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2015-06-16
1
© 2012 Pearson Education, Inc. Slide 1-1
PreClass Notes: Chapter 2
• From Essential University Physics 3rd Edition
• by Richard Wolfson, Middlebury College
• ©2016 by Pearson Education, Inc.
• Narration and extra little notes by Jason Harlow,
University of Toronto
• This video is meant for University of Toronto
students taking PHY131.
© 2012 Pearson Education, Inc. Slide 1-2
Outline
“The study of motion without
regard to its cause is called
kinematics” – R.Wolfson
• 2.1 Average Velocity
• 2.2 Instantaneous Velocity
• 2.3 Acceleration
• 2.4 Constant Acceleration
• 2.5 Acceleration due to
Gravity, Freefall
• 2.6 Non-constant
Acceleration
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© 2012 Pearson Education, Inc. Slide 1-3
Position and Displacement
• In one dimension, position can be described by a
positive or negative number on a number line, also
called a coordinate system.
– Position zero, the origin of the coordinate system, is
arbitrary and you’re free to choose it wherever it’s
convenient.
• Displacement is change in position.
– For motion along the x direction, displacement is
designated ∆x:
∆x = x2–x1
where x1 and x2 are the initial and final positions,
respectively.
© 2012 Pearson Education, Inc. Slide 1-4
Constant Velocity
For uniform motion, the
position-versus-time
graph is a straight line
The average velocity is
the slope of the position-
versus-time graph
The SI units of velocity
are m/s.
𝑣 =∆𝑥
∆𝑡= slope of the position vs. time graph
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© 2012 Pearson Education, Inc. Slide 1-5
Vocabulary Review…
The distance an object travels is a scalar quantity (no
direction given, always positive)
The displacement of an object is a vector quantity,
equal to the final position minus the initial position
An object’s speed v is scalar quantity (no direction
given, always positive)
Velocity is a vector quantity that includes direction
In one dimension, the direction of velocity is specified
by the + or − sign
© 2012 Pearson Education, Inc. Slide 1-6
Example 1: You drive from
International Falls to Des Moines in
10 hr. What was your displacement
and average velocity?
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© 2012 Pearson Education, Inc. Slide 1-7
GOT IT?
• When an object moves from one point in space to
another, the magnitude of its displacement is
A. either less than or equal to the distance traveled.
B. either greater than or equal to the distance traveled.
C. either greater than or smaller than the distance
traveled.
D. always equal to the distance traveled.
E. either greater than, smaller than, or equal to the
distance traveled.
© 2012 Pearson Education, Inc. Slide 1-8
Instantaneous Velocity
An object that is speeding up or slowing down is not in
uniform motion
In this case, the position-versus-time graph is not a straight
line
We can determine the average speed 𝑣 between any two
times separated by time interval Δt by finding the slope of the
straight-line connection between the two points
The instantaneous velocity is the is the object’s velocity at a
single instant of time t
The average velocity 𝑣 = Δx/Δt becomes a better and better
approximation to the instantaneous velocity as Δt gets smaller
and smaller
𝑣 = lim∆𝑡→0
∆𝑥
∆𝑡=𝑑𝑥
𝑑𝑡
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© 2012 Pearson Education, Inc. Slide 1-9
Instantaneous Velocity
The instantaneous velocity at time t is the average velocity
during a time interval Δt centered on t, as Δt approaches zero
In calculus, this is called the derivative of x with respect to t
Graphically, Δx/Δt is the slope of a straight line
In the limit Δt 0, the straight line is tangent to the curve
The instantaneous velocity at time t is the slope of the line
that is tangent to the position-versus-time graph at time t
v = the slope of the position-versus-time graph at t
© 2012 Pearson Education, Inc. Slide 1-10
GOT IT?
• The figure shows position-versus-time graphs for four
objects. Which starts slowly and then speeds up?
A. B. C. D.
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© 2012 Pearson Education, Inc. Slide 1-11
Using Calculus to Find Derivatives
• In calculus, the derivative gives the result of the
limiting procedure.
– Derivatives of powers are straightforward:
– Other common derivatives include the trig functions:
© 2012 Pearson Education, Inc. Slide 1-12
Acceleration
• Sometimes an object’s velocity changes as it moves.
• Acceleration describes a change in velocity.
• Consider an object whose velocity changes from to
during the time interval ∆t.
• The quantity is the change in velocity.
• The rate of change of velocity is called the average
acceleration:
The Yamaha VMAX accelerates
from 0 to 60 mph in 2.5 s.
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© 2012 Pearson Education, Inc. Slide 1-13
Acceleration
Imagine a competition between a
Volkswagen Beetle and a Porsche
to see which can achieve a velocity
of 30 m/s in the shortest time
The table shows the velocity of
each car, and the figure shows the
velocity-versus-time graphs
Both cars achieved every
velocity between 0 and 30 m/s, so
neither is faster
But for the Porsche, the rate at
which the velocity changed was ∆𝑣
∆𝑡=30 m/s
6.0 s= 5.0 (m/s)/s
© 2012 Pearson Education, Inc. Slide 1-14
Motion with Constant Acceleration
The SI units of acceleration are (m/s)/s, or m/s2
It is the rate of change of velocity, and measures how
quickly or slowly an object’s velocity changes
The average acceleration during a time interval Δt is
Graphically, 𝑎 is the slope of a straight-line velocity-versus-
time graph
If acceleration is constant, the acceleration a is the same as
𝑎.
Acceleration, like velocity, is a vector quantity and has both
magnitude and direction
𝑎 =∆𝑣
∆𝑡
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© 2012 Pearson Education, Inc. Slide 1-15
GOT IT?
• What is the slope of a line connecting two points
on a velocity-versus-time graph?
A. Instantaneous velocity
B. Average velocity
C. Average acceleration
D. Instantaneous acceleration
E. None of the above
© 2012 Pearson Education, Inc. Slide 1-16
Chapter 2 Big Idea
• From the Chapter 2 Summary on page 27:
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© 2012 Pearson Education, Inc. Slide 1-17
Motion with constant velocity Motion with constant acceleration
t
x
t
x
t
v
t
v
t
a
t
a
© 2012 Pearson Education, Inc. Slide 1-18
Constant Acceleration
• When acceleration is constant, then position,
velocity, acceleration, and time are related by
where x0 and v0 are initial values at time t = 0, and x
and v are the values at an arbitrary time t.
0
10 02
210 0 2
2 2
0 02
v v at
x x v v t
x x v t at
v v a x x
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© 2012 Pearson Education, Inc. Slide 1-19
2.5 The Acceleration of Gravity
The motion of an object moving
under the influence of gravity only,
and no other forces, is called free
fall
Two objects dropped from the
same height will, if air resistance
can be neglected, hit the ground at
the same time and with the same
speed
Consequently, any two objects in
free fall, regardless of their mass,
have the same acceleration:
The apple and feather seen
here are falling in a vacuum.
© 2012 Pearson Education, Inc. Slide 1-20
The Acceleration of Gravity
The velocity graph is a
straight line with a slope:
where g is a positive
number which is equal to
9.80 m/s2 on the surface
of the earth
Other planets have
different values of g
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© 2012 Pearson Education, Inc. Slide 1-21
The Acceleration of Gravity
• The equations for constant acceleration apply for
free fall.
– In a coordinate system with y axis upward, they
read:
0
10 02
210 0 2
2 2
0 02
v v gt
y y v v t
y y v t gt
v v g y y
© 2012 Pearson Education, Inc. Slide 1-22
2.6 Non-Constant Acceleration
Figure (a) shows a realistic
velocity-versus-time graph for a car
leaving a stop sign
The graph is not a straight line, so
this is not motion with a constant
acceleration
Figure (b) shows the car’s
acceleration graph
The instantaneous acceleration a
is the slope of the line that is tangent
to the velocity-versus-time curve at
time t
a = the slope of the velocity-versus-time graph at t
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© 2012 Pearson Education, Inc. Slide 1-23
Finding Velocity from Acceleration
Suppose we know an object’s velocity to be v1 at an initial
time t1
We also know the acceleration as a function of time
between t1 and some later time t2
We can compute the final velocity as
The integral may be interpreted graphically as the area
under the acceleration curve as between t1 and t2
𝑣2 = 𝑣1 + 𝑡1
𝑡2
𝑎 𝑑𝑡