Title: Physics 211: Lecture 2 Todays Agenda
1Physics 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
2Review
- For constant acceleration we found
x
t
v
t
a
t
3Recall what you saw
41-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
5Gravity 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!
6Problem
- 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)
7Problem
- First choose coordinate system.
- Origin and y-direction.
- Next write down position equation
-
- Realize that v0y 0.
1000 m
y 0
8Problem
- Solve for time t when y 0 given that y0 1000
m. -
- Recall
- Solve for vy
-
-
y0 1000 m
y 0
9Lecture 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
10Lecture 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
11Lecture 2, Act 11D Free fall
- We can also just use the equation directly
Alice
same !!
Bill
v0
Alice
Bill
v0
y 0
12Vectors
- 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.
13Vectors...
- There are two common ways of indicating that
something is a vector quantity - Boldface notation A
- Arrow notation
A
14Vectors...
- 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
15Vectors...
- 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.
16Unit 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
17Vector 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!!
18Vector 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
19Lecture 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)
20Lecture 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
213-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?
223-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
233-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)
242-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
25x 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
26Lecture 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
27Lecture 2, Act 3Solution
- The distance a ball will go is simply x
(horizontal speed) x (time in air) v0x t
28Lecture 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!!
29Problem
- 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
30Problem...
- 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
31Problem...
- Use geometry to figure out v0x and v0y
g
Find v0x v cos ?. and v0y v sin ?.
y
v
v0y
?
y0
v0x
x
32Problem...
- 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!!
33Lecture 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
34Shooting 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 ! )
35Shooting the Monkey...
r r0
- If there were no gravity, simply aim
at the monkey
r v0t
36Shooting the Monkey...
r r0 - 1/2 g t2
- With gravity, still aim at the monkey!
r v0 t - 1/2 g t2
37RecapShooting 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
38Recap 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