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Chapter 2 Kinematics in One Dimension

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Page 1: Chapter 2 Kinematics in One Dimension. Kinematics –Kinema is Greek for “motion” –Kinematics → Describing motion Kinematics describes motion in terms of

Chapter 2

Kinematics

in One Dimension

Page 2: Chapter 2 Kinematics in One Dimension. Kinematics –Kinema is Greek for “motion” –Kinematics → Describing motion Kinematics describes motion in terms of

• Kinematics– Kinema is Greek for “motion”– Kinematics → Describing motion

• Kinematics describes motion in terms of – position– displacement– velocity (average and instantaneous)– acceleration

• Dynamics– Describing how interactions can change motion

• Mechanics– Kinematics and dynamics.

Page 3: Chapter 2 Kinematics in One Dimension. Kinematics –Kinema is Greek for “motion” –Kinematics → Describing motion Kinematics describes motion in terms of

For one-dimensional motion, plus (+) and minus (-) are used to specify the vector direction. Plus (+) is at 0° along the positive x axis and minus (-) is at 180° along the negative x axis.

Position x is the location of the object

initial position final position

positive xdirection

x axis at 0°

Page 4: Chapter 2 Kinematics in One Dimension. Kinematics –Kinema is Greek for “motion” –Kinematics → Describing motion Kinematics describes motion in terms of

position initial ox

position final x

ntdisplaceme oxxx

Change Δ always means (final value) – (initial value)

Displacement Δx is the change in position

x= 0

Page 5: Chapter 2 Kinematics in One Dimension. Kinematics –Kinema is Greek for “motion” –Kinematics → Describing motion Kinematics describes motion in terms of

2 mo x

7.0 mx

5 m x

Example: Displacement in the positive x direction

initial Displacement is the change

final

7 m 2 m 5 mo x x x

ntdisplaceme oxxx

Displacement is +5 m

Page 6: Chapter 2 Kinematics in One Dimension. Kinematics –Kinema is Greek for “motion” –Kinematics → Describing motion Kinematics describes motion in terms of

Example: Displacement in the negative x direction

2 mx

7 mo x

5 m x

initial

Displacement is the changefinal

2 m 7 m 5 mo x x x

Displacement is - 5 m

ntdisplaceme oxxx

Page 7: Chapter 2 Kinematics in One Dimension. Kinematics –Kinema is Greek for “motion” –Kinematics → Describing motion Kinematics describes motion in terms of

Average velocity is the displacement divided by the elapsedtime.

DisplacementAverage velocity

Elapsed time

ttt o

o

xxx

v

SI units for velocity: meters per second

Velocity is the displacement in one second.

v "bar" means average

m

s

Page 8: Chapter 2 Kinematics in One Dimension. Kinematics –Kinema is Greek for “motion” –Kinematics → Describing motion Kinematics describes motion in terms of

Example 2 The World’s Fastest Jet-Engine CarAndy Green in the car ThrustSSC set a world record of 341.1 m/s in 1997. The driver makes two runs through the course, one in each direction, to adjust for wind effects. Determine the average velocity for each run.

1609 m m339.5

4.740 s st

x

v

1609 m m342.7

4.695 s st

x

v

Vector directions are shown with +/- signs.

Page 9: Chapter 2 Kinematics in One Dimension. Kinematics –Kinema is Greek for “motion” –Kinematics → Describing motion Kinematics describes motion in terms of

timeElapsed

Distance speed Average

SI units for speed: meters per second

In this course, speed will mean the magnitude of the velocity.

Ignore the textbook definition of speed

textbook definition:

m

s

Page 10: Chapter 2 Kinematics in One Dimension. Kinematics –Kinema is Greek for “motion” –Kinematics → Describing motion Kinematics describes motion in terms of

Instantaneous velocity is the average velocity for a very short time interval.

0 0lim = limt t t

x

v v

average velocity

instantaneous velocity

Average velocity is the average during some time interval.

Instantaneous velocity is the velocity at a specific moment.

Page 11: Chapter 2 Kinematics in One Dimension. Kinematics –Kinema is Greek for “motion” –Kinematics → Describing motion Kinematics describes motion in terms of

ttt o

o

vvv

a

Average acceleration is the velocity change in one second.

Velocity changeAverage acceleration

Elapsed time

"bar" means average

Page 12: Chapter 2 Kinematics in One Dimension. Kinematics –Kinema is Greek for “motion” –Kinematics → Describing motion Kinematics describes motion in terms of

Example 3 Increasing velocity: Determine the average acceleration.

0 km/ho v

260km hv

s 0ot s 29t

260 09

29 s 0 s so

o

km km kmh h h

t t

v va

260km hv

s 29t0 km/ho v

s 0ot

v

a

v and a are in the same direction so v increases

Page 13: Chapter 2 Kinematics in One Dimension. Kinematics –Kinema is Greek for “motion” –Kinematics → Describing motion Kinematics describes motion in terms of

Acceleration is the velocity change each second.

kmVelocity change is +9 each second.

h

v

a

v and a are in the same direction so v increases

Page 14: Chapter 2 Kinematics in One Dimension. Kinematics –Kinema is Greek for “motion” –Kinematics → Describing motion Kinematics describes motion in terms of

Acceleration is the velocity change each second

mVelocity change is -5 each second.

s

v

a

v and a are in opposite directions so v decreases

Page 15: Chapter 2 Kinematics in One Dimension. Kinematics –Kinema is Greek for “motion” –Kinematics → Describing motion Kinematics describes motion in terms of

8 m mVelocity = Slope 4

2 s s

x

t

Graphical representation of kinematic quantities

Position graph with a constant slope

Page 16: Chapter 2 Kinematics in One Dimension. Kinematics –Kinema is Greek for “motion” –Kinematics → Describing motion Kinematics describes motion in terms of

Position graph with three different slopes

2m

vs

0m

vs

1m

vs

Velocity = Slope

Page 17: Chapter 2 Kinematics in One Dimension. Kinematics –Kinema is Greek for “motion” –Kinematics → Describing motion Kinematics describes motion in terms of

Position graph with a variable slope

Velocity = Slope

x

t

265.2

5

x m mv

t s s

Page 18: Chapter 2 Kinematics in One Dimension. Kinematics –Kinema is Greek for “motion” –Kinematics → Describing motion Kinematics describes motion in terms of

2

m12 msAcceleration = Slope 62 s s

v

t

Velocity graph with a constant slope

Page 19: Chapter 2 Kinematics in One Dimension. Kinematics –Kinema is Greek for “motion” –Kinematics → Describing motion Kinematics describes motion in terms of

Your success in physics critically depends on your ability to correctly distinguish and correctly use technical terms as the terms are defined in physics.

velocity and acceleration are different physical quantities with different units

velocity is position change each second

acceleration is velocity change each second

velocity is different from velocity change

Page 20: Chapter 2 Kinematics in One Dimension. Kinematics –Kinema is Greek for “motion” –Kinematics → Describing motion Kinematics describes motion in terms of

1. position (at time t), x

2. initial velocity (at time t=0), vo

3. acceleration (constant), a

4. final velocity (at time t), v

5. final time, t

The kinematic equations relate these 5 variables for situations where the acceleration is constant and allow us to solve for two of these quantities that are unknown.

Five kinematic variables

Page 21: Chapter 2 Kinematics in One Dimension. Kinematics –Kinema is Greek for “motion” –Kinematics → Describing motion Kinematics describes motion in terms of

Five kinematic equations for constant acceleration cases

tvvx o 21

221 attvx o

atvv o

axvv o 222

x vt

Position equations Velocity equations

Use these equations to solve for any 2 missing variables.

You need to know 3 of the 5 variables to find the missing 2 !

Obtained from the other equations by eliminating t.

Derivation of the kinematic equations is shown at the end of the slides.

Page 22: Chapter 2 Kinematics in One Dimension. Kinematics –Kinema is Greek for “motion” –Kinematics → Describing motion Kinematics describes motion in terms of

Success Strategy [ Very important steps !! ]

1. Make a drawing.2. Draw direction arrows. (displacement, velocity, acceleration)3. Label the positive (+) and negative (-) directions.4. Label all know quantities. 5. Use a table to organize known values with correct units. 6. Make sure you have three of the five kinematic quantities.7. Select the appropriate equations and solve.

There may be two possible answers because quadratic equations have 2 roots.

For multi-segmented motion, remember that the final velocity of one segment is the initial velocity for the next segment.

Page 23: Chapter 2 Kinematics in One Dimension. Kinematics –Kinema is Greek for “motion” –Kinematics → Describing motion Kinematics describes motion in terms of

Example:

Find the final position xv

a same directions

so v increases

x a v vo t

m s

? ? 8s

2

m

sm

s

m

s

22m

s 6

m

s

Page 24: Chapter 2 Kinematics in One Dimension. Kinematics –Kinema is Greek for “motion” –Kinematics → Describing motion Kinematics describes motion in terms of

212

212 2

2

6 8 s 2 8 s

112 m

6 2 8 s

m22

s

o

o

x v t at

m mx

s s

x

m mv v at

s s

v

x a v vo t

m s

? ? 8s

2

m

sm

s

m

s

22m

s 6

m

s

Page 25: Chapter 2 Kinematics in One Dimension. Kinematics –Kinema is Greek for “motion” –Kinematics → Describing motion Kinematics describes motion in terms of

Example 6 Airplane take-off

Find the final position x

??x

v

a

same directions so v increases

x a v vo t

m s

? 0 ?

2

m

sm

s

m

s

231m

s 62

m

s

Page 26: Chapter 2 Kinematics in One Dimension. Kinematics –Kinema is Greek for “motion” –Kinematics → Describing motion Kinematics describes motion in terms of

0

2

221 12 2 2

m62 0 31

s

2

m0 2 31 2 62

so

v v at

m mt

s s

t s

mx v t at s s m

s

Example 6 Airplane take-off

x a v vo t

m s

? 0 ?

2

m

sm

s

m

s

231m

s 62

m

s

Page 27: Chapter 2 Kinematics in One Dimension. Kinematics –Kinema is Greek for “motion” –Kinematics → Describing motion Kinematics describes motion in terms of

In the absence of air resistance, all bodies at the same location above the Earth fall vertically with the same acceleration. If the distance of the fall is small compared to the radius of the Earth, then the acceleration remains constant throughout the motion.

This idealized motion is called free-fall and the accelerationof a freely falling body is called the acceleration due to gravity. The direction of this acceleration is downward.

29.8m

gs

The magnitude of the acceleration is called "g".

Free fall -- motion only influenced by gravity

Page 28: Chapter 2 Kinematics in One Dimension. Kinematics –Kinema is Greek for “motion” –Kinematics → Describing motion Kinematics describes motion in terms of

2

2

9.8

9.8

mg

sm

as

downward

y axis positive upwardnegative downward

a

y

air resistance influencesfalling

no air (vacuum)(not vacuum cleaner)

air

v

v

Page 29: Chapter 2 Kinematics in One Dimension. Kinematics –Kinema is Greek for “motion” –Kinematics → Describing motion Kinematics describes motion in terms of

A stone is dropped from the top of a tall building. What is the displacement y of the stone after 3 s of free fall?

y a v vo tm s

? -9.8 m/s2 ? 0 m/s 3 s

2

m

sm

s

m

s

212

212 2

0 3 s 9.8 3 s

44.1 m

oy v t at

m my

s s

y

a

Page 30: Chapter 2 Kinematics in One Dimension. Kinematics –Kinema is Greek for “motion” –Kinematics → Describing motion Kinematics describes motion in terms of

y a v vo t

? ? ? +5 m/s ?

A coin is tossed upward with an initial speed of 5 m/s. How high does the coin go above its release point? Ignore air resistance.

Only one value is given in the wording of this problem. You are expected to add two values by thinking.

Vertical velocity always momentarily zero at the top .

v

a

Page 31: Chapter 2 Kinematics in One Dimension. Kinematics –Kinema is Greek for “motion” –Kinematics → Describing motion Kinematics describes motion in terms of

y a v vo t

? -9.8 m/s2 0 m/s +5.00 m/s ?

2

2

2

m m m0 5 9.8

s s s

m m5 9.8

s sm

5s 0.51m

9.8s

ov v at

t

t

t s

212

212 2

m m5 0.51 9.8 0.51

s s

2.55 1.27 1.28

oy v t at

y s s

y m m m

Page 32: Chapter 2 Kinematics in One Dimension. Kinematics –Kinema is Greek for “motion” –Kinematics → Describing motion Kinematics describes motion in terms of

Acceleration versus Velocity

There are three parts to the motion of the coin.

On the way up, the vector velocity is upward and the vector acceleration is downward so the velocity change is downward (v gets less upward).

At the top, the vector velocity is momentarily zero and the vector acceleration is downward so the velocity change is downward (v gets more downward).

On the way down, the vector velocity is downward and the acceleration vector is downward so the velocity change is downward (v gets more downward).

The velocity changes, but does the acceleration change?

v a

v a

0 v a

Page 33: Chapter 2 Kinematics in One Dimension. Kinematics –Kinema is Greek for “motion” –Kinematics → Describing motion Kinematics describes motion in terms of

The End

Page 34: Chapter 2 Kinematics in One Dimension. Kinematics –Kinema is Greek for “motion” –Kinematics → Describing motion Kinematics describes motion in terms of

Derivation of the kinematic equations

Page 35: Chapter 2 Kinematics in One Dimension. Kinematics –Kinema is Greek for “motion” –Kinematics → Describing motion Kinematics describes motion in terms of

o

o

tt

xxv

0ox 0ot

x vt

We assume the object is at the origin at time to = 0.

t

xv

12 ov v v Also, for constant acceleration cases

position equation

and

Deriving the kinematic equations ......

Velocity definition

multiply both sides by t

Page 36: Chapter 2 Kinematics in One Dimension. Kinematics –Kinema is Greek for “motion” –Kinematics → Describing motion Kinematics describes motion in terms of

o

o

tt

vva

t

vva o

ovvat

atvv o

0ot

Velocity equation

Acceleration definition

multiply both sides by t

Page 37: Chapter 2 Kinematics in One Dimension. Kinematics –Kinema is Greek for “motion” –Kinematics → Describing motion Kinematics describes motion in terms of

1 12 2

12

212

o

o o o

o o

o

v v at

v v v v v at

x vt

x v v at t

x v t at

another position equation