A particle moving along a straight line can move in only two directions. We can
take its motion to be positive in one of these directions and negative in the other.
For a particle moving in three dimensions, however, a plus sign or minus sign is no
longer enough to indicate a direction. Instead, we must use a *vector*.

A *vector* has magnitude as well as direction, and vectors follow certain
(vector) rules of combination, which we examine in this chapter. A *vector
quantity* is a quantity that has both a magnitude and a direction and
thus can be represented with a vector. Some physical quantities that are vector
quantities are displacement, velocity, and acceleration.

Figure 3-1 (a) All three arrows have the same magnitude and direction and thus
represent the same displacement.

Not all physical quantities involve a direction.Temperature, pressure, energy,
mass, and time, for example, do not "point" in the spatial sense. We call such
quantities *scalars*, and we deal with them by the rules of ordinary algebra.
A single value, with a sign (as in a temperature of -40^{o}F), specifies a scalar.

The simplest vector quantity is displacement, or change of position. A vector
that represents a displacement is called, reasonably, a *displacement vector*.
(Similarly, we have velocity vectors and acceleration vectors.) If a particle changes
its position by moving from A to B in Fig. 3-1a, we say that it undergoes a
displacement from A to B, which we represent with an arrow pointing from A to B.
The arrow specifies the vector graphically. To distinguish vector symbols from other
kinds of arrows in this book, we use the outline of a triangle as the arrowhead.

Figure 3-1 (b) All three paths connecting the two points correspond to the same displacement vector.

In Fig. 3-1a, the arrows from A to B, from A' to B', and from A" to B" have
the same magnitude and direction. Thus, they specify identical displacement
vectors and represent the same *change of position* for the particle. A vector can be
shifted without changing its value if its length and direction are not changed.

The displacement vector tells us nothing about the actual path that the particle takes. In Fig. 3-1b, for example, all three paths connecting points A and B correspond to the same displacement vector, that of Fig. 3-1a. Displacement vectors represent only the overall effect of the motion, not the motion itself.

**Adding Vectors Geometrically**

Figure 3-2 (a) AC is the vector sum of the vectors AB and BC.

Suppose that, as in the vector diagram of Fig. 3-2a, a particle moves from A to B
and then later from B to C. We can represent its overall displacement (no matter
what its actual path) with two successive displacement vectors, AB and BC.
The net displacement of these two displacements is a single displacement from A
to C. We call AC the *vector sum* (or *resultant*) of the vectors AB and BC.
This sum is not the usual algebraic sum.

Figure 3-2 (b) The same vectors relabeled.

In Fig. 3-2b, we redraw the vectors of Fig. 3-2a and relabel them in the way
that we shall use from now on, namely, with an arrow over an italic symbol, as
in. If we want to indicate only the magnitude of the vector (a quantity that lacks
a sign or direction), we shall use the italic symbol, as in a, b, and s. (You can use
just a handwritten symbol.) A symbol with an overhead arrow always implies
both properties of a vector, magnitude and direction. We can represent the relation
among the three vectors in Fig. 3-2b with the *vector equation*

$\overrightarrow{s}=\overrightarrow{a}+\overrightarrow{b}$ (3-1)

which says that the vector $\overrightarrow{s}$ is the vector sum of vectors $\overrightarrow{a}\text{and}\overrightarrow{b}$. The symbol + in Eq. 3-1 and the words "sum" and "add" have different meanings for vectors than they do in the usual algebra because they involve both magnitude and direction.

Figure 3-2 suggests a procedure for adding two-dimensional vectors $\overrightarrow{a}\text{and}\overrightarrow{b}$ geometrically. (1) On paper, sketch vector $\overrightarrow{a}$ to some convenient scale and at the proper angle. (2) Sketch vector $\overrightarrow{b}$ to the same scale, with its tail at the head of vector $\overrightarrow{a}$, again at the proper angle. (3) The vector sum $\overrightarrow{s}$ is the vector that extends from the tail of $\overrightarrow{a}$ to the head of $\overrightarrow{b}$.

The two vectors and can be added in either order; see Eq. 3-2.

**Properties**. Vector addition, defined in this way, has two important
properties. First, the order of addition does not matter. Adding
$\overrightarrow{a}\text{to}\overrightarrow{b}$
gives the same result as adding
$\overrightarrow{b}\text{to}\overrightarrow{a}$ (Fig. 3-3); that is,

$\overrightarrow{a}+\overrightarrow{b}=\overrightarrow{b}+\overrightarrow{a}$ (commutative law) (3-2)

Second, when there are more than two vectors, we can group them in any order
as we add them. Thus, if we want to add vectors
$\overrightarrow{a}\text{,}\overrightarrow{b}\text{,}\text{and}\overrightarrow{c}$,
we can add
$\overrightarrow{a}\text{and}\overrightarrow{b}$
first and then add their vector sum to
$\overrightarrow{c}$. We can also add
$\overrightarrow{b}\text{and}\overrightarrow{c}$
first and then add *that* sum to
$\overrightarrow{a}$. We get the same result either way, as shown in Fig. 3-4. That is,

The three vectors can be grouped in any way as they are added; see Eq. 3-3.

$(\overrightarrow{a}+\overrightarrow{b})+\overrightarrow{c}=\overrightarrow{a}+\left(\overrightarrow{b}\right)+\overrightarrow{c}$ (associative law) (3-3).

**figure 3-4** The three vectors

Figure 3-5 The vectors have the same magnitude and opposite directions

The vector $\overrightarrow{\mathrm{-b}}$ is a vector with the same magnitude as but the opposite direction (see Fig. 3-5). Adding the two vectors in Fig. 3-5 would yield

$\overrightarrow{b}+\left(\overrightarrow{\mathrm{-b}}\right)=0$Thus, adding $\overrightarrow{\mathrm{-b}}$ has the effect of subtracting $\overrightarrow{b}$. We use this property to define the difference between two vectors: let

$\overrightarrow{d}=\overrightarrow{a}-\overrightarrow{b}$. Then$\overrightarrow{d}=\overrightarrow{a}-\overrightarrow{b}=\overrightarrow{a}+\left(\overrightarrow{\mathrm{-b}}\right)$ (vector subtraction) (3-4)

Figure 3-6 (a)

that is, we find the difference vector $\overrightarrow{d}$ by adding the vector $\overrightarrow{\mathrm{-b}}$ to the vector $\overrightarrow{a}$. Figure 3-6 shows how this is done geometrically.

As in the usual algebra, we can move a term that includes a vector symbol from one side of a vector equation to the other, but we must change its sign. For example, if we are given Eq. 3-4 and need to solve for $\overrightarrow{a}$, we can rearrange the equation as

$\overrightarrow{d}+\overrightarrow{b}=\overrightarrow{a}$or

$\overrightarrow{a}=\overrightarrow{d}+\overrightarrow{b}$

Figure 3-6 (b) To subtract vector from vector, add vector
$\overrightarrow{\mathrm{-b}}$
to vector $\overrightarrow{a}.$

Remember that, although we have used displacement vectors here, the rules for addition and subtraction hold for vectors of all kinds, whether they represent velocities, accelerations, or any other vector quantity. However, we can add only vectors of the same kind. For example, we can add two displacements, or two velocities, but adding a displacement and a velocity makes no sense. In the arithmetic of scalars, that would be like trying to add 21 s and 12 m.

**About the Authors**

David Halliday was an American physicist known for his physics textbooks, *Physics and
Fundamentals of Physics*, which he wrote with Robert Resnick. Both textbooks have
been in continuous use since 1960 and are available in more than 47 languages.

Robert Resnick was a physics educator and author of physics textbooks. He was born in Baltimore, Maryland on January 11, 1923 and graduated from the Baltimore City College high school in 1939. He received his B.A. in 1943 and his Ph.D. in 1949, both in physics from Johns Hopkins University.

The 10th edition of Halliday's Fundamentals of Physics, Extended building upon previous issues by offering several new features and additions. The new edition offers most accurate, extensive and varied set of assessment questions of any course management program in addition to all questions including some form of question assistance including answer specific feedback to facilitate success. The text also offers multimedia presentations (videos and animations) of much of the material that provide an alternative pathway through the material for those who struggle with reading scientific exposition.

Furthermore, the book includes math review content in both a self-study module for more in-depth review and also in just-in-time math videos for a quick refresher on a specific topic. The Halliday content is widely accepted as clear, correct, and complete. The end-of-chapters problems are without peer. The new design, which was introduced in 9e continues with 10e, making this new edition of Halliday the most accessible and reader-friendly book on the market.

A Reader says,"As many reviewers have noted, this is a great physics book used widely in university technical programs as a first course in technical physics, with calculus. I find it is the one book I start with when trying to understand physical concepts at a useful but basic level. It has broad coverage and is well written . To go beyond this book requires specialized books on each topic of interest (electromagnetics, quantum mechanics, thermodynamics, etc.)."

Reader Frank says, "The treatment is sound, thorough, and clear. I’ve owned the early editions of Halliday and Resnick for years. I’m very happy that I updated my library with this 10th edition. The topics are covered in a very logical order. The study features and worked examples are outstanding. Don’t hesitate to buy this book! Reading it is awesome on the Kindle app on the iPad."

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