chapter 6 review due 5/21

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Pre-Calculus 1/31/2007 Chapter 6 Review Due 5/21 # 2 – 22 even # 53 – 59 odd # 62 – 70 even # 74, 81, 86 (p. 537)

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Chapter 6 Review Due 5/21. # 2 – 22 even # 53 – 59 odd # 62 – 70 even # 74, 81, 86 (p. 537). Vector Formulas. Unit Vectors:. Horizontal/Vertical components:. Angle between Vectors:. Projections:. 6.1 Vectors in a Plane Day # 1. RS starts at R and goes to S. v =. direction. - PowerPoint PPT Presentation

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Page 1: Chapter 6 Review Due 5/21

Pre-Calculus

1/31/2007

Chapter 6 ReviewDue 5/21

Chapter 6 ReviewDue 5/21

# 2 – 22 even# 53 – 59 odd# 62 – 70 even

# 74, 81, 86

(p. 537)

Page 2: Chapter 6 Review Due 5/21

Pre-Calculus

1/31/2007

Vector FormulasVector Formulas

v 1

u or vv v

v cos v sin

gu v

cosu v

v 2

u vproj u v

v

g

Unit Vectors:Unit Vectors:

Horizontal/Verticalcomponents:

Horizontal/Verticalcomponents:

Angle between Vectors:Angle between Vectors:

Projections:Projections:

Page 3: Chapter 6 Review Due 5/21

Pre-Calculus

1/31/2007

6.1 Vectors in a Plane

Day # 1

6.1 Vectors in a Plane

Day # 1

Page 4: Chapter 6 Review Due 5/21

Pre-Calculus

1/31/2007

magnitude (size) direction

force acceleration velocity

RS starts at R and goes to S

v = 1 2v , v

Starts at (0, 0) and goes to (x, y)

Page 5: Chapter 6 Review Due 5/21

Pre-Calculus

1/31/2007

A

B

v

7 3 4

1 ( 4) 3

AB

2 2d 3 4 25 5

v = 3,4

equivalent

Page 6: Chapter 6 Review Due 5/21

Pre-Calculus

1/31/2007

5 2,( 1) 33,2

PQ vuuur

2 23 2 9 4 13

2

slope3

P

Q

Page 7: Chapter 6 Review Due 5/21

Pre-Calculus

1/31/2007

Vector addition

Vector multiplication (multiplying a vector by a scalar or real number)

1 2 1 2 1 1 2 2u ,u v , v u v ,u v

sum

1 2 1 2ku k u ,u ku ,ku

initial point terminal

point

parallelogram law

Page 8: Chapter 6 Review Due 5/21

Pre-Calculus

1/31/2007

unit vector

unit vector

v 1

u or vv v

direction v

Page 9: Chapter 6 Review Due 5/21

Pre-Calculus

1/31/2007

direction angle

v cos v sin

Page 10: Chapter 6 Review Due 5/21

Pre-Calculus

1/31/2007

25o

o o70 cos 25 ,70 sin 25

250 63.44,433.01 29.38

2 2v w ( 186.56) (462.59) 498.79mph

462.59

tan186.56

o65o25

63.44,29.58

186.56,462.59

o111.96

Page 11: Chapter 6 Review Due 5/21

Pre-Calculus

1/31/2007

6.2 Dot Product of Vectors

Day # 1

6.2 Dot Product of Vectors

Day # 1

Page 12: Chapter 6 Review Due 5/21

Pre-Calculus

1/31/2007

dot product

work done

vectors scalar (real number)

g 1 1 2 2u v u v u v

g gu v v u g 2u u u g0 u 0 u (v w ) u v u wg g g

g g g(cu) v u (cv) c(u v) g g g(u v) w u w v w +

Page 13: Chapter 6 Review Due 5/21

Pre-Calculus

1/31/2007

gu v

cosu v

Theorem: Angles Between VectorsTheorem: Angles Between Vectors

If θ is the angle between the nonzero vectors u and v, then

g1 u vcos

u v

Page 14: Chapter 6 Review Due 5/21

Pre-Calculus

1/31/2007

Proving Vectors are OrthagonalProving Vectors are Orthagonal

u 3,2

v 8,12

Prove that the vectors are orthagonal:

g ou v u v cos 90 0

gu v 0

Page 15: Chapter 6 Review Due 5/21

Pre-Calculus

1/31/2007

Proving Vectors are ParallelProving Vectors are Parallel

u 3,2

v 6, 4

Prove that the vectors are parallel:

The vectors u and v are parallel if and only if:

u = kvfor some constant k

Page 16: Chapter 6 Review Due 5/21

Pre-Calculus

1/31/2007

Proving Vectors are NeitherProving Vectors are Neither

u 3,2

v 4, 6

Show that the vectors are neither:

If 2 vectors u and v are not orthagonal or parallel:then they are NEITHER

Page 17: Chapter 6 Review Due 5/21

Pre-Calculus

1/31/2007

vector projection

vproj u

v 2

u vproj u v

vg

vu proj u

Page 18: Chapter 6 Review Due 5/21

Pre-Calculus

1/31/2007

Unit CircleUnit Circle

Page 19: Chapter 6 Review Due 5/21

Pre-Calculus

1/31/2007

6.4 Polar Equations

Day # 1

6.4 Polar Equations

Day # 1

Page 20: Chapter 6 Review Due 5/21

Pre-Calculus

1/31/2007

polar coordinate system pole polar axis

polar coordinates ( r, θ )

directed distance

directed angle polar axisline OP

O polar axis

P

Page 21: Chapter 6 Review Due 5/21

Pre-Calculus

1/31/2007

3, 2 n

4

53, 2 n

4

2,75 360n

2,255 360n

Page 22: Chapter 6 Review Due 5/21

Pre-Calculus

1/31/2007

Polar Cartesian (rectangular)pole origin polar axis

positive x – axis

y

rP(r, θ)

y = r sin θ

x = r cos θ

Page 23: Chapter 6 Review Due 5/21

Pre-Calculus

1/31/2007

y

tanx

1 ytan

x

2 2 2r x y 2 2r x y

so

soy

rP(x, y)

Page 24: Chapter 6 Review Due 5/21

Pre-Calculus

1/31/2007

Helpful HintsHelpful Hints

Polar to Rectangular1. multiply cos or sin

by r so you can convert to x or y

2. r2 = x2 + y2

3. re-write sec and csc as

4. complete the square as necessary

Rectangular to Polar1. replace x and y with

rcos and rsin2. when given a “squared

binomial”, multiply it out3. x2 + y2 = r2

1 1

andcos sin

(x – a)2 + (y – b)2 = c2

Where the center of the circle is (a, b) and the radius is c

(x – a)2 + (y – b)2 = c2

Where the center of the circle is (a, b) and the radius is c

Page 25: Chapter 6 Review Due 5/21

Pre-Calculus

1/31/2007

6.5 Graphs of Polar Equations

Day # 1

6.5 Graphs of Polar Equations

Day # 1

Page 26: Chapter 6 Review Due 5/21

Pre-Calculus

1/31/2007

General Form:

r = a cos n θ

r = a sin n θ

Petals:

n: odd n petals

n: even 2n petals

n: odd n: even

cos one petal on pos. x-axis

sin one petal on half of y-axis

cos petals on each side of each axis

sin no petals on axes

Page 27: Chapter 6 Review Due 5/21

Pre-Calculus

1/31/2007

General Form:

r = a + b sin θ

r = a + b cos θ

Symmetry:

sin: about y – axis

cos: about x – axis

when , there is an “inner loop” (#5)a

1b

when , it touches the origin; “cardioid” (#6)a

1b

when , it’s called a “dimpled limacon” (#7) a

1 2b

when , it is a “convex limacon” (#8)a

2b

Page 28: Chapter 6 Review Due 5/21

Pre-Calculus

1/31/2007

We analyze polar graphs much the same way we do graphs of rectangular equations. The domain is the set of possible inputs for . The range is the set of outputs for r. The domain and range can be read from the “trace” or “table” features on your calculator. We are also interested in the maximum value of . This is the maximum distance from the pole. This can be found using trace, or by knowing the range of the function.

Symmetry can be about the x-axis, y-axis, or origin, just as it was in rectangular equations.

Continuity, boundedness, and asymptotes are analyzed the same way they were for rectangular equations.

ANALYZING POLAR GRAPHSANALYZING POLAR GRAPHS

r

Page 29: Chapter 6 Review Due 5/21

Pre-Calculus

1/31/2007

What happens in either type of equation when the constants are negative? Draw sketches to show the results.

Rose Curve when “a” is negative(“n” can’t be negative, by definition)

Rose Curve when “a” is negative(“n” can’t be negative, by definition)

• if n is even, picture doesn’t change…just the order that the points are plotted changes

•if n is odd, the graph is reflected over the x – axis

r asin(n ) r asin(n ) r 2sin(3 )

r 2sin(3 )

Page 30: Chapter 6 Review Due 5/21

Pre-Calculus

1/31/2007

What happens in either type of equation when the constants are negative? Draw sketches to show the results.

Rose Curve when “a” is negative(“n” can’t be negative, by definition)

Rose Curve when “a” is negative(“n” can’t be negative, by definition)

• if n is even, picture doesn’t change…just the order that the points are plotted changes

•if n is odd, the graph is reflected over the y – axis

r acos(n ) r acos(n ) r 2cos(3 )

r 2cos(3 )

Page 31: Chapter 6 Review Due 5/21

Pre-Calculus

1/31/2007

What happens in either type of equation when the constants are negative? Draw sketches to show the results.

Limacon Curve when “b” is negative (minus in front of the b)(“a” can’t be negative, by definition)

• when r = a + bsinθ, the majority of the curve is around the positive y – axis.

•when r = a – bsinθ, the curve flips over the x – axis.

r a bsin r a bsin r 1 2sin

r 1 2sin

Page 32: Chapter 6 Review Due 5/21

Pre-Calculus

1/31/2007

What happens in either type of equation when the constants are negative? Draw sketches to show the results.

Limacon Curve when “b” is negative (minus in front of the b)(“a” can’t be negative, by definition)

• when r = a + bcos θ, the majority of the curve is around the positive x – axis.

•when r = a – bcos θ, the curve flips over the y – axis.

r a bcos r a bcos r 1 2cos

r 1 2cos