Describing Motion. the study of motion motion is a change in position two branches Mechanics.
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Transcript of Describing Motion. the study of motion motion is a change in position two branches Mechanics.
• Chapter 3 is about one-dimensional motion, as on a number line
Mathematical Representations of Motion—The Basics
Mathematical Representations of Motion—The Basics
• Origin: A reference point• to the left—negative• to the right—positive
Mathematical Representations of Motion—The Basics
Mathematical Representations of Motion—The Basics
• When motion is vertical:• up—positive• down—negative
Mathematical Representations of Motion—The Basics
Mathematical Representations of Motion—The Basics
• An object has moved if at one time its position is x1 and at another time its position is x2.
Mathematical Representations of Motion—The Basics
Mathematical Representations of Motion—The Basics
• An object’s position at a time can be represented by an ordered pair: (t1, x1) or (t2, x2)
Mathematical Representations of Motion—The Basics
Mathematical Representations of Motion—The Basics
DisplacementDisplacement• the change in position
between two distinct points
• often different from the distance traveled
Scalars and VectorsScalars and Vectors
• a scalar contains just one piece of information
• a vector contains two: magnitude and direction
• vectors are represented in bold: d, v, etc.
Scalars and VectorsScalars and Vectors
• for vectors in one-dimensional motion, subscripts may be used, such as dx
• this will represent a change in position
What do we know about the family’s travels?
What do we know about the family’s travels?
a. displacement = 2 km northSince displacement is a
vector, a direction must be indicated.
Example 3-1Example 3-1
What do we know about the family’s travels?
What do we know about the family’s travels?
b. the car has traveled 10 kmSince distance is a scalar, no
direction needs to be indicated.
Example 3-1Example 3-1
What do we know about the family’s travels?
What do we know about the family’s travels?
c. the displacement is zero, since its final and initial positions are the same
When d = 0, no direction is necessary.
Example 3-1Example 3-1
What do we know about the family’s travels?
What do we know about the family’s travels?
d. the car has traveled 20 km
Example 3-1Example 3-1
• the speed of an object at any one moment
• the slope of the position-time curve at that point
Instantaneous SpeedInstantaneous Speed
The slope is easy to find if the position-time curve is linear, but what if it is a
curve?We can use a tangent line.
Instantaneous SpeedInstantaneous Speed
Can you see why graph (c) is the best estimate for a
tangent line?
Instantaneous SpeedInstantaneous Speed
Be sure to recognize the difference between average
speed and instantaneous speed.
For which one can you get a speeding ticket??
Instantaneous SpeedInstantaneous Speed
AccelerationAcceleration• change in velocity with
respect to time• to calculate average
acceleration:
a =ΔvΔt
AccelerationAcceleration• average acceleration
can be calculated as the slope of a velocity-time graph
a =ΔvΔt
First Equation of MotionFirst Equation of Motion
• often used if you want to know the final velocity when you know the initial velocity and acceleration
v2x = v1x + axΔt
Determining Displacement Algebraically
Determining Displacement Algebraically
dx = ½(v1x + v2x )Δt
dx = vxΔt
Determining Displacement Geometrically
Determining Displacement Geometrically
• the area “under the curve” of a velocity-time graph is equal to the displacement of the moving object
Second Equation of Motion
Second Equation of Motion
• two common forms:
dx = v1xΔt + ½ax(Δt)²
x2 = x1 + v1xΔt + ½ax(Δt)²
Third Equation of MotionThird Equation of Motion
• two common forms:• two common forms:
dx =v2x² – v1x²
2ax
x2 = x1 +v2x² – v1x²
2ax
Equations of MotionEquations of MotionThese are used to solve most problems involving
straight-line, constant acceleration motion.
Sometimes there will be more than one possible
method.
Free FallFree Fall• an object falls under the
influence of gravity alone with negligible air resistance
• near earth’s surface:
g = gy = -9.81 m/s²
Free FallFree Fall• the equations of motion are
easily adapted by replacing the acceleration with gy:
v2y = v1y + gyΔtFirst Equation of Motion: