copyright © 2009 pearson addison-wesley 7.4-1 7 applications of trigonometry and vectors

32
Copyright © 2009 Pearson Addison-Wesley 7.4-1 7 Application s of Trigonometr y and Vectors

Upload: francis-robbins

Post on 16-Jan-2016

216 views

Category:

Documents


0 download

TRANSCRIPT

Page 1: Copyright © 2009 Pearson Addison-Wesley 7.4-1 7 Applications of Trigonometry and Vectors

Copyright © 2009 Pearson Addison-Wesley 7.4-1

7Applications of Trigonometry and Vectors

Page 2: Copyright © 2009 Pearson Addison-Wesley 7.4-1 7 Applications of Trigonometry and Vectors

Copyright © 2009 Pearson Addison-Wesley 7.4-2

7.1 Oblique Triangles and the Law of Sines

7.2 The Ambiguous Case of the Law of Sines

7.3 The Law of Cosines

7.4 Vectors, Operations, and the Dot Product

7.5 Applications of Vectors

7Applications of Trigonometry and Vectors

Page 3: Copyright © 2009 Pearson Addison-Wesley 7.4-1 7 Applications of Trigonometry and Vectors

Copyright © 2009 Pearson Addison-Wesley

1.1-3

7.4-3

Vectors, Operations, and the Dot Product

7.4

Basic Terminology ▪ Algebraic Interpretation of Vectors ▪ Operations with Vectors ▪ Dot Product and the Angle Between Vectors

Page 4: Copyright © 2009 Pearson Addison-Wesley 7.4-1 7 Applications of Trigonometry and Vectors

Copyright © 2009 Pearson Addison-Wesley 7.4-4

Basic Terminology

Scalar: The magnitude of a quantity. It can be represented by a real number.

A vector in the plane is a directed line segment.

Consider vector OP

O is called the initial point

P is called the terminal point

Page 5: Copyright © 2009 Pearson Addison-Wesley 7.4-1 7 Applications of Trigonometry and Vectors

Copyright © 2009 Pearson Addison-Wesley 7.4-5

Basic Terminology

Magnitude: length of a vector, expressed as|OP|

Two vectors are equal if and only if they have the same magnitude and same direction.

Vectors OP and PO have the same magnitude, but opposite directions.|OP| = |PO|

Page 6: Copyright © 2009 Pearson Addison-Wesley 7.4-1 7 Applications of Trigonometry and Vectors

Copyright © 2009 Pearson Addison-Wesley 7.4-6

Basic Terminology

A = B C = D A ≠ E A ≠ F

Page 7: Copyright © 2009 Pearson Addison-Wesley 7.4-1 7 Applications of Trigonometry and Vectors

Copyright © 2009 Pearson Addison-Wesley 7.4-7

Sum of Two Vectors

The sum of two vectors is also a vector. The vector sum A + B is called the resultant.

Two ways to represent the sum of two vectors

Page 8: Copyright © 2009 Pearson Addison-Wesley 7.4-1 7 Applications of Trigonometry and Vectors

Copyright © 2009 Pearson Addison-Wesley 7.4-8

Sum of Two Vectors

The sum of a vector v and its opposite –v has magnitude 0 and is called the zero vector.

To subtract vector B from vector A, find the vector sum A + (–B).

Page 9: Copyright © 2009 Pearson Addison-Wesley 7.4-1 7 Applications of Trigonometry and Vectors

Copyright © 2009 Pearson Addison-Wesley 7.4-9

Scalar Product of a Vector

The scalar product of a real number k and a vector u is the vector k ∙ u, with magnitude |k| times the magnitude of u.

Page 10: Copyright © 2009 Pearson Addison-Wesley 7.4-1 7 Applications of Trigonometry and Vectors

Copyright © 2009 Pearson Addison-Wesley 7.4-10

Algebraic Interpretation of Vectors

A vector with its initial point at the origin is called a position vector.

A position vector u with its endpoint at the point (a, b) is written

Page 11: Copyright © 2009 Pearson Addison-Wesley 7.4-1 7 Applications of Trigonometry and Vectors

Copyright © 2009 Pearson Addison-Wesley 7.4-11

Algebraic Interpretation of Vectors

The numbers a and b are the horizontal component and vertical component of vector u.

The positive angle between the x-axis and a position vector is the direction angle for the vector.

Page 12: Copyright © 2009 Pearson Addison-Wesley 7.4-1 7 Applications of Trigonometry and Vectors

Copyright © 2009 Pearson Addison-Wesley

1.1-12

7.4-12

Magnitude and Direction Angle of a Vector a, b

The magnitude (length) of a vector u = a, b is given by

The direction angle θ satisfieswhere a ≠ 0.

Page 13: Copyright © 2009 Pearson Addison-Wesley 7.4-1 7 Applications of Trigonometry and Vectors

Copyright © 2009 Pearson Addison-Wesley

1.1-13

7.4-13

Example 1 FINDING MAGNITUDE AND DIRECTION ANGLE

Find the magnitude and direction angle for u = 3, –2.

Magnitude:

Direction angle:

Page 14: Copyright © 2009 Pearson Addison-Wesley 7.4-1 7 Applications of Trigonometry and Vectors

Copyright © 2009 Pearson Addison-Wesley

1.1-14

7.4-14

Example 1 FINDING MAGNITUDE AND DIRECTION ANGLE (continued)

Graphing calculator solution:

Page 15: Copyright © 2009 Pearson Addison-Wesley 7.4-1 7 Applications of Trigonometry and Vectors

Copyright © 2009 Pearson Addison-Wesley

1.1-15

7.4-15

Horizontal and Vertical Components

The horizontal and vertical components, respectively, of a vector u having magnitude |u| and direction angle θ are given by

or

Page 16: Copyright © 2009 Pearson Addison-Wesley 7.4-1 7 Applications of Trigonometry and Vectors

Copyright © 2009 Pearson Addison-Wesley

1.1-16

7.4-16

Example 2 FINDING HORIZONTAL AND VERTICAL COMPONENTS

Vector w has magnitude 25.0 and direction angle 41.7°. Find the horizontal and vertical components.

Horizontal component: 18.7

Vertical component: 16.6

Page 17: Copyright © 2009 Pearson Addison-Wesley 7.4-1 7 Applications of Trigonometry and Vectors

Copyright © 2009 Pearson Addison-Wesley

1.1-17

7.4-17

Example 2 FINDING HORIZONTAL AND VERTICAL COMPONENTS

Graphing calculator solution:

Page 18: Copyright © 2009 Pearson Addison-Wesley 7.4-1 7 Applications of Trigonometry and Vectors

Copyright © 2009 Pearson Addison-Wesley

1.1-18

7.4-18

Example 3 WRITING VECTORS IN THE FORM a, b

Write each vector in the figure in the form a, b.

Page 19: Copyright © 2009 Pearson Addison-Wesley 7.4-1 7 Applications of Trigonometry and Vectors

Copyright © 2009 Pearson Addison-Wesley

1.1-19

7.4-19

Properties of Parallelograms

1. A parallelogram is a quadrilateral whose opposite sides are parallel.

2. The opposite sides and opposite angles of a parallelogram are equal, and adjacent angles of a parallelogram are supplementary.

3. The diagonals of a parallelogram bisect each other, but do not necessarily bisect the angles of the parallelogram.

Page 20: Copyright © 2009 Pearson Addison-Wesley 7.4-1 7 Applications of Trigonometry and Vectors

Copyright © 2009 Pearson Addison-Wesley

1.1-20

7.4-20

Example 4 FINDING THE MAGNITUDE OF A RESULTANT

Two forces of 15 and 22 newtons act on a point in the plane. (A newton is a unit of force that equals .225 lb.) If the angle between the forces is 100°, find the magnitude of the resultant vector.

The angles of the parallelogram adjacent to P measure 80° because the adjacent angles of a parallelogram are supplementary.

Use the law of cosines with ΔPSR or ΔPQR.

Page 21: Copyright © 2009 Pearson Addison-Wesley 7.4-1 7 Applications of Trigonometry and Vectors

Copyright © 2009 Pearson Addison-Wesley

1.1-21

7.4-21

Example 4 FINDING THE MAGNITUDE OF A RESULTANT (continued)

The magnitude of the resultant vector is about24 newtons.

Page 22: Copyright © 2009 Pearson Addison-Wesley 7.4-1 7 Applications of Trigonometry and Vectors

Copyright © 2009 Pearson Addison-Wesley

1.1-22

7.4-22

Vector Operations

For any real numbers a, b, c, d, and k,

Page 23: Copyright © 2009 Pearson Addison-Wesley 7.4-1 7 Applications of Trigonometry and Vectors

Copyright © 2009 Pearson Addison-Wesley

1.1-23

7.4-23

Example 5 PERFORMING VECTOR OPERATIONS

Let u = –2, 1 and v = 4, 3. Find the following.

(a) u + v

(b) –2u

(c) 4u – 3v

= –2, 1 + 4, 3 = –2 + 4, 1 + 3 = 2, 4

= –2 ∙ –2, 1 = –2(–2), –2(1) = 4, –2

= 4 ∙ –2, 1 – 3 ∙ 4, 3

= –8, 4 –12, 9

= –8 – 12, 4 – 9 = –20,–5

Page 24: Copyright © 2009 Pearson Addison-Wesley 7.4-1 7 Applications of Trigonometry and Vectors

Copyright © 2009 Pearson Addison-Wesley 7.4-24

Unit Vectors

A unit vector is a vector that has magnitude 1.

i = 1, 0 j = 0, 1

Page 25: Copyright © 2009 Pearson Addison-Wesley 7.4-1 7 Applications of Trigonometry and Vectors

Copyright © 2009 Pearson Addison-Wesley 7.4-25

Unit Vectors

Any vector a, b can be expressed in the form ai + bj using the unit vectors i and j.

Page 26: Copyright © 2009 Pearson Addison-Wesley 7.4-1 7 Applications of Trigonometry and Vectors

Copyright © 2009 Pearson Addison-Wesley

1.1-26

7.4-26

Dot Product

The dot product (or inner product) of the two vectors u = a, b and v = c, d is denoted u ∙ v, read “u dot v,” and is given by

u ∙ v = ac + bd.

Page 27: Copyright © 2009 Pearson Addison-Wesley 7.4-1 7 Applications of Trigonometry and Vectors

Copyright © 2009 Pearson Addison-Wesley

1.1-27

7.4-27

Example 6 FINDING DOT PRODUCTS

Find each dot product.

(a) 2, 3 ∙ 4, –1 = 2(4) + 3(–1) = 5

(b) 6, 4 ∙ –2, 3 = 6(–2) + 4(3) = 0

Page 28: Copyright © 2009 Pearson Addison-Wesley 7.4-1 7 Applications of Trigonometry and Vectors

Copyright © 2009 Pearson Addison-Wesley

1.1-28

7.4-28

Properties of the Dot Product

For all vectors u, v, and w and real number k,

(a) u ∙ v = v ∙ u

(b) u ∙ (v + w) = u ∙ v + u ∙ w

(c) (u + v) ∙ w = u ∙ w + v ∙ w

(d) (ku) ∙ v = k(u ∙ v) = u ∙ kv

(e) 0 ∙ u = 0

(f) u ∙ u = |u|2

Page 29: Copyright © 2009 Pearson Addison-Wesley 7.4-1 7 Applications of Trigonometry and Vectors

Copyright © 2009 Pearson Addison-Wesley

1.1-29

7.4-29

Geometric Interpretation of the Dot Product

If θ is the angle between the two nonzero vectors u and v, where 0° ≤ θ ≤ 180°, then

or

Page 30: Copyright © 2009 Pearson Addison-Wesley 7.4-1 7 Applications of Trigonometry and Vectors

Copyright © 2009 Pearson Addison-Wesley

1.1-30

7.4-30

Example 7 FINDING THE ANGLE BETWEEN TWO VECTORS

Find the angle θ between the two vectors u = 3, 4 and v = 2, 1.

Page 31: Copyright © 2009 Pearson Addison-Wesley 7.4-1 7 Applications of Trigonometry and Vectors

Copyright © 2009 Pearson Addison-Wesley 7.4-31

Dot Products

For angles θ between 0° and 180°, cos θ is positive, 0, or negative when θ is less than, equal to, or greater than 90°, respectively.

Page 32: Copyright © 2009 Pearson Addison-Wesley 7.4-1 7 Applications of Trigonometry and Vectors

Copyright © 2009 Pearson Addison-Wesley

1.1-32

7.4-32

Note

If a ∙ b = 0 for two nonzero vectors a and b, then cos θ = 0 and θ = 90°. Thus, a and b are perpendicular or orthogonal vectors.