in chapter 1, we talked about parametric equations

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In chapter 1, we talked about parametric equations. Parametric equations can be used to describe motion that is not a function. x f t y gt If f and g have derivatives at t, then the parametrized curve also has a derivative at t.

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In chapter 1, we talked about parametric equations. Parametric equations can be used to describe motion that is not a function. If f and g have derivatives at t , then the parametrized curve also has a derivative at t. The formula for finding the slope of a parametrized curve is:. - PowerPoint PPT Presentation

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Page 1: In chapter 1, we talked about  parametric  equations

In chapter 1, we talked about parametric equations.Parametric equations can be used to describe motion that is not a function.

x f t y g t

If f and g have derivatives at t, then the parametrized curve also has a derivative at t.

Page 2: In chapter 1, we talked about  parametric  equations

The formula for finding the slope of a parametrized curve is:

dy

dy dtdxdxdt

This makes sense if we think about canceling dt.

Page 3: In chapter 1, we talked about  parametric  equations

The formula for finding the slope of a parametrized curve is:

dy

dy dtdxdxdt

We assume that the denominator is not zero.

Page 4: In chapter 1, we talked about  parametric  equations

To find the second derivative of a parametrized curve, we find the derivative of the first derivative:

dydtdxdt

2

2

d y

dx dy

dx

1. Find the first derivative (dy/dx).2. Find the derivative of dy/dx with respect to t.

3. Divide by dx/dt.

Page 5: In chapter 1, we talked about  parametric  equations

22 3

2Find as a function of if and .

d yt x t t y t t

dx

Page 6: In chapter 1, we talked about  parametric  equations

22 3

2Find as a function of if and .

d yt x t t y t t

dx

1. Find the first derivative (dy/dx).

dy

dy dtydxdxdt

21 3

1 2

t

t

Page 7: In chapter 1, we talked about  parametric  equations

2. Find the derivative of dy/dx with respect to t.

21 3

1 2

dy d t

dt dt t

2

2

2 6 6

1 2

t t

t

Quotient Rule

Page 8: In chapter 1, we talked about  parametric  equations

3. Divide by dx/dt.

2

2

d y

dx

dxdt

dydt

2

2

2 6 6

1 2

1 2

t t

t

t

2

3

2 6 6

1 2

t t

t

Page 9: In chapter 1, we talked about  parametric  equations

Ldx

dt

dy

dtdt

a

b F

HGIKJ FHG

IKJz 2 2

The equation for the length of a parametrized curve is similar to our previous “length of curve” equation:

Page 10: In chapter 1, we talked about  parametric  equations

1. Revolution about the -axis 0x y 2 2

2b

a

dx dyS y dt

dt dt

2. Revolution about the -axis 0y x

2 2

2b

a

dx dyS x dt

dt dt

Page 11: In chapter 1, we talked about  parametric  equations

This curve is:

sin 2

2cos 5

x t t t

y t t t

Page 12: In chapter 1, we talked about  parametric  equations

Warning:

Only some of this is review.

Page 13: In chapter 1, we talked about  parametric  equations

Quantities that we measure that have magnitude but not direction are called scalars.

Quantities such as force, displacement or velocity that have direction as well as magnitude are represented by directed line segments.

A

B

initialpoint

terminalpoint

AB

The length is AB

Page 14: In chapter 1, we talked about  parametric  equations

A

B

initialpoint

terminalpoint

AB

A vector is represented by a directed line segment.

Vectors are equal if they have the same length and direction (same slope).

Page 15: In chapter 1, we talked about  parametric  equations

A vector is in standard position if the initial point is at the origin.

x

y

1 2,v v

The component form of this vector is: 1 2,v vv

Page 16: In chapter 1, we talked about  parametric  equations

A vector is in standard position if the initial point is at the origin.

x

y

1 2,v v

The component form of this vector is: 1 2,v vv

The magnitude (length) of 1 2,v vv is:2 2

1 2v v v

Page 17: In chapter 1, we talked about  parametric  equations

P

Q

(-3,4)

(-5,2)

The component form of

PQ

is: 2, 2 v

v(-2,-2) 2 2

2 2 v

8 2 2

Page 18: In chapter 1, we talked about  parametric  equations

If 1v Then v is a unit vector.

0,0 is the zero vector and has no direction.

Page 19: In chapter 1, we talked about  parametric  equations

Vector Operations:

1 2 1 2Let , , , , a scalar (real number).u u v v k u v

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

(Add the components.)

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

(Subtract the components.)

Page 20: In chapter 1, we talked about  parametric  equations

Vector Operations:

Scalar Multiplication:1 2,k ku kuu

Negative (opposite): 1 21 ,u u u u

Page 21: In chapter 1, we talked about  parametric  equations

v

vu

u

u+vu + v is the resultant vector.

(Parallelogram law of addition)

Page 22: In chapter 1, we talked about  parametric  equations

The angle between two vectors is given by:

1 1 1 2 2cosu v u v

u v

This comes from the law of cosines.See page 524 for the proof if you are interested.

Page 23: In chapter 1, we talked about  parametric  equations

The dot product (also called inner product) is defined as:

1 1 2 2cos u v u v u v u v

Read “u dot v”

This could be substituted in the formula for the angle between vectors to give:

1cos

u v

u v

Page 24: In chapter 1, we talked about  parametric  equations

Application: Example 7

A Boeing 727 airplane, flying due east at 500mph in still air, encounters a 70-mph tail wind acting in the direction of 60o north of east. The airplane holds its compass heading due east but, because of the wind, acquires a new ground speed and direction. What are they?

N

E

Page 25: In chapter 1, we talked about  parametric  equations

Application: Example 7

A Boeing 727 airplane, flying due east at 500mph in still air, encounters a 70-mph tail wind acting in the direction of 60o north of east. The airplane holds its compass heading due east but, because of the wind, acquires a new ground speed and direction. What are they?

N

Eu

Page 26: In chapter 1, we talked about  parametric  equations

Application: Example 7

A Boeing 727 airplane, flying due east at 500mph in still air, encounters a 70-mph tail wind acting in the direction of 60o north of east. The airplane holds its compass heading due east but, because of the wind, acquires a new ground speed and direction. What are they?

N

E

v

u

60o

Page 27: In chapter 1, we talked about  parametric  equations

Application: Example 7

A Boeing 727 airplane, flying due east at 500mph in still air, encounters a 70-mph tail wind acting in the direction of 60o north of east. The airplane holds its compass heading due east but, because of the wind, acquires a new ground speed and direction. What are they?

N

E

v

u

We need to find the magnitude and direction of the resultant vector u + v.

u+v

Page 28: In chapter 1, we talked about  parametric  equations

N

E

v

u

The component forms of u and v are:

u+v

500,0u

70cos60 ,70sin 60v

500

70

35,35 3v

Therefore: 535,35 3 u v

538.4 22535 35 3 u v

and: 1 35 3tan

535 6.5

Page 29: In chapter 1, we talked about  parametric  equations

N

E

The new ground speed of the airplane is about 538.4 mph, and its new direction is about 6.5o north of east.

538.4

6.5o