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Department of Physics and Applied Physics 95.141, Fall 2013, Lecture 5
Course website: http://faculty.uml.edu/Andriy_Danylov/Teaching/PhysicsI
Lecture Capture:
http://echo360.uml.edu/danylov2013/physics1fall.html
Lecture 5
Kinematics in two dimensions
09.18.2013 Physics I
Department of Physics and Applied Physics 95.141, Fall 2013, Lecture 5
Chapter 3: Sections 3.6 – 3.8 Vector kinematics Projectile motion
Outline
Department of Physics and Applied Physics 95.141, Fall 2013, Lecture 5
Vector Kinematics
• Kinematics in more than one dimension • Previously described 1D displacement as Δx, where
motion could only be positive or negative. • In more than 1D, displacement is a vector
v
Department of Physics and Applied Physics 95.141, Fall 2013, Lecture 5
Displacement
)1(12 Dxxx −=∆
12 rrr −=∆x
y
displacement (in unit vector notation): jyyixxr ˆ)(ˆ)( 1212 −+−=∆
1t
2tIn two or three dimensions, the displacement is a vector:
ij
jyixrjyixr ˆˆˆˆ222111 +=+=
Department of Physics and Applied Physics 95.141, Fall 2013, Lecture 5
Average Velocity
x
y
tr
ttrrv
∆∆
=−−
=
12
12
1t2t
Average velocity is the displacement divided by the elapsed time
As Δt and Δr become smaller and smaller, the average velocity approaches the instantaneous velocity.
Department of Physics and Applied Physics 95.141, Fall 2013, Lecture 5
Instantaneous velocity
1vThe instantaneous velocity indicates how fast the object moves and the direction of motion at each instant of time
2r
3r
2v
3v
x
y
Department of Physics and Applied Physics 95.141, Fall 2013, Lecture 5
Instantaneous acceleration
The instantaneous acceleration is in the direction of ,and is given by:
12 vvv −=∆
1v
2r
2v
x
y
1v
2v v∆
Average acceleration
2
2
dtrda
=
Department of Physics and Applied Physics 95.141, Fall 2013, Lecture 5
Using unit vectors
kvjvivkdtdxj
dtdyi
dtdx
dtrdv zyx
ˆˆˆˆˆˆ ++=++==
kdt
dvjdt
dvi
dtdva zyx ˆˆˆ ++=
Department of Physics and Applied Physics 95.141, Fall 2013, Lecture 5
Example Problem
Given position as a function of time, find instantaneous velocity and instantaneous acceleration at t=3s
kita ˆ2ˆ8)( +=
kikistv ˆ6ˆ24ˆ)32(ˆ)38()3( +=⋅+⋅==
Acceleration is constant
Department of Physics and Applied Physics 95.141, Fall 2013, Lecture 5
Projectile motion
A projectile is an object moving in two dimensions under the influence of Earth's gravity; its path is a parabola.
Department of Physics and Applied Physics 95.141, Fall 2013, Lecture 5
• X and Y motions are completely independent • Work the problem as two one-dimensional problems Each dimension obey different equations
Projectile motion
Department of Physics and Applied Physics 95.141, Fall 2013, Lecture 5
By splitting the equations of motion into component form, we can solve problems one direction at a time
2D Motion with constant acceleration
tavvtatvrr
+=
++=
0
221
00
There is only one parameter, which connects X and Y motion: time
Department of Physics and Applied Physics 95.141, Fall 2013, Lecture 5
)(2
02
02
221
00
0
xxavv
tatvxxtavv
xxx
xx
xxx
−+=
++=
+=
No forces in x direction.
Air resistance is neglected
Projectile motion X direction
ax = 0 2
02
xx vv =
0
0
0 xx vv 0=
00 tvxx x+=
vx is constant!!!!
Department of Physics and Applied Physics 95.141, Fall 2013, Lecture 5
Projectile motion Y- direction )(2
02
02
221
00
0
yyavv
tatvyy
tavv
yyy
yy
yyy
−+=
++=
+=
y
g
y
g
ay = -g
ay = g
if then
if then
)(2
02
02
221
00
0
yygvv
gttvyy
gtvv
yy
y
yy
−−=
−+=
−=
)(2
02
02
221
00
0
yygvv
gttvyy
gtvv
yy
y
yy
−+=
++=
+=
x
x
Department of Physics and Applied Physics 95.141, Fall 2013, Lecture 5
Projectile Motion: Concept Test 1
A helicopter moving at a constant horizontal velocity to the right drops a package when at position A. Which of the marked trajectories is closest to that observed by a stationary person on the ground?
observer
Department of Physics and Applied Physics 95.141, Fall 2013, Lecture 5
• Draw diagram, choose coordinate system
• Knowns and unknowns • Divide equations into x and y • Solve, noting that in the x and y
calculations the common parameter is the time interval t
Helicopter flying horizontally at 70m/s wants to drop supplies on mountain top 200m below. How far in advance (horizontal distance) should the package be dropped?
Example (Rescue Helicopter)
g
Department of Physics and Applied Physics 95.141, Fall 2013, Lecture 5
2
21 gttvyy oyo −+=
common parameter is time t Solve y-equations to find t Plug t into x-equations to
find x
Example (Rescue Helicopter)
mmx
447)39.6(70
==
00 =x 00 =y m/s 700 =xv 00 =yv
0=xa gay −=
?=x m 200−=y )(2
02
02
221
00
0
yygvv
gttvyy
gtvv
yy
y
yy
−−=
−+=
−=
xx
x
vvtvxx
0
00
=+=
0 0
gyt 2
−=
tvxx x00 +=
gyvx x
20 −=
0
ssm
mt 39.6/8.9
)200(22 =
−−
=
ConcepTest 2 Dropping the Ball I
From the same height (and at the same time), one ball is dropped and another ball is fired horizontally. Which one will hit the ground first?
A) the “dropped” ball B) the “fired” ball C) they both hit at the same time D) it depends on how hard the ball
was fired E) it depends on the initial height
From the same height (and at the same time), one ball is dropped and another ball is fired horizontally. Which one will hit the ground first?
A) the “dropped” ball B) the “fired” ball C) they both hit at the same time D) it depends on how hard the ball
was fired E) it depends on the initial height
Both of the balls are falling vertically under the influence of
gravity. They both fall from the same height. Therefore, they will
hit the ground at the same time. The fact that one is moving
horizontally is irrelevant—remember that the x and y motions are
completely independent !!
ConcepTest 2 Dropping the Ball I
Department of Physics and Applied Physics 95.141, Fall 2013, Lecture 5
A golf ball is hit with initial velocity v0 at an angle θ0 above the horizontal. Draw diagram and choose coordinate system
Fill in knowns
x
y
v0
v0x
v0y θ0
Example (Golf Ball)
00 =x 00 =y
0=xa gay −=000 cos θvv x = 000 sin θvv y =
g
Department of Physics and Applied Physics 95.141, Fall 2013, Lecture 5
A golf ball is hit with initial velocity v0 at an angle θ0 above the horizontal.
Find: the time of flight (how long the ball is in the air) This depends only on the y-component equations, as the motion in y direction stops the flight.
Since both y0 and y are zero at the beginning/end
y=0 when the ball was hit
The second is the time of flight gv
t y021
2 tand 0 ==
Cont. Example (Golf Ball).
0 0
y=0 when the ball landed
Department of Physics and Applied Physics 95.141, Fall 2013, Lecture 5
gvR oo θθ cossin2 0
2
=
A golf ball is hit with initial velocity v0 at an angle θ0 above the horizontal.
Find: Range (how far does ball travel on flat ground) Use constant x-velocity to calculate how far ball travels
horizontally during time of flight (Range)
gv
gv
t y θsin22 002 ==time of flight
000 cos θvvv xx ==Constant x velocity
Range
Maximum Range
Cont. Example (Golf Ball)
200 tvxxR x ⋅+==
°== 4512sin 00 θθ or
gvo 0
2 2sin θ=
when
Range
0
Department of Physics and Applied Physics 95.141, Fall 2013, Lecture 5
A golf ball is hit with initial velocity v0 at an angle θ0 above the horizontal.
Find: trajectory (height y as a function of position x)
Since common parameter is time t, eliminate t to get y(x)
Cont. Example (Golf Ball)
Equation of parabola
Which of the
three punts
has the
longest hang
time? D) all have the same hang time
A B C
h
The time in the air is determined by the vertical motion!
Because all of the punts reach the same height, they all
stay in the air for the same time.
ConcepTest 3. Punts I
)(2 02
02 yygvv yy −−= 2
21 tatvyy yoyo ++=
A B
C) both at the same time
A battleship simultaneously fires two shells at two enemy
submarines. The shells are launched with the same initial
velocity. If the shells follow the trajectories shown, which
submarine gets hit first ?
The flight time is fixed by the motion in the y-direction. The higher an object goes, the longer it stays in flight. The shell hitting submarine #2 goes less high, therefore it stays in flight for less time than the other shell. Thus, submarine #2 is hit first.
ConcepTest 4 Punts II
Department of Physics and Applied Physics 95.141, Fall 2013, Lecture 5
Relative Motion: Clicker Quiz
A helicopter moving at a constant horizontal velocity to the right drops a package when at position A. Which of the marked trajectories is closest to that observed by a person on the helicopter?
observer
Department of Physics and Applied Physics 95.141, Fall 2013, Lecture 5
Solving Problems Involving Projectile Motion
1. Read the problem carefully, and choose the object(s) you are going to analyze.
2. Draw a diagram.
3. Choose an origin and a coordinate system.
4. Decide on the time interval; this is the same in both directions, and includes only the time the object is moving with constant acceleration g.
5. Examine the x and y motions separately.
6. List known and unknown quantities. Remember that vx never changes, and that vy = 0 at the highest point.
7. Plan how you will proceed. Use the appropriate equations; you may have to combine some of them.
Department of Physics and Applied Physics 95.141, Fall 2013, Lecture 5
Thank you See you on Monday