Calculus Volume 3

# 2.3The Dot Product

Calculus Volume 32.3 The Dot Product

### Learning Objectives

• 2.3.1 Calculate the dot product of two given vectors.
• 2.3.2 Determine whether two given vectors are perpendicular.
• 2.3.3 Find the direction cosines of a given vector.
• 2.3.4 Explain what is meant by the vector projection of one vector onto another vector, and describe how to compute it.
• 2.3.5 Calculate the work done by a given force.

If we apply a force to an object so that the object moves, we say that work is done by the force. In Introduction to Applications of Integration on integration applications, we looked at a constant force and we assumed the force was applied in the direction of motion of the object. Under those conditions, work can be expressed as the product of the force acting on an object and the distance the object moves. In this chapter, however, we have seen that both force and the motion of an object can be represented by vectors.

In this section, we develop an operation called the dot product, which allows us to calculate work in the case when the force vector and the motion vector have different directions. The dot product essentially tells us how much of the force vector is applied in the direction of the motion vector. The dot product can also help us measure the angle formed by a pair of vectors and the position of a vector relative to the coordinate axes. It even provides a simple test to determine whether two vectors meet at a right angle.

### The Dot Product and Its Properties

We have already learned how to add and subtract vectors. In this chapter, we investigate two types of vector multiplication. The first type of vector multiplication is called the dot product, based on the notation we use for it, and it is defined as follows:

### Definition

The dot product of vectors $u=〈u1,u2,u3〉u=〈u1,u2,u3〉$ and $v=〈v1,v2,v3〉v=〈v1,v2,v3〉$ is given by the sum of the products of the components

$u·v=u1v1+u2v2+u3v3.u·v=u1v1+u2v2+u3v3.$
(2.3)

Note that if u and v are two-dimensional vectors, we calculate the dot product in a similar fashion. Thus, if $u=〈u1,u2〉u=〈u1,u2〉$ and $v=〈v1,v2〉,v=〈v1,v2〉,$ then

$u·v=u1v1+u2v2.u·v=u1v1+u2v2.$

When two vectors are combined under addition or subtraction, the result is a vector. When two vectors are combined using the dot product, the result is a scalar. For this reason, the dot product is often called the scalar product. It may also be called the inner product.

### Example 2.21

#### Calculating Dot Products

1. Find the dot product of $u=〈3,5,2〉u=〈3,5,2〉$ and $v=〈−1,3,0〉.v=〈−1,3,0〉.$
2. Find the scalar product of $p=10i−4j+7kp=10i−4j+7k$ and $q=−2i+j+6k.q=−2i+j+6k.$

### Checkpoint2.21

Find $u·v,u·v,$ where $u=〈2,9,−1〉u=〈2,9,−1〉$ and $v=〈−3,1,−4〉.v=〈−3,1,−4〉.$

Like vector addition and subtraction, the dot product has several algebraic properties. We prove three of these properties and leave the rest as exercises.

### Theorem2.3

#### Properties of the Dot Product

Let $u,u,$ $v,v,$ and $ww$ be vectors, and let c be a scalar.

$i.u·v=v·uCommutative propertyii.u·(v+w)=u·v+u·wDistributive propertyiii.c(u·v)=(cu)·v=u·(cv)Associative propertyiv.v·v=‖v‖2Property of magnitudei.u·v=v·uCommutative propertyii.u·(v+w)=u·v+u·wDistributive propertyiii.c(u·v)=(cu)·v=u·(cv)Associative propertyiv.v·v=‖v‖2Property of magnitude$

#### Proof

Let $u=〈u1,u2,u3〉u=〈u1,u2,u3〉$ and $v=〈v1,v2,v3〉.v=〈v1,v2,v3〉.$ Then

$u·v=〈u1,u2,u3〉·〈v1,v2,v3〉=u1v1+u2v2+u3v3=v1u1+v2u2+v3u3=〈v1,v2,v3〉·〈u1,u2,u3〉=v·u.u·v=〈u1,u2,u3〉·〈v1,v2,v3〉=u1v1+u2v2+u3v3=v1u1+v2u2+v3u3=〈v1,v2,v3〉·〈u1,u2,u3〉=v·u.$

The associative property looks like the associative property for real-number multiplication, but pay close attention to the difference between scalar and vector objects:

$c(u·v)=c(u1v1+u2v2+u3v3)=c(u1v1)+c(u2v2)+c(u3v3)=(cu1)v1+(cu2)v2+(cu3)v3=〈cu1,cu2,cu3〉·〈v1,v2,v3〉=c〈u1,u2,u3〉·〈v1,v2,v3〉=(cu)·v.c(u·v)=c(u1v1+u2v2+u3v3)=c(u1v1)+c(u2v2)+c(u3v3)=(cu1)v1+(cu2)v2+(cu3)v3=〈cu1,cu2,cu3〉·〈v1,v2,v3〉=c〈u1,u2,u3〉·〈v1,v2,v3〉=(cu)·v.$

The proof that $c(u·v)=u·(cv)c(u·v)=u·(cv)$ is similar.

The fourth property shows the relationship between the magnitude of a vector and its dot product with itself:

$v·v=〈v1,v2,v3〉·〈v1,v2,v3〉=(v1)2+(v2)2+(v3)2=[(v1)2+(v2)2+(v3)2]2=‖v‖2.v·v=〈v1,v2,v3〉·〈v1,v2,v3〉=(v1)2+(v2)2+(v3)2=[(v1)2+(v2)2+(v3)2]2=‖v‖2.$

Note that the definition of the dot product yields $0·v=0.0·v=0.$ By property iv., if $v·v=0,v·v=0,$ then $v=0.v=0.$

### Example 2.22

#### Using Properties of the Dot Product

Let $a=〈1,2,−3〉,a=〈1,2,−3〉,$ $b=〈0,2,4〉,b=〈0,2,4〉,$ and $c=〈5,−1,3〉.c=〈5,−1,3〉.$ Find each of the following products.

1. $(a·b)c(a·b)c$
2. $a·(2c)a·(2c)$
3. $‖b‖2‖b‖2$

### Checkpoint2.22

Find the following products for $p=〈7,0,2〉,p=〈7,0,2〉,$ $q=〈−2,2,−2〉,q=〈−2,2,−2〉,$ and $r=〈0,2,−3〉.r=〈0,2,−3〉.$

1. $(r·p)q(r·p)q$
2. $‖p‖2‖p‖2$

### Using the Dot Product to Find the Angle between Two Vectors

When two nonzero vectors are placed in standard position, whether in two dimensions or three dimensions, they form an angle between them (Figure 2.44). The dot product provides a way to find the measure of this angle. This property is a result of the fact that we can express the dot product in terms of the cosine of the angle formed by two vectors.

Figure 2.44 Let θ be the angle between two nonzero vectors u and v such that $0 ≤ θ ≤ π . 0 ≤ θ ≤ π .$

### Theorem2.4

#### Evaluating a Dot Product

The dot product of two vectors is the product of the magnitude of each vector and the cosine of the angle between them:

$u·v=‖u‖‖v‖cosθ.u·v=‖u‖‖v‖cosθ.$
(2.4)

#### Proof

Place vectors u and v in standard position and consider the vector $v−uv−u$ (Figure 2.45). These three vectors form a triangle with side lengths $‖u‖,‖v‖,and‖v−u‖.‖u‖,‖v‖,and‖v−u‖.$

Figure 2.45 The lengths of the sides of the triangle are given by the magnitudes of the vectors that form the triangle.

Recall from trigonometry that the law of cosines describes the relationship among the side lengths of the triangle and the angle θ. Applying the law of cosines here gives

$‖v−u‖2=‖u‖2+‖v‖2−2‖u‖‖v‖cosθ.‖v−u‖2=‖u‖2+‖v‖2−2‖u‖‖v‖cosθ.$

The dot product provides a way to rewrite the left side of this equation:

$‖v−u‖2=(v−u)·(v−u)=(v−u)·v−(v−u)·u=v·v−u·v−v·u+u·u=v·v−u·v−u·v+u·u=‖v‖2−2u·v+‖u‖2.‖v−u‖2=(v−u)·(v−u)=(v−u)·v−(v−u)·u=v·v−u·v−v·u+u·u=v·v−u·v−u·v+u·u=‖v‖2−2u·v+‖u‖2.$

Substituting into the law of cosines yields

$‖v−u‖2=‖u‖2+‖v‖2−2‖u‖‖v‖cosθ‖v‖2−2u·v+‖u‖2=‖u‖2+‖v‖2−2‖u‖‖v‖cosθ−2u·v=−2‖u‖‖v‖cosθu·v=‖u‖‖v‖cosθ.‖v−u‖2=‖u‖2+‖v‖2−2‖u‖‖v‖cosθ‖v‖2−2u·v+‖u‖2=‖u‖2+‖v‖2−2‖u‖‖v‖cosθ−2u·v=−2‖u‖‖v‖cosθu·v=‖u‖‖v‖cosθ.$

We can use this form of the dot product to find the measure of the angle between two nonzero vectors. The following equation rearranges Equation 2.3 to solve for the cosine of the angle:

$cosθ=u·v‖u‖‖v‖.cosθ=u·v‖u‖‖v‖.$
(2.5)

Using this equation, we can find the cosine of the angle between two nonzero vectors. Since we are considering the smallest angle between the vectors, we assume $0°≤θ≤180°0°≤θ≤180°$ (or $0≤θ≤π0≤θ≤π$ if we are working in radians). The inverse cosine is unique over this range, so we are then able to determine the measure of the angle $θ.θ.$

### Example 2.23

#### Finding the Angle between Two Vectors

Find the measure of the angle between each pair of vectors.

1. i + j + k and 2ij – 3k
2. $〈2,5,6〉〈2,5,6〉$ and $〈−2,−4,4〉〈−2,−4,4〉$

### Checkpoint2.23

Find the measure of the angle, in radians, formed by vectors $a=〈1,2,0〉a=〈1,2,0〉$ and $b=〈2,4,1〉.b=〈2,4,1〉.$ Round to the nearest hundredth.

The angle between two vectors can be acute $(0 obtuse $(−1 or straight $(cosθ=−1).(cosθ=−1).$ If $cosθ=1,cosθ=1,$ then both vectors have the same direction. If $cosθ=0,cosθ=0,$ then the vectors, when placed in standard position, form a right angle (Figure 2.46). We can formalize this result into a theorem regarding orthogonal (perpendicular) vectors.

Figure 2.46 (a) An acute angle has $0 < cos θ < 1 . 0 < cos θ < 1 .$ (b) An obtuse angle has $−1 < cos θ < 0 . −1 < cos θ < 0 .$ (c) A straight line has $cos θ = −1 . cos θ = −1 .$ (d) If the vectors have the same direction, $cos θ = 1 . cos θ = 1 .$ (e) If the vectors are orthogonal (perpendicular), $cos θ = 0 . cos θ = 0 .$

### Theorem2.5

#### Orthogonal Vectors

The nonzero vectors u and v are orthogonal vectors if and only if $u·v=0.u·v=0.$

#### Proof

Let u and v be nonzero vectors, and let $θθ$ denote the angle between them. First, assume $u·v=0.u·v=0.$ Then

$‖u‖‖v‖cosθ=0.‖u‖‖v‖cosθ=0.$

However, $‖u‖≠0‖u‖≠0$ and $‖v‖≠0,‖v‖≠0,$ so we must have $cosθ=0.cosθ=0.$ Hence, $θ=90°,θ=90°,$ and the vectors are orthogonal.

Now assume u and v are orthogonal. Then $θ=90°θ=90°$ and we have

$u·v=‖u‖‖v‖cosθ=‖u‖‖v‖cos90°=‖u‖‖v‖(0)=0.u·v=‖u‖‖v‖cosθ=‖u‖‖v‖cos90°=‖u‖‖v‖(0)=0.$

The terms orthogonal, perpendicular, and normal each indicate that mathematical objects are intersecting at right angles. The use of each term is determined mainly by its context. We say that vectors are orthogonal and lines are perpendicular. The term normal is used most often when measuring the angle made with a plane or other surface.

### Example 2.24

#### Identifying Orthogonal Vectors

Determine whether $p=〈1,0,5〉p=〈1,0,5〉$ and $q=〈10,3,−2〉q=〈10,3,−2〉$ are orthogonal vectors.

### Checkpoint2.24

For which value of x is $p=〈2,8,−1〉p=〈2,8,−1〉$ orthogonal to $q=〈x,−1,2〉?q=〈x,−1,2〉?$

### Example 2.25

#### Measuring the Angle Formed by Two Vectors

Let $v=〈2,3,3〉.v=〈2,3,3〉.$ Find the measures of the angles formed by the following vectors.

1. v and i
2. v and j
3. v and k

### Checkpoint2.25

Let $v=〈3,−5,1〉.v=〈3,−5,1〉.$ Find the measure of the angles formed by each pair of vectors.

1. v and i
2. v and j
3. v and k

The angle a vector makes with each of the coordinate axes, called a direction angle, is very important in practical computations, especially in a field such as engineering. For example, in astronautical engineering, the angle at which a rocket is launched must be determined very precisely. A very small error in the angle can lead to the rocket going hundreds of miles off course. Direction angles are often calculated by using the dot product and the cosines of the angles, called the direction cosines. Therefore, we define both these angles and their cosines.

### Definition

The angles formed by a nonzero vector and the coordinate axes are called the direction angles for the vector (Figure 2.48). The cosines for these angles are called the direction cosines.

Figure 2.48 Angle α is formed by vector v and unit vector i. Angle β is formed by vector v and unit vector j. Angle γ is formed by vector v and unit vector k.

In Example 2.25, the direction cosines of $v=〈2,3,3〉v=〈2,3,3〉$ are $cosα=222,cosα=222,$ $cosβ=322,cosβ=322,$ and $cosγ=322.cosγ=322.$ The direction angles of v are $α=1.130rad,α=1.130rad,$ $β=0.877rad,β=0.877rad,$ and $γ=0.877rad.γ=0.877rad.$

### Projections

As we have seen, addition combines two vectors to create a resultant vector. But what if we are given a vector and we need to find its component parts? We use vector projections to perform the opposite process; they can break down a vector into its components. The magnitude of a vector projection is a scalar projection. For example, if a child is pulling the handle of a wagon at a 55° angle, we can use projections to determine how much of the force on the handle is actually moving the wagon forward (Figure 2.49). We return to this example and learn how to solve it after we see how to calculate projections.

Figure 2.49 When a child pulls a wagon, only the horizontal component of the force propels the wagon forward.

### Definition

The vector projection of v onto u is the vector labeled projuv in Figure 2.50. It has the same initial point as u and v and the same direction as u, and represents the component of v that acts in the direction of u. If $θθ$ represents the angle between u and v, then, by properties of triangles, we know the length of $projuvprojuv$ is $‖projuv‖=‖v‖cosθ.‖projuv‖=‖v‖cosθ.$ When expressing $cosθcosθ$ in terms of the dot product, this becomes

$‖projuv‖=‖v‖cosθ=‖v‖(|u·v|‖u‖‖v‖)=|u·v|‖u‖.‖projuv‖=‖v‖cosθ=‖v‖(|u·v|‖u‖‖v‖)=|u·v|‖u‖.$

We now multiply by a unit vector in the direction of u to get $projuv:projuv:$

$projuv=u·v‖u‖(1‖u‖u)=u·v‖u‖2u.projuv=u·v‖u‖(1‖u‖u)=u·v‖u‖2u.$
(2.6)

The length of this vector is also known as the scalar projection of v onto u and is denoted by

$‖projuv‖=compuv=|u·v|‖u‖.‖projuv‖=compuv=|u·v|‖u‖.$
(2.7)
Figure 2.50 The projection of v onto u shows the component of vector v in the direction of u.

### Example 2.27

#### Finding Projections

Find the projection of v onto u.

1. $v=〈3,5,1〉v=〈3,5,1〉$ and $u=〈−1,4,3〉u=〈−1,4,3〉$
2. $v=3i−2jv=3i−2j$ and $u=i+6ju=i+6j$

Sometimes it is useful to decompose vectors—that is, to break a vector apart into a sum. This process is called the resolution of a vector into components. Projections allow us to identify two orthogonal vectors having a desired sum. For example, let $v=〈6,−4〉v=〈6,−4〉$ and let $u=〈3,1〉.u=〈3,1〉.$ We want to decompose the vector v into orthogonal components such that one of the component vectors has the same direction as u.

We first find the component that has the same direction as u by projecting v onto u. Let $p=projuv.p=projuv.$ Then, we have

$p=u·v‖u‖2u=18−49+1u=75u=75〈3,1〉=〈215,75〉.p=u·v‖u‖2u=18−49+1u=75u=75〈3,1〉=〈215,75〉.$

Now consider the vector $q=v−p.q=v−p.$ We have

$q=v−p=〈6,−4〉−〈215,75〉=〈95,−275〉.q=v−p=〈6,−4〉−〈215,75〉=〈95,−275〉.$

Clearly, by the way we defined q, we have $v=q+p,v=q+p,$ and

$q·p=〈95,−275〉·〈215,75〉=9(21)25+−27(7)25=18925−18925=0.q·p=〈95,−275〉·〈215,75〉=9(21)25+−27(7)25=18925−18925=0.$

Therefore, q and p are orthogonal.

### Example 2.28

#### Resolving Vectors into Components

Express $v=〈8,−3,−3〉v=〈8,−3,−3〉$ as a sum of orthogonal vectors such that one of the vectors has the same direction as $u=〈2,3,2〉.u=〈2,3,2〉.$

### Checkpoint2.27

Express $v=5i−jv=5i−j$ as a sum of orthogonal vectors such that one of the vectors has the same direction as $u=4i+2j.u=4i+2j.$

### Example 2.29

#### Scalar Projection of Velocity

A container ship leaves port traveling $15°15°$ north of east. Its engine generates a speed of 20 knots along that path (see the following figure). In addition, the ocean current moves the ship northeast at a speed of 2 knots. Considering both the engine and the current, how fast is the ship moving in the direction $15°15°$ north of east? Round the answer to two decimal places.

### Checkpoint2.28

Repeat the previous example, but assume the ocean current is moving southeast instead of northeast, as shown in the following figure.

### Work

Now that we understand dot products, we can see how to apply them to real-life situations. The most common application of the dot product of two vectors is in the calculation of work.

From physics, we know that work is done when an object is moved by a force. When the force is constant and applied in the same direction the object moves, then we define the work done as the product of the force and the distance the object travels: $W=Fd.W=Fd.$ We saw several examples of this type in earlier chapters. Now imagine the direction of the force is different from the direction of motion, as with the example of a child pulling a wagon. To find the work done, we need to multiply the component of the force that acts in the direction of the motion by the magnitude of the displacement. The dot product allows us to do just that. If we represent an applied force by a vector F and the displacement of an object by a vector s, then the work done by the force is the dot product of F and s.

### Definition

When a constant force is applied to an object so the object moves in a straight line from point P to point Q, the work W done by the force F, acting at an angle θ from the line of motion, is given by

$W=F·PQ→=‖F‖‖PQ→‖cosθ.W=F·PQ→=‖F‖‖PQ→‖cosθ.$
(2.8)

Let’s revisit the problem of the child’s wagon introduced earlier. Suppose a child is pulling a wagon with a force having a magnitude of 8 lb on the handle at an angle of 55°. If the child pulls the wagon 50 ft, find the work done by the force (Figure 2.51).

Figure 2.51 The horizontal component of the force is the projection of F onto the positive x-axis.

We have

$W=‖F‖‖PQ→‖cosθ=8(50)(cos(55°))≈229ft·lb.W=‖F‖‖PQ→‖cosθ=8(50)(cos(55°))≈229ft·lb.$

In U.S. standard units, we measure the magnitude of force $‖F‖‖F‖$ in pounds. The magnitude of the displacement vector $‖PQ→‖‖PQ→‖$ tells us how far the object moved, and it is measured in feet. The customary unit of measure for work, then, is the foot-pound. One foot-pound is the amount of work required to move an object weighing 1 lb a distance of 1 ft straight up. In the metric system, the unit of measure for force is the newton (N), and the unit of measure of magnitude for work is a newton-meter (N·m), or a joule (J).

### Example 2.30

#### Calculating Work

A conveyor belt generates a force $F=5i−3j+kF=5i−3j+k$ that moves a suitcase from point $(1,1,1)(1,1,1)$ to point $(9,4,7)(9,4,7)$ along a straight line. Find the work done by the conveyor belt. The distance is measured in meters and the force is measured in newtons.

### Checkpoint2.29

A constant force of 30 lb is applied at an angle of 60° to pull a handcart 10 ft across the ground (Figure 2.52). What is the work done by this force?

Figure 2.52

### Section 2.3 Exercises

For the following exercises, the vectors u and v are given. Calculate the dot product $u·v.u·v.$

123 .

$u=〈3,0〉,u=〈3,0〉,$ $v=〈2,2〉v=〈2,2〉$

124 .

$u=〈3,−4〉,u=〈3,−4〉,$ $v=〈4,3〉v=〈4,3〉$

125 .

$u=〈2,2,−1〉,u=〈2,2,−1〉,$ $v=〈−1,2,2〉v=〈−1,2,2〉$

126 .

$u=〈4,5,−6〉,u=〈4,5,−6〉,$ $v=〈0,−2,−3〉v=〈0,−2,−3〉$

For the following exercises, the vectors a, b, and c are given. Determine the vectors $(a·b)c(a·b)c$ and $(a·c)b.(a·c)b.$ Express the vectors in component form.

127 .

$a=〈2,0,−3〉,a=〈2,0,−3〉,$ $b=〈−4,−7,1〉,b=〈−4,−7,1〉,$ $c=〈1,1,−1〉c=〈1,1,−1〉$

128 .

$a=〈0,1,2〉,a=〈0,1,2〉,$ $b=〈−1,0,1〉,b=〈−1,0,1〉,$ $c=〈1,0,−1〉c=〈1,0,−1〉$

129 .

$a=i+j,a=i+j,$ $b=i−k,b=i−k,$ $c=i−2kc=i−2k$

130 .

$a=i−j+k,a=i−j+k,$ $b=j+3k,b=j+3k,$ $c=−i+2j−4kc=−i+2j−4k$

For the following exercises, the two-dimensional vectors a and b are given.

1. Find the measure of the angle $θθ$ between a and b. Express the answer in radians rounded to two decimal places, if it is not possible to express it exactly.
2. Is $θθ$ an acute angle?
131 .

[T] $a=〈3,−1〉,a=〈3,−1〉,$ $b=〈−4,0〉b=〈−4,0〉$

132 .

[T] $a=〈2,1〉,a=〈2,1〉,$ $b=〈−1,3〉b=〈−1,3〉$

133 .

$u=3i,u=3i,$ $v=4i+4jv=4i+4j$

134 .

$u=5i,u=5i,$ $v=−6i+6jv=−6i+6j$

For the following exercises, find the measure of the angle between the three-dimensional vectors a and b. Express the answer in radians rounded to two decimal places, if it is not possible to express it exactly.

135 .

$a=〈3,−1,2〉,a=〈3,−1,2〉,$ $b=〈1,−1,−2〉b=〈1,−1,−2〉$

136 .

$a=〈0,−1,−3〉,a=〈0,−1,−3〉,$ $b=〈2,3,−1〉b=〈2,3,−1〉$

137 .

$a=i+j,a=i+j,$ $b=j−kb=j−k$

138 .

$a=i−2j+k,a=i−2j+k,$ $b=i+j−2kb=i+j−2k$

139 .

[T] $a=3i−j−2k,a=3i−j−2k,$ $b=v+w,b=v+w,$ where $v=−2i−3j+2kv=−2i−3j+2k$ and $w=i+2kw=i+2k$

140 .

[T] $a=3i−j+2k,a=3i−j+2k,$ $b=v−w,b=v−w,$ where $v=2i+j+4kv=2i+j+4k$ and $w=6i+j+2kw=6i+j+2k$

For the following exercises determine whether the given vectors are orthogonal.

141 .

$a=〈x,y〉,a=〈x,y〉,$ $b=〈−y,x〉,b=〈−y,x〉,$ where x and y are nonzero real numbers

142 .

$a=〈x,x〉,a=〈x,x〉,$ $b=〈−y,y〉,b=〈−y,y〉,$ where x and y are nonzero real numbers

143 .

$a=3i−j−2k,a=3i−j−2k,$ $b=−2i−3j+kb=−2i−3j+k$

144 .

$a=i−j,a=i−j,$ $b=7i+2j−kb=7i+2j−k$

145 .

Find all two-dimensional vectors a orthogonal to vector $b=〈3,4〉.b=〈3,4〉.$ Express the answer in component form.

146 .

Find all two-dimensional vectors a orthogonal to vector $b=〈5,−6〉.b=〈5,−6〉.$ Express the answer by using standard unit vectors.

147 .

Determine all three-dimensional vectors u orthogonal to vector $v=〈1,1,0〉.v=〈1,1,0〉.$ Express the answer by using standard unit vectors.

148 .

Determine all three-dimensional vectors u orthogonal to vector $v=i−j−k.v=i−j−k.$ Express the answer in component form.

149 .

Determine the real number $αα$ such that vectors $a=2i+3ja=2i+3j$ and $b=9i+αjb=9i+αj$ are orthogonal.

150 .

Determine the real number $αα$ such that vectors $a=−3i+2ja=−3i+2j$ and $b=2i+αjb=2i+αj$ are orthogonal.

151 .

[T] Consider the points $P(4,5)P(4,5)$ and $Q(5,−7).Q(5,−7).$

1. Determine vectors $OP→OP→$ and $OQ→.OQ→.$ Express the answer by using standard unit vectors.
2. Determine the measure of angle O in triangle OPQ. Express the answer in degrees rounded to two decimal places.
152 .

[T] Consider points $A(1,1),A(1,1),$ $B(2,−7),B(2,−7),$ and $C(6,3).C(6,3).$

1. Determine vectors $BA→BA→$ and $BC→.BC→.$ Express the answer in component form.
2. Determine the measure of angle B in triangle ABC. Express the answer in degrees rounded to two decimal places.
153 .

Determine the measure of angle A in triangle ABC, where $A(1,1,8),A(1,1,8),$ $B(4,−3,−4),B(4,−3,−4),$ and $C(−3,1,5).C(−3,1,5).$ Express your answer in degrees rounded to two decimal places.

154 .

Consider points $P(3,7,−2)P(3,7,−2)$ and $Q(1,1,−3).Q(1,1,−3).$ Determine the angle between vectors $OP→OP→$ and $OQ→.OQ→.$ Express the answer in degrees rounded to two decimal places.

For the following exercises, determine which (if any) pairs of the following vectors are orthogonal.

155 .

$u=〈3,7,−2〉,u=〈3,7,−2〉,$ $v=〈5,−3,−3〉,v=〈5,−3,−3〉,$ $w=〈0,1,−1〉w=〈0,1,−1〉$

156 .

$u=i−k,u=i−k,$ $v=5j−5k,v=5j−5k,$ $w=10jw=10j$

157 .

Use vectors to show that a parallelogram with equal diagonals is a rectangle.

158 .

Use vectors to show that the diagonals of a rhombus are perpendicular.

159 .

Show that $u·(v+w)=u·v+u·wu·(v+w)=u·v+u·w$ is true for any vectors u, v, and w.

160 .

Verify the identity $u·(v+w)=u·v+u·wu·(v+w)=u·v+u·w$ for vectors $u=〈1,0,4〉,u=〈1,0,4〉,$ $v=〈−2,3,5〉,v=〈−2,3,5〉,$ and $w=〈4,−2,6〉.w=〈4,−2,6〉.$

For the following problems, the vector u is given.

1. Find the direction cosines for the vector u.
2. Find the direction angles for the vector u expressed in degrees. (Round the answer to the nearest integer.)
161 .

$u = 〈 2 , 2 , 1 〉 u = 〈 2 , 2 , 1 〉$

162 .

$u = i − 2 j + 2 k u = i − 2 j + 2 k$

163 .

$u = 〈 −1 , 5 , 2 〉 u = 〈 −1 , 5 , 2 〉$

164 .

$u = 〈 2 , 3 , 4 〉 u = 〈 2 , 3 , 4 〉$

165 .

Consider $u=〈a,b,c〉u=〈a,b,c〉$ a nonzero three-dimensional vector. Let $cosα,cosα,$ $cosβ,cosβ,$ and $cosγcosγ$ be the directions of the cosines of u. Show that $cos2α+cos2β+cos2γ=1.cos2α+cos2β+cos2γ=1.$

166 .

Determine the direction cosines of vector $u=i+2j+2ku=i+2j+2k$ and show they satisfy $cos2α+cos2β+cos2γ=1.cos2α+cos2β+cos2γ=1.$

For the following exercises, the vectors u and v are given.

1. Find the vector projection $w=projuvw=projuv$ of vector v onto vector u. Express your answer in component form.
2. Find the scalar projection $compuvcompuv$ of vector v onto vector u.
167 .

$u=5i+2j,u=5i+2j,$ $v=2i+3jv=2i+3j$

168 .

$u=〈−4,7〉,u=〈−4,7〉,$ $v=〈3,5〉v=〈3,5〉$

169 .

$u=3i+2k,u=3i+2k,$ $v=2j+4kv=2j+4k$

170 .

$u=〈4,4,0〉,u=〈4,4,0〉,$ $v=〈0,4,1〉v=〈0,4,1〉$

171 .

Consider the vectors $u=4i−3ju=4i−3j$ and $v=3i+2j.v=3i+2j.$

1. Find the component form of vector $w=projuvw=projuv$ that represents the projection of v onto u.
2. Write the decomposition $v=w+qv=w+q$ of vector v into the orthogonal components w and q, where w is the projection of v onto u and q is a vector orthogonal to the direction of u.
172 .

Consider vectors $u=2i+4ju=2i+4j$ and $v=4j+2k.v=4j+2k.$

1. Find the component form of vector $w=projuvw=projuv$ that represents the projection of v onto u.
2. Write the decomposition $v=w+qv=w+q$ of vector v into the orthogonal components w and q, where w is the projection of v onto u and q is a vector orthogonal to the direction of u.
173 .

A methane molecule has a carbon atom situated at the origin and four hydrogen atoms located at points $P(1,1,−1),Q(1,−1,1),R(−1,1,1),andS(−1,−1,−1)P(1,1,−1),Q(1,−1,1),R(−1,1,1),andS(−1,−1,−1)$ (see figure).

1. Find the distance between the hydrogen atoms located at P and R.
2. Find the angle between vectors $OS→OS→$ and $OR→OR→$ that connect the carbon atom with the hydrogen atoms located at S and R, which is also called the bond angle. Express the answer in degrees rounded to two decimal places.
174 .

[T] Find the vectors that join the center of a clock to the hours 1:00, 2:00, and 3:00. Assume the clock is circular with a radius of 1 unit.

175 .

Find the work done by force $F=〈5,6,−2〉F=〈5,6,−2〉$ (measured in Newtons) that moves a particle from point $P(3,−1,0)P(3,−1,0)$ to point $Q(2,3,1)Q(2,3,1)$ along a straight line (the distance is measured in meters).

176 .

[T] A sled is pulled by exerting a force of 100 N on a rope that makes an angle of $25°25°$ with the horizontal. Find the work done in pulling the sled 40 m. (Round the answer to one decimal place.)

177 .

[T] A father is pulling his son on a sled at an angle of $20°20°$ with the horizontal with a force of 25 lb (see the following image). He pulls the sled in a straight path of 50 ft. How much work was done by the man pulling the sled? (Round the answer to the nearest integer.)

178 .

[T] A car is towed using a force of 1600 N. The rope used to pull the car makes an angle of 25° with the horizontal. Find the work done in towing the car 2 km. Express the answer in joules $(1J=1N·m)(1J=1N·m)$ rounded to the nearest integer.

179 .

[T] A boat sails north aided by a wind blowing in a direction of $N30°EN30°E$ with a magnitude of 500 lb. How much work is performed by the wind as the boat moves 100 ft? (Round the answer to two decimal places.)

180 .

Vector $p=〈150,225,375〉p=〈150,225,375〉$ represents the price of certain models of bicycles sold by a bicycle shop. Vector $n=〈10,7,9〉n=〈10,7,9〉$ represents the number of bicycles sold of each model, respectively. Compute the dot product $p·np·n$ and state its meaning.

181 .

[T] Two forces $F1F1$ and $F2F2$ are represented by vectors with initial points that are at the origin. The first force has a magnitude of 20 lb and the terminal point of the vector is point $P(1,1,0).P(1,1,0).$ The second force has a magnitude of 40 lb and the terminal point of its vector is point $Q(0,1,1).Q(0,1,1).$ Let F be the resultant force of forces $F1F1$ and $F2.F2.$

1. Find the magnitude of F. (Round the answer to one decimal place.)
2. Find the direction angles of F. (Express the answer in degrees rounded to one decimal place.)
182 .

[T] Consider $r(t)=〈cost,sint,2t〉r(t)=〈cost,sint,2t〉$ the position vector of a particle at time $t∈[0,30],t∈[0,30],$ where the components of r are expressed in centimeters and time in seconds. Let $OP→OP→$ be the position vector of the particle after 1 sec.

1. Show that all vectors $PQ→,PQ→,$ where $Q(x,y,z)Q(x,y,z)$ is an arbitrary point, orthogonal to the instantaneous velocity vector $v(1)v(1)$ of the particle after 1 sec, can be expressed as $PQ→=〈x−cos1,y−sin1,z−2〉,PQ→=〈x−cos1,y−sin1,z−2〉,$ where $xsin1−ycos1−2z+4=0.xsin1−ycos1−2z+4=0.$ The set of point Q describes a plane called the normal plane to the path of the particle at point P.
2. Use a CAS to visualize the instantaneous velocity vector and the normal plane at point P along with the path of the particle.
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