Chapter 11
Calculus Early Transcendentals: Pearson New International Edition · 331 exercises
Problem 40
Find the point of the curve at which the curvature is a maximum.
\(y=\ln \cos x\) for \(-\pi / 2
7 step solution
Problem 40
Find the equation of the sphere with center \((1,1,4)\) that is tangent to the plane \(x+y=12\).
4 step solution
Problem 41
Find two perpendicular vectors \(\mathbf{u}\) and \(\mathbf{v}\) such that each is also perpendicular to \(\mathbf{w}=\langle-4,2,5\rangle\).
4 step solution
Problem 41
Find the tangential and normal components \(\left(a_{T}\right.\) and \(a_{N}\) ) of the acceleration vector at \(t\). Then evaluate at \(t=t_{1}\). \(\mathbf{r}(t)=3 t \mathbf{i}+3 t^{2} \mathbf{j} ; t_{1}=\frac{1}{3}\)
6 step solution
Problem 41
$$ \int_{0}^{1}\left(e^{t} \mathbf{i}+e^{-t} \mathbf{j}\right) d t $$
4 step solution
Problem 41
Describe the graph in three-space of each equation. (a) \(z=2\) (b) \(x=y\) (c) \(x y=0\) (d) \(x y z=0\) (e) \(x^{2}+y^{2}=4\) (f) \(z=\sqrt{9-x^{2}-y^{2}}\)
6 step solution
Problem 42
Find the vector emanating from the origin whose terminal point is the midpoint of the segment joining \((3,2,-1)\) and \((5,-7,2)\).
4 step solution
Problem 42
Find the tangential and normal components \(\left(a_{T}\right.\) and \(a_{N}\) ) of the acceleration vector at \(t\). Then evaluate at \(t=t_{1}\). \(\mathbf{r}(t)=t^{2} \mathbf{i}+t \mathbf{j} ; t_{1}=1\)
6 step solution
Problem 42
$$ \int_{-1}^{1}\left[(1+t)^{3 / 2} \mathbf{i}+(1-t)^{3 / 2} \mathbf{j}\right] d t $$
8 step solution
Problem 42
The sphere \((x-1)^{2}+(y+2)^{2}+(z+1)^{2}=10\) intersects the plane \(z=2\) in a circle. Find the circle's center and radius.
4 step solution
Problem 43
Which of the following do not make sense? (a) \(\mathbf{u} \cdot(\mathbf{v} \cdot \mathbf{w})\) (b) \((\mathbf{u} \cdot \mathbf{w})+\mathbf{w}\) (c) \(\|\mathbf{u}\|(\mathbf{v} \cdot \mathbf{w})\) (d) \((\mathbf{u} \cdot \mathbf{v}) \mathbf{w}\)
5 step solution
Problem 43
Find the tangential and normal components \(\left(a_{T}\right.\) and \(a_{N}\) ) of the acceleration vector at \(t\). Then evaluate at \(t=t_{1}\). \(\mathbf{r}(t)=(2 t+1) \mathbf{i}+\left(t^{2}-2\right) \mathbf{j} ; t_{1}=-1\)
6 step solution
Problem 43
A point moves around the circle \(x^{2}+y^{2}=25\) at constant angular speed of 6 radians per second starting at \((5,0)\). Find expressions for \(\mathbf{r}(t), \mathbf{v}(t),\|\mathbf{v}(t)\|\), and a \((t)\) (see Example 3 ).
7 step solution
Problem 43
An object's position \(P\) changes so that its distance from \((1,2,-3)\) is always twice its distance from \((1,2,3)\). Show that \(P\) is on a sphere and find its center and radius.
6 step solution
Problem 44
Find the tangential and normal components \(\left(a_{T}\right.\) and \(a_{N}\) ) of the acceleration vector at \(t\). Then evaluate at \(t=t_{1}\). \(\mathbf{r}(t)=a \cos t \mathbf{i}+a \sin t \mathbf{j} ; t_{1}=\pi / 6\)
5 step solution
Problem 44
Consider the motion of a particle along a helix given by \(\mathbf{r}(t)=\sin t \mathbf{i}+\cos t \mathbf{j}+\left(t^{2}-3 t+2\right) \mathbf{k}\), where the \(\mathbf{k}\) component measures the height in meters above the ground and \(t \geq 0\). (a) Does the particle ever move downward? (b) Does the particle ever stop moving? (c) At what times does it reach a position 12 meters above the ground? (d) What is the velocity of the particle when it is 12 meters above the ground?
4 step solution
Problem 44
An object's position \(P\) changes so that its distance from \((1,2,-3)\) always equals its distance from \((2,3,2)\). Find the equation of the plane on which \(P\) lies.
6 step solution
Problem 45
Find the tangential and normal components \(\left(a_{T}\right.\) and \(a_{N}\) ) of the acceleration vector at \(t\). Then evaluate at \(t=t_{1}\). \(\mathbf{r}(t)=a \cosh t \mathbf{i}+a \sinh t \mathbf{j} ; t_{1}=\ln 3\)
6 step solution
Problem 45
The solid spheres \((x-1)^{2}+(y-2)^{2}+(z-1)^{2} \leq 4\) and \((x-2)^{2}+(y-4)^{2}+(z-3)^{2} \leq 4\) intersect in a solid. Find its volume.
6 step solution
Problem 46
Find the tangential and normal components \(\left(a_{T}\right.\) and \(a_{N}\) ) of the acceleration vector at \(t\). Then evaluate at \(t=t_{1}\). \(x(t)=1+3 t, y(t)=2-6 t ; t_{1}=2\)
6 step solution
Problem 47
In Problems 45-50, give a proof of the indicated property for two-dimensional vectors. Use \(\mathbf{u}=\left\langle u_{1}, u_{2}\right\rangle, \mathbf{v}=\left\langle v_{1}, v_{2}\right\rangle\), and \(\mathbf{w}=\left\langle w_{1}, w_{2}\right\rangle\). $$ c(\mathbf{u} \cdot \mathbf{v})=(c \mathbf{u}) \cdot \mathbf{v} $$
4 step solution
Problem 47
Find the tangential and normal components \(\left(a_{T}\right.\) and \(a_{N}\) ) of the acceleration vector at \(t\). Then evaluate at \(t=t_{1}\). \(\mathbf{r}(t)=(t+1) \mathbf{i}+3 t \mathbf{j}+t^{2} \mathbf{k} ; t_{1}=1\)
6 step solution
Problem 47
Describe in general terms the following "helical" type motions: (a) \(\mathbf{r}(t)=\sin t \mathbf{i}+\cos t \mathbf{j}+t \mathbf{k}\) (b) \(\mathbf{r}(t)=\sin t^{3} \mathbf{i}+\cos t^{3} \mathbf{j}+t^{3} \mathbf{k}\) (c) \(\mathbf{r}(t)=\sin \left(t^{3}+\pi\right) \mathbf{i}+t^{3} \mathbf{j}+\cos \left(t^{3}+\pi\right) \mathbf{k}\) (d) \(\mathbf{r}(t)=t \sin t \mathbf{i}+t \cos t \mathbf{j}+t \mathbf{k}\) (e) \(\mathbf{r}(t)=t^{-2} \sin t \mathbf{i}+t^{-2} \cos t \mathbf{j}+t \mathbf{k}, t>0\) (f) \(\mathbf{r}(t)=t^{2} \sin (\ln t) \mathbf{i}+\ln t \mathbf{j}+t^{2} \cos (\ln t) \mathbf{k}, t>1\)
6 step solution
Problem 47
47\. The curve defined by \(x=a \cos t, y=a \sin t, z=c t\) is a helix. Hold \(a\) fixed and use a CAS to obtain a parmetric plot of the helix for various values of \(c\). What effect does \(c\) have on the curve?
5 step solution
Problem 48
In Problems 45-50, give a proof of the indicated property for two-dimensional vectors. Use \(\mathbf{u}=\left\langle u_{1}, u_{2}\right\rangle, \mathbf{v}=\left\langle v_{1}, v_{2}\right\rangle\), and \(\mathbf{w}=\left\langle w_{1}, w_{2}\right\rangle\). $$ \mathbf{u} \cdot(\mathbf{v}+\mathbf{w})=\mathbf{u} \cdot \mathbf{v}+\mathbf{u} \cdot \mathbf{w} $$
6 step solution
Problem 48
Find the tangential and normal components \(\left(a_{T}\right.\) and \(a_{N}\) ) of the acceleration vector at \(t\). Then evaluate at \(t=t_{1}\). \(x=t, y=t^{2}, z=t^{3} ; t_{1}=2\)
7 step solution
Problem 49
In Problems 45-50, give a proof of the indicated property for two-dimensional vectors. Use \(\mathbf{u}=\left\langle u_{1}, u_{2}\right\rangle, \mathbf{v}=\left\langle v_{1}, v_{2}\right\rangle\), and \(\mathbf{w}=\left\langle w_{1}, w_{2}\right\rangle\). $$ \mathbf{0} \cdot \mathbf{u}=0 $$
5 step solution
Problem 49
Find the tangential and normal components \(\left(a_{T}\right.\) and \(a_{N}\) ) of the acceleration vector at \(t\). Then evaluate at \(t=t_{1}\). \(x=e^{-t}, y=2 t, z=e^{t} ; t_{1}=0\)
7 step solution
Problem 50
In Problems 45-50, give a proof of the indicated property for two-dimensional vectors. Use \(\mathbf{u}=\left\langle u_{1}, u_{2}\right\rangle, \mathbf{v}=\left\langle v_{1}, v_{2}\right\rangle\), and \(\mathbf{w}=\left\langle w_{1}, w_{2}\right\rangle\). $$ \mathbf{u} \cdot \mathbf{u}=\|\mathbf{u}\|^{2} $$
6 step solution
Problem 50
Find the tangential and normal components \(\left(a_{T}\right.\) and \(a_{N}\) ) of the acceleration vector at \(t\). Then evaluate at \(t=t_{1}\). \(\mathbf{r}(t)=(t-2)^{2} \mathbf{i}-t^{2} \mathbf{j}+t \mathbf{k} ; t_{1}=2\)
6 step solution
Problem 51
Given the two nonparallel vectors \(\mathbf{a}=3 \mathbf{i}-2 \mathbf{j}\) and \(\mathbf{b}=-3 \mathbf{i}+4 \mathbf{j}\) and another vector \(\mathbf{r}=7 \mathbf{i}-8 \mathbf{j}\), find scalars \(k\) and \(m\) such that \(\mathbf{r}=k \mathbf{a}+m \mathbf{b}\).
6 step solution
Problem 51
Find the tangential and normal components \(\left(a_{T}\right.\) and \(a_{N}\) ) of the acceleration vector at \(t\). Then evaluate at \(t=t_{1}\). \(\mathbf{r}(t)=\left(t-\frac{1}{3} t^{3}\right) \mathbf{i}-\left(t+\frac{1}{3} t^{3}\right) \mathbf{j}+t \mathbf{k} ; t_{1}=3\)
6 step solution
Problem 52
Given the two nonparallel vectors \(\mathbf{a}=-4 \mathbf{i}+3 \mathbf{j}\) and \(\mathbf{b}=2 \mathbf{i}-\mathbf{j}\) and another vector \(\mathbf{r}=6 \mathbf{i}-7 \mathbf{j}\), find scalars \(k\) and \(m\) such that \(\mathbf{r}=k \mathbf{a}+m \mathbf{b}\).
6 step solution
Problem 52
Find the tangential and normal components \(\left(a_{T}\right.\) and \(a_{N}\) ) of the acceleration vector at \(t\). Then evaluate at \(t=t_{1}\). \(\mathbf{r}(t)=t \mathbf{i}+\frac{1}{3} t^{3} \mathbf{j}+t^{-1} \mathbf{k}, t>0 ; t_{1}=1\)
6 step solution
Problem 53
Show that the vector \(\mathbf{n}=a \mathbf{i}+b \mathbf{j}\) is perpendicular to the line with equation \(a x+b y=c\). Hint: Let \(P_{1}\left(x_{1}, y_{1}\right)\) and \(P_{2}\left(x_{2}, y_{2}\right)\) be two points on the line and show that \(\mathbf{n} \cdot \overrightarrow{P_{1} P_{2}}=0\).
5 step solution
Problem 53
Sketch the path for a particle if its position vector is \(\mathbf{r}=\sin t \mathbf{i}+\sin 2 t \mathbf{j}, 0 \leq t \leq 2 \pi\) (you should get a figure eight). Where is the acceleration zero? Where does the acceleration vector point to the origin?
6 step solution
Problem 54
Prove that \(\|\mathbf{u}+\mathbf{v}\|^{2}+\|\mathbf{u}-\mathbf{v}\|^{2}=2\|\mathbf{u}\|^{2}+2\|\mathbf{v}\|^{2}\).
4 step solution
Problem 54
The position vector of a particle at time \(t \geq 0\) is $$ \mathbf{r}(t)=(\cos t+t \sin t) \mathbf{i}+(\sin t-t \cos t) \mathbf{j} $$ (a) Show that the speed \(d s / d t=t\). (b) Show that \(a_{T}=1\) and \(a_{N}=t\).
5 step solution
Problem 55
Prove that \(\mathbf{u} \cdot \mathbf{v}=\frac{1}{4}\|\mathbf{u}+\mathbf{v}\|^{2}-\frac{1}{4}\|\mathbf{u}-\mathbf{v}\|^{2}\).
5 step solution
Problem 55
If, for a particle, \(a_{T}=0\) for all \(t\), what can you conclude about its speed? If \(a_{N}=0\) for all \(t\), what can you conclude about its curvature?
4 step solution
Problem 56
Find the angle between a main diagonal of a cube and one of its faces.
8 step solution
Problem 57
Find the smallest angle between the main diagonals of a rectangular box 4 feet by 6 feet by 10 feet.
8 step solution
Problem 57
Consider the motion of a particle along a helix given by \(\mathbf{r}(t)=\sin t \mathbf{i}+\cos t \mathbf{j}+\left(t^{2}-3 t+2\right) \mathbf{k}\), where the \(\mathbf{k}\) component measures the height in meters above the ground and \(t \geq 0\). If the particle leaves the helix and moves along the line tangent to the helix when it is 12 meters above the ground, give the direction vector for the line.
5 step solution
Problem 58
Find the angles formed by the diagonals of a cube.
8 step solution
Problem 58
An object moves along the curve \(y=\sin 2 x\). Without doing any calculating, decide where \(a_{N}=0\).
5 step solution
Problem 59
Find the work done by the force \(\mathbf{F}=3 \mathbf{i}+10 \mathbf{j}\) newtons in moving an object 10 meters north (i.e., in the \(\mathbf{j}\) direction).
4 step solution
Problem 59
A dog is running counterclockwise around the circle \(x^{2}+y^{2}=400\) (distances in feet). At the point \((-12,16)\), it is running at 10 feet per second and is speeding up at 5 feet per second per second. Express its acceleration a at the point first in terms of \(\mathbf{T}\) and \(\mathbf{N}\), and then in terms of \(\mathbf{i}\) and \(\mathbf{j}\).
7 step solution
Problem 60
Find the work done by a force of 100 newtons acting in the direction \(S 70^{\circ} \mathrm{E}\) in moving an object 30 meters east.
3 step solution
Problem 61
Find the work done by the force \(\mathbf{F}=6 \mathbf{i}+8 \mathbf{j}\) pounds in moving an object from \((1,0)\) to \((6,8)\), where distance is in feet.
4 step solution
Problem 61
A car traveling at constant speed \(v\) rounds a level curve, which we take to be a circle of radius \(R\). If the car is to avoid sliding outward, the horizontal frictional force \(F\) exerted by the road on the tires must at least balance the centrifugal force pulling outward. The force \(F\) satisfies \(F=\mu m g\), where \(\mu\) is the coefficient of friction, \(m\) is the mass of the car, and \(g\) is the acceleration of gravity. Thus, \(\mu m g \geq m v^{2} / R\). Show that \(v_{R}\), the speed beyond which skidding will occur, satisfies $$ v_{R}=\sqrt{\mu g R} $$ and use this to determine \(v_{R}\) for a curve with \(R=400\) feet and \(\mu=0.4\). Use \(g=32\) feet per second per second.
6 step solution