Kinematics
the description of motion
(2.1) Motion along a Straight Line
average velocity, vav-x – displacement divided by time interval
vav-x = x2 – x1 t2 – t1
= x
t
displacement, x – change in position represented by a vector from P1 to P2
ex. x1 = 19 m x2 = 277 m
x-t graphs
• slope of line connecting P1 and P2 = vav-x
(2.2) Instantaneous Velocity
• limit of average velocity as time interval shrinks to zero
vx = lim
t0 t
x dx dt
=
derivative of position with respect to time
*on x-t graph, instantaneous velocity at any point = slope
Example 2.1
a) Find the cheetah’s displacement during the time interval from t1= 1.0 s and t2 = 2.0 s
b) Find the average velocity.
c) Find the instantaneous velocity at t = 1.0 and 2.0 s
Derive an expression for the instantaneous velocity as a function of time.
Review of x-t and v
x-t graphs
x-t graph:
_________________ indicates object’s position
_________________ indicates object’s speed
_________________ indicates object’s direction
steepness of slope value on x-axis
Review of x-t and v
x-t graphs
vx-t graph:
_________________ indicates object’s speed
_________________ indicates object’s direction
value on vx-axis
sign of v
(2.3) Average and Instantaneous
Acceleration
• acceleration describes the rate of change of
velocity with time
aav-x = v2x – v1x t2 – t1
= vx
• instantaneous acceleration is the limit of average
acceleration as time interval shrinks to zero
ax = lim
t0 t
vx dvx dt
v
x-t graphs
*on vx-t graph, instantaneous
acceleration at any point = slope of tangent to
Example 2.3
vx = 60 m/s + (0.5 m/s3)t2
a) Find the average acceleration between t1 =1.0 s and t2 = 3.0 s.
Relationship between ax and x
dvx dt
ax = = dtd dtdx = dtd2x2
• ax is the second derivative of x
• second derivative is directly related to the
Concavity of
x-t graph
a
xv
xconcave up positive increasing
concave
down negative decreasing
no concavity zero constant
x
v
x
a
x
d
er
iv
at
iv
e
an
tid
(2.6) Velocity and Position by
Integration
On trans-Atlantic flights an accelerometer is used
to measure the plane’s acceleration. From these
measurements, the
velocity and position may be found.
Graphical Approach to Integrals
• since aav-x = vx/t, we
can write:
vx = aav-xt
• but that can be represented
by the area of these green rectangles
• in the limit that t0, the rectangles become very
skinny and . . .
• we can find the change in vx during some time
interval by summing the areas of all the skinny rectangles in that interval
• this process is called integration, and it’s
equivalent to finding the area under the ax-t
curve
dv
x=
a
xdt
v2x
v1x
t2
t1
= integral symbol (elongated “s” for sum)v
2x- v
1x =
a
xdt
t2
• by repeating this procedure with the vx-t graph, we
can find the change in x during some time interval
x
2– x
1 =
v
xdt
t2
t1
• if we choose t1 = 0 and t2 any later time, and if
we call the initial position x0 and the initial velocity v0x, then we have:
x
=x
0 +
v
xdt
t
0
v
x =v
0x +
a
xdt
t
x(t)
=x
0 +
v
xdt
t
0
v
x(t)
=v
0x +
a
xdt
t
0
Example 2.9
At t = 0, when Sally is driving her 1965 Mustang at 10 m/s she passes a signpost at x = 50 m. Her
acceleration is given by:
ax = 2.0 m/s2 – (0.10 m/s3) t
a) Derive expressions for her velocity and position as functions of time.
Describe Sally’s motion, then graph a vs. t
Graph v vs. t and x vs. t.
Example 2.9
At t = 0, when Sally is driving her 1965 Mustang at 10 m/s she passes a signpost at x = 50 m. Her
acceleration is given by:
ax = 2.0 m/s2 – (0.10 m/s3) t
b) At what time is her velocity greatest?
c) What is her maximum velocity?
(2.4) Motion with Constant
Acceleration
• Let’s use a calculus-based approach (just to be different from last year)
• If we assume that ax(t) = ax, then:
vx =
x =
v0x + axt
• by combining these two, we get another useful
(and familiar, I hope) equation:
vx2 =
Try problem 1.13 from ActivPhysics Online
“Car Catches Truck”
www.aw.com/young11
v0x2 + 2a
Problem 2.61
Assume the light turns yellow right now and stays yellow for 3.0 s. If the driver steps on the brake, the car slows at -3.7 m/s2. If he instead
steps on the gas pedal, the car accelerates at 3.2 m/s2. To avoid being in the intersection at
the instant that the light turns red, should the driver step on the brake or the gas?
(2.5) Free Fall
• use the equations for constant acceleration, but
in the y direction
• let ay = -g = - 9.8 m/s2
vy = v0y + ayt
y = y0 +v0yt +1/2 ayt2
vy2 = v
Sketch y, vy, and ay vs. t graphs for a ball thrown upwards at 5 m/s.
y
t
vy
t
ay
Free Fall formulas?
vy = v0y + ayt
y = y0 +v0yt +1/2 ayt2
vy2 = v
Try problem 1.7 from ActivPhysics Online
“Balloonist Drops Lemonade”