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SECTION 1 DISPLACEMENT AND VELOCITY Chapter 2 Motion in One Dimension.

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SECTION 1 DISPLACEMENT AND VELOCITY Chapter 2 Motion in One Dimension
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Page 1: SECTION 1 DISPLACEMENT AND VELOCITY Chapter 2 Motion in One Dimension.

SECTION 1DISPLACEMENT AND VELOCITY

Chapter 2 Motion in One Dimension

Page 2: SECTION 1 DISPLACEMENT AND VELOCITY Chapter 2 Motion in One Dimension.

Motion

Motion happens all around us in different directions and different speeds.

One – dimensional motion is the simplest form of motion. Example : Commuter train can move only forward

and backward along the straight track.

Page 3: SECTION 1 DISPLACEMENT AND VELOCITY Chapter 2 Motion in One Dimension.

Motion

Motion takes place over time and depends on frame of reference.

Frame of Reference – what you use to measure changes in position.

Page 4: SECTION 1 DISPLACEMENT AND VELOCITY Chapter 2 Motion in One Dimension.

Frame of Reference

Frame of reference is basically what you are using to measure changes in position of an object.

If an object is at rest (not moving), its position does not change with respect to a frame of reference.

As any object moves from one position to another, the length of the straight line drawn from its initial position to the object’s final position is called the displacement of the object.

Page 5: SECTION 1 DISPLACEMENT AND VELOCITY Chapter 2 Motion in One Dimension.

Displacement

Displacement is a change in position.

Displacement = final position – initial position.

Displacement is not always equal to the distance traveled.

Displacement can be positive or negative! in your book (unless

stated otherwise) RIGHT & UP will be considered positive and LEFT & DOWN will be considered negative.

Page 6: SECTION 1 DISPLACEMENT AND VELOCITY Chapter 2 Motion in One Dimension.

Displacement

Displacement is not always equal to the distance traveled.

Page 7: SECTION 1 DISPLACEMENT AND VELOCITY Chapter 2 Motion in One Dimension.

Displacement

Displacement can be positive or negative.

There are only two directions to move on X axis and two to move on Y axis Right : Positive Left : Negative Up: Positive Down : Negative

Page 8: SECTION 1 DISPLACEMENT AND VELOCITY Chapter 2 Motion in One Dimension.

Displacement

Page 9: SECTION 1 DISPLACEMENT AND VELOCITY Chapter 2 Motion in One Dimension.

Velocity

Average Velocity is displacement of an object (Δx) divided by time interval (Δt). Equation : vavg = Δx = xf-xi

Δt tf-ti

Average Velocity can be positive or negative depending on the sign of the displacement. If displacement is negative, avg. velocity is negative. Time interval is always positive

Page 10: SECTION 1 DISPLACEMENT AND VELOCITY Chapter 2 Motion in One Dimension.

Guided Practice

Open Books to pg. 44

Page 11: SECTION 1 DISPLACEMENT AND VELOCITY Chapter 2 Motion in One Dimension.

Velocity is not the same as speed.

Velocity describes motion with direction and magnitude (numerical value); speed has no direction, only magnitude.Ex: 55 m/s and 55 m/s North

Velocity Vs. Speed

Page 12: SECTION 1 DISPLACEMENT AND VELOCITY Chapter 2 Motion in One Dimension.

SECTION 2 ACCELERATION

Chapter 2One Dimensional Motion

Page 13: SECTION 1 DISPLACEMENT AND VELOCITY Chapter 2 Motion in One Dimension.

Velocity can be interpreted graphically…

Page 14: SECTION 1 DISPLACEMENT AND VELOCITY Chapter 2 Motion in One Dimension.

The motion of an object moving with constant velocity will provide a straight-line graph of position versus time. The slope of this graph indicates the average velocity.

Page 15: SECTION 1 DISPLACEMENT AND VELOCITY Chapter 2 Motion in One Dimension.

2-2 Acceleration

Acceleration measures the rate of change in velocity (usually per second).

Acceleration has dimensions of length divided by time squared.

The units of acceleration in SI are meters per second per second. m/s2

Page 16: SECTION 1 DISPLACEMENT AND VELOCITY Chapter 2 Motion in One Dimension.

Acceleration

Three ways to Accelerate:

Object speeding up

Object slowing down

Object changing direction

Page 17: SECTION 1 DISPLACEMENT AND VELOCITY Chapter 2 Motion in One Dimension.

Formula for Average Acceleration

Average Acceleration =

Change in velocity time required for change

ORa avg = vf – vi

tf - ti

Page 18: SECTION 1 DISPLACEMENT AND VELOCITY Chapter 2 Motion in One Dimension.

Let’s Practice with Average Acceleration...

Turn to page 49 in your books and we can work on practice 2B.

Page 19: SECTION 1 DISPLACEMENT AND VELOCITY Chapter 2 Motion in One Dimension.

Acceleration is Velocity/Time

Acceleration has direction and magnitude.

The slope and shape of a graph plotting velocity vs. time describes the object’s motion.

When velocity on graph is increasing : acceleration is positivedecreasing : acceleration is negative constant : there is no acceleration

Page 20: SECTION 1 DISPLACEMENT AND VELOCITY Chapter 2 Motion in One Dimension.

Motion with constant acceleration.

Page 21: SECTION 1 DISPLACEMENT AND VELOCITY Chapter 2 Motion in One Dimension.

Velocity Vs. Time Graphs

Page 22: SECTION 1 DISPLACEMENT AND VELOCITY Chapter 2 Motion in One Dimension.

Review - Displacement with constant uniform Acceleration

Displacement depends on acceleration, initial velocity, and time.

Displacement with constant uniform acceleration is equal to :

ΔX = ½ (initial velocity + final velocity)(time interval)

Page 23: SECTION 1 DISPLACEMENT AND VELOCITY Chapter 2 Motion in One Dimension.

Solving for Final Velocity (Vf)

Final velocity depends on initial velocity, acceleration, and time.

aavg = Δv = vf - vi

Δt tf - tiDisplacement of an object depends on initial

velocity, final velocity, and time.

Δx = ½ (vi + vf) Δt How can we solve for displacement if we don’t

have final velocity?

Page 24: SECTION 1 DISPLACEMENT AND VELOCITY Chapter 2 Motion in One Dimension.

Solving for Vf & Displacement

By rearranging the equation for acceleration, we can find a value for the final velocity.

vf = vi + aΔt

To find displacement of an object moving with uniform acceleration we substitute the above expression for vf into our displacement formula.

Δx = vi Δt + ½ a(Δt)2

Page 25: SECTION 1 DISPLACEMENT AND VELOCITY Chapter 2 Motion in One Dimension.

Guided Practice

Sample Problem 2D on pg. 55

Page 26: SECTION 1 DISPLACEMENT AND VELOCITY Chapter 2 Motion in One Dimension.

Final Velocity after Any Displacement

We can also obtain an expression that relates displacement, velocity, and acceleration without using time interval.

vf2 = vi

2 + 2aΔx

Page 27: SECTION 1 DISPLACEMENT AND VELOCITY Chapter 2 Motion in One Dimension.

Guided Practice

Sample Problem 2E pg. 57

Page 28: SECTION 1 DISPLACEMENT AND VELOCITY Chapter 2 Motion in One Dimension.

SECTION 3FALLING OBJECTS

Chapter 2 One Dimensional Motion

Page 29: SECTION 1 DISPLACEMENT AND VELOCITY Chapter 2 Motion in One Dimension.

Free Fall

Free fall is acceleration due to gravity.

Free fall acceleration is constant. Magnitude of free fall is 9.81 m/s2

Direction of free fall is directed downward. negative direction (-)

Free fall is denoted with the symbol g. (Sometimes may be ‘a’ for acceleration due to gravity)

Page 30: SECTION 1 DISPLACEMENT AND VELOCITY Chapter 2 Motion in One Dimension.

Free Fall

In a vacuum, in the absence of air resistance, all objects fall at the same rate.

Page 31: SECTION 1 DISPLACEMENT AND VELOCITY Chapter 2 Motion in One Dimension.

What goes up must come down.

What causes an object that has been thrown up into the air to come back down?

Free-Fall Acceleration due to gravity is always directed downward and pulling an object towards Earth’s surface.

Page 32: SECTION 1 DISPLACEMENT AND VELOCITY Chapter 2 Motion in One Dimension.

Recall Information

Remember we learned about a formula that can be used to find final velocity at ANY displacement…

vf2 = vi

2 + 2aΔx

We use this same formula but we change x to y

vf2 = vi

2 + 2aΔy

Page 33: SECTION 1 DISPLACEMENT AND VELOCITY Chapter 2 Motion in One Dimension.

Guided Practice

Open books to pg. 63 Sample Problem 2F


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