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Getting Help
The Physics Learning Center
GTA Office Hours
Supplemental Instruction:
Every Wednesday Starting Next Wednesday January 26th
7 8:30 PM Fisher Hall Room 130
Get Help
Exam III
April 5th 6:00 7:30 PM
All conflicts must be resolved by
April 1st 5PM
E-mail [email protected]
with a detailed description of the nature
of your conflict (class, time) if you need
to take thi
Some Energy Exercises
Energy Problems :
What are the concepts we have to work with?
Mechanical Energy
K = 1 mv 2
2
Gravitational potential
energy
Spring
energy
( E la
ene stic po
rgy
te n
)
t ia l
Ch.
Work Part 1
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Learning Objectives
Learning
To
define work
To
use the work-kinetic energy
theorem to solve energy-related
problems
09/12/13
2
Work
What is the relationship between Kin
W o rkP a rt2
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Exam III Scores (Avg = 115.8 pts, 77.2 %)
12
10
6
4
2
0
Score
Frequency
8
F o rc e s c h a ng e a no b je c ts kine tic e ne rg y b yd o ing
wo rk.
Object moving fro
Work/EnergyTransfer
Revisited
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System Energy Esys = K + U + Eth
Mechanical Energy
K = 1 mv 2
2
Emech = K + U
U = mgy
Due to: vertical
position y in
gravitational field
and/or
U = 1
Last Time :
For Conservative forces
Conservation of
Mechanical Energy
For Non-Conservative forces
like Friction
Mechanical Energy is
Dissipated (as Heat)
cfw_Wnc = Eth
Emech = 0
K f + U f = Ki + U i
Newtons Theory
Of Gravity
Learning Objectives
To
understand the historical
significance of the Newtonian
synthesis
To
study the dynamics associated
with a distance-dependent force
To
understand satell
Newtonian Gravity II
Physics 2100
(2011)
MTU
Reminder
Thursday
9/12/13
: MasteringPhysics HW # 14
2
Newtons Law of Gravity
r
m1
r
F2 on 1
F1 on 2
r
F1 on 2
m2
Gm1m2
= F2 on 1 =
r2
The forces are direc
Welcome to PH2100!
Welcome
Introductory Classical Mechanics
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Introductions
Introductions
Lecturer (section 0B)
Dr. Brian Fick
All PH2100 Questions
Wil Slough
213 Fisher
[email protected]
Kinematics in Two Dimensions
Kinematics
Part 1
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Two-Dimensional Motion
Two-Dimensional
Ski Jumping
09/12/13
2
Ski Jumping Motion Diagram
Ski
Start
r
vi
r
v
r
vf
r
vi
r
vf
r
v
r
vi
r
Last Lecture .
Kinematics - the Description of motion
Some Simplifications :
Assume motion is along a straight line.
Linear Motion
Assume that objects are treated as
geometric points. Particle Model
G
Exam I
February 1st
6:00 7:30 PM
All conflicts must be resolved by
January 28th 5PM
E-mail [email protected]
with a detailed description of the nature
of your conflict (class, time) if you need
to take
Kinematics in Two Dimensions
Kinematics
Part 2
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Uniform Circular Motion
Last time :
Angular Position
Angular velocity
Tangential Speed
s
(radians)
r
d
= lim
=
t 0 t
dt
vt
r`
[]
Getting Help
GTA Office Hours
Supplemental Instruction:
Tonight !
Every Wednesday 7 8:30 PM Fisher Hall Room 130
Get Help with
Assigned Chapter Problems
MasteringPhysics Problems
Exam Preparatio
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Getting Help
The Physics Learning Center
GTA Office Hours
Supplemental Instruction:
Every Wednesday Starting Next Wednesday January 26th
7 8:30 PM Fisher Hall Room 130
Get Help
N
e
w
t
o
n
s
T
h
i
r
d
L
a
w
P
a
r
t
2
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Newtons 3rd Law
Last Time :
How to deal with more than one object!
A
r
FBonA
B
r
nA
r
r
FAonB = FBonA
r
FAonB
r
nB
r
FBonA
r
FAonB
r
F(G )
Exam III
April 5th 6:00 7:30 PM
All conflicts must be resolved by
April 1st 5PM
E-mail [email protected]
with a detailed description of the nature
of your conflict (class, time) if you need
to take thi
Impulse-Momentum Theorem
Impulse-Momentum
Momentum:
( in x-direction )
px = mv x
Impulse-momentum theorem:
An impulse delivered to a particle
changes the particles momentum.
09/12/13
Impulse:
( in x-d
Impulse and Momentum
Part 1
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The Fundamental Questions
The
How
do we describe motion?
Kinematics
What are the causes of changes in motion?
Dynamics
What properties of a system of pa
Exam I
February 1st
6:00 7:30 PM
All conflicts must be resolved by
January 28th 5PM
E-mail [email protected]
with a detailed description of the nature
of your conflict (class, time) if you need
to take
Kinematics
in One-Dimension:
Part 1
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Kinematics
in One-Dimension:
Part 1
Re-Introduction
Lecturer Wil Slough
All PH2100 Questions
Wil Slough
213 Fisher
[email protected]
09/12/13
3
I
Exam I
February 1st
6:00 7:30 PM
All conflicts must be resolved by
January 28th 5PM
E-mail [email protected]
with a detailed description of the nature
of your conflict (class, time) if you need
to take
Exam I
February 1st
6:00 7:30 PM
All conflicts must be resolved by
January 28th 5PM
E-mail [email protected]
with a detailed description of the nature
of your conflict (class, time) if you need
to take
Exam I
February 1st
6:00 7:30 PM
All conflicts must be resolved by
Today! January 28th 5PM
E-mail [email protected]
with a detailed description of the nature
of your conflict (class, time) if you need
Review
for Exam I
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09/12/13
Exam I Feb 1
st
6 to 7:30 PM
Location: according to first letter of your last name
See Room Assignment Posting On BlackBoard
Material: Chapters 1 4 in
Force and Motion
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How to do well in PH2100. Reboot
Explanation
Lecture
Text
Assigned Problems
Training
Not Scored
Solutions Posted
On BlackBoard
On-line
Homework
Scored
Exams
Scored
Dynamics I: Motion Along a Line
Part 1
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Frequency
Exam I Scores (Avg = 122.3 out of 150 pts, 81.6 %)
Score
Learning Objectives
Learning
To learn to use free-body diagrams
To under
Dynamics I: Motion Along a Line
Part 1
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Frequency
Exam I Scores (Avg = 122.3 out of 150 pts, 81.6 %)
Score
Learning Objectives
Learning
To learn to use free-body diagrams
To under