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TRANSCRIPT
Martha Casquete
Would you risk your live driving drunk?
Intro
Motion
Position and displacement
Average velocity and average speed
Instantaneous velocity and speed
Acceleration
Constant acceleration: A special case
Free fall acceleration
Assignments: For next class: Finish reading Ch. 2, read Chapter 3
(Vectors) HW3 Set due next Tuesday, 9/10 Pg. 48 – 52: 5, 11, 18, 40, 49 (8th edition)
Question/Observation Thursdays
Research Q/O Tuesdays with HW (due date
Tuesdays)
Units: Length, Mass, and Time
Order of magnitude calculations
Dimensional Analysis
Conversion of Units
Significant digits (on your own)
Need to know something from your experience:
◦ Average length of french fry: 3 inches or 8 cm, 0.08 m
◦ Earth to moon distance: 250,000 miles
◦ In meters: 1.6 x 2.5 X 105 km = 4 X 108 m
105.0m 108
m 104 10
2
8
ff
Example
What is the dimension of acceleration? a = v/ t 2 ( velocity / time2 ) a = ( L / T ) / T = L / T 2
Everything moves!
Motion is one of the main topics of this course
Simplification: Moving object is a particle or moves like a particle: “point object”
Simplest case: Motion along straight line, 1 dimension
Continental - McAllen
La Guardia -NY
What is motion? Change of position over time.
How can we represent position along a straight line?
Position definition: ◦ Defines a starting point: origin (x = 0), x relative to
origin ◦ Direction: positive (right or up), negative (left or down) ◦ It depends on time: t = 0 (start clock), x(t=0) does not
have to be zero.
Position has units of [Length]: meters.
x = + 2.5 m
x = - 3 m
...... F ,a ,
v
A vector quantity is characterized by having both a magnitude and a direction. ◦ Displacement, Velocity, Acceleration, Force … ◦ Denoted in boldface type with an arrow over the top.
A scalar quantity has magnitude, but no direction. ◦ Distance, Mass, Temperature, Time …
For the motion along a straight line, the direction is represented simply by + and – signs. ◦ + sign: Right or Up. ◦ - sign: Left or Down.
Any motion involves three concepts ◦ Displacement ◦ Velocity ◦ Acceleration
Displacement is a change of position in time.
Displacement:
It is a vector quantity.
It has both magnitude and direction: + or - sign
It has units of [length]: meters.
)()( iiff txtxx
x1 (t1) = + 2.5 m x2 (t2) = - 2.0 m Δx = -2.0 m - 2.5 m = -4.5 m
x1 (t1) = - 3.0 m x2 (t2) = + 1.0 m Δx = +1.0 m + 3.0 m = +4.0 m
Position is usually measured and referenced to an origin:
◦ At time= 0 seconds Joe is 10 meters to the right of the
lamp ◦ origin = lamp ◦ positive direction = to the right of the lamp ◦ position vector :
10 meters
Joe O
-x +x 10 meters
Joe xi
One second later Joe is 15 meters to the right of the lamp
Displacement is just change in position.
◦ x = xf - xi
10 meters 15 meters
O x = xf - xi = 5 meters
t = tf - ti = 1 second
xf
Displacement in space ◦ From A to B: Δx = xB – xA = 52 m – 30 m = 22 m
◦ From A to C: Δx = xc – xA = 38 m – 30 m = 8 m
◦ Sometimes displacement is confused with distance. It is important that you understand the difference between distance and displacement.
Distance is the length of a path followed by a particle ◦ from A to B: d = |xB – xA| = |52 m – 30 m| = 22 m
◦ from A to C: d = |xB – xA|+ |xC – xB| = 22 m + |38 m – 52 m| = 36 m
Displacement is not Distance.
Every day, I travel a distance of 108 miles from Brownsville/Rancho Viejo to Edinburg and back.
Every day, at 8:20pm I noticed that I have displaced myself zero miles. Where am I?
What is the distance between one side of the wall and the other in the classroom?
If I pace it, what will be my displacement?
Displacement is not Distance.
Velocity is the rate of change of position.
Velocity is a vector quantity.
Velocity has both magnitude and direction.
Velocity has a unit of [length/time]: meter/second.
Definition: ◦ Average velocity
◦ Average speed
◦ Instantaneous
velocity
avg
total distances
t
0lim
t
x dxv
t dt
t
xx
t
xv
if
avg
Average velocity
It is slope of line segment.
Dimension: [length/time].
SI unit: m/s.
It is a vector.
Displacement sets its sign.
t
xx
t
xv
if
avg
Average speed
Dimension: [length/time], m/s.
Scalar: No direction involved.
Not necessarily close to Vavg: ◦ Savg = (6m + 6m)/(3s+3s) = 2
m/s
◦ Vavg = (0 m)/(3s+3s) = 0 m/s
avg
total distances
t
Under which of the following conditions is the magnitude of the average velocity of a particle moving in one dimension smaller than the average speed over some time interval?
a) a particle moves in the +x direction without reversing.
b) a particle moves in the –x direction without reversing
c) a particle moves in the +x direction and then reverses the direction of its motion.
d) there are no conditions for which this is true
Instantaneous means “at some given instant”. The instantaneous velocity indicates what is happening at every point of time.
Limiting process: ◦ Chords approach the tangent as Δt => 0
◦ Slope measure rate of change of position
Instantaneous velocity:
It is a vector quantity.
Dimension: [Length/time], m/s.
It is the slope of the tangent line to x(t).
Instantaneous velocity v(t) is a function of time.
0lim
t
x dxv
t dt
A cheetah is crouched in ambush 20 m to the east of an observer’s blind. At time t= 0 the cheetah charges an antelope in a clearing 50 m east of the observer. The cheetah runs along a straight line. Later analysis of a videotape shows that during the first 2.0 s of the attack, the cheetah’s coordinator x varies with time according to the equation x = 20m + (5.0m/s2 )t2 a) Find the displacement of the cheetah during the interval between t1 = 1.0 s and t2 = 2.0 s
b) Find the average velocity during the same time interval. c) Find the average velocity at time t1 = 1.0 s by taking ∆t = 0.1 s. d) Derive a general expression for the instantaneous velocity as a function of time, and from it find v at t = 1.0 s and = 2.0 s.
Uniform velocity is constant velocity
The instantaneous velocities are always the same, all the instantaneous velocities will also equal the average velocity
Begin with then
t
xx
t
xv
if
x
tvxx xif
x
x(t)
t 0
xi
xf
v
v(t)
t 0 tf
vx
ti
Changing velocity (non-uniform) means an acceleration is present.
Acceleration is the rate of change of velocity.
Acceleration is a vector quantity.
Acceleration has both magnitude and direction.
Acceleration has a unit of [length/time2]: m/s2.
Definition: ◦ Average acceleration
◦ Instantaneous acceleration if
if
avgtt
vv
t
va
2
2
0lim
dt
vd
dt
dx
dt
d
dt
dv
t
va
t
Average acceleration
Velocity as a function of time
When the sign of the velocity and the acceleration are the same (either positive or negative), then the speed is increasing
When the sign of the velocity and the acceleration are in the opposite directions, the speed is decreasing
Average acceleration is the slope of the line connecting the initial and final velocities on a velocity-time graph
if
if
avgtt
vv
t
va
tavtv avgif )(
2
2
0lim
dt
vd
dt
dx
dt
d
dt
dv
t
va
t
The limit of the average acceleration as the time interval goes to zero
When the instantaneous accelerations are always the same, the acceleration will be uniform. The instantaneous acceleration will be equal to the average acceleration
September 8, 2008
Velocity and acceleration are in the same direction
Acceleration is uniform (blue arrows maintain the same length)
Velocity is increasing (red arrows are getting longer)
Positive velocity and positive acceleration
atvtv if )(
Position is a function of time:
Velocity is the rate of change of position.
Acceleration is the rate of change of velocity.
Position Velocity Acceleration
Graphical relationship between x, v, and a
)(txx
dt
dv
t
va
t
lim
00lim
t
x dxv
t dt
dt
d
dt
d
atvv 0
2
21
0 attvx
Uniform acceleration is constant
Kinematic Equations
xavv 22
0
2
tvvtvx )(2
10
Given initial conditions: ◦ a(t) = constant = a, v(t=0) = v0, x(t=0) = x0
Start with
We have
Shows velocity as a function of acceleration and
time Use when you don’t know and aren’t asked to
find the displacement
atvv 0
at
vv
t
vv
tt
vv
t
vaavg
00
0
0
0
Given initial conditions:
◦ a(t) = constant = a, v(t=0) = v0, x(t=0) = x0
Start with
Since velocity change at a constant rate, we have
Gives displacement as a function of velocity and time
Use when you don’t know and aren’t asked for the acceleration
t
x
t
xxvavg
0
tvvtvx avg )(2
10
Given initial conditions: ◦ a(t) = constant = a, v(t=0) = v0, x(t=0) = x0
Start with
We have
Gives displacement as a function of time, initial velocity and acceleration
Use when you don’t know and aren’t asked to find the final velocity
2
002
1atvxxx
tatvvtvvx )(2
1)(
2
1000
atvv 0
tvvtvx avg )(2
10
Given initial conditions: ◦ a(t) = constant = a, v(t=0) = v0, x(t=0) = x0
Start with
We have
Gives velocity as a function of acceleration and
displacement Use when you don’t know and aren’t asked for the
time
)(22 0
2
0
2
0
2 xxavxavv
a
vvt 0
at
vv
t
vaavg
0
a
vvvvvv
atvvx
2))((
2
1)(
2
12
0
2
000
Read the problem Draw a diagram ◦ Choose a coordinate system, label initial and final
points, indicate a positive direction for velocities and accelerations
Label all quantities, be sure all the units are consistent ◦ Convert if necessary
Choose the appropriate kinematic equation Solve for the unknowns ◦ You may have to solve two equations for two
unknowns
Check your results ◦ Estimate and compare ◦ Check units
An electron in a cathode-ray tube accelerates from a speed of 2.00 X 10 m/s over 1.50 cm. (a) in what time interval does the electron travel this 1.50 cm? (b) What is the acceleration
Earth gravity provides a constant acceleration. Most important case of constant acceleration.
Free-fall acceleration is independent of mass.
Magnitude: |a| = g = 9.8 m/s2
Direction: always downward, so ag is negative if define “up” as positive,
a = -g = -9.8 m/s2
Try to pick origin so that xi = 0
y
Galileo Galilei (1564 - 1642
gtvv 0
2
002
1gttvxx
Two important equation:
Begin with t0 = 0, v0 = 0, x0 = 0
So, t2 = 2|x|/g same for two balls!
Assuming the leaning tower of Pisa is 150 ft high, neglecting air resistance,
t = (21500.305/9.8)1/2 = 3.05 s
x
0
What do you need?
Ruler
Pencil
Paper
Brain
Volunteer with two fingers
This is the simplest type of motion It lays the groundwork for more complex motion Kinematic variables in one dimension
◦ Position x(t) m L ◦ Velocity v(t) m/s L/T ◦ Acceleration a(t) m/s2 L/T2 ◦ All depend on time ◦ All are vectors: magnitude and direction vector:
Equations for motion with constant acceleration: missing quantities ◦ x – x0
◦ v
◦ t
◦ a ◦ v0
2
21
0 atvtxx
tvvxx )( 021
0
September 8, 2008
atvv 0
2
21
00 attvxx
)(2 0
2
0
2xxavv