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Motion in One Dimension Chapter 2. 2.1 Displacement & Velocity Learning Objectives. Describe motion in terms of displacement, time, and velocity Calculate the displacement of an object traveling at a known velocity for a specific time interval
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2.1 Displacement & VelocityLearning Objectives • Describe motion in terms of displacement, time, and velocity • Calculate the displacement of an object traveling at a known velocity for a specific time interval • Construct and interpret graphs of position versus time
Scalar Quantities & Vector Quantities • Scalar quantities have magnitude • Example: speed 15 m/s • Vector quantities have magnitude and direction • Example: velocity 15 m/s North
Displacement • Net change in position of an object • Straight line distance from beginning to end • Is not the same as distance
Displacement • Displacement is a vector quantity • Indicates change in location of a body ∆x = xf - xi • It is specified by a magnitude and a direction. • Displacement does not take into account the path followed between xi and xf .
Displacement is change in position www.cnx.org
Describing Motion Describing motion requires a frame of reference http://www.sfu.ca/phys/100/lectures/lecture5/lecture5.html
Determining Displacement In these examples, position is determined with respect to the origin, displacement wrt x1 http://www.sfu.ca/phys/100/lectures/lecture5/lecture5.html
Indicating Direction of Displacement Direction can be indicated by sign, degrees, or geographical directions.
Displacement • In this example, the body moved 10 units to get from A to B. • Distance = length traveled = 10 units • Displacement = net change in position ≈ 5.1 units, NE
Velocity • Example • A squirrel runs in a westerly direction from one tree to another, covering 55 meters in 32 seconds. Calculate the squirrel’s average velocity • vavg = ∆x / ∆t • vavg = 55 m / 32 s • vavg = 1.7 m/s west
Velocity can be interpreted graphically: Position Time Graphs
Velocity can be interpreted graphically: Position Time Graphs
Position-Time Graphs Object at rest? Traveling slowly in a positive direction? Traveling in a negative direction? Traveling quickly in a positive direction? dev.physicslab.org
Instantaneous Velocity • Is not average velocity • Is velocity of an object at any given moment in time or at a specific point in the object’s path
Instantaneous Velocity • Velocity at any point on an x-t graph • Velocity at a given point in time • Is the slope of a line tangent to the x-t curve
Average velocity compared to instantaneous velocity Instantaneous velocity is the slope of the tangent line at any particular point in time.
2.2 AccelerationLearning Objectives • Describe motion in terms of changing velocity • Compare graphical representations of accelerated and non-accelerated motions • Apply kinematic equations to calculate distance, time, or velocity under conditions of constant acceleration
Changes in Velocity • Acceleration is the rate of change of velocity • a = ∆v/∆t • a = (vf – vi) / (tf – ti) • Since velocity is a vector quantity, velocity can change in magnitude or direction • Acceleration occurs whenever there is a change in speed or direction of movement.
Dimensions of acceleration • a = ∆v/∆t • = meters per second per second • = m/s/s • = m/s2 • Sample problems 2B
Acceleration is a vector quantity • Has magnitude and direction • Both velocity & acceleration can have (+) and (-) values • Whether –a indicates slowing down or speeding up depends upon the sign of velocity
Velocity-Time Graphs What would a position-time graph look like? Acceleration-time graph? www.gcsescience.com
Free-fall motion graphs v-t graph x-t graph
Velocity & Acceleration Velocity acceleration_ __ Motion + + speeding up (-) (-) speeding up + (-) slowing down (-) + slowing down
Final velocity after any displacement A baby sitter pushes a stroller from rest, accelerating at 0.500 m/s2. Find the velocity after the stroller travels 4.75m. (p. 57) Identify the variables. Solve for the unknown. Substitute and solve. Practice 2E, p. 58
2.3 Falling Objects Objectives • Relate the motion of a freely falling body to motion with constant acceleration. • Calculate displacement, velocity, and time at various points in the motion of a freely falling object. • Compare the motions of different objects in free fall.
Free Fall • In the absence of air resistance, all objects fall to earth with a constant acceleration • The rate of fall is independent of mass • In a vacuum, heavy objects and light objects fall at the same rate. • The acceleration of a free-falling object is the acceleration of gravity, g • g = 9.81m/s2 memorize this value!
Free Fall • Free fall is the motion of a body when only the force due to gravity is acting on the body. • The acceleration on an object in free fall is called the acceleration due to gravity, or free-fall acceleration. • Free-fall acceleration is denoted with the symbols ag(generally) or g(on Earth’s surface).
Free Fall Acceleration • Free-fall acceleration is the same for all objects, regardless of mass. • This book will use the value g= 9.81 m/s2. • Free-fall acceleration on Earth’s surface is –9.81 m/s2 at all points in the object’s motion. • Consider a ball thrown up into the air. • Moving upward: velocity is decreasing, acceleration is –9.81 m/s2 • Top of path: velocity is zero, acceleration is –9.81 m/s2 • Moving downward: velocity is increasing, acceleration is –9.81 m/s2
Free-Fall Problem • A tennis ball is tossed vertically with an initial velocity 0f 6.0 m/s. How high will the ball go? How long will the ball be in the air until it returns to its starting point? • Known: vi = 6.0 m/s; a = -g = -9.81 m/s2 • How high? vf2 = vi2 + 2aΔy solve for Δy • vf = vi + aΔt solve for Δt • Since the ball goes up Δt and comes down Δt, time in the air is 2Δt
Sample Problem • Falling Object • Jason hits a volleyball so that it moves with an initial velocity of 6.0 m/s straight upward. • If the volleyball starts from 2.0 m above the floor, • how long will it be in the air before it strikes the floor?
Sample Problem, continued 1. Define Given: Unknown: vi= +6.0 m/s Δt = ? a = –g = –9.81 m/s2 Δy = –2.0 m • Diagram: • Place the origin at the • Starting point of the ball • (yi = 0 at ti = 0).
2. Plan Choose an equation or situation: Both ∆t and vf are unknown. We can determine ∆t if we know vf Solve for vf then substitute & solve for ∆t 3. Calculate Rearrange the equation to isolate the unknowns: vf= - 8.7 m/s Δt = 1.50 s