For Exercises 1 to 4, at the indicated point, compute the velocity vector, the acceleration vector, the speed, and the equation of the tangent line.
\({\bf c}(t)=(t^3+1,e^{-t},\cos\, (\pi t/2)), \hbox{at } t=1\)
\({\bf c}(t)=(t^2-1,\cos\, (t^2),t^4), \hbox{at }t=\sqrt{\pi}\)
\({\bf c}(t)=(e^t,\sin t,\cos t), \hbox{at }t=0\)
\({\bf c}(t)=\displaystyle\frac{t^2}{1+t^2}{\bf i}+t{\bf j}+ {\bf k}, \hbox{at }t=2\)
Calculate the tangent and acceleration vectors for the helix \({\bf c}(t)=(\cos t,\sin t ,t)\) at \(t=\pi/4\).
Calculate the tangent and acceleration vector for the cycloid \({\bf c}(t)=(t-\sin t,1-\cos t)\) at \(t=\pi/4\) and sketch.
Let a particle of mass \(m\) move on the path \({\bf c}(t) = (t^2,\sin t,\cos t).\) Compute the force acting on the particle at \(t=0\).
Let \(\textbf{c}(t)=(\cos t, \sin t, \sqrt3 t)\) be a path in \(\mathbb R^3\).
Let \(\textbf{F}(x, y, z)=(\sin(xz), e^{xy}, x^2y^3z^5)\).
Verify that the gravitational force field \(\textbf{F}(x, y, z)=-A\displaystyle\frac{(x, y, z)}{(x^2+y^2+z^2)^{3/2}}\), where \(A\) is some constant, is curl free away from the origin.
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Show that the vector field \(\textbf{V}(x, y, z)=2x\textbf{i} -3y\textbf{j}+4z\textbf{k}\) is not the curl of any vector field.
Express the arc length of the curve \(x^2 =y^3 =z^5\) between \(x=1\) and \(x=4\) as an integral, using a suitable parametrization.
Find the arc length of \({\bf c}(t)=t{\bf i}+(\log t){\bf j}+2\sqrt{2t}{\bf k}\) for \(1\leq t\leq 2\).
A particle is constrained to move around the unit circle in the \(xy\) plane according to the formula \((x,y,z)=(\cos\, (t^2),\sin \,(t^2),0),t\geq 0\).
A particle of mass \(m\) moves under the influence of a force \({\bf F}=-k{\bf r}\), where \(k\) is a constant and \({\bf r}(t)\) is the position of the particle at time \(t\).
Write the curve described by the equations \(x-1=2y+1=3z+2\) in parametric form.
Write the curve \(x=y^3=z^2+1\) in parametric form.
Show that \({\bf c}(t)=(1/(1-t),0,e^t/(1-t))\) is a flow line of the vector field defined by \({\bf F}(x,y,z)=(x^2,0,\) \(z(1+x))\).
Let \({\bf F}(x,y)=f(x^2+y^2)[-y{\bf i}+x{\bf j}]\) for a function \(f\) of one variable. What equation must \(g(t)\) satisfy for \[ {\bf c}(t)=[\cos g(t)]{\bf i}+[\sin g(t)]{\bf j} \] to be a flow line for \({\bf F}\)?
Compute \(\nabla \,{\cdot}\, {\bf F}\) and \(\nabla \times {\bf F}\,\) for the vector fields in Exercises 21 to 24.
\({\bf F}=2x{\bf i}+3y{\bf j}+4z{\bf k}\)
\({\bf F}=x^2{\bf i}+y^2{\bf j}+z^2{\bf k}\)
\({\bf F}=(x+y){\bf i}+(y+z){\bf j}+(z+x){\bf k}\)
\({\bf F}=x{\bf i}+3xy{\bf j}+z{\bf k}\)
Compute the divergence and curl of the vector fields in Exercises 25 and 26 at the points indicated.
\({\bf F}(x,y,z)=y{\bf i}+z{\bf j}+x{\bf k}\), at the point (1, 1, 1)
\({\bf F}(x,y,z)=(x+y)^3{\bf i}+(\sin xy){\bf j}+(\cos xyz){\bf k}\), at the point (2, 0, 1)
Calculate the gradients of the functions in Exercises 27 to 30, and verify that \(\nabla \times \nabla f={\bf 0}.\)
\(f(x,y)=e^{xy}+\cos\, (xy)\)
\(f(x,y)=\displaystyle\frac{x^2-y^2}{x^2+y^2}\)
\(f(x,y)=e^{x^2}-\cos\, (xy^2)\)
\(f(x,y)=\tan^{-1}\,(x^2+y^2)\)
Let \({\bf F}(x,y)=f(x^2+y^2)[-y{\bf i}+x{\bf j}]\), as in Exercise 20. Calculate div \({\bf F}\) and curl \({\bf F}\) and discuss your answers in view of the results of Exercise 20.
Let a particle of mass \(m\) move along the elliptical helix \({\bf c}(t)\,{=}\,(4 \cos t, \sin t, t)\).
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In meteorology, the negative pressure gradient \({\bf G}\) is a vector quantity that points from regions of high pressure to regions of low pressure, normal to the lines of constant pressure (isobars).
A sphere of mass \(m\), radius \(a\), and uniform density has potential \(u\) and gravitational force \({\bf F}\), at a distance \(r\) from the center (0, 0, 0), given by \begin{eqnarray*} u=\frac{3m}{2a}-\frac{mr^2}{2a^3},{\bf F}&=&-\frac{m}{a^3}{\bf r}\qquad(r\leq a);\\[6pt] u=\frac{m}{r},{\bf F}&=&-\frac{m}{r^3}{\bf r}\qquad(r >a).\\[-11pt] \end{eqnarray*} Here, \(r=\|{\bf r}\|,{\bf r}=x{\bf i}+y{\bf j}+ z{\bf k}\).
A circular helix that lies on the cylinder \(x^2+y^2=R^2\) with pitch \(\rho\) may be described parametrically by \[ x=R\cos \theta,\qquad y=R\sin \theta,\qquad z=\rho \theta,\qquad \theta \geq 0. \] A particle slides under the action of gravity (which acts parallel to the \(z\) axis) without friction along the helix. If the particle starts out at the height \(z_0 >0\), then when it reaches the height \(z\) along the helix, its speed is given by \[ \frac{{\it ds}}{{\it dt}}=\sqrt{(z_0-z)2g}, \] where \(s\) is arc length along the helix, \(g\) is the constant of gravity, \(t\) is time, and \(0 \leq z\leq z_0\).
A sphere of radius 10 centimeters (cm) with center at \((0,\,0,\,0)\) rotates about the \(z\) axis with angular velocity 4 in such a direction that the rotation looks counterclockwise from the positive \(z\) axis.
Find the speed of the students in a classroom located at a latitude 49\(^{\circ}\)N due to the rotation of the earth. (Ignore the motion of the earth about the sun, the sun in the galaxy, etc.; the radius of the earth is 3960 miles.)
1Most scientists acknowledge that \({\bf F}=m{\bf a}\) is the single most important equation in all of science and engineering.
2For more information and history, consult S. Hildebrandt and A. J. Tromba, The Parsimonious Universe: Shape and Form in the Natural World, Springer-Verlag, New York/Berlin, 1995.
3For more information about Poincaré, see F. Diacu and P. Holmes, Celestial Encounters. The Origins of Chaos and Stability, Princeton University Press: Princeton, NJ, 1996.
4Several of these problems make use of the formula \[ \int\sqrt{x^2+a^2}{\,d} x={\textstyle\frac{1}{2}}\big[x\sqrt{x^2+a^2}+a^2\log \,(x+\sqrt{x^2+a^2})\big]+C \] from the table of integrals in the back of the book.