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Department of Physics and Applied Physics95.141, F2010, Lecture 4
Exam Prep Problem
• Vince Carter’s vertical leap is 43”. – A) (10pts) With what initial vertical velocity does Carter
leave the ground?
– B) (10pts) What is his hang time?
– C) (10pts) Assuming Carter leaps straight up at t=0s and lands at just after t=T, draw the vectors for James’ displacement, velocity, and acceleration at:
• i) The instant he leaves the ground (t=0s)
• ii) t=T/4
• iii) t=T/2
• iv) t=3T/4
• v) t=T
Department of Physics and Applied Physics95.141, F2010, Lecture 4
Exam Prep Problem
• Vince Carter’s vertical leap is 43”. – A) (10pts) With what initial vertical velocity does
James leave the ground?
Department of Physics and Applied Physics95.141, F2010, Lecture 4
Exam Prep Problem
• Vince Carter’s vertical leap is 43”. – B) (10pts) What is his hang time?
Department of Physics and Applied Physics95.141, F2010, Lecture 4
Exam Prep Problem
• Vince Carter’s vertical leap is 43”. – C) (10pts) Assuming Carter leaps straight up at t=0s
and lands at just after t=T, draw the vectors for James’ displacement, velocity, and acceleration at:0t 4
Tt 2Tt 4
3Tt Tt
avy
avy
avy
avy
avy
Department of Physics and Applied Physics95.141, F2010, Lecture 4
Outline
• Lecture 3 Review• 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, F2010, Lecture 4
Lecture 3 Review
• Freely falling body problems– Batman’s bat-hook
• Scalars and Vectors• Graphical description of vectors and vector
addition.• Vector components• Mathematical description of vector addition
(addition of components)• Unit Vectors
Department of Physics and Applied Physics95.141, F2010, 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, F2010, Lecture 4
Vector Kinematics12 xxx
12 rrr
Now, instead of describing displacement in terms of either vertical or horizontal position, we can talk about a displacement vector!
x
y
Department of Physics and Applied Physics95.141, F2010, 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, F2010, 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, F2010, 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, F2010, Lecture 4
Instantaneous Velocity (math)
• To find the instantaneous velocity, we can take the derivative of the position vector with respect to time:
ktzjtyitxr ˆ)(ˆ)(ˆ)(
Department of Physics and Applied Physics95.141, F2010, 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, F2010, Lecture 4
Acceleration Vector
• Average acceleration:
• Instantaneous acceleration
Department of Physics and Applied Physics95.141, F2010, 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, F2010, 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, F2010, 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
Department of Physics and Applied Physics95.141, F2010, 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, F2010, 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
Department of Physics and Applied Physics95.141, F2010, 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, F2010, 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, F2010, 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, F2010, 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, F2010, 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, F2010, 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, F2010, Lecture 4
Relative Velocity
• Two velocities:
5m/s
25m/s
Department of Physics and Applied Physics95.141, F2010, 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, F2010, Lecture 4
Relative Velocity
• What is Kirk’s velocity when he hits the ground?– Assume he leaps when car is moving 20m/s
Department of Physics and Applied Physics95.141, F2010, 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, F2010, 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?