wednesday, sept. 15, 2010 phys 1441-002, fall 2010 dr. jaehoon yu 1 phys 1441 – section 002...

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Wednesday, Sept. 15, 2010 PHYS 1441-002, Fall 2010 Dr. Jaehoon Yu 1 PHYS 1441 – Section 002 Lecture #4 Wednesday, Sept. 15, 2010 Dr. Jaehoon Yu One Dimensional Motion Instantaneous Velocity and Speed Acceleration Motion under constant acceleration One dimensional Kinematic Equations How do we solve kinematic problems? Falling motions

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Page 1: Wednesday, Sept. 15, 2010 PHYS 1441-002, Fall 2010 Dr. Jaehoon Yu 1 PHYS 1441 – Section 002 Lecture #4 Wednesday, Sept. 15, 2010 Dr. Jaehoon Yu One Dimensional

Wednesday, Sept. 15, 2010

PHYS 1441-002, Fall 2010 Dr. Jaehoon Yu

1

PHYS 1441 – Section 002Lecture #4

Wednesday, Sept. 15, 2010Dr. Jaehoon Yu

• One Dimensional Motion• Instantaneous Velocity and Speed• Acceleration• Motion under constant acceleration• One dimensional Kinematic Equations• How do we solve kinematic problems?• Falling motions

Page 2: Wednesday, Sept. 15, 2010 PHYS 1441-002, Fall 2010 Dr. Jaehoon Yu 1 PHYS 1441 – Section 002 Lecture #4 Wednesday, Sept. 15, 2010 Dr. Jaehoon Yu One Dimensional

Announcements• E-mail subscription

– A test message was sent out yesterday!• Thanks for your replies!• If you haven’t yet, please check your e-mail and reply ONLY TO ME!

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• 1st term exam– Non-comprehensive – Time: 1 – 2:20pm, Wednesday, Sept. 22– Coverage: Appendices A.1 – A.8 and CH1.1 – what we finish coming

Monday, Sept. 20

• Quiz results– Class average: 8.3/16

• Equivalent to 52/100

– Top score: 16/16

• Colloquium at 4pm today in SH101– Physics faculty research expo!!

Wednesday, Sept. 15, 2010

2PHYS 1441-002, Fall 2010 Dr. Jaehoon Yu

Page 3: Wednesday, Sept. 15, 2010 PHYS 1441-002, Fall 2010 Dr. Jaehoon Yu 1 PHYS 1441 – Section 002 Lecture #4 Wednesday, Sept. 15, 2010 Dr. Jaehoon Yu One Dimensional
Page 4: Wednesday, Sept. 15, 2010 PHYS 1441-002, Fall 2010 Dr. Jaehoon Yu 1 PHYS 1441 – Section 002 Lecture #4 Wednesday, Sept. 15, 2010 Dr. Jaehoon Yu One Dimensional

Wednesday, Sept. 15, 2010

PHYS 1441-002, Fall 2010 Dr. Jaehoon Yu

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Reminder: Special Problems for Extra Credit• Derive the quadratic equation for yx2-zx+v=0

5 points• Derive the kinematic equation

from first principles and the known kinematic equations 10 points

• You must show your OWN work in detail to obtain the full credit• Must be in much more detail than in pg. 19 of this lecture note!!!

• Due Monday, Sept. 27

2 2

0 02v v a x x

Page 5: Wednesday, Sept. 15, 2010 PHYS 1441-002, Fall 2010 Dr. Jaehoon Yu 1 PHYS 1441 – Section 002 Lecture #4 Wednesday, Sept. 15, 2010 Dr. Jaehoon Yu One Dimensional

Wednesday, Sept. 15, 2010

PHYS 1441-002, Fall 2010 Dr. Jaehoon Yu

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Displacement, Velocity and SpeedOne dimensional displacement is defined as:

ixxx f

The average velocity is defined as: xv

The average speed is defined as: Total Distance Traveled

Total Elapsed Timev

f

f

i

i

x x

t t

x

t

Displacement per unit time in the period throughout the motion

Displacement is the difference between initial and final potions of the motion and is a vector quantity. How is this different than distance?

Displacement

Elapsed Time

Unit? m/s

Unit? m

Unit? m/s

Page 6: Wednesday, Sept. 15, 2010 PHYS 1441-002, Fall 2010 Dr. Jaehoon Yu 1 PHYS 1441 – Section 002 Lecture #4 Wednesday, Sept. 15, 2010 Dr. Jaehoon Yu One Dimensional

Wednesday, Sept. 15, 2010

PHYS 1441-002, Fall 2010 Dr. Jaehoon Yu

6

Example 2.1

2 1f ix x x x x • Displacement:

• Average Velocity: f

f

ix

i

x xv

t t

• Average Speed:

Total Distance Traveled

Total Time Intervalv

The position of a runner as a function of time is plotted as moving along the x axis of a coordinate system. During a 3.00-s time interval, the runner’s position changes from x1=50.0m to x2=30.5 m, as shown in the figure. What was the runner’s average velocity? What was the average speed?

30.5 50.0 19.5( )m

2 1

2 1

x x x

t t t

19.5

6.50( / )3.00

m s

50.0 30.5 19.56.50( / )

3.00 3.00m s

Page 7: Wednesday, Sept. 15, 2010 PHYS 1441-002, Fall 2010 Dr. Jaehoon Yu 1 PHYS 1441 – Section 002 Lecture #4 Wednesday, Sept. 15, 2010 Dr. Jaehoon Yu One Dimensional

Wednesday, Sept. 15, 2010 PHYS 1441-002, Fall 2010 Dr. Jaehoon Yu

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How far does a jogger run in 1.5 hours (5400 s) if his average speed is 2.22 m/s?

Average speed

Distance

Example Distance Run by a Jogger

Distance Elapsed time

Average speed Elapsed time

2.22 m s 5400 s 12000 m

Page 8: Wednesday, Sept. 15, 2010 PHYS 1441-002, Fall 2010 Dr. Jaehoon Yu 1 PHYS 1441 – Section 002 Lecture #4 Wednesday, Sept. 15, 2010 Dr. Jaehoon Yu One Dimensional

Wednesday, Sept. 15, 2010

PHYS 1441-002, Fall 2010 Dr. Jaehoon Yu

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Andy Green in the car ThrustSSC set a world record of 341.1 m/s in 1997. To establish such a record, the driver makes two runs through the course, one in each direction to nullify wind effects. From the data, determine the average velocity for each run.

Example: The World’s Fastest Jet-Engine Car

vr

t

xr

1609 m339.5m s

4.740 s

vr

t

xr

1609 m342.7 m s

4.695 s

What is the speed?

What is the speed?

v vr

v vr

339.5m s

342.7 m s

342.7 m s

Page 9: Wednesday, Sept. 15, 2010 PHYS 1441-002, Fall 2010 Dr. Jaehoon Yu 1 PHYS 1441 – Section 002 Lecture #4 Wednesday, Sept. 15, 2010 Dr. Jaehoon Yu One Dimensional

Wednesday, Sept. 15, 2010

PHYS 1441-002, Fall 2010 Dr. Jaehoon Yu

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Instantaneous Velocity and Speed• Can average quantities tell you the detailed story of

the whole motion?

xx

vt

Δt 0lim

*Magnitude of Vectors are Expressed in absolute values

•Instantaneous speed is the size (magnitude) of the velocity vector:

xx

vt

Δt 0lim

• Instantaneous velocity is defined as:– What does this mean?

• Displacement in an infinitesimal time interval• Average velocity over a very short amount of time

NO!!

Page 10: Wednesday, Sept. 15, 2010 PHYS 1441-002, Fall 2010 Dr. Jaehoon Yu 1 PHYS 1441 – Section 002 Lecture #4 Wednesday, Sept. 15, 2010 Dr. Jaehoon Yu One Dimensional

Wednesday, Sept. 15, 2010

PHYS 1441-002, Fall 2010 Dr. Jaehoon Yu

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Position vs Time Plot

timet1 t2 t3t=0

Position

x=0

x11 2 3

1. Running at a constant velocity (go from x=0 to x=x1 in t1, Displacement is + x1 in t1 time interval)

2. Velocity is 0 (go from x1 to x1 no matter how much time changes)3. Running at a constant velocity but in the reverse direction as 1. (go

from x1 to x=0 in t3-t2 time interval, Displacement is - x1 in t3-t2 time interval)

It is useful to understand motions to draw them on position vs time plots.

Page 11: Wednesday, Sept. 15, 2010 PHYS 1441-002, Fall 2010 Dr. Jaehoon Yu 1 PHYS 1441 – Section 002 Lecture #4 Wednesday, Sept. 15, 2010 Dr. Jaehoon Yu One Dimensional

Wednesday, Sept. 15, 2010

PHYS 1441-002, Fall 2010 Dr. Jaehoon Yu

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Page 12: Wednesday, Sept. 15, 2010 PHYS 1441-002, Fall 2010 Dr. Jaehoon Yu 1 PHYS 1441 – Section 002 Lecture #4 Wednesday, Sept. 15, 2010 Dr. Jaehoon Yu One Dimensional

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PHYS 1441-002, Fall 2010 Dr. Jaehoon Yu

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Velocity vs Time Plot

Page 13: Wednesday, Sept. 15, 2010 PHYS 1441-002, Fall 2010 Dr. Jaehoon Yu 1 PHYS 1441 – Section 002 Lecture #4 Wednesday, Sept. 15, 2010 Dr. Jaehoon Yu One Dimensional

Wednesday, Sept. 15, 2010

PHYS 1441-002, Fall 2010 Dr. Jaehoon Yu

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Displacement, Velocity and Speed

xx

vt

Δt 0lim

Displacement ixxx f

Average velocityt

x

tt

xxv

i

ix

f

f

Average speed Spent Time Total

Traveled Distance Totalv

Instantaneous velocity

Instantaneous speed xx

vt

Δt 0lim

Page 14: Wednesday, Sept. 15, 2010 PHYS 1441-002, Fall 2010 Dr. Jaehoon Yu 1 PHYS 1441 – Section 002 Lecture #4 Wednesday, Sept. 15, 2010 Dr. Jaehoon Yu One Dimensional

Wednesday, Sept. 15, 2010

PHYS 1441-002, Fall 2010 Dr. Jaehoon Yu

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Acceleration

xa xv analogs to

xa xx

vt

Δt 0limanalogs to

Change of velocity in time (what kind of quantity is this?)

•Average acceleration:

•Instantaneous acceleration: Average acceleration over a very short amount of time.

xf

f

xi

i

v v

t t

xv

t

f

f

i

i

x x

t t

x

t

xv

t

Δt 0

lim

Vector!

Unit? m/s2Dimension? [LT-2]

Page 15: Wednesday, Sept. 15, 2010 PHYS 1441-002, Fall 2010 Dr. Jaehoon Yu 1 PHYS 1441 – Section 002 Lecture #4 Wednesday, Sept. 15, 2010 Dr. Jaehoon Yu One Dimensional

Wednesday, Sept. 15, 2010

PHYS 1441-002, Fall 2010 Dr. Jaehoon Yu

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Acceleration vs Time Plot

What does this plot tell you?Yes, you are right!!The acceleration of this motion is a constant!!

Page 16: Wednesday, Sept. 15, 2010 PHYS 1441-002, Fall 2010 Dr. Jaehoon Yu 1 PHYS 1441 – Section 002 Lecture #4 Wednesday, Sept. 15, 2010 Dr. Jaehoon Yu One Dimensional

Wednesday, Sept. 15, 2010

PHYS 1441-002, Fall 2010 Dr. Jaehoon Yu

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Example 2.3

xa )/(2.40.5

21

0.5

021 2sm

A car accelerates along a straight road from rest to 75km/h in 5.0s.

What is the magnitude of its average acceleration?

xfv

xiv

)/(105.4

1000

36002.4 242

hkm

0 /m s

75000

3600

m

s21 /m s

xf xi

f i

v v

t t

xv

t

Page 17: Wednesday, Sept. 15, 2010 PHYS 1441-002, Fall 2010 Dr. Jaehoon Yu 1 PHYS 1441 – Section 002 Lecture #4 Wednesday, Sept. 15, 2010 Dr. Jaehoon Yu One Dimensional

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PHYS 1441-002, Fall 2010 Dr. Jaehoon Yu

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Few Confusing Things on Acceleration• When an object is moving in a constant velocity (v=v0), there is

no acceleration (a=0)– Is there any acceleration when an object is not moving?

• When an object is moving faster as time goes on, (v=v(t) ), acceleration is positive (a>0).– Incorrect, since the object might be moving in negative direction initially

• When an object is moving slower as time goes on, (v=v(t) ), acceleration is negative (a<0)– Incorrect, since the object might be moving in negative direction initially

• In all cases, velocity is positive, unless the direction of the movement changes.– Incorrect, since the object might be moving in negative direction initially

• Is there acceleration if an object moves in a constant speed but changes direction? The answer is YES!!

Page 18: Wednesday, Sept. 15, 2010 PHYS 1441-002, Fall 2010 Dr. Jaehoon Yu 1 PHYS 1441 – Section 002 Lecture #4 Wednesday, Sept. 15, 2010 Dr. Jaehoon Yu One Dimensional

Wednesday, Sept. 15, 2010

PHYS 1441-002, Fall 2010 Dr. Jaehoon Yu

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One Dimensional Motion• Let’s focus on the simplest case: acceleration is a constant (a=a0)• Using the definitions of average acceleration and velocity, we can derive

equations of motion (description of motion, velocity and position as a function of time)

xa (If tf=t and ti=0) xfv

For constant acceleration, average velocity is a simple numeric average

xv

fx Resulting Equation of Motion becomes

xv

fx

xi xv a txa

xf

f

xi

i

v v

t t

xf xi

x

v va

t

2

xi xfv v

2

2

xi xv a t

1

2xi xv a t

f

f

i

i

x x

t t

f ixx x

vt

(If tf=t and ti=0) xix v t

xix v t 21

2i xi xx v t a t

Page 19: Wednesday, Sept. 15, 2010 PHYS 1441-002, Fall 2010 Dr. Jaehoon Yu 1 PHYS 1441 – Section 002 Lecture #4 Wednesday, Sept. 15, 2010 Dr. Jaehoon Yu One Dimensional

Wednesday, Sept. 15, 2010

PHYS 1441-002, Fall 2010 Dr. Jaehoon Yu

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One Dimensional Motion cont’d

fx

xa

Average velocity

t Since

fx

Substituting t in the above equation,

xv

2xfv

Solving for t

Resulting in

2

xi xfv vxix v t

2xi xf

i

v vx t

xf xiv v

t

xf xi

x

v x

a

2xf xi xf xi

ix

v v v vx

a

2 2

2xf xi

ix

v vx

a

2 2xi x f iv a x x

Page 20: Wednesday, Sept. 15, 2010 PHYS 1441-002, Fall 2010 Dr. Jaehoon Yu 1 PHYS 1441 – Section 002 Lecture #4 Wednesday, Sept. 15, 2010 Dr. Jaehoon Yu One Dimensional

Wednesday, Sept. 15, 2010

PHYS 1441-002, Fall 2010 Dr. Jaehoon Yu

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Kinematic Equations of Motion on a Straight Line Under Constant Acceleration

tavtv xxixf

2

2

1tatvxx xxiif

1 1

2 2f xi xf xix x v t v v t

ifxf xxavv xxi 222

Velocity as a function of time

Displacement as a function of velocities and time

Displacement as a function of time, velocity, and acceleration

Velocity as a function of Displacement and acceleration

You may use different forms of Kinetic equations, depending on the information given to you for specific physical problems!!