PHYS 1443 – Section 003 Lecture #2
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Transcript of PHYS 1443 – Section 003 Lecture #2
Monday, Sept. 9, 2002 PHYS 1443-003, Fall 2002Dr. Jaehoon Yu
1
PHYS 1443 – Section 003Lecture #2
Wednesday, Sept. 9, 2002Dr. Jaehoon Yu
1. One dimensional motion w/ constant acceleration2. Kinetimatic equations of motion3. Free fall4. Coordinate systems 5. Vector; its properties, operations and components6. Two dimensional motion
• Displacement, Velocity, and Speed• Projectile Motion• Uniform Circular Motion
Today’s homework is homework #3, due 1am, next Monday!!
Monday, Sept. 9, 2002 PHYS 1443-003, Fall 2002Dr. Jaehoon Yu
2
Announcements
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• e-mail:15 of you have subscribed so far. – This is the primary communication tool. So do it ASAP.– A test message will be sent this Wednesday.
• Homework registration: 44 of you have registered (I have 56 of you)– Roster will be locked at the end of the day Wednesday, Sept. 11
Monday, Sept. 9, 2002 PHYS 1443-003, Fall 2002Dr. Jaehoon Yu
3
One Dimensional Motion• Let’s start with the simplest case: acceleration is constant (a=a0)• Using definitions of average acceleration and velocity, we can draw
equations of motion (description of motion, velocity and position as a function of time)
t
vv
tt
vva
xi
i
xix
xf
f
xf
If tf=t and ti=0 tavv xxixf
For constant acceleration, simple numeric average
t
xx
tt
xxv
i
i
ix
f
f
f
If tf=t and ti=0
2
2
1tatvxtvxx xxiixif
Resulting Equation of Motion becomes
tavtavvv
v xxixxixfxi
x
2
1
2
2
2
tvxx xif
Monday, Sept. 9, 2002 PHYS 1443-003, Fall 2002Dr. Jaehoon Yu
4
Kinetic Equations of Motion on a Straight Line Under Constant Acceleration tavtv xxixf
2
2
1tatvxx xxiif
tvvtvxx xixfxif 2
1
2
1
ifxf xxavv xxi 222
Velocity as a function of time
Displacement as a function of velocity 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!!
Monday, Sept. 9, 2002 PHYS 1443-003, Fall 2002Dr. Jaehoon Yu
5
Example 2.8
• Let’s call the time interval for police to catch the car; T• Set up an equation:Police catches the violator when his final
position is the same as the violator’s.22 00.3
2
1
2
1TaTx Police
f )1(0.451 TTvx Carf
)1(0.4500.32
1 ; 2 TTxx Car
fPolicef
a
acbbx
cbxax
2
4
are 0for Solutions
2
2
A car traveling at constant speed of 45.0m/s (~162km/hr or ~100miles/hr), police starts chasing the car at the constant acceleration of 3.00m/s2, one second after the car passes him. How long does it take for police to catch the violator?
Ex02-08.ip
00.300.3000.1 2 TT
possible)(not 00.1or (possible) 0.31 TT
Monday, Sept. 9, 2002 PHYS 1443-003, Fall 2002Dr. Jaehoon Yu
6
Free Fall• Free fall is a motion under the influence of gravitational pull
(gravity) only; Which direction is a freely falling object moving?• Gravitational acceleration is inversely proportional to the
distance between the object and the center of the earth• The gravitational acceleration is g=9.80m/s2 on the surface of
the earth, most of the time.• The direction of gravitational acceleration is ALWAYS toward
the center of the earth, which we normally call (-y); where up and down direction are indicated as the variable “y”
• Thus the correct denotation of gravitational acceleration on the surface of the earth is g=-9.80m/s2
Monday, Sept. 9, 2002 PHYS 1443-003, Fall 2002Dr. Jaehoon Yu
7
Example 2.12Stone was thrown straight upward at t=0 with +20.0m/s initial velocity on the roof
of a 50.0m high building, 1. Find the time the stone reaches at maximum height (v=0)2. Find the maximum height3. Find the time the stone reaches its original height4. Find the velocity of the stone when it reaches its original height5. Find the velocity and position of the stone at t=5.00s
g=-9.80m/s2
st
ttavv yyif
04.280.9
0.20
00.080.90.20
1
)(4.704.200.50
)04.2()80.9(2
104.2200.50
2
1
2
2
m
tatvyy yyiif
2
st 08.4204.2 3 Other ways?
)/(0.2008.4)80.9(0.20 smtavv yyiyf 4
)(5.27)00.5()80.9(2
100.50.200.50
2
1
2
2
m
tatvyy yyiif
5-Position
)/(0.29
00.5)80.9(0.20
sm
tavv yyiyf
5-Velocity
Ex02-12.ip
Monday, Sept. 9, 2002 PHYS 1443-003, Fall 2002Dr. Jaehoon Yu
8
Coordinate Systems• Makes it easy to express locations or positions• Two commonly used systems, depending on convenience
– Cartesian (Rectangular) Coordinate System• Coordinates are expressed in (x,y)
– Polar Coordinate System • Coordinates are expressed in (r)
• Vectors become a lot easier to express and compute
O (0,0)
(x1,y1)=(r)r
sin
cos
ry
rx
How are Cartesian and Polar coordinates related?
1
1tan
21
21
x
y
yxr
y1
x1
+x
+y
Monday, Sept. 9, 2002 PHYS 1443-003, Fall 2002Dr. Jaehoon Yu
9
Example 3.1 Cartesian Coordinate of a point in the xy plane are (x,y)= (-3.50,-2.50)m. Find the polar coordinates of this point.
y
x
(-3.50,-2.50)m
r
s
)(30.45.18
50.250.322
22
m
yxr
s 180
7
5
50.3
50.2tan
s
5.357
5tan 1
s
2165.35180180 s
Monday, Sept. 9, 2002 PHYS 1443-003, Fall 2002Dr. Jaehoon Yu
10
Vector and ScalarVector quantities have both magnitude (size) and direction
Scalar quantities have magnitude onlyCan be completely specified with a value and its unit
Force, gravitational pull, momentum
Normally denoted in BOLD BOLD letters, FF, or a letter with arrow on top FTheir sizes or magnitudes are denoted with normal letters, F, or absolute values: For F
Energy, heat, mass, weightNormally denoted in normal letters, E
Both have units!!!
Monday, Sept. 9, 2002 PHYS 1443-003, Fall 2002Dr. Jaehoon Yu
11
Properties of Vectors• Two vectors are the same if their and the are the
same, no matter where they are on a coordinate system.
x
y
AABB
EE
DD
CC
FF
Which ones are the same vectors?
A=B=E=DA=B=E=D
Why aren’t the others?
C:C: The same magnitude but opposite direction: C=-A:C=-A:A negative vector
F:F: The same direction but different magnitude
sizes directions
Monday, Sept. 9, 2002 PHYS 1443-003, Fall 2002Dr. Jaehoon Yu
12
Vector Operations• Addition:
– Triangular Method: One can add vectors by connecting the head of one vector to the tail of the other (head-to-tail)
– Parallelogram method: Connect the tails of the two vectors and extend– Addition is commutative: Changing order of operation does not affect the results
A+B=B+AA+B=B+A, A+B+C+D+E=E+C+A+B+DA+B+C+D+E=E+C+A+B+D
AA
BBAA
BB=AA
BBA+BA+B
• Subtraction: – The same as adding a negative vector:A A - B = A B = A + (-BB)
AA-B-B Since subtraction is the equivalent to adding
a negative vector, subtraction is also commutative!!!
• Multiplication by a scalar is increasing the magnitude A, BA, B=2A A
AA B=2AB=2A
AB 2
Fig03-07.ip
A+BA+BA+BA+B
A-BA-B
OR
Monday, Sept. 9, 2002 PHYS 1443-003, Fall 2002Dr. Jaehoon Yu
13
Example 3.2A car travels 20.0km due north followed by 35.0km in a direction 60.0o west of north. Find the magnitude and direction of resultant displacement.
N
E
r
22 sincos BBAr
20AA
BB
60cos
60sintan 1
BA
B
Find other
ways to solve this problem…
cos2sincos 2222 ABBA
cos222 ABBA
60cos0.350.2020.350.20 22
)(2.482325 km
60cos0.350.20
60sin0.35tan 1
N W wrt to9.385.37
3.30tan 1
Monday, Sept. 9, 2002 PHYS 1443-003, Fall 2002Dr. Jaehoon Yu
14
Components and Unit Vectors• Coordinate systems are useful in expressing vectors in their components
(Ax,Ay)AA
Ay
Ax
x
y
22
sin
cos
yx
y
x
AAA
AA
AA
AA
AAA
222
22
sincos
sincos
}Components(+,+)
(-,+)
(-,-) (+,-)• Unit vectors are dimensionless vectors whose magnitude are exactly 1
• Unit vectors are usually expressed in i,j,k or • Vectors can be expressed using components and unit vectors
kji , ,
jAiAjAiAA yx sincos So the above vector AA can be written as
Monday, Sept. 9, 2002 PHYS 1443-003, Fall 2002Dr. Jaehoon Yu
15
Examples 3.3 & 3.4Find the resultant vector which is the sum of AA=(2.0ii+2.0jj) and B B =(2.0ii-4.0jj)
mjiji
jijiBAC
0.20.40.40.20.20.2
0.40.20.20.2
Find the resultant displacement of three consecutive displacements: dd11=(15ii+30j j +12kk)cm, dd22=(23ii+14j j -5.0kk)cm, and dd11=(-13ii+15jj)cm
)(650.75925 222 cmD
)(5.4200.4160.20.4 22 mC
)(0.75925
0.512151430132315
cmkji
kjiD
jikjikji
dddD
15130.51423123015
321
270.4
0.2tantan 11
x
y
C
C
Monday, Sept. 9, 2002 PHYS 1443-003, Fall 2002Dr. Jaehoon Yu
16
Displacement, Velocity, and Acceleration in 2-dim
• Displacement: if rrr
• Average Velocity: if
if
tt
rr
t
rv
• Instantaneous Velocity: dt
rd
t
rv
t
0
lim
• Average Acceleration if
if
tt
vv
t
va
• Instantaneous Acceleration: 2
2
0lim
dt
rd
dt
rd
dt
d
dt
vd
t
va
t
How is each of these quantities defined in 1-D?