Slide 7.3 - 1 Copyright © 2008 Pearson Education, Inc. Publishing as Pearson Addison-Wesley
Slide 7.3 - 1 Copyright © 2008 Pearson Education, Inc. Publishing as Pearson Addison-Wesley
Copyright © 2008 Pearson Education, Inc. Publishing as Pearson Addison-Wesley
OBJECTIVES
Vectors
Learn to represent vectors geometrically.Learn to represent vectors algebraically.Learn the definition of a unit vector. Learn to write a vector in terms of its magnitude and direction.Learn the definition of the dot product.Learn to find the angle between two vectors.Learn the definition of work.
SECTION 7.3
1
2
3
4
5
6
7
Slide 7.3 - 3 Copyright © 2008 Pearson Education, Inc. Publishing as Pearson Addison-Wesley
VECTORSMany physical quantities, such as length, area, volume, mass, and temperature, are completely described by their magnitudes in appropriate units. Such quantities are called scalar quantities. Other physical quantities, such as velocity, acceleration, and force, are not completely determined until both a magnitude (size) and a direction are specified. For example, the movement of wind is usually described by its speed (magnitude) and the direction. The wind speed and wind direction together form a vector quantity called the wind velocity.
Slide 7.3 - 4 Copyright © 2008 Pearson Education, Inc. Publishing as Pearson Addison-Wesley
GEOMETRIC VECTORS
A vector can be represented geometrically by a line segment with an arrowhead. The direction of the arrow specifies the direction of the vector. The length of the arrow describes its magnitude. The tail of the arrow is called the initial point of the vector, and the tip of the arrow the terminal point. We shall denote vectors by lowercase boldface type, such as a, b, i, j, u, v, and w. When discussing vectors, we refer to real numbers as scalars. Scalars will be denoted by lower case italic type, such as a, b, x, y, and z.
Slide 7.3 - 5 Copyright © 2008 Pearson Education, Inc. Publishing as Pearson Addison-Wesley
GEOMETRIC VECTORS
If the initial point of a vector v is P and the terminal point is Q, we write
v PQu ruu
.
The magnitude (or norm)of a vector v PQ
u ruu,
denoted byv , or PQu ruu
,is the length of the vector v and is a scalar quantity.
Slide 7.3 - 6 Copyright © 2008 Pearson Education, Inc. Publishing as Pearson Addison-Wesley
EQUIVALENT VECTORS
Two vectors having the same length and same direction are called equivalent vectors.
Slide 7.3 - 7 Copyright © 2008 Pearson Education, Inc. Publishing as Pearson Addison-Wesley
EQUIVALENT VECTORS
Equivalent vectors are regarded as equal even though they may be located in different positions.
Slide 7.3 - 8 Copyright © 2008 Pearson Education, Inc. Publishing as Pearson Addison-Wesley
ZERO VECTOR
The vector of length zero is called the zero vector and is denoted by 0. The zero vector has zero magnitude and arbitrary direction. If vectors v and a, have the same length and opposite direction, then a is the opposite vector of v and we write a = –v.
Slide 7.3 - 9 Copyright © 2008 Pearson Education, Inc. Publishing as Pearson Addison-Wesley
VECTOR ADDITION (TRIANGLE RULE)
Let v and w be any two vectors. Place the vector w so that its initial point coincides with the terminal point of v. The vector v + w, called the resultant vector, is represented by the arrow from the initial point of v to the terminal point of w.
v
wv + w
Slide 7.3 - 10 Copyright © 2008 Pearson Education, Inc. Publishing as Pearson Addison-Wesley
VECTOR ADDITION (PARALLELOGRAM RULE)
Place vectors v and w so that their initial points coincide. Form a parallelogram with v and w as the adjacent sides. The vector with the same initial point as the initial points of v and w that coincides withthe diagonal of the parallelogram represents the resultant vector, v + w.
Note that:v + w = w + v
Slide 7.3 - 11 Copyright © 2008 Pearson Education, Inc. Publishing as Pearson Addison-Wesley
VECTOR SUBTRACTION
For any two vectors v and w, v – w = v + (–w), where –w is the opposite of w.
Slide 7.3 - 12 Copyright © 2008 Pearson Education, Inc. Publishing as Pearson Addison-Wesley
SCALAR MULTIPLES OF VECTORS
Let v be a vector and c a scalar (a real number). The vector cv is called the scalar multiple of v.
If c > 0, cv has the same direction as v and magnitude c||v||.
If c < 0, cv has the opposite direction as v and magnitude |c| ||v||.
If c = 0, cv = 0v = 0.
Slide 7.3 - 13 Copyright © 2008 Pearson Education, Inc. Publishing as Pearson Addison-Wesley
EXAMPLE 1 Geometric Vectors
Use the vectors u, v, and w to graph each vector.
a. u – 2w b. 2v – u + w
Solution
a. u – 2w
Slide 7.3 - 14 Copyright © 2008 Pearson Education, Inc. Publishing as Pearson Addison-Wesley
EXAMPLE 1 Geometric Vectors
Solution continued
b. 2v – u + w
Slide 7.3 - 15 Copyright © 2008 Pearson Education, Inc. Publishing as Pearson Addison-Wesley
ALGEBRAIC VECTORS
Specifying the terminal point of the vector will completely determine the vector. For the position vector v with initial point at the origin O and terminal point at P(v1, v2), we denote the vector by
A vector drawn with its initial point at the origin is called a position vector.
v OPu ruu
v1,v2 .
Slide 7.3 - 16 Copyright © 2008 Pearson Education, Inc. Publishing as Pearson Addison-Wesley
COMPONENTS OF VECTORS
A point is denoted (v1, v2),
We call v1 and v2 the components of the vector v; v1 is the first component, and v2 is the second component.
v1,v2 .we denote a vector
v v1,v2The magnitude offollows directly from the Pythagorean Theorem,
v v12 v2
2 .
Slide 7.3 - 17 Copyright © 2008 Pearson Education, Inc. Publishing as Pearson Addison-Wesley
EQUIVALENT VECTORS
points must coincide.
If equivalent vectors, v and w, are located so that their initial are at the origin, then their terminal
w w1,w2 .v v1,v2
v w if and only ifv1 w1 and v2 w2
v v1,v2
Slide 7.3 - 18 Copyright © 2008 Pearson Education, Inc. Publishing as Pearson Addison-Wesley
REPRESENTING A VECTORAS A POSITION VECTOR
The vector with initial
point P(x1, y1) and terminal
point Q(x2, y2) is equal to
the position vectorw x2 x1, y2 y1 .
PQu ruu
Slide 7.3 - 19 Copyright © 2008 Pearson Education, Inc. Publishing as Pearson Addison-Wesley
EXAMPLE 2 Representing a Vector in the Cartesian Plane
Let v be the vector with initial point P(4, –2) and terminal point Q(–1, 3).Write v as a position vector.Solution
v has:initial point P(4, –2), so x1 = 4 and y1 = –2terminal point Q(–1, 3), so x2 = –1 and y2 = 3
v 1 4, 3 2 v 5, 5
v x2 x1, y2 y1Thus,
Slide 7.3 - 20 Copyright © 2008 Pearson Education, Inc. Publishing as Pearson Addison-Wesley
ARITHMETIC OPERATIONS ON VECTORS
are vectors and c is any scalar, then
v w v1 w1,v2 w2
If v v1,v2 and w w1,w2
v w v1 w1,v2 w2
cv cv1,cv2
Slide 7.3 - 21 Copyright © 2008 Pearson Education, Inc. Publishing as Pearson Addison-Wesley
EXAMPLE 3 Operations on Vectors
Find each expression.a. v + w b. –2v c. 2v – w d. ||2v – w||
b. 2v 2 2, 3
Solution a. v w 2, 3 4,1
Let v 2, 3 and w 4,1 .
2 4, 31
2, 4
22, 23 4, 6
Slide 7.3 - 22 Copyright © 2008 Pearson Education, Inc. Publishing as Pearson Addison-Wesley
EXAMPLE 3 Operations on Vectors
Solution continuedc. 2v w 2 2, 3 4,1
d. 2v w 8,5
4,6 4,1
4 4 ,6 1
8,5
2v w 82 52
2v w 64 25 89
Slide 7.3 - 23 Copyright © 2008 Pearson Education, Inc. Publishing as Pearson Addison-Wesley
UNIT VECTORS
A unit vector has length 1.
1
vv.
The unit vector in the same direction as v is given by
Slide 7.3 - 24 Copyright © 2008 Pearson Education, Inc. Publishing as Pearson Addison-Wesley
EXAMPLE 4 Finding a Unit Vector
Find a unit vector u in the direction of v 3, 4 .
Solution
v 3 2 4 2 25 5
First, find the magnitude of v 3, 4 .
u 1
vv
1
53, 4
3
5,
4
5Now,
u 3
5
2
4
5
2
9
25
16
25
25
251
Check:
Slide 7.3 - 25 Copyright © 2008 Pearson Education, Inc. Publishing as Pearson Addison-Wesley
UNIT VECTORS i AND jIn a Cartesian coordinate plane, two unit vectors that lie along the coordinate axes are particularly important. These are the vectors
i 1,0 and j 0,1 .
A vector v from (0, 0) to (v1, v2) can be represented in the form
v v1i v2 j
v v12 v2
2 .with
Slide 7.3 - 26 Copyright © 2008 Pearson Education, Inc. Publishing as Pearson Addison-Wesley
EXAMPLE 5 Vectors Involving i and j
Find each expression for u = 4i + 7j and v = 2i + 5j.
Solutiona. u – 3v = (4i + 7j) – 3(2i + 5j)
2 2 8 2
a. u – 3v b. ||u – 3v||
= 4i + 7j – 6i – 15j = (4 – 6)i + (7 – 15)j= –2i – 8j
b. u 3v 2i 8 j
68 2 17
Slide 7.3 - 27 Copyright © 2008 Pearson Education, Inc. Publishing as Pearson Addison-Wesley
VECTORS IN TERMS OFMAGNITUDE AND DIRECTION
Let v v1,v2
that is the smallest positive angle that v makes with the positive x-axis. The angle is called the direction angle of v.
v v cosi sin j The formula
be a position vector, and suppose
expresses a vector v in terms of its magnitude ||v|| and its direction angle .
Slide 7.3 - 28 Copyright © 2008 Pearson Education, Inc. Publishing as Pearson Addison-Wesley
EXAMPLE 6Writing a Vector with Given Length and Direction Angle
Solutionv v cosi sin j
v 3 cos3
i sin3
j
v 31
2i
3
2j
v 3
2i
3 3
2j
Write the vector with magnitude 3 that makes an angle of with the positive x-axis.
3
Slide 7.3 - 29 Copyright © 2008 Pearson Education, Inc. Publishing as Pearson Addison-Wesley
THE DOT PRODUCT
For two vectors v v1,v2 and w w1,w2 ,
the dot product of v and w, denoted v • w, is
defined as:
v w v1,v2 w1,w2 v1w1 v2w2
Slide 7.3 - 30 Copyright © 2008 Pearson Education, Inc. Publishing as Pearson Addison-Wesley
EXAMPLE 7 Finding the Dot Product
Find the dot product v • w.a. v 2, 3 and w 3, 4
b. v 3i 5 j and w 2i 3j
Solution a. v w 2, 3 3, 4
2 3 3 4 6 12 6
3,5 2, 3
3 2 5 3 6 15 9
b. v w 3i 5 j 2i 3j
Slide 7.3 - 31 Copyright © 2008 Pearson Education, Inc. Publishing as Pearson Addison-Wesley
PROPERTIES OF THE DOT PRODUCT
1. uv v u
2. u v w uv uw3. 0v 0
4. v v v2
5. cu v c uv u cv
If u, v, and w are vectors and c is a scalar, then
Slide 7.3 - 32 Copyright © 2008 Pearson Education, Inc. Publishing as Pearson Addison-Wesley
THE DOT PRODUCT ANDTHE ANGLE BETWEEN TWO VECTORS
v w v w cos
Let (0 ≤ ≤ π) be the angle between two nonzero vectors v and w. Then:
cos v wv w
or
Slide 7.3 - 33 Copyright © 2008 Pearson Education, Inc. Publishing as Pearson Addison-Wesley
EXAMPLE 11 Using Vectors in Air Navigation
An F-15 fighter jet is flying over Mount Rushmore at an airspeed (speed in still air) of 800 miles per hour on a bearing of N 30º E. The velocity of wind is 40 miles per hour in the direction of S 45º E. Find the actual speed and direction (relative to the ground) of the plane. Round each answer to the nearest tenth.
Set up a coordinate system with north along the positive y-axis.
Solution
Slide 7.3 - 34 Copyright © 2008 Pearson Education, Inc. Publishing as Pearson Addison-Wesley
EXAMPLE 11 Using Vectors in Air Navigation
Letv be the air velocity (plane),w be the wind velocity, andr be the resultant ground
velocity of the plane.Then,
Solution continued
v 800 cos60º i sin 60º j w 40 cos 45º i sin 45º j
r 800 cos60º i sin 60º j 40 cos 45º i sin 45º j r v w
Slide 7.3 - 35 Copyright © 2008 Pearson Education, Inc. Publishing as Pearson Addison-Wesley
Solution continued
r 800 cos60º 40 cos 45º i 800sin 60º 40sin 45º j
EXAMPLE 11 Using Vectors in Air Navigation
r 800 cos60º40 cos 45º 2 800sin 60º 40sin 45º 2
r 790.6
The ground speed of the F-15 is approximately 790.6 miles per hour.
To find the actual direction (bearing) of the plane, find the angle between r and j (unit vector in the direction north).
Slide 7.3 - 36 Copyright © 2008 Pearson Education, Inc. Publishing as Pearson Addison-Wesley
Solution continued
cos jrj r
EXAMPLE 11 Using Vectors in Air Navigation
cos 0.8405
The direction of the F-15 relative to the ground is approximately N 32.8º E.
cos 800sin 60º 40sin 45º
790.6
cos 1 0.8405 32.8º
Slide 7.3 - 37 Copyright © 2008 Pearson Education, Inc. Publishing as Pearson Addison-Wesley
DEFINITION OF WORK
W FPQu ruu
The work W done by a constant force F in moving an object from a point P to a point Q is defined by
Slide 7.3 - 38 Copyright © 2008 Pearson Education, Inc. Publishing as Pearson Addison-Wesley
EXAMPLE 12 Computing Work
A child pulls a wagon along a level ground, with a force of 40 pounds along the handle on the wagon that makes an angle of 42º with the horizontal. How much work has she done by pulling the wagon 150 feet?
W 40 150 cos 42º
W 4458.87 foot-pounds
Solution
W FPQu ruu
W F PQu ruuu
cos