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Department of Physics and Applied Physics95.141, F2009, Lecture 4
Physics I95.141
LECTURE 49/16/09
Department of Physics and Applied Physics95.141, F2009, Lecture 4
Administrative Notes
• Masteringphysics.com– Feedback welcome!– Keep it civil, respectful
• These are to help you review the previous lecture and prepare for the upcoming.
• They are a tool for me to make sure people understand the material and
• For you to make sure you understand the material
– I recognize that issues like hints and sig figs are causing some confusion.
– Grading focus will be more on attempting the problems and spending time working on them, not necessarily final score.
• Help in class.• HW Review sessions
Department of Physics and Applied Physics95.141, F2009, Lecture 4
Example Problem II (Lecture 3)• Batman launches his grappling bat-hook upwards, if the walkway it
attaches to is 25m above Batman’s Batbelt, at what bat-velocity must the hook be launched at in order to make it to the beam? (Ignore the mass of the cord and air resistance)
3) Choose bat-equation(s)
4) Solve
2
)(2
2
1
22
2
o
oo
oo
o
vvv
xxavv
attvxx
atvv
Department of Physics and Applied Physics95.141, F2009, Lecture 4
Outline
• Vector Kinematics• Relative Motion
• What do we know?– Units/Dimensions/Measurement/SigFigs– Kinematic equations– Freely falling objects– Vectors
Department of Physics and Applied Physics95.141, F2009, Lecture 4
Vector Review• If I have 3 vectors given by:
kjiV
kjiV
kjiV
ˆ4ˆ3ˆ3
ˆ3ˆ1ˆ2
ˆ10ˆ2ˆ4
3
2
1
• Which of the following vectors corresponds to321 VVVVR
kjiVd
kjiVc
kjiVb
kiVa
R
R
R
R
ˆ3ˆ6ˆ3)
ˆ11ˆ6ˆ9)
ˆ3ˆ6ˆ9)
ˆ3ˆ3)
Department of Physics and Applied Physics95.141, F2009, Lecture 4
Vector Kinematics
• We can now do kinematics in more than one dimension– This is helpful, because we live in a 3D world!
• We previously described displacement as Δx, but this was for 1D, where motion could only be positive or negative.
• In more than 1 dimension, displacement is a vector
v
r
Department of Physics and Applied Physics95.141, F2009, Lecture 4
Vector Kinematics12 xxx
12 rrr
Department of Physics and Applied Physics95.141, F2009, Lecture 4
Vector Kinematics
• In unit vectors, we can write the displacement vector as:
• We can now rewrite our expression for average velocity:
Department of Physics and Applied Physics95.141, F2009, Lecture 4
Vector Kinematics
• Average velocity only tells part of the story• Just like for motion in 1D, we can let Δt get smaller and smaller….• Gives instantaneous velocity vector:
t
r
tv
0
lim
Department of Physics and Applied Physics95.141, F2009, Lecture 4
Velocity Vector
• The magnitude of the average velocity vector is NOT equal to the average speed.
• But the magnitude of the instantaneous velocity vector is equal to the instantaneous speed at that time
Department of Physics and Applied Physics95.141, F2009, Lecture 4
Instantaneous Velocity (math)
• To find the instantaneous velocity, we can take the derivative of the position vector with respect to time:
kvjvivdt
rdk
dt
dzj
dt
dyi
dt
dx
dt
rdv zyx
ˆˆˆˆˆˆ
Department of Physics and Applied Physics95.141, F2009, Lecture 4
Example
• Say we are given the position of an object to be:
ktjeittr t ˆ)2sin(ˆ2ˆ)14()( 2
• Can we find the velocity as a function of time?
Department of Physics and Applied Physics95.141, F2009, Lecture 4
Acceleration Vector
• Average acceleration:
• Instantaneous acceleration
Department of Physics and Applied Physics95.141, F2009, Lecture 4
Acceleration
• Acceleration will be non-zero not only for a change in speed, but for movement at constant speed but changing direction
kdt
zdj
dt
ydi
dt
xd
kdt
dvj
dt
dvi
dt
dv
dt
vda yyx
ˆˆˆ
ˆˆˆ
2
2
2
2
2
2
• An object moves around a circle at a constant speed. It’s acceleration must then be:– A) 0– B) Constant– C) Constantly changing
Department of Physics and Applied Physics95.141, F2009, Lecture 4
Example Problem
• Imagine we are given the position of an object as a function of time– Find displacement at t=1s and t=3s– Find velocity and acceleration as a function of time– Find velocity and acceleration at t=3s
jtmitttrs
ms
ms
m ˆ)(3)(3ˆ)(2)(4)( 3232
Department of Physics and Applied Physics95.141, F2009, Lecture 4
Example Problem
• Imagine we are given the position of an object as a function of time– Find displacement at t=1s and t=3s– Find velocity and acceleration as a function of time– Find velocity and acceleration at t=3s
jtmitttrs
ms
ms
m ˆ)(3)(3ˆ)(2)(4)( 3232
Department of Physics and Applied Physics95.141, F2009, Lecture 4
Example Problem
• Imagine we are given the position of an object as a function of time– Find displacement at t=1s and t=3s– Find velocity and acceleration as a function of time– Find velocity and acceleration at t=3s
jtita
jtittv
sm
sm
sm
sm
sm
ˆ)(18ˆ)(4)(
ˆ)(9ˆ)(4)(4)(
32
322
Department of Physics and Applied Physics95.141, F2009, Lecture 4
Example Problem
• Let’s say we are told that a Force causes an object to accelerate in the -y direction at 5m/s2. The object has an initial velocity in the +x direction of 10m/s, and in the +y direction of 15 m/s, and starts at the point (0,0).
– A) Give the initial velocity vector of the object
– B) Plot x(t) vs. t
– C) Plot y(t) vs. t
– D) Plot the object’s trajectory in the xy plane
Department of Physics and Applied Physics95.141, F2009, Lecture 4
Example Problem• Let’s say we are told that a Force causes an object to
accelerate in the -y direction at 5m/s2. The object has an initial velocity in the +x direction of 10m/s, and in the +y direction of 15 m/s, and starts at the point (0,0)..– A) Give the initial velocity vector of the object
20
20
vx
vy
3.56,18 smv
Department of Physics and Applied Physics95.141, F2009, Lecture 4
Example Problem• Let’s say we are told that a Force causes an object to accelerate in
the -y direction at 5m/s2. The object has an initial velocity in the +x direction of 10m/s, and in the +y direction of 15 m/s, and starts at the point (0,0).– Before we solve B-D, let’s determine equations of motion
(METHOD I)
Department of Physics and Applied Physics95.141, F2009, Lecture 4
Example Problem• Let’s say we are told that a Force causes an object to accelerate in
the -y direction at 5m/s2. The object has an initial velocity in the +x direction of 10m/s, and in the +y direction of 15 m/s, and starts at the point (0,0).– Before we solve B-D, let’s determine equations of motion
(METHOD II)
Department of Physics and Applied Physics95.141, F2009, Lecture 4
Example Problem• Let’s say we are told that a Force causes an object to accelerate in
the -y direction at 5m/s2. The object has an initial velocity in the +x direction of 10m/s, and in the +y direction of 15 m/s, and starts at the point (0,0).– B) Plot x(t) vs t
10
100
t(s)
x(t)
time x(t)
0 0m
1 10m
2 20m
5 50m
10 100m
ttvtx ox 10)(
Department of Physics and Applied Physics95.141, F2009, Lecture 4
Example Problem• Let’s say we are told that a Force causes an object to accelerate in
the -y direction at 5m/s2. The object has an initial velocity in the +x direction of 10m/s, and in the +y direction of 15 m/s, starts at (0,0).– C) Plot y(t) vs t
time y(t)
0 0m
1 12.5m
2 20m
3 22.5m
4 20m
5 12.5
10 -100
22 5.2152
1)( ttattvty oy
Department of Physics and Applied Physics95.141, F2009, Lecture 4
Example ProblemD) Plot object trajectory
• Choose coordinate system
time x(t) y(t)
0 0m 0m
1 10m 12.5m
2 20m 20m
3 30m 22.5m
4 40m 20m
5 50 12.5
10 100 -100
25.215)( ttty
ttx 10)(
2025.5.1)( xxxy
Department of Physics and Applied Physics95.141, F2009, Lecture 4
Relative Velocity
• So far we have looked at adding displacement vectors
• May also find situations where we need to add velocity vectors
Department of Physics and Applied Physics95.141, F2009, Lecture 4
Relative Velocity
• You might remember
5m/s
25m/s
Department of Physics and Applied Physics95.141, F2009, Lecture 4
Relative Velocity
• In this case, our hero would presumably prefer not to be decapitated by the bridge
• So we are interested in his velocity relative to the bridge• He is on a train moving at +25 m/s relative to the bridge• His velocity relative to the train is -5m/s• So his velocity relative to the bridge is:
Department of Physics and Applied Physics95.141, F2009, Lecture 4
Relative Velocity (Example 1)
• Imagine you are on a barge floating down the river with the current
• You walk diagonally across the barge with a velocity
• What is your velocity with respect to the water?
• With respect to the river bank?
iv sm
river
3
jiv sm
sm ˆ2ˆ2bargeon walk
Department of Physics and Applied Physics95.141, F2009, Lecture 4
Another River Problem
• A boat’s speed in still water is 1.85m/s. If you want to directly cross a stream with a current 1.2m/s, what upstream angle should you take?
4.40
Department of Physics and Applied Physics95.141, F2009, Lecture 4
In Class Demo
• I am going to shoot the rocket into the classroom standing still. – Where will it land with respect to my position?
• A) In front of me?• B) Behind me?• C) Same position?
x
y
?
Department of Physics and Applied Physics95.141, F2009, Lecture 4
In Class Demo
• I am going to shoot the rocket into the classroom walking forward. – Where will it land with respect to my position?
• A) In front of me?• B) Behind me?• C) Same position?
x
y
vo
?
Department of Physics and Applied Physics95.141, F2009, Lecture 4
Today We Learned….
• Vector kinematics– Displacement vector – Average velocity vector– Inst. Velocity vector– Average acceleration vector– Inst. Acceleration vector– Vector equations of motion
• Relative Velocity