chapter 2 kinematics in one dimension

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Chapter 2 Kinematics in one Dimension January 18, 2022

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Chapter 2 Kinematics in one Dimension. September 17, 2014. Going around in circles …. . s=pathlength. A. x. A. . B. x=displacement. B. t=time interval (A,B) = 10 seconds. Seconds. . s. A. x. . B. DEFINITIONS. s=path length or total distance traveled. - PowerPoint PPT Presentation

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Page 1: Chapter 2 Kinematics in one Dimension

Chapter 2Kinematics in one Dimension

April 24, 2023

Page 2: Chapter 2 Kinematics in one Dimension

Going around in circles …

A

B

s=pathlength

Seconds

x=displacement

xA

B

t=time interval (A,B) = 10 seconds

Page 3: Chapter 2 Kinematics in one Dimension

ABs

x

DEFINITIONS

s=path length or total distance traveled.

x=displacement = NET distance traveled. Difference between final and initial position independent of the path.

t=time of the trip. Usually measured in seconds.

Page 4: Chapter 2 Kinematics in one Dimension

More Definitions

average speed = distance traveled (s) / time taken [meters/sec.]

average velocity= displacement/time [m/s]

Note: the actual SYMBOL used for distance and displacement will usually change with the context of the problem.

Page 5: Chapter 2 Kinematics in one Dimension

smsm

txvelocity /5.5

1055~

10s

-40m

m/s 41040

sm

txvelocity

Page 6: Chapter 2 Kinematics in one Dimension

In the limit -

x

t txvavg

dtdx

txLimv

In the limit of t0, velocity is the slope of the tangent to the x-t curve!

Page 7: Chapter 2 Kinematics in one Dimension

vtxx

vtxx

vdtdx

vdtdxdtdxv

if

if

t

t

x

x i

f

i

0

For v=constant

Page 8: Chapter 2 Kinematics in one Dimension

Constant Velocity

v

xi

xf

x=0

xf – xi= distance traveled = v t

MOTION DOESN’T ALWAYS START AT THE ORIGIN

Page 9: Chapter 2 Kinematics in one Dimension

Question

253 2 ttx

The position of a particle as a function of time is given by theequation below.

(a) What is the position of the particle at t=2 seconds?(b) What is the velocity of the particle at t= 2 seconds?(c) At what time is the particle’s velocity = 0?(d) Is the particle ever at the origin? When?

Page 10: Chapter 2 Kinematics in one Dimension

Conclusion

Velocity is not the same at all times. It is changing A changing velocity is called an acceleration.

dtdva

tv

tvv

a initialfinalaverage

Page 11: Chapter 2 Kinematics in one Dimension

Acceleration in Pictures

Constant Velocity

Constant Acceleration

Page 12: Chapter 2 Kinematics in one Dimension

Average Acceleration

Acceleration is the rate of change of the velocity.

Dimensions are L/t2

SI units are m/s²

Page 13: Chapter 2 Kinematics in one Dimension

Example – Constant acceleration a=1 m/s2Time (s) Velocity (m/s)

0 0

1 1

2 2

3 3

4 4

5 5

6 6

7 7

8 8

9 9

10 10

11 11

12 12

13 13

14 14

15 15

16 16

17 17

18 18

19 19

20 20

0

5

10

15

20

25

0 5 10 15 20 25

time (s)v

(m/s

)

atvv

vvatvtva

f

initialf

0

Page 14: Chapter 2 Kinematics in one Dimension

Instantaneous Acceleration

The instantaneous acceleration is the limit of the average acceleration as t approaches 0

2

20lim x x

x t

v dv d xat dt dt

Page 15: Chapter 2 Kinematics in one Dimension

Calculus

2

2

dtxd

dtdva

dtdxv

Page 16: Chapter 2 Kinematics in one Dimension

Instantaneous Acceleration -- graph The slope of the

velocity vs. time graph is the acceleration

The green line represents the instantaneous acceleration

The blue line is the average acceleration

Page 17: Chapter 2 Kinematics in one Dimension

Acceleration and Velocity, 1

When an object’s velocity and acceleration are in the same direction, the object is speeding up

When an object’s velocity and acceleration are in the opposite direction, the object is slowing down

Page 18: Chapter 2 Kinematics in one Dimension

Example

Acceleration and velocity are in opposite directions Acceleration is uniform (blue arrows maintain the same

length) Velocity is decreasing (red arrows are getting shorter) Positive velocity and negative acceleration

Page 19: Chapter 2 Kinematics in one Dimension

Some math. Assume constant acceleration

atvv

atvv

attadtaadtvvdv

adtdv

adtdv

f

tv

v

t

f

f

0

0

000 )0(

constant

0

Page 20: Chapter 2 Kinematics in one Dimension

More …

200

200

000

0

0

0

2121

0

attvxx

attvxx

tdtadtvdx

atdtdtvdx

atvdtdx

atvv

ttx

x

Page 21: Chapter 2 Kinematics in one Dimension

One more calculus trick: the the chain rulechain rule

axvv

vvxxa

vdvdxa

vdvadxdxdvv

dtdx

dxdv

dtdva

f

f

v

v

x

x

f

2

0for x

)(21)(

20

2

0

20

20

00

Page 22: Chapter 2 Kinematics in one Dimension

Kinematic Equations -- summary from the book.

Page 23: Chapter 2 Kinematics in one Dimension

Kinematic Equations

The kinematic equations may be used to solve any problem involving one-dimensional motion with a constant acceleration

You may need to use two of the equations to solve one problem

Many times there is more than one way to solve a problem

Page 24: Chapter 2 Kinematics in one Dimension

Kinematic Equations, specific

For constant a, Can determine an object’s velocity at any time t

when we know its initial velocity and its acceleration

Does not give any information about displacement

Page 25: Chapter 2 Kinematics in one Dimension

Kinematic Equations, specific

For constant acceleration,

The average velocity can be expressed as the arithmetic mean of the initial and final velocities

2xi xf

x

v vv

Page 26: Chapter 2 Kinematics in one Dimension

Kinematic Equations, specific

For constant acceleration,

Gives final position in terms of velocity and acceleration

Doesn’t tell you about final velocity

212f i xi xx x v t a t

Page 27: Chapter 2 Kinematics in one Dimension

Graphical Look at Motion – displacement – time curve The slope of the curve

is the velocity The curved line

indicates the velocity is changing Therefore, there is an

acceleration

Page 28: Chapter 2 Kinematics in one Dimension

Graphical Look at Motion – velocity – time curve The slope gives the

acceleration The straight line

indicates a constant acceleration

Page 29: Chapter 2 Kinematics in one Dimension

The zero slope indicates a constant acceleration

Graphical Look at Motion – acceleration – time curve

Page 30: Chapter 2 Kinematics in one Dimension

Let’s get real and throw something out of a building and watch it fall.This is called free fall.

Page 31: Chapter 2 Kinematics in one Dimension

Freely Falling Objects

A freely falling object is any object moving freely under the influence of gravity alone.

It does not depend upon the initial motion of the object Dropped – released from rest Thrown downward Thrown upward

Page 32: Chapter 2 Kinematics in one Dimension

Acceleration of Freely Falling Object The acceleration of an object in free fall is directed

downward, regardless of the initial motion The magnitude of free fall acceleration is g = 9.80

m/s2

g decreases with increasing altitude g varies with latitude 9.80 m/s2 is the average at the Earth’s surface

In the English/American system, g=32 ft/sec2.

Page 33: Chapter 2 Kinematics in one Dimension

Acceleration of Free Fall/Rise, cont. We will neglect air resistance Free fall motion is constantly accelerated

motion in one dimension Use the kinematic equations to solve

problems.

Page 34: Chapter 2 Kinematics in one Dimension

Free Fall ExampleLet’s drop an object from the topof this building by simply releasing it.

How long will it take to get to the ground?

How fast will it be going when it gets to theground?

What color is the object?

Issues –

Where is the origin?IS y the same thing as x?? How can that be???