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(1)

Kinematics

the description of motion

(2)
(3)

(2.1) Motion along a Straight Line

average velocity, vav-x – displacement divided by time interval

vav-x = x2x1 t2t1

= x

t

displacement, x – change in position represented by a vector from P1 to P2

ex. x1 = 19 m x2 = 277 m

(4)

x-t graphs

• slope of line connecting P1 and P2 = vav-x

(5)

(2.2) Instantaneous Velocity

limit of average velocity as time interval shrinks to zero

vx = lim

t0 t

x dx dt

=

derivative of position with respect to time

*on x-t graph, instantaneous velocity at any point = slope

(6)

Example 2.1

(7)

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.

(8)

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

(9)

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

(10)

(2.3) Average and Instantaneous

Acceleration

acceleration describes the rate of change of

velocity with time

aav-x = v2xv1x t2t1

= vx

(11)

instantaneous acceleration is the limit of average

acceleration as time interval shrinks to zero

ax = lim

t0 t

vx dvx dt

(12)

v

x

-t graphs

*on vx-t graph, instantaneous

acceleration at any point = slope of tangent to

(13)

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.

(14)

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

(15)

Concavity of

x-t graph

a

x

v

x

concave up positive increasing

concave

down negative decreasing

no concavity zero constant

(16)

x

v

x

a

x

d

er

iv

at

iv

e

an

tid

(17)

(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.

(18)

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 . . .

(19)

• 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

x

dt

v2x

v1x

t2

t1

= integral symbol (elongated “s” for sum)

v

2x

- v

1x =

a

x

dt

t2

(20)

• 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

x

dt

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

x

dt

t

0

v

x =

v

0x +

a

x

dt

t

(21)

x(t)

=

x

0 +

v

x

dt

t

0

v

x

(t)

=

v

0x +

a

x

dt

t

0

(22)

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.

(23)

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?

(24)

(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

(25)

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

(26)

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?

(27)

(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

(28)

Sketch y, vy, and ay vs. t graphs for a ball thrown upwards at 5 m/s.

y

t

vy

t

ay

(29)

Free Fall formulas?

vy = v0y + ayt

y = y0 +v0yt +1/2 ayt2

vy2 = v

(30)

Try problem 1.7 from ActivPhysics Online

“Balloonist Drops Lemonade”

www.aw.com/young11

www.aw.com/young11

References

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