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Chapter 2 Motion in One Dimension

Chapter 2 Motion in One Dimension

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Chapter 2 Motion in One Dimension. Motion is relative. An object can be moving with respect to one object and at the same time be at rest or moving at a different speed with respect to another. Frame of Reference. Is the point with which a motion is described. - PowerPoint PPT Presentation

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Page 1: Chapter 2  Motion in One Dimension

Chapter 2 Motion in

One Dimension

Page 2: Chapter 2  Motion in One Dimension

Motion is relative.

Page 3: Chapter 2  Motion in One Dimension

An object can be moving with respect to one object and at the same time be at rest or moving at a different speed with respect to another.

Page 4: Chapter 2  Motion in One Dimension

Frame of Reference

Is the point with which a motion is described.

Page 5: Chapter 2  Motion in One Dimension

How fast are you moving

at this moment?

Page 6: Chapter 2  Motion in One Dimension

Depends upon how you look at it?

If you look at it from the point of view with the room, most of you are not moving.

Page 7: Chapter 2  Motion in One Dimension

If you look at it from the point of view from outer space, then you are moving as fast as the earth is rotating.

Page 8: Chapter 2  Motion in One Dimension

Or from out side the solar system, the earth is moving

around the sun at a speed of

approximately 100,000 km/hr.

Page 9: Chapter 2  Motion in One Dimension

Relative Motion Animation

Page 10: Chapter 2  Motion in One Dimension

Vector A physical quantity that has both magnitude and direction.

Page 11: Chapter 2  Motion in One Dimension

Ex:10 km, North

15 m/s, SW

Page 12: Chapter 2  Motion in One Dimension

ScalarA physical quantity that has magnitude, but no direction.

Page 13: Chapter 2  Motion in One Dimension

Ex: 55 km/hr

19 m

Page 14: Chapter 2  Motion in One Dimension

Distance How far an object has moved.

No direction, therefore a scalar.

Ex: 20 km

Page 15: Chapter 2  Motion in One Dimension

DisplacementThe change in position of an

object

Page 16: Chapter 2  Motion in One Dimension

Difference b/n Distance & Displacement

Page 17: Chapter 2  Motion in One Dimension

Displacement

=

Change in position

=Final position – Initial position

Page 18: Chapter 2  Motion in One Dimension

x = xf – xi

Page 19: Chapter 2  Motion in One Dimension

Note: Displacement is not always equal to distance moved.

Page 20: Chapter 2  Motion in One Dimension

Displacement has a specific

direction, therefore it is a

vector.

Page 21: Chapter 2  Motion in One Dimension

Displacement can be positive (+) or negative

(-).

Page 22: Chapter 2  Motion in One Dimension

On the x-axis displacement to the right is (+) and displacement to the left is (-).

On the y-axis displacement upwards is (+) and displacement downwards is (-).

Page 23: Chapter 2  Motion in One Dimension

Speed

Measure of how fast something

is moving.

Page 24: Chapter 2  Motion in One Dimension

Is the distance covered per unit of time.

ex: 72 km/hr or 20 m/s

Page 25: Chapter 2  Motion in One Dimension

Speed Unitsm/s, km/hr, or cm/s, same as velocity units.

Since speed has no direction, it is a scalar.

Page 26: Chapter 2  Motion in One Dimension

The fast speed possible is the speed of light.

Which is 3 x 108 m/s (299,792,458 m/s)

Page 27: Chapter 2  Motion in One Dimension

Instantaneous Speed

Is the speed of an object at any instant.

Page 28: Chapter 2  Motion in One Dimension

Instantaneous Speed

Is the speed of an object at any instant.Ex: speedometer reading

Page 29: Chapter 2  Motion in One Dimension

Average SpeedThe total distance divided by the time

interval during which the displacement occurred. (Vavg)

Page 30: Chapter 2  Motion in One Dimension

Change in position

Vavg = ---------------------- Change in time

total distance = -----------------------

time interval

Page 31: Chapter 2  Motion in One Dimension

Xvavg = ------ t

Page 32: Chapter 2  Motion in One Dimension

xf – xi

vavg = --------- t

Page 33: Chapter 2  Motion in One Dimension
Page 34: Chapter 2  Motion in One Dimension

The cheetah averages 70 m/s over 30 seconds. How far does it travel in those 30 seconds?

                            

   

Page 35: Chapter 2  Motion in One Dimension

VelocityIs the rate of change

of displacement.It is speed with a direction. (vector)

Page 36: Chapter 2  Motion in One Dimension

The Vavg can

be (+) or (-), depending on the sign of the displacement.

Page 37: Chapter 2  Motion in One Dimension

Three Ways to Change Velocity 

Page 38: Chapter 2  Motion in One Dimension

Three Ways to Change Velocity 

Page 39: Chapter 2  Motion in One Dimension

Ex 1: During a trip, a plane flies directly

East with an average velocity of 35 m/s. What distance does

the plane cover in 45 minutes?

Page 40: Chapter 2  Motion in One Dimension

G: Vavg = 35 m/s, t= 45 min= 2700 s

U: X = ?

E: X = (Vavg )(t)S: X=(35m/s)(2700s)S: X = 94,500 m, E

Page 41: Chapter 2  Motion in One Dimension

With your group, work together to solve practice problems: 2, 4, and 6 on page 44 (HP). Do these

problems in your notes. I will check for them in the

notebook check. Also use the GUESS method.

Page 42: Chapter 2  Motion in One Dimension

2) 3.1 km4) 3 hr6a) 6.4 Hour6b) 77 km/hr South

Page 43: Chapter 2  Motion in One Dimension

Velocity is not the same as

speed.

Page 44: Chapter 2  Motion in One Dimension

Uniform MotionBoth velocity/speed and direction of the body/object remain

the same.

Page 45: Chapter 2  Motion in One Dimension

Accelerated Motion

Is when the velocity/speed of

the object is changing.

Page 46: Chapter 2  Motion in One Dimension

Acceleration (aavg)

Is the rate of change of velocity.

How fast you change your velocity

Page 47: Chapter 2  Motion in One Dimension

How do you know your accelerating?

Page 48: Chapter 2  Motion in One Dimension

How do you know your accelerating?

Page 49: Chapter 2  Motion in One Dimension

aavg has direction and magnitude; therefore, it is a

vector.

Page 50: Chapter 2  Motion in One Dimension

Change in Velocity

aavg = ---------------

Time interval

for change

Page 51: Chapter 2  Motion in One Dimension

v vf – vi

aavg = --- = ---------

t t

Page 52: Chapter 2  Motion in One Dimension
Page 53: Chapter 2  Motion in One Dimension

Units: m/s2 or cm/s2

Page 54: Chapter 2  Motion in One Dimension

If acceleration is negative (-) it means the object is slowing down or decelerating

Page 55: Chapter 2  Motion in One Dimension

Uniform Accelerated Motion

Constant acceleration,meaning the velocity changes by

the same amount each time interval.

Page 56: Chapter 2  Motion in One Dimension

Ex 2: A car slows down with an acceleration of –1.5 m/s2. How long does it take for the car to stop

from 15.0 m/s to 0.0 m/s?

Page 57: Chapter 2  Motion in One Dimension

G: aavg = -1.5 m/s2, vf = 0.0m/s vi = 15 m/s

U: t = ?

E: aavg = (vf – vi) / t

or t = (vf – vi) / aavg

Page 58: Chapter 2  Motion in One Dimension

t = (0m/s – 15 m/s)

(-1.5 m/s2)

t = 10 s

Page 59: Chapter 2  Motion in One Dimension

Do practice problems, on page 49 (HP), #2 and 4.

Work together with groups. These must be in

notes and you need to use the GUESS Method

to solve them.

Page 60: Chapter 2  Motion in One Dimension

Displacement (x) depends upon: aavg, vi ,

and t.

Page 61: Chapter 2  Motion in One Dimension

For an object moving with a uniform acceleration.

The vavg is the average of the vi and the vf.

Page 62: Chapter 2  Motion in One Dimension

vi + vf

vavg = ------- 2

Page 63: Chapter 2  Motion in One Dimension

By setting both vavg equations equal to each

other.

x vi + vf

----- = ------- t 2

Page 64: Chapter 2  Motion in One Dimension

Multiply both side by t

x = ½ (vi + vf)t

Page 65: Chapter 2  Motion in One Dimension

Ex 3: Adam, in his AMC Pacer, is moving at a velocity of 27 m/s, he applies the brakes and comes to a stop in 5.5 seconds. How far did

move before he came to a stop?

Page 66: Chapter 2  Motion in One Dimension

G: vi =27 m/s vf =0 m/s t= 5.5 s

U: x E: x = ½ (vi + vf)tS: x = ½(27 m/s+

0m/s)5.5sS: x = 74.3 m

Page 67: Chapter 2  Motion in One Dimension

Final velocity (vf) depends upon: vi,

t, & aavg

From the aavg equation:

Page 68: Chapter 2  Motion in One Dimension

Multiple both sides by time

(t)

aavgt = vf - vi

Page 69: Chapter 2  Motion in One Dimension

Then add vi to both sides.

vf = vi + aavgt

Page 70: Chapter 2  Motion in One Dimension

Ex 4: A pilot flying at 60 m/s opens the throttles

to the engines, uniformly accelerating the jet at a rate of 0.75

m/s2 for 8 seconds, what is his final speed?

Page 71: Chapter 2  Motion in One Dimension

G: aavg= 0.75 m/s2, t=8s, vi= 60 m/s

U: vf = ?

E: vf = vi + aavg t

S: vf =60 m/s +

(0.75m/s2 x 8 s)S: vf = 66 m/s

Page 72: Chapter 2  Motion in One Dimension

With our final speed equation, we can

substitute it into the x equation. This allows us to find x without

knowing vf.

Page 73: Chapter 2  Motion in One Dimension

We are going to substitute

vf = vi + aavgt into

x = ½ (vi + vf)t

Page 74: Chapter 2  Motion in One Dimension

Where vf is, replace it with

(vi + aavgt)x = ½ (vi + vi + aavgt)t

x = ½ (2vit + aavgt2)

x = vit + ½ aavgt2

Page 75: Chapter 2  Motion in One Dimension

Ex 5: A plane flying at 80 m/s is uniformly

accelerated at a rate of 2 m/s2. What distance will it travel during a 10 second interval after acceleration

begins?

Page 76: Chapter 2  Motion in One Dimension

G: t= 10 s, a =2m/s2, vi = 80 m/s,

U: x = ?

E: x = vit + ½ a t2

S: x = (80 m/s)(10 s) + ½(2 m/s2)(10 s)2

S: x = 900 m

Page 77: Chapter 2  Motion in One Dimension

Open books to page 56 and read it. Try

and follow the algebra and

substitution for our last equation.

Page 78: Chapter 2  Motion in One Dimension

Final velocity after any displacement.

vf2 = vi

2 + 2aavgx

Page 79: Chapter 2  Motion in One Dimension

Ex 6: A bullet leaves the barrel of a gun, 0.5 m long, with a muzzle

velocity of 500 m/s. Find (a) its acceleration and

(b) the time it was in the barrel.

Page 80: Chapter 2  Motion in One Dimension

G: x=0.5 m, vf =500m/s, vi = 0 m/s

U: aavg = ?

E: vf2 – vi

2 = 2aavgx or aavg = (vf

2 – vi2) / 2x

S: aavg =(500 2 – 0 2)/(2 x 0.5)

S: aavg = 2.5 x 105 m/s2

Page 81: Chapter 2  Motion in One Dimension

G: x =0.5 m, vf =500m/s vi = 0 m/s

U: t = ?

E: x = vit + ½ aavgt2 or t2 = 2 x /aavg

S: t2 = 2(0.5) / 2.5 x 105 S: t = 0.002 s

Page 82: Chapter 2  Motion in One Dimension

Free Falling Objects

Galileo showed that a body falls with a

constant acceleration of 9.81 m/s2.

Page 83: Chapter 2  Motion in One Dimension

Acceleration of Gravity

g = – 9.81 m/s2

(For convenience we will use –

10 m/s2)

Page 84: Chapter 2  Motion in One Dimension

That means after 1 sec the object will have increased its

speed by 10 m/s.So if starting from rest:

After 1 sec – 10 m/sAfter 2 sec – 20 m/sAfter 3 sec – 30 m/s

Page 85: Chapter 2  Motion in One Dimension

Ex 7: A stone dropped from a cliff hits the

ground 3 seconds later. Find (a) the speed with which the stone hits the

ground, and (b) the distance it fell.

Page 86: Chapter 2  Motion in One Dimension

G: t =3 sec,vi =0 m/s aavg = g = - 10 m/s2

U: vf = ?

E: vf = vi + aavgt

S:vf=0 m/s+(- 10 m/s2)(3s)

S: vf = - 30 m/s

Page 87: Chapter 2  Motion in One Dimension

G: t =3 sec, vi =0 m/s aavg = g = –9.81 m/s2

U: x= ?

E: x = vi t + ½ aavgt 2

S: x = (0 m/s)(3 s) + ½ (– 10 m/s2)(3 s)2

S: x = – 45 m

Page 88: Chapter 2  Motion in One Dimension

Free falling bodies always have the same downward acceleration

Even though an object may be moving upwards, its acceleration is downwards.

Page 89: Chapter 2  Motion in One Dimension

The velocity is positive, but is decreasing.

When it reaches the peak, the velocity is

zero, but still accelerating downwards.

Page 90: Chapter 2  Motion in One Dimension

Then the object begins to fall with

a negative velocity.

Page 91: Chapter 2  Motion in One Dimension

A ball is thrown straight up with

an initial velocity of 30 m/s.

Page 92: Chapter 2  Motion in One Dimension

t (s) y (m) Vf (m/s) Aavg

(m/s2)0.001.002.003.004.005.006.00

Page 93: Chapter 2  Motion in One Dimension

t (s) y (m) Vf (m/s) Aavg

(m/s2)0.00 -101.00 -102.00 -103.00 -104.00 -105.00 -106.00 -10

Page 94: Chapter 2  Motion in One Dimension

t (s) y (m) Vf (m/s) Aavg

(m/s2)

0.00 30 -101.00 20 -102.00 10 -103.00 0 -104.00 -10 -105.00 -20 -106.00 -30 -10

Page 95: Chapter 2  Motion in One Dimension

t (s) y (m) Vf (m/s) Aavg

(m/s2)

0.00 0 30 -101.00 25 20 -102.00 40 10 -103.00 45 0 -104.00 40 -10 -105.00 25 -20 -106.00 0 -30 -10

Page 96: Chapter 2  Motion in One Dimension

Ex 8: Amber hits a volleyball, so that it moves with an initial

velocity of 6m/s straight upward. If the ball starts from 2 m off the floor. How long will it remain in the air before hitting

the floor? Assume she is the last person to touch it.

Page 97: Chapter 2  Motion in One Dimension

G: Vi = 6 m/s, x = -2 m, aavg= -10 m/s2

U: t :There is no easy equation to use so we need to find t

Page 98: Chapter 2  Motion in One Dimension

So we need to find the Vf first.

E: vf2 = vi

2 + 2aavgx

S: vf2 =(6m/s)2 +

2(-10 m/s2)(- 2m)S: vf = +/- 8.7 m/s, since its

moving downwards its – 8.7 m/s

Page 99: Chapter 2  Motion in One Dimension

Now we can find the time t.

E: aavg = (vf – vi) / t or

t = (vf – vi) / aavg

S: t = (- 8.7 m/s – 6m/s) / (-10 m/s2)

S: t = 1.47 s