}\right]}\) \(\newcommand{\cfivevec}[5]{\left[\begin{array}{c}#1 \\ #2 \\ #3 \\ #4 \\ #5 \\ \end{array}\right]}\) \(\newcommand{\mattwo}[4]{\left[\begin{array}{rr}#1 \amp #2 \\ #3 \amp #4 \\ \end{array}\right]}\) \(\newcommand{\laspan}[1]{\text{Span}\{#1\}}\) \(\newcommand{\bcal}{\cal B}\) \(\newcommand{\ccal}{\cal C}\) \(\newcommand{\scal}{\cal S}\) \(\newcommand{\wcal}{\cal W}\) \(\newcommand{\ecal}{\cal E}\) \(\newcommand{\coords}[2]{\left\{#1\right\}_{#2}}\) \(\newcommand{\gray}[1]{\color{gray}{#1}}\) \(\newcommand{\lgray}[1]{\color{lightgray}{#1}}\) \(\newcommand{\rank}{\operatorname{rank}}\) \(\newcommand{\row}{\text{Row}}\) \(\newcommand{\col}{\text{Col}}\) \(\renewcommand{\row}{\text{Row}}\) \(\newcommand{\nul}{\text{Nul}}\) \(\newcommand{\var}{\text{Var}}\) \(\newcommand{\corr}{\text{corr}}\) \(\newcommand{\len}[1]{\left|#1\right|}\) \(\newcommand{\bbar}{\overline{\bvec}}\) \(\newcommand{\bhat}{\widehat{\bvec}}\) \(\newcommand{\bperp}{\bvec^\perp}\) \(\newcommand{\xhat}{\widehat{\xvec}}\) \(\newcommand{\vhat}{\widehat{\vvec}}\) \(\newcommand{\uhat}{\widehat{\uvec}}\) \(\newcommand{\what}{\widehat{\wvec}}\) \(\newcommand{\Sighat}{\widehat{\Sigma}}\) \(\newcommand{\lt}{<}\) \(\newcommand{\gt}{>}\) \(\newcommand{\amp}{&}\) \(\definecolor{fillinmathshade}{gray}{0.9}\)True or false?
- \(\vecs{ \nabla} \cdot(\textbf{a} \times\vecs{r} ) = 0\text{,}\) where \(\textbf{a}\) is a constant vector in \(\mathbb{R}^3\), and \(\vecs{r} \) is the vector field \(\vecs{r} = (x, y, z)\text{.}\)
- \(\vecs{ \nabla} \times(\vecs{ \nabla} f) = 0\) for all scalar fields \(f\) on \(\mathbb{R}^3\) with continuous second partial derivatives.
- \(\vecs{ \nabla} \cdot(f \vecs{F} ) = \vecs{ \nabla} (f)\cdot \vecs{F} + f \vecs{ \nabla} \cdot\vecs{F} \text{,}\) for every vector field \(\vecs{F} \) in \(\mathbb{R}^3\) with continuous partial derivatives, and every scalar function \(f\) in \(\mathbb{R}^3\) with continuous partial derivatives.
- Suppose \(\vecs{F} \) is a vector field with continuous partial derivatives in the region \(D\text{,}\) where \(D\) is \(\mathbb{R}^3\) without the origin. If \(\vecs{ \nabla} \cdot\vecs{F} \gt 0\) throughout \(D\text{,}\) then the flux of \(F\) through the sphere of radius \(5\) with center at the origin is positive.
- If a vector field \(\vecs{F} \) is defined and has continuous partial derivatives everywhere in \(\mathbb{R}^3\text{,}\) and it satisfies \(\vecs{ \nabla} \cdot\vecs{F} = 0\text{,}\) everywhere, then, for every sphere, the flux out of one hemisphere is equal to the flux into the opposite hemisphere.
- If \(\vecs{r} (t)\) is a twice continuously differentiable path in \(\mathbb{R}^2\) with constant curvature \(\kappa\text{,}\) then \(\vecs{r} (t)\) parametrizes part of a circle of radius \(1/\kappa\text{.}\)
- The vector field \(\vecs{F} = \left( -\frac{y}{x^2+y^2}\,,\,\frac{x}{x^2+y^2}\right)\) is conservative in its domain, which is \(\mathbb{R}^2\text{,}\) without the origin.
- If a vector field \(\vecs{F} = (P, Q)\) in \(\mathbb{R}^2\) has \(Q = 0\) everywhere in \(\mathbb{R}^2\text{,}\) then the line integral \(\oint\vecs{F} \cdot\text{d}\vecs{r} \) is zero, for every simple closed curve in \(\mathbb{R}^2\text{.}\)
- If the acceleration and the speed of a moving particle in \(\mathbb{R}^3\) are constant, then the motion is taking place along a spiral.
True or false?
- \(\vecs{ \nabla} \times(\textbf{a} \times\vecs{r} ) = 0\text{,}\) where \(\textbf{a}\) is a constant vector in \(\mathbb{R}^3\), and \(\vecs{r} \) is the vector field \(\vecs{r} = (x, y, z)\text{.}\)
- \(\vecs{ \nabla} \cdot(\vecs{ \nabla} f) = 0\) for all scalar fields \(f\) on \(\mathbb{R}^3\) with continuous second partial derivatives.
- \(\vecs{ \nabla} (\vecs{ \nabla} \cdot \vecs{F} ) = 0\) for every vector field \(\vecs{F} \) on \(\mathbb{R}^3\) with continuous second partial derivatives.
- Suppose \(\vecs{F} \) is a vector field with continuous partial derivatives in the region \(D\text{,}\) where \(D\) is \(\mathbb{R}^3\) without the origin. If \(\vecs{ \nabla} \cdot\vecs{F} = 0\text{,}\) then the flux of \(\vecs{F} \) through the sphere of radius \(5\) with center at the origin is \(0\text{.}\)
- Suppose \(\vecs{F} \) is a vector field with continuous partial derivatives in the region \(D\text{,}\) where \(D\) is \(\mathbb{R}^3\) without the origin. If \(\vecs{ \nabla} \times\vecs{F} =\vecs{0}\) then \(\oint_C\vecs{F} \cdot\text{d}\vecs{r} \) is zero, for every simple and smooth closed curve \(C\) in \(\mathbb{R}^3\) which avoids the origin.
- If a vector field \(\vecs{F} \) is defined and has continuous partial derivatives everywhere in \(\mathbb{R}^3\text{,}\) and it satisfies \(\vecs{ \nabla} \cdot\vecs{F} \gt 0\text{,}\) everywhere, then, for every sphere, the flux out of one hemisphere is larger than the flux into the opposite hemisphere.
- If \(\vecs{r} (t)\) is a path in \(\mathbb{R}^3\) with constant curvature \(\kappa\text{,}\) then \(\vecs{r} (t)\) parametrizes part of a circle of radius \(1/\kappa\text{.}\)
- The vector field \(\vecs{F} = \left( -\frac{y}{x^2+y^2}\,,\,\frac{x}{x^2+y^2} \,,\,z\right)\) is conservative in its domain, which is \(\mathbb{R}^3\text{,}\) without the \(z\)-axis.
- If all flow lines of a vector field in \(\mathbb{R}^3\) are parallel to the \(z\)-axis, then the circulation of the vector field around every closed curve is \(0\text{.}\)
- If the speed of a moving particle is constant, then its acceleration is orthogonal to its velocity.
- True or false? If \(\vecs{r} (t)\) is the position at time \(t\) of an object moving in \(\mathbb{R}^3\text{,}\) and \(\vecs{r} (t)\) is twice differentiable, then \(|\vecs{r} ''(t)|\) is the tangential component of its acceleration.
- Let \(\vecs{r} (t)\) is a smooth curve in \(\mathbb{R}^3\) with unit tangent, normal and binormal vectors \(\hat{\textbf{T}}(t)\text{,}\) \(\hat{\textbf{N}}(t)\text{,}\) \(\hat{\textbf{B}}(t)\text{.}\) Which two of these vectors span the plane normal to the curve at \(\vecs{r} (t)\text{?}\)
- True or false? If \(\vecs{F} = P\hat{\pmb{\imath}} + Q\hat{\pmb{\jmath}} + R\hat{\mathbf{k}}\) is a vector field on \(\mathbb{R}^3\) such that \(P\text{,}\) \(Q\text{,}\) \(R\) have continuous first order derivatives, and if \(\vecs{ \nabla} \times\vecs{F} = \vecs{0}\) everywhere on \(\mathbb{R}^3\), then \(\vecs{F} \) is conservative.
- True or false? If \(\vecs{F} = P\hat{\pmb{\imath}} + Q\hat{\pmb{\jmath}} + R\hat{\mathbf{k}}\) is a vector field on \(\mathbb{R}^3\) such that \(P\text{,}\) \(Q\text{,}\) \(R\) have continuous second order derivatives, then \(\vecs{ \nabla} \times(\vecs{ \nabla} \cdot F) = 0\text{.}\)
- True or false? If \(\vecs{F} \) is a vector field on \(\mathbb{R}^3\) such that \(|\vecs{F} (x, y, z)| = 1\) for all \(x\text{,}\) \(y\text{,}\) \(z\text{,}\) and if \(S\) is the sphere \(x^2 + y^2 + z^2 = 1\text{,}\) then \(\iint_S \vecs{F} \cdot\hat{\textbf{n}}\,\text{d}S = 4\pi\text{.}\)
- True or false? Every closed surface \(S\) in \(\mathbb{R}^3\) is orientable. (Recall that \(S\) is closed if it is the boundary of a solid region \(E\text{.}\))
- In the curve shown below (a helix lying in the surface of a cone), is the curvature increasing, decreasing, or constant as z increases?
- Of the two functions shown below, one is a function \(f(x)\) and one is its curvature \(\kappa(x)\text{.}\) Which is which?
- Let \(C\) be the curve of intersection of the cylinder \(x^2 + z^2 = 1\) and the saddle \(xz = y\text{.}\) Parametrise \(C\text{.}\) (Be sure to specify the domain of your parametrisation.)
- Let \(H\) be the helical ramp (also known as a helicoid) which revolves around the \(z\)-axis in a clockwise direction viewed from above, beginning at the y-axis when \(z = 0\text{,}\) and rising \(2\pi\) units each time it makes a full revolution. Let \(S\) be the the portion of \(H\) which lies outside the cylinder \(x^2 + y^2 = 4\text{,}\) above the \(z = 0\) plane and below the \(z = 5\) plane. Choose one of the following functions and give the domain on which the function you have chosen parametrizes S. (Hint: Only one of the following functions is possible.)
- \(\displaystyle \vecs{r} (u, v) = \big(u \cos v, u \sin v, u\big)\)
- \(\displaystyle \vecs{r} (u, v) = \big(u \cos v, u \sin v, v\big)\)
- \(\displaystyle \vecs{r} (u, v) = \big(u \sin v, u \cos v, u\big)\)
- \(\displaystyle \vecs{r} (u, v) = \big(u \sin v, u \cos v, v\big)\)
- Write down a parametrized curve of zero curvature and arclength \(1\text{.}\) (Be sure to specify the domain of your parametrisation.)
- If \(\vecs{ \nabla} \cdot\vecs{F} \) is a constant \(C\) on all of \(\mathbb{R}^3\text{,}\) and \(S\) is a cube of unit volume such that the flux outward through each side of \(S\) is \(1\text{,}\) what is \(C\text{?}\)
- Let
\[ \vecs{F} (x, y) = \big(ax + by\,,\, cx + dy\big) \nonumber \]
Give the full set of \(a\text{,}\) \(b\text{,}\) \(c\) and \(d\) such that \(\vecs{F} \) is conservative. - If \(\vecs{r} (s)\) has been parametrized by arclength (i.e. \(s\) is arclength), what is the arclength of \(\vecs{r} (s)\) between \(s = 3\) and \(s = 5\text{?}\)
- Let \(\vecs{F} \) be a 2D vector field which is defined everywhere except at the points marked \(P\) and \(Q\text{.}\) Suppose that \(\vecs{ \nabla} \times\vecs{F} = 0\) everywhere on the domain of \(\vecs{F} \text{.}\) Consider the five curves \(R\text{,}\) \(S\text{,}\) \(T\text{,}\) \(U\text{,}\) and \(V\) shown in the picture.
Which of the following is necessarily true?
- \(\displaystyle \int_S \vecs{F} \cdot\text{d}\vecs{r} = \int_T \vecs{F} \cdot\text{d}\vecs{r} \)
- \(\displaystyle \int_R \vecs{F} \cdot\text{d}\vecs{r} = \int_S \vecs{F} \cdot\text{d}\vecs{r} = \int_T \vecs{F} \cdot\text{d}\vecs{r} = \int_U \vecs{F} \cdot\text{d}\vecs{r} = 0\)
- \(\displaystyle \int_R \vecs{F} \cdot\text{d}\vecs{r} + \int_S \vecs{F} \cdot\text{d}\vecs{r} + \int_T \vecs{F} \cdot\text{d}\vecs{r} = \int_U \vecs{F} \cdot\text{d}\vecs{r} \)
- \(\displaystyle \int_U \vecs{F} \cdot\text{d}\vecs{r} = \int_R \vecs{F} \cdot\text{d}\vecs{r} + \int_S \vecs{F} \cdot\text{d}\vecs{r} \)
- \(\displaystyle \int_V \vecs{F} \cdot\text{d}\vecs{r} = 0\)
- Write down a 3D vector field \(\vecs{F} \) such that for all closed surfaces \(S\text{,}\) the volume enclosed by \(S\) is equal to
\[ \iint_S \vecs{F} \cdot \hat{\textbf{n}}\,\text{d}S \nonumber \]
- Consider the vector field \(\vecs{F} \) in the \(xy\)-plane shown below. Is the \(\hat{\mathbf{k}}^{\rm th}\) component of \(\vecs{ \nabla} \times\vecs{F} \) at \(P\) positive, negative or zero?
Say whether the following statements are true or false.
- If \(\vecs{F} \) is a 3D vector field defined on all of \(\mathbb{R}^3\), and \(S_1\) and \(S_2\) are two surfaces with the same boundary, but \(\iint_{S_1} \vecs{F} \cdot\hat{\textbf{n}}\,\text{d}S \ne \iint_{S_2} \vecs{F} \cdot\hat{\textbf{n}}\,\text{d}S\text{,}\) then \(\vecs{ \nabla} \cdot\vecs{F} \) is not zero anywhere.
- If \(\vecs{F} \) is a vector field satisfying \(\vecs{ \nabla} \times\vecs{F} \) = 0 whose domain is not simply-connected, then \(\vecs{F} \) is not conservative.
- The osculating circle of a curve \(C\) at a point has the same unit tangent vector, unit normal vector, and curvature as \(C\) at that point.
- A planet orbiting a sun has period proportional to the cube of the major axis of the orbit.
- For any 3D vector field \(\vecs{F} \text{,}\) \(\vecs{ \nabla} \cdot(\vecs{ \nabla} \times\vecs{F} )\) = 0.
- A field whose divergence is zero everywhere in its domain has closed surfaces \(S\) in its domain.
- The gravitational force field is conservative.
- If \(\vecs{F} \) is a field defined on all of \(\mathbb{R}^3\) such that \(\int_C \vecs{F} \cdot \text{d}\vecs{r} = 3\) for some curve \(C\text{,}\) then \(\vecs{ \nabla} \times\vecs{F} \) is non-zero at some point.
- The normal component of acceleration for a curve of constant curvature is constant.
- The curve defined by
\[ \vecs{r} _1(t) = \cos(t^4)\,\hat{\pmb{\imath}} + 3t^4\hat{\pmb{\jmath}},\qquad -\infty \lt t \lt \infty, \nonumber \]
is the same as the curve defined by\[ \vecs{r} _2(t) = \cos t\,\hat{\pmb{\imath}} + 3t\,\hat{\mathbf{k}},\qquad -\infty \lt t \lt \infty \nonumber \]
Which of the following statements are true (T) and which are false (F)?
All real valued functions \(f(x,y,z)\) and all vector fields \(\vecs{F} (x, y, z)\) have domain \(\mathbb{R}^3\) unless specified otherwise.
- If \(f\) is a continuous real valued function and \(S\) a smooth oriented surface, then
\[ \iint_S f\, \text{d}S = -\iint_{-S} f\,\text{d}S \nonumber \]
where `\(-S\)' denotes the surface \(S\) but with the opposite orientation. - Suppose the components of the vector field \(\vecs{F} \) have continuous partial derivatives. If \(\iint_S\vecs{ \nabla} \times\vecs{F} \cdot\hat{\textbf{n}}\,\text{d}S=0\) for every closed smooth surface, then \(\vecs{F} \) is conservative.
- Suppose \(S\) is a smooth surface bounded by a smooth simple closed curve \(C\text{.}\) The orientation of \(C\) is determined by that of \(S\) as in Stokes' theorem. Suppose the real valued function \(f\) has continuous partial derivatives. Then
\[ \int_C f\,\text{d}x =\iint_S \left(\frac{\partial f}{\partial z}\hat{\pmb{\jmath}} - \frac{\partial f}{\partial y}\hat{\mathbf{k}}\right)\cdot\hat{\textbf{n}}\,\text{d}S \nonumber \]
- Suppose the real valued function \(f(x,y,z)\) has continuous second order partial derivatives. Then
\[ (\vecs{ \nabla} f ) \times (\vecs{ \nabla} f ) = \vecs{ \nabla} \times (\vecs{ \nabla} f ) \nonumber \]
- The curve parameterized by
\[ \vecs{r} (t) = \big(2 + 4t^3 \,,\, -t^3 \,,\, 1 - 2t^3\big)\qquad -\infty \lt t \lt \infty \nonumber \]
has curvature \(\kappa(t) = 0\) for all \(t\text{.}\) - If a smooth curve is parameterized by \(\vecs{r} (s)\) where \(s\) is arc length, then its tangent vector satisfies
\[ |\vecs{r} '(s)| = 1 \nonumber \]
- If \(S\) is the sphere \(x^2 + y^2 + z^2 = 1\) and \(\vecs{F} \) is a constant vector field, then \(\iint_S \vecs{F} \cdot\hat{\textbf{n}}\, \text{d}S = 0\text{.}\)
- There exists a vector field \(\vecs{F} \) whose components have continuous second order partial derivatives such that \(\vecs{ \nabla} \times\vecs{F} = (x, y, z)\text{.}\)
The vector field \(\vecs{F} = P (x, y)\,\hat{\pmb{\imath}} + Q(x, y)\,\hat{\pmb{\jmath}}\) is plotted below.
In the following questions, give the answer that is best supported by the plot.
- The derivative \(P_y\) at the point labelled \(A\) is (a) positive, (b) negative, (c) zero, (d) there is not enough information to tell.
- The derivative \(Q_x\) at the point labelled \(A\) is (a) positive, (b) negative, (c) zero, (d) there is not enough information to tell.
- The curl of \(\vecs{F} \) at the point labelled \(A\) is (a) in the direction of \(+\hat{\mathbf{k}}\) (b) in the direction of \(-\hat{\mathbf{k}}\) (c) zero (d) there is not enough information to tell.
- The work done by the vector field on a particle travelling from point \(B\) to point \(C\) along the curve \(\mathcal{C}_1\) is (a) positive (b) negative (c) zero (d) there is not enough information to tell.
- The work done by the vector field on a particle travelling from point \(B\) to point \(C\) along the curve \(\mathcal{C}_2\) is (a) positive (b) negative (c) zero (d) there is not enough information to tell.
- The vector field \(\vecs{F} \) is (a) the gradient of some function \(f\) (b) the curl of some vector field \(\textbf{G}\) (c) not conservative (d) divergence free.
Which of the following statements are true (T) and which are false (F)?
- The curve defined by
\[ \vecs{r} _1(t) = \cos(t^2 )\,\hat{\pmb{\imath}} + \sin(t^2 )\,\hat{\pmb{\jmath}} + 2t^2\,\hat{\mathbf{k}},\qquad -\infty \lt t \lt \infty \nonumber \]
is the same as the curve defined by\[ \vecs{r} _2 (t) = \cos t\,\hat{\pmb{\imath}} + \sin t\,\hat{\pmb{\jmath}} + 2t\,\hat{\mathbf{k}},\qquad -\infty \lt t \lt \infty \nonumber \]
- The curve defined by
\[ \vecs{r} _1(t) = \cos(t^2)\,\hat{\pmb{\imath}} + \sin(t^2 )\,\hat{\pmb{\jmath}} + 2t^2\,\hat{\mathbf{k}},\qquad 0 \le t \le 1 \nonumber \]
is the same as the curve defined by\[ \vecs{r} _2(t) = \cos t\,\hat{\pmb{\imath}} + \sin t\,\hat{\pmb{\jmath}} + 2t\,\hat{\mathbf{k}},\qquad 0 \le t \le 1 \nonumber \]
- If a smooth curve is parameterized by \(\vecs{r} (s)\) where \(s\) is arc length, then its tangent vector satisfies
\[ |\vecs{r} '(s)| = 1 \nonumber \]
- If \(\vecs{r} (t)\) defines a smooth curve \(C\) in space that has constant curvature \(\kappa \gt 0\text{,}\) then \(C\) is part of a circle with radius \(1/\kappa\text{.}\)
- If the speed of a moving object is constant, then its acceleration is orthogonal to its velocity.
- The vector field
\[ \vecs{F} (x, y, z) = \frac{-y}{x^2+y^2} \hat{\pmb{\imath}} + \frac{x}{x^2+y^2} \hat{\pmb{\jmath}} + z\hat{\mathbf{k}} \nonumber \]
is conservative. - Suppose the vector field \(\vecs{F} (x, y, z)\) is defined on an open domain and its components have continuous partial derivatives. If \(\vecs{ \nabla} \times\vecs{F} = 0\text{,}\) then \(\vecs{F} \) is conservative.
- The region \(D =\left \{ (x, y) \big|B x^2 + y^2 \gt 1 \right \}\) is simply connected.
- The region \(D = \left \{ (x, y) \big|B y - x^2 \gt 0 \right \}\) is simply connected.
- If \(\vecs{F} \) is a vector field whose components have two continuous partial derivatives, then
\[ \iint_S \vecs{ \nabla} \times \vecs{F} \cdot\hat{\textbf{n}}\, \text{d}S = 0 \nonumber \]
when \(S\) is the boundary of a solid region \(E\) in \(\mathbb{R}^3\text{.}\)
Which of the following statements are true (T) and which are false (F)?
- If a smooth curve \(C\) is parameterized by \(\vecs{r} (s)\) where \(s\) is arc length, then the tangent vector \(\vecs{r} '(s)\) satisfies \(|\vecs{r} '(s)| = 1\text{.}\)
- If \(\vecs{r} (t)\) defines a smooth curve \(C\) in space that has constant curvature \(\kappa \gt 0\text{,}\) then \(C\) is part of a circle with radius \(1/\kappa\text{.}\)
- Suppose \(\vecs{F} \) is a continuous vector field with open domain \(D\text{.}\) If
\[ \int_C \vecs{F} \cdot \text{d}\vecs{r} = 0 \nonumber \]
for every piecewise smooth closed curve \(C\) in \(D\text{,}\) then \(\vecs{F} \) is conservative. - Suppose \(\vecs{F} \) is a vector field with open domain \(D\text{,}\) and the components of \(\vecs{F} \) have continuous partial derivatives. If \(\vecs{ \nabla} \times \vecs{F} = 0\) everywhere on \(D\text{,}\) then \(\vecs{F} \) is conservative.
- The curve defined by
\[ \vecs{r} _1(t) = \cos(t^2)\,\hat{\pmb{\imath}} + \sin(t^2)\,\hat{\pmb{\jmath}} + 2t^2\,\hat{\mathbf{k}},\qquad -\infty \lt t \lt \infty \nonumber \]
is the same as the curve defined by\[ \vecs{r} _2 (t) = \cos t\,\hat{\pmb{\imath}} + \sin t\,\hat{\pmb{\jmath}} + 2t\,\hat{\mathbf{k}},\qquad -\infty \lt t \lt \infty \nonumber \]
- The curve defined by
\[ \vecs{r} _1(t) = \cos(t^2)\,\hat{\pmb{\imath}} + \sin(t^2)\,\hat{\pmb{\jmath}} + 2t^2\,\hat{\mathbf{k}},\qquad 0\le t \le 1 \nonumber \]
is the same as the curve defined by\[ \vecs{r} _2 (t) = \cos t\,\hat{\pmb{\imath}} + \sin t\,\hat{\pmb{\jmath}} + 2t\,\hat{\mathbf{k}},\qquad 0\le t\le 1 \nonumber \]
- Suppose \(\vecs{F} (x, y, z)\) is a vector field whose components have continuous second order partial derivatives. Then \(\vecs{ \nabla} \cdot (\vecs{ \nabla} \times F) = 0\text{.}\)
- Suppose the real valued function \(f(x, y, z)\) has continuous second order partial derivatives. Then \(\vecs{ \nabla} \cdot(\vecs{ \nabla} f) = 0\text{.}\)
- The region \(D = \left \{ (x, y) \big| x^2 + y^2 \gt 1 \right \}\) is simply connected.
- The region \(D = \left \{ (x, y) \big| y - x^2 \gt 0 \right \}\) is simply connected.
Let \(\vecs{F} \text{,}\) \(\textbf{G}\) be vector fields, and \(f\text{,}\) \(g\) be scalar fields. Assume \(\vecs{F} \text{,}\) \(\textbf{G}\text{,}\) \(f\text{,}\) \(g\) are defined on all of \(\mathbb{R}^3\) and have continuous partial derivatives of all orders everywhere. Mark each of the following as True (T) or False (F).
- If \(C\) is a closed curve and \(\vecs{ \nabla} f=\vecs{0}\text{,}\) then \(\int_C f\,\text{d}s=0\text{.}\)
- If \(\vecs{r} (t)\) is a parametrization of a smooth curve \(C\) and the binormal \(\textbf{B}(t)\) is constant then \(C\) is a straight line.
- If \(\vecs{r} (t)\) is the position of a particle which travels with constant speed, then \(\vecs{r} '(t)\cdot\vecs{r} ''(t)=0\text{.}\)
- If \(C\) is a path from points \(A\) to \(B\text{,}\) then the line integral \(\int_C\big(\vecs{F} \times\textbf{G}\big)\cdot\text{d}\vecs{r} \) is independent of the path \(C\text{.}\)
- The line integral \(\int_C f\,\text{d}s\) does not depend of the orientation of the curve \(C\text{.}\)
- If \(S\) is a parametric surface \(\vecs{r} (u,v)\) then a normal to \(S\) is given by
\[\begin{gather*} \frac{\partial\vecs{r} }{\partial u}\times \frac{\partial\vecs{r} }{\partial u} \end{gather*}\]
- The surface area of the parametric surface \(S\) given by \(\vecs{r} (u,v) = x(u,v)\,\hat{\pmb{\imath}} + y(u,v)\,\hat{\pmb{\jmath}} + z(u,v)\,\hat{\mathbf{k}}\text{,}\) \((u,v)\in D\text{,}\) is given by
\[\begin{gather*} \iint_D \left(1+\big(\tfrac{\partial z}{\partial u}\big)^2 +\big(\tfrac{\partial z}{\partial v}\big)^2\right)^{1/2} \text{d}u\text{d}v \end{gather*}\]
- If \(\vecs{F} \) is the velocity field of an incompressible fluid then \(\vecs{ \nabla} \cdot\vecs{F} =0\text{.}\)
- \(\displaystyle \vecs{ \nabla} \cdot\big(\vecs{F} \times\textbf{G}\big) = (\vecs{ \nabla} \cdot\vecs{F} )\textbf{G} + (\vecs{ \nabla} \cdot\textbf{G})\vecs{F} \)
Say whether the following statements are true (T) or false (F). You may assume that all functions and vector fields are defined everywhere and have derivatives of all orders everywhere.
- The divergence of \(\vecs{ \nabla} \times\vecs{F} \) is zero, for every \(\vecs{F} \text{.}\)
- In a simply connected region, \(\int_C \vecs{F} \cdot\text{d}\vecs{r} \) depends only on the endpoints of \(C\text{.}\)
- If \(\vecs{ \nabla} f = 0\text{,}\) then \(f\) is a constant function.
- If \(\vecs{ \nabla} \times\vecs{F} = \vecs{0}\text{,}\) then \(\vecs{F} \) is a constant vector field.
- If \(\vecs{ \nabla} \cdot\vecs{F} = 0\text{,}\) then \(\iint_S\vecs{F} \cdot\hat{\textbf{n}}\, \text{d}S = 0\) for every closed surface \(S\text{.}\)
- If \(\int_C \vecs{F} \cdot \text{d}\vecs{r} = 0\) for every closed curve \(C\text{,}\) then \(\vecs{ \nabla} \times\vecs{F} = 0\text{.}\)
- If \(\vecs{r} (t)\) is a path in three space with constant speed \(|\vecs{v} (t)|\text{,}\) then the acceleration is perpendicular to the tangent vector, i.e. \(\textbf{a}\cdot\hat{\textbf{T}} = 0\text{.}\)
- If \(\vecs{r} (t)\) is a path in three space with constant curvature \(\kappa\text{,}\) then \(\vecs{r} (t)\) parameterizes part of a circle of radius \(1/\kappa\text{.}\)
- Let \(\vecs{F} \) be a vector field and suppose that \(S_1\) and \(S_2\) are oriented surfaces with the same boundary curve \(C\text{,}\) and \(C\) is given the direction that is compatible with the orientations of \(S_1\) and \(S_2\). Then \(\iint_{S 1} \vecs{F} \cdot\hat{\textbf{n}}\, \text{d}S = \iint_{S 2} \vecs{F} \cdot\hat{\textbf{n}}\, \text{d}S\text{.}\)
- Let \(A(t)\) be the area swept out by the trajectory of a planet from time \(t=0\) to time \(t\text{.}\) The \(\dfrac{dA}{dt}\) is constant.
Find the correct identity, if \(f\) is a function and \(\textbf{G}\) and \(\vecs{F} \) are vector fields. Select the true statement.
- \(\displaystyle \vecs{ \nabla} \cdot(f \vecs{F} ) = f \vecs{ \nabla} \times(\vecs{F} ) + (\vecs{ \nabla} f ) \times\vecs{F} \)
- \(\displaystyle \vecs{ \nabla} \cdot(f \vecs{F} ) = f \vecs{ \nabla} \cdot(\vecs{F} ) + \vecs{F} \cdot \vecs{ \nabla} f\)
- \(\displaystyle \vecs{ \nabla} \times(f \vecs{F} ) = f \vecs{ \nabla} \cdot(\vecs{F} ) + \vecs{F} \cdot \vecs{ \nabla} f\)
- None of the above are true.
True or False. Consider vector fields \(\vecs{F} \) and scalar functions \(f\) and \(g\) which are defined and smooth in all of three-dimensional space. Let \(\vecs{r} =(x,y,z)\) represent a variable point in space, and let \(\boldsymbol{\omega} = (\omega_1,\omega_2,\omega_3)\) be a constant vector. Let \(\Omega\) be a smoothly bounded domain with outer normal \(\hat{\textbf{n}}\text{.}\) Which of the following are identites, always valid under these assumptions?
- \(\displaystyle \vecs{ \nabla} \cdot\vecs{ \nabla} f = 0\)
- \(\displaystyle \vecs{F} \times\vecs{ \nabla} f = f\,\vecs{ \nabla} \cdot\vecs{F} \)
- \(\displaystyle \vecs{ \nabla} ^2 f = \vecs{ \nabla} (\vecs{ \nabla} \cdot f)\)
- \(\displaystyle \vecs{ \nabla} \times\vecs{ \nabla} f = \vecs{0}\)
- \(\displaystyle (\vecs{ \nabla} \times f)+(\vecs{ \nabla} \times g) = \vecs{ \nabla} f\times\vecs{ \nabla} g\)
- \(\displaystyle \vecs{ \nabla} \cdot\vecs{ \nabla} \times\vecs{F} = 0\)
- \(\vecs{ \nabla} \cdot\frac{\vecs{r} }{|\vecs{r} |^2} = 0\) for \(\vecs{r} \ne\vecs{0}\)
- \(\displaystyle \vecs{ \nabla} \times(\boldsymbol{\omega}\times\vecs{r} ) = \vecs{0}\)
- \(\displaystyle \iiint_\Omega f\vecs{ \nabla} \cdot\vecs{F} \,\text{d}V =-\iiint_\Omega \vecs{ \nabla} f\cdot\vecs{F} \,\text{d}V +\iint_{\partial\Omega} f\vecs{F} \cdot\hat{\textbf{n}}\,\text{d}S\)
- \(\displaystyle \iint_{\partial\Omega} f\hat{\textbf{n}}\,\text{d}S =- \iiint_\Omega \vecs{ \nabla} f\,\text{d}V\)
Determine if the given statements are True or False. Provide a reason or a counterexample.
- A constant vector field is conservative on \(\mathbb{R}^3\text{.}\)
- If \(\vecs{ \nabla} \cdot\vecs{F} = 0\) for all points in the domain of \(\vecs{F} \) then \(\vecs{F} \) is a constant vector field.
- Let \(\vecs{r} (t)\) be a parametrization of a curve \(C\) in \(\mathbb{R}^3\text{.}\) If \(\vecs{r} (t)\) and \(\dfrac{d\vecs{r} }{dt}\) are orthogonal at all points of the curve \(C\text{,}\) then \(C\) lies on the surface of a sphere \(x^2 + y^2 + z^2 = a^2\) for some \(a \gt 0\text{.}\)
- The curvature \(\kappa\) at a point on a curve depends on the orientation of the curve.
- The domain of a conservative vector field must be simply connected.
Provide a short answer to each question.
- Compute \(\vecs{ \nabla} \cdot\big(x^2 y\,\hat{\pmb{\imath}} + e^y \sin x\,\hat{\pmb{\jmath}} + e^{zx}\,\hat{\mathbf{k}}\big)\)
- Compute \(\vecs{ \nabla} \times(\cos x^2\,\hat{\pmb{\imath}} - y^3 z\,\hat{\pmb{\jmath}} + xz\,\hat{\mathbf{k}}\big)\)
- Let
\[ \vecs{F} = \frac{x}{x^2+y^2}\hat{\pmb{\imath}} +\frac{y}{x^2+y^2}\hat{\pmb{\jmath}} +z^2\,\hat{\mathbf{k}} \nonumber \]
and let \(D\) be the domain of \(\vecs{F} \text{.}\) Consider the following four statments.
- \(D\) is connected
- \(D\) is disconnected
- \(D\) is simply connected
- \(D\) is not simply connected
Choose one of the following:
- (II) and (III) are true
- (I) and (III) are true
- (I) and (IV) are true
- (II) and (IV) are true
- Not enough information to determine
- True or False? If the speed of a particle is constant then the acceleration of the particle is zero. If your answer is True, provide a reason. If your answer is False, provide a counter example.
Are each of the following statements True or False? Recall that \(f \in C^k\) means that all derivatives of \(f\) up to order \(k\) exist and are continuous.
- \(\vecs{ \nabla} \times(f \vecs{ \nabla} f ) = \vecs{0}\) for all \(C^2\) scalar functions \(f\) in \(\mathbb{R}^3\text{.}\)
- \(\vecs{ \nabla} \cdot(f\vecs{F} ) = \vecs{ \nabla} f \cdot\vecs{F} + f\vecs{ \nabla} \cdot \vecs{F} \) for all \(C^1\) scalar functions \(f\) and \(C^1\) vector fields \(\vecs{F} \) in \(\mathbb{R}^3\text{.}\)
- A smooth space curve \(C\) with constant curvature \(\kappa = 0\) must be a part of a straight line.
- A smooth space curve \(C\) with constant curvature \(\kappa \ne 0\) must be part of a circle of radius \(1/\kappa\text{.}\)
- If \(f\) is any smooth function defined in \(\mathbb{R}^3\) and if \(C\) is any circle, then \(\int_C\vecs{ \nabla} f\cdot\text{d}\vecs{r} =0\text{.}\)
- Suppose \(\vecs{F} \) is a smooth vector field in \(\mathbb{R}^3\) and \(\vecs{ \nabla} \cdot\vecs{F} =0\) everywhere. Then, for every sphere, the flux out of one hemisphere is equal to the flux into the opposite hemisphere.
- Let \(\vecs{F} (x, y,z)\) be a continuously differentiable vector field which is defined for every \((x, y, z)\text{.}\) Then, \(\iint_S\vecs{ \nabla} \times\vecs{F} \cdot\hat{\textbf{n}}\,\text{d}S=0\) for any closed surface \(S\text{.}\) (A closed surface is a surface that is the boundary of a solid region.)
True or false (reasons must be given):
- If a smooth vector field on \(\mathbb{R}^3\) is curl free and divergence free, then its potential is harmonic. By definition, \(\phi(x,y,z)\) is harmonic if \(\big(\frac{\partial^2 }{\partial x^2} +\frac{\partial^2 }{\partial y^2} +\frac{\partial^2 }{\partial z^2}\big) \phi(x,y,z)=0\text{.}\)
- If \(\vecs{F} \) is a smooth conservative vector field on \(\mathbb{R}^3\text{,}\) then its flux through any smooth closed surface is zero.
The following statements may be true or false. Decide which. If true, give a proof. If false, provide a counter-example.
- If \(f\) is any smooth function defined in \(\mathbb{R}^3\) and if \(C\) is any circle, then \(\int_{C}\vecs{ \nabla} f \cdot \text{d}\vecs{r} =0\text{.}\)
- There is a vector field \(\vecs{F} \) that obeys \(\vecs{ \nabla} \times\vecs{F} =x\,\hat{\pmb{\imath}}+y\,\hat{\pmb{\jmath}}+z\,\hat{\mathbf{k}}\text{.}\)
Short answers:
- Let \(S\) be the level surface \(f(x,y,z)=0\text{.}\) Why is \(\int_C \vecs{ \nabla} f\cdot \text{d}\vecs{r} =0\) for any curve \(C\) on \(S\text{?}\)
- A point moving in space with position \(\vecs{r} (t)\) at time \(t\) satisfies the condition \(\textbf{a}(t)=f(t)\vecs{r} (t)\) for all \(t\) for some real valued function \(f\text{.}\) Why is \(\vecs{v} \times\vecs{r} \) a constant vector?
- Why is the trajectory of the point in (b) contained in a plane?
- Is the binormal vector, \(\hat{\textbf{B}}\text{,}\) of a particle moving in space, always orthogonal to the unit tangent vector \(\hat{\textbf{T}}\) and unit normal \(\hat{\textbf{N}}\text{?}\)
- If the curvature of the path of a particle moving in space is constant, is the acceleration zero when maximum speed occurs?
A region \(R\) is bounded by a simple closed curve \(\mathcal{C}\text{.}\) The curve \(\mathcal{C}\) is oriented such that \(R\) lies to the left of \(\mathcal{C}\) when walking along \(\mathcal{C}\) in the direction of \(\mathcal{C}\text{.}\) Determine whether or not each of the following expressions is equal to the area of \(R\text{.}\) You must justify your conclusions.
- \(\displaystyle \frac{1}{2} \int_\mathcal{C} -y \,d x +x \,d y\)
- \(\displaystyle \frac{1}{2} \int_\mathcal{C} -x \,d x + y \,d y\)
- \(\displaystyle \int_\mathcal{C} y \,d x\)
- \(\displaystyle \int_\mathcal{C} 3y\,d x + 4x \,d y\)
Say whether each of the following statements is true or false and explain why.
- A moving particle has velocity and acceleration vectors that satisfy \(|\vecs{v} | = 1\) and \(|\textbf{a}|=1\) at all times. Then the curvature of this particle's path is a constant.
- If \(\vecs{F} \) is any smooth vector field defined in \(\mathbb{R}^3\) and if \(S\) is any sphere, then
\[ \iint_{S}\vecs{ \nabla} \times\vecs{F} \cdot\hat{\textbf{n}}\,\text{d}S=0 \nonumber \]
Here \(\hat{\textbf{n}}\) is the outward normal to \(S\text{.}\) - If \(\vecs{F} \) and \(\textbf{G}\) are smooth vector fields in \(\mathbb{R}^3\) and if \(\displaystyle \oint_C \vecs{F} \cdot \text{d}\vecs{r} =\oint_C \textbf{G}\cdot \text{d}\vecs{r} \) for every circle \(C\text{,}\) then \(\vecs{F} =\textbf{G}\text{.}\)
Three quickies:
- A moving particle with position \(\vecs{r} (t) = (x(t),y(t),z(t))\) satisfies
\[ \textbf{a} = f(\vecs{r} ,\vecs{v} )\vecs{r} \nonumber \]
for some scalar-valued function \(f\text{.}\) Prove that \(\vecs{r} \times\vecs{v} \) is constant. - Calculate \(\iint_\mathcal{S}(x\,\hat{\pmb{\imath}} - y\,\hat{\pmb{\jmath}} + z^2\,\hat{\mathbf{k}})\cdot \hat{\textbf{n}}\text{d}S\text{,}\) where \(\mathcal{S}\) is the boundary of any solid right circular cylinder of radius \(b\) with one base in the plane \(z=1\) and the other base in the plane \(z=3\text{.}\)
- Let \(\vecs{F} \) and \(\textbf{G}\) be smooth vector fields defined in \(\mathbb{R}^3\text{.}\) Suppose that, for every circle \(C\text{,}\) we have \(\oint_{C} \vecs{F} \cdot \text{d}\vecs{r} =\iint_S \textbf{G}\cdot \hat{\textbf{n}}\,\text{d}S\text{,}\) where \(S\) is the oriented disk with boundary \(C\text{.}\) Prove that \(\textbf{G}=\vecs{ \nabla} \times\vecs{F} \text{.}\)