chapter 1

72
Chapter 1 The Study of Motion

Upload: wren

Post on 06-Jan-2016

18 views

Category:

Documents


0 download

DESCRIPTION

Chapter 1. The Study of Motion. Units. We can classify almost all quantities in terms of the fundamental physical quantities : LengthL MassM TimeT For example: Speed has units L/T (miles per hour). Units , cont’d. SI (Système International) Units: MKS: L = meters (m) - PowerPoint PPT Presentation

TRANSCRIPT

Page 1: Chapter 1

Chapter 1

The Study of Motion

Page 2: Chapter 1

2

Units

We can classify almost all quantities in terms of the fundamental physical quantities: Length L Mass M Time T

For example: Speed has units L/T (miles per hour)

Page 3: Chapter 1

3

Units, cont’d

SI (Système International) Units: MKS:

L = meters (m) M = kilograms (kg) T = seconds (s)

CGS: L = centimeters (cm) M = grams (g or gm) T = seconds (s)

Page 4: Chapter 1

4

Units, cont’d

British (or Imperial) Units: L = feet (ft) M = slugs or pound-mass (lbm) T = seconds (s)

We will use mostly SI but we need to know how to convert back and forth.

Page 5: Chapter 1

5

Units, cont’d

The back of your book provides numerous conversions. Here are some:

1 inch = 2.54 cm 1 m = 3.281 ft 1 mile = 5280 ft 1 km = 0.621 mi

Page 6: Chapter 1

6

Units, cont’d

We can use these to convert a compound unit:

mi 5280 ft 1 m 1 h 1min70

h 1 mi 3.281 ft 60min 60s

m31.2

s

Page 7: Chapter 1

7

Converting units

Look at your original units. Determine the units you want to have. Find the conversion you need. Write the conversion as a fraction that

replaces the original unit with the new unit.

Page 8: Chapter 1

8

ExampleProblem 1.1

A yacht is 20 m long. Express this length in feet.

Page 9: Chapter 1

9

Example

A yacht is 20 m long. Express this length in feet.

3.281 ft20 m 20 3.281 ft

1 m65.62 ft

66 ft

ANSWER:

Page 10: Chapter 1

10

Example

How many liters are in a five gallon bucket? There are four quarts in a gallon.

Page 11: Chapter 1

11

Example

How many liters are in a five gallon bucket? There are four quarts in a gallon.

4 qt 0.95 L5 gal 5 4 0.95 L

1 gal 1 qt

19 L

ANSWER:

Page 12: Chapter 1

12

Metric prefixes

Sometimes a unit is too small or too big for a particular measurement.

To overcome this, we use a prefix.

Page 13: Chapter 1

13

Metric prefixes, cont’d

Power of 10 Prefix Symbol1015 peta P1012 tera T109 giga G106 mega M103 kilo k10-2 centi c10-3 milli m10-6 micro 10-9 nano n10-12 pico p10-15 femto f

Page 14: Chapter 1

14

Metric prefixes, cont’d

Some examples: 1 centimeter= 10-2 meters = 0.01 m 1 millimeter = 10-3 meters = 0.001 m 1 kilogram = 103 grams = 1,000 g

Page 15: Chapter 1

15

Frequency and period

We define frequency as the number of events per a given amount of time.

When an event occurs repeatedly, we say that the event is periodic.

The amount of time between events is the period.

Page 16: Chapter 1

16

Frequency and period, cont’d

The symbols we use to represent frequency are period are: frequency: f period: T

They are related by

1 1period or

frequencyT

f

Page 17: Chapter 1

17

Frequency and period, cont’d

The standard unit of frequency is the Hertz (Hz). It is equivalent to 1 cycle per second.

Page 18: Chapter 1

18

ExampleExample 1.1

A mechanical stopwatch uses a balance wheel that rotates back and forth 10 times in 2 seconds. What is the frequency of the balance wheel?

Page 19: Chapter 1

19

ExampleExample 1.1

A mechanical stopwatch uses a balance wheel that rotates back and forth 10 times in 2 seconds. What is the frequency of the balance wheel?

10 cycles5 Hz.

2 sf

ANSWER:

Page 20: Chapter 1

20

Speed

Speed is the rate of change of distance from a reference point.

It is the rate of movement. It equals the distance something travels

divided by the elapsed time.

total distanceaverage speed

total elapsed time

Page 21: Chapter 1

21

Speed, cont’d

In mathematical notation,

So we can write speed as

final initial

final initial

total distance

total elapsed time

f i

f i

d d d d

t t t t

final initial

final initial

f i

f i

d dd dv

t t t t

d

t

Page 22: Chapter 1

22

Speed, cont’d

The symbol is the Greek letter delta and represents the change in.

As the time interval becomes shorter and shorter, we approach the instantaneous speed.

Page 23: Chapter 1

23

Speed, cont’d

If we know the average speed and how long something travels at that speed, we can find the distance it travels:

d vt

Page 24: Chapter 1

24

Speed, cont’d

We say that the distance is proportional to the elapsed time:

Using the speed gives us an equality, i.e., an equal sign, so we call v the proportionality constant.

d t

Page 25: Chapter 1

25

Speed, cont’d

Note that speed is relative. It depends upon what you are measuring your

speed against. Consider someone running on a ship.

Page 26: Chapter 1

26

Speed, cont’d

If you are on the boat, she is moving at

as seen on ship 8 mphv

Page 27: Chapter 1

27

Speed, cont’d

If you are on the dock, she is moving at

as seen on dock 8 mph 20 mph

28 mph

v

Page 28: Chapter 1

28

Example

When lightning strikes, you see the flash almost immediately but the thunder typically lags behind. The speed of light is 3 × 108 m/s and the speed of sound is about 345 m/s. If the lightning flash is one mile away, how long does it take the light and sound to reach you?

Page 29: Chapter 1

29

ANSWER:

For the thunder:

For the flash:

Example

1600 m

345 m/s

4.6 s

soundsound

sound

dt

v

8

1600 m

3 10 m/s

0.0000053 s

lightlight

light

dt

v

Page 30: Chapter 1

30

Velocity

Velocity is the speed in a particular direction. It tells us not only “how fast” (like speed) but

also how fast in “what direction.”

Page 31: Chapter 1

31

Velocity, cont’d

In common language, we don’t distinguish between the two. This sets you up for confusion in a physics

class. During a weather report, you might be given

the wind-speed is 15 mph from the west.

Page 32: Chapter 1

32

Velocity, cont’d

The speed of the wind is 15 mph. The wind is blowing in a direction from the

west to the east. So you are actually given the wind velocity.

Page 33: Chapter 1

33

Vector addition

Quantities that convey a magnitude and a direction, like velocity, are called vectors.

We represent vectors by an arrow. The length indicates

the magnitude.

Page 34: Chapter 1

34

Vector addition, cont’d

Consider again someone running on a ship. If in the

same directions, the vectors add.

Page 35: Chapter 1

35

Vector addition, cont’d

Consider again someone running on a ship. If in the

opposite directions, the vectors subtract.

Page 36: Chapter 1

36

Vector addition, cont’d

What if the vectors are in different directions?

Page 37: Chapter 1

37

Vector addition, cont’d

The resulting velocity of the bird (from the bird’s velocity and the wind) is a combination of the magnitude and direction of each velocity.

Page 38: Chapter 1

38

Vector addition, cont’d

We can find the resulting magnitude of the Pythagorean theorem.

2 2 2

2 2

c a b

c a b

b

ac

Page 39: Chapter 1

39

Vector addition, cont’d

Let’s find the net speed of the bird? (Why didn’t I say net velocity?)

10

8

6

2 26 8 100

10

Page 40: Chapter 1

40

Vector addition, cont’d

Here are more examples, illustrating that even if the bird flies with the same velocity, the effect of the wind can be constructive or destructive.

Page 41: Chapter 1

41

Acceleration

Acceleration is the change in velocity divided by the elapsed time.

It measures the rate of change of velocity. Mathematically,

va

t

Page 42: Chapter 1

42

Acceleration, cont’d

The units are

In SI units, we might use m/s2. For cars, we might see mph/s.

2

/L T L La

T T T T

Page 43: Chapter 1

43

Acceleration, cont’d

A common way to express acceleration is in terms of g’s.

One g is the acceleration an object experiences as it falls near the Earth’s surface: g = 9.8 m/s2. So if you experience 2g during a collision,

your acceleration was 19.6 m/s2.

Page 44: Chapter 1

44

Acceleration, cont’d

There is an important point to realize about acceleration:

It is the change in velocity.

Page 45: Chapter 1

45

Acceleration, cont’d

Since velocity is speed and direction, there are three ways it can change: change in speed, change in direction, or change in both speed & direction.

The change in direction is an important case often misunderstood.

Page 46: Chapter 1

46

Acceleration, cont’d

If you drive through a curve with the cruise control set to 65 mph, you are accelerating. Not because your speed changes. But because your direction is changing.

There must be an acceleration because items on your dash go sliding around.

More on this in chapter 2.

Page 47: Chapter 1

47

ExampleExample 1.3

A car accelerates from 20 to 25 m/s in 4 seconds as it passes a truck. What is its acceleration?

Page 48: Chapter 1

48

ANSWER:

The problem gives us

The acceleration is:

ExampleExample 1.3

20 m/s

25 m/s

4 s

i

f

v

v

t

225 m/s 20 m/s1.25 m/s

4 s

f iv vva

t t

Page 49: Chapter 1

49

CHECK:

Does this make sense?

The car needs to increase its speed 5 m/s in 4 seconds.

If it increased 1 m/s every second, it would only reach 24 m/s.

So we should expect an answer slightly more than 1 m/s every second.

ExampleExample 1.3

Page 50: Chapter 1

50

ExampleExample 1.4

After a race, a runner takes 5 seconds to come to a stop from a speed of 9 m/s. Find her acceleration.

Page 51: Chapter 1

51

ANSWER:

The problem gives us

The acceleration is:

ExampleExample 1.3

9 m/s

0 m/s

5 s

i

f

v

v

t

20 m/s 9 m/s1.8 m/s

5 s

f iv vva

t t

Page 52: Chapter 1

52

CHECK:

Does this make sense?

If she was traveling at 10 m/s, reducing her speed 2 m/s every second would stop her in 5 seconds.

What’s up with the minus sign?

ExampleExample 1.3

Page 53: Chapter 1

53

Centripetal acceleration

Remember that acceleration can result from a change in the velocity’s direction.

Imagine a car rounding a curve. The car’s velocity must keep changing toward

the center of the curve in order to stay on the road.

Page 54: Chapter 1

54

Centripetal acceleration

Remember that acceleration can result from a change in the velocity’s direction.

Imagine a car rounding a curve. The car’s velocity

must keep changing toward the center of the curve in order to stay on the road.

Page 55: Chapter 1

55

Centripetal acceleration, cont’d

So there is an acceleration toward the center of the curve.

Centripetal acceleration is the acceleration associated with an object moving in a circular path. Centripetal means “center-seeking.”

Page 56: Chapter 1

56

Centripetal acceleration, cont’d

For an object traveling with speed v on a circle of radius r , then its centripetal acceleration is

2va

r

Page 57: Chapter 1

57

Centripetal acceleration, cont’d

Note that the centripetal acceleration is: proportional to the speed-squared

inversely proportional to the radius

2a v

1a

r

Page 58: Chapter 1

58

ExampleExample 1.5

Let’s estimate the acceleration of a car as it goes around a curve. The radius of a segment of a typical cloverleaf is 20 meters, and a car might take the curve with a constant speed of 10 m/s.

Page 59: Chapter 1

59

ANSWER:

The problem gives us

The acceleration is:

ExampleExample 1.5

20 m

10 m/s

r

v

22

2 22

10 m/s

20 m

100 m /s5 m/s

20 m

va

r

Page 60: Chapter 1

60

ExampleProblem 1.18

An insect sits on the edge of a spinning record that has a radius of 0.15 m. The insect’s speed is about 0.5 m/s when the record is turning at 33-1/3 rpm. What is the insect’s acceleration?

Page 61: Chapter 1

61

ANSWER:

The problem gives us

The acceleration is:

ExampleProblem 1.18

0.15 m

0.5 m/s

r

v

22

2 22

0.5 m/s

0.15 m

0.25 m /s1.7 m/s

0.15 m

va

r

Page 62: Chapter 1

62

Simple types of motion— zero velocity The simplest type of motion is obviously no

motion. The object has no velocity. So it never moves. The position of the object, relative to some

reference, is constant.

Page 63: Chapter 1

63

Simple types of motion— constant velocity The next simplest type of motion is uniform

motion. In physics, uniform means constant.

The object’s velocity does not change. So its position, relative to some reference, is

proportional to time.

Page 64: Chapter 1

64

Simple types of motion— constant velocity, cont’d

If we plot the object’s distance versus time, we get this graph. Notice that if we double the time interval, then

we double the object’s distance.

Page 65: Chapter 1

65

Simple types of motion— constant velocity, cont’d

The slope of the line gives us the speed.

Page 66: Chapter 1

66

Simple types of motion— constant velocity, cont’d

If an object moves faster, then the line has a larger speed.

So the graph has a steeper slope.

Page 67: Chapter 1

67

Simple types of motion— constant acceleration The next type of motion is uniform

acceleration in a straight line. The acceleration does not change. So the object’s speed is proportional to the

elapsed time.

speed acceleration time

v at

Page 68: Chapter 1

68

Simple types of motion— constant acceleration, cont’d

A common example is free fall. Free fall means gravity is the only thing

changing an object’s motion. The speed is:

2(9.8 m/s )

mph(22 )

s

v t

v t

Page 69: Chapter 1

69

Simple types of motion— constant acceleration, cont’d

If we plot speed versus time, the slope is the acceleration:

va

t

Page 70: Chapter 1

70

Simple types of motion— constant acceleration, cont’d

For an object starting from rest, v = 0, then the average speed is

12

0average speed

2

at

at

Page 71: Chapter 1

71

Simple types of motion— constant acceleration, cont’d

The distance is the average speed multiplied by the elapsed time:

12

212

d average speed t

at t

at

Page 72: Chapter 1

72

Simple types of motion— constant acceleration, cont’d

If we graph the distance versus time, the curve is not a straight line. The distance is

proportional to the square of the time.

2d t