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Physics 211: Lecture 2 Todays Agenda

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The speed of the balls when they hit the ground are vA and vB respectively. ... Since the motion up and back down is symmetric, intuition should tell you that v ... – PowerPoint PPT presentation

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Title: Physics 211: Lecture 2 Todays Agenda


1
Physics 211 Lecture 2Todays Agenda
  • Recap of 1-D motion with constant acceleration
  • 1-D free fall has constant acceleration
  • Review of Vectors
  • Halftime
  • 3-D Kinematics
  • Shoot the monkey
  • Baseball
  • Independence of x and y components

2
Review
  • For constant acceleration we found

x
t
v
  • From which we derived

t
a
t
3
Recall what you saw
4
1-D Free-Fall
  • This is a nice example of constant acceleration
    (gravity)
  • In this case, acceleration is caused by the force
    of gravity
  • Usually pick y-axis upward
  • Acceleration of gravity is down

y
t
v
t
a
y
t
ay ? g
5
Gravity facts
Penny feather
  • g does not depend on the nature of the material!
  • Galileo (1564-1642) figured this out without
    fancy clocks rulers!
  • On the surface of the earth, gravity acts to give
    a constant acceleration
  • demo - feather penny in vacuum
  • Nominally, g 9.81 m/s2
  • At the equator g 9.78 m/s2
  • At the North pole g 9.83 m/s2
  • More on gravity in a few lectures!

6
Problem
  • The pilot of a hovering helicopter drops a lead
    brick from a height of 1000 m. How long does it
    take to reach the ground and how fast is it
    moving when it gets there? (neglect air
    resistance)

7
Problem
  • First choose coordinate system.
  • Origin and y-direction.
  • Next write down position equation
  • Realize that v0y 0.

1000 m
y 0
8
Problem
  • Solve for time t when y 0 given that y0 1000
    m.
  • Recall
  • Solve for vy

y0 1000 m
y 0
9
Lecture 2, Act 11D free fall
  • Alice and Bill are standing at the top of a cliff
    of height H. Both throw a ball with initial
    speed v0, Alice straight down and Bill straight
    up. The speed of the balls when they hit the
    ground are vA and vB respectively. Which of the
    following is true
  • (a) vA lt vB (b) vA vB (c) vA gt
    vB

v0
Bill
Alice
v0
H
vA
vB
10
Lecture 2, Act 11D Free fall
  • Since the motion up and back down is symmetric,
    intuition should tell you that v v0
  • We can prove that your intuition is correct

Equation
This looks just like Bill threw the ball down
with speed v0, sothe speed at the bottom
shouldbe the same as Alices ball.
Bill
v0
v v0
H
y 0
11
Lecture 2, Act 11D Free fall
  • We can also just use the equation directly

Alice
same !!
Bill
v0
Alice
Bill
v0
y 0
12
Vectors
  • A vector is an object with both magnitude and
    direction.
  • In 1 dimension, we could specify direction with a
    or - sign. For example, in the previous
    problem ay -g etc.
  • In 2 or 3 dimensions, we need more than a sign to
    specify the direction of something
  • To illustrate this, consider the position vector
    r in 2 dimensions.

13
Vectors...
  • There are two common ways of indicating that
    something is a vector quantity
  • Boldface notation A
  • Arrow notation

A
14
Vectors...
  • The components (in a particular coordinate
    system) of r, the position vector, are its
    (x,y,z) coordinates in that coordinate system
  • r (rx ,ry ,rz ) (x,y,z)
  • Consider this in 2-D (since its easier to draw)
  • rx x r cos ???
  • ry y r sin ???

where r r
(x,y)
y
????arctan( y / x )
r
?
x
15
Vectors...
  • The magnitude (length) of r is found using the
    Pythagorean theorem

r
y
x
  • The length of a vector clearly does not depend on
    its direction.

16
Unit Vectors
  • A Unit Vector is a vector having length 1 and no
    units
  • It is used to specify a direction
  • Unit vector u points in the direction of U
  • Often denoted with a hat u รป
  • Useful examples are the Cartesian unit vectors
    i, j, k
  • point in the direction of the x, y and z axes

17
Vector addition
  • Consider the vectors A and B. Find A B.

B
B
A
A
A
C A B
B
  • To add two vectors, place the head of one at the
    tail of the other
  • We can arrange the vectors as we want, as long as
    we maintain their length and direction!!

18
Vector addition using components
  • Consider C A B.
  • (a) C (Ax i Ay j) (Bx i By j) (Ax
    Bx)i (Ay By)j
  • (b) C (Cx i Cy j)
  • Comparing components of (a) and (b)
  • Cx Ax Bx
  • Cy Ay By

By
C
B
Bx
A
Ay
Ax
19
Lecture 2, Act 2Vectors
  • Vector A (0,2,1)
  • Vector B (3,0,2)
  • Vector C (1,-4,2)

What is the resultant vector, D, from adding
ABC?
(a) (3,5,-1) (b) (4,-2,5) (c) (5,-2,4)
20
Lecture 2, Act 2Solution
D (AXi AYj AZk) (BXi BYj BZk) (CXi
CYj CZk) (AX BX CX)i (AY BY
CY)j (AZ BZ CZ)k (0 3 1)i (2 0
- 4)j (1 2 2)k 4,-2,5
21
3-D Kinematics !!!
  • The position, velocity, and acceleration of a
    particle in 3 dimensions can be expressed as
  • r x i y j z k
  • v vx i vy j vz k (i , j , k
    unit vectors )
  • a ax i ay j az k
  • We have already seen the 1-D kinematics equations

What are the units of these vectors?
22
3-D Kinematics
  • For 3-D, we simply apply the 1-D equations to
    each of the component equations.
  • Which can be combined into the vector
    definitions
  • r r(t) v dr / dt a d2r / dt2

23
3-D Kinematics
  • So for constant acceleration we can integrate to
    get
  • a const
  • v v0 a t
  • r r0 v0 t 1/2 a t2
  • (where a, v0, and r0, are all constant vectors
    and
  • v(t) and r(t)
  • are vectors that are functions of time)

24
2-D Kinematics
  • Most 3-D problems can be reduced to 2-D problems
    when acceleration is constant
  • Choose y axis to be along direction of
    acceleration
  • Choose x axis to be along the other direction
    of motion
  • Example Throwing a baseball (neglecting air
    resistance)
  • Acceleration is constant (gravity)
  • Choose y axis up ay -g
  • Choose x axis along the ground in the direction
    of the throw

25

x and y components of motion are independent.
Cart
  • A man on a train tosses a ball straight up in the
    air.
  • View this from two reference frames

26
Lecture 2, Act 3Motion in 2D
  • Two footballs are thrown from the same point on a
    flat field. Both are thrown at an angle of 30o
    above the horizontal. Ball 2 has twice the
    initial speed of ball 1. If ball 1 is caught a
    distance D1 from the thrower, how far away from
    the thrower D2 will the receiver of ball 2 be
    when he catches it?
  • Assume the receiver and QB are the same height
  • (a) D2 2D1 (b) D2 4D1 (c) D2 8D1

27
Lecture 2, Act 3Solution
  • The distance a ball will go is simply x
    (horizontal speed) x (time in air) v0x t

28
Lecture 2, Act 3Solution
x v0x t
  • So the time spent in the air is proportional to
    v0y
  • Since the angles are the same, both v0y and v0x
    for ball 2are twice those of ball 1.
  • Ball 2 is in the air twice as long as ball 1, but
    it also has twice the horizontal speed, so it
    will go 4 times as far!!

29
Problem
  • Barry Bonds clobbers a fastball toward
    center-field. The ball is hit 1 m (yo ) above
    the plate, and its initial velocity is 36.5 m/s
    (v ) at an angle of 30o (?) above horizontal.
    The center-field wall is 113 m (D) from the plate
    and is 3 m (h) high.
  • What time does the ball reach the fence?
  • Does Barry get a home run?

v
h
?
y0
D
30
Problem...
  • Choose y axis up.
  • Choose x axis along the ground in the direction
    of the hit.
  • Choose the origin (0,0) to be at the plate.
  • Say that the ball is hit at t 0, x(0) x0
    0. y(0) y0 1m
  • Equations of motion are
  • vx v0x vy v0y - gt
  • x vxt y y0 v0y t - 1/ 2 gt2

y
x
31
Problem...
  • Use geometry to figure out v0x and v0y

g
Find v0x v cos ?. and v0y v sin ?.
y
v
v0y
?
y0
v0x
x
32
Problem...
  • The time to reach the wall is t D / vx
    (easy!)
  • We have an equation that tell us y(t) y0 v0y
    t - g t2/ 2
  • So, were done....now we just plug in the
    numbers
  • Find
  • vx 36.5 cos(30) m/s 31.6 m/s
  • vy 36.5 sin(30) m/s 18.25 m/s
  • t (113 m) / (31.6 m/s) 3.58 s
  • y(t) (1.0 m) (18.25 m/s)(3.58 s)

    - (0.5)(9.8 m/s2)(3.58 s)2
  • (1.0 65.3 - 62.8) m 3.5 m
  • Since the wall is 3 m high, Bonds gets the
    homer!!

33
Lecture 2, Act 42D free fall
  • Alice and Bill are standing at the top of a
    cliff. Alice drops her ball at the same time
    that Bill throws his horizontally as hard as he
    can. Which ball hits the ground first?
  • (a) Alices (b) Bills (c) both hit at the
    same time

Alice
Bill
34
Shooting the Monkey(tranquilizer gun)
  • Where does the zookeeper aim if he wants to hit
    the monkey?
  • ( He knows the monkey willlet go as soon as he
    shoots ! )

35
Shooting the Monkey...

r r0
  • If there were no gravity, simply aim

at the monkey
r v0t
36
Shooting the Monkey...
r r0 - 1/2 g t2
  • With gravity, still aim at the monkey!

r v0 t - 1/2 g t2
37
RecapShooting the monkey...
x v0 t y -1/2 g t2
  • This may be easier to think about.
  • Its exactly the same idea!!
  • They both have the same Vy(t) in this case

x x0 y -1/2 g t2
38
Recap of Lecture 2
  • Recap of 1-D motion with constant acceleration.
    (Text 2-3)
  • 1-D Free-Fall
  • example
  • Review of Vectors (Text 1-6)
  • 3-D Kinematics (Text 3-1 3-2)
  • Shoot the monkey
  • Baseball problem
  • Independence of x and y components
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