motions under non constant acceleration n.
Skip this Video
Download Presentation
Motions under non-constant acceleration

Loading in 2 Seconds...

play fullscreen
1 / 59

Motions under non-constant acceleration - PowerPoint PPT Presentation

  • Uploaded on

Motions under non-constant acceleration. How do we know the position from the velocity function v(t) ?. Displacement from a Velocity - Time Graph.

I am the owner, or an agent authorized to act on behalf of the owner, of the copyrighted work described.
Download Presentation

PowerPoint Slideshow about 'Motions under non-constant acceleration' - calista-kennedy

Download Now An Image/Link below is provided (as is) to download presentation

Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author.While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server.

- - - - - - - - - - - - - - - - - - - - - - - - - - E N D - - - - - - - - - - - - - - - - - - - - - - - - - -
Presentation Transcript
motions under non constant acceleration

Motions under non-constant acceleration

How do we know the position from the velocity function v(t)?

displacement from a velocity time graph
Displacement from a Velocity - Time Graph
  • The displacement of a particle during the time interval ti to tf is equal to the area under the curve between the initial and final points on a velocity-time curve
displacement during a time interval
Displacement during a time interval
  • First, we divide the time range from Ta to Tf into N equal intervals
  • Displacement Dxn during the n-th interval
total displacement from t a to t f
Total displacement from Ta to Tf

In the limit as N approaches to infinite, the time interval Dt becomes smaller and smaller.

Displacement is the area under the curve of v(t).

position x f at t f with initial position x a at t a
Position xf at Tf with initial position xa at Ta

If the function v(t) is constant in time,

velocity v f at t f with initial velocity v a at t a
Velocity vf at Tf with initial velocity va at Ta

If the function a(t) is constant in time,

chapter 3

Chapter 3

Motion in Two Dimensions

3 1 position and displacement
3.1 Position and Displacement
  • The position of an object is described by its position vector,
  • The displacement of the object is defined as the change in its position

Fig 3.1

average velocity
Average Velocity
  • The average velocity is the ratio of the displacement to the time interval for the displacement
    • The direction of the average velocity is the direction of the displacement vector,

Fig 3.2

average velocity cont
Average Velocity, cont
  • The average velocity between points is independent of the path taken
    • This is because it is dependent on the displacement, which is also independent of the path
    • If a particle starts its motion at some point and returns to this point via any path, its average velocity is zero for this trip since its displacement is zero
instantaneous velocity
Instantaneous Velocity
  • The instantaneous velocity is the limit of the average velocity as ∆t approaches zero
instantaneous velocity cont
Instantaneous Velocity, cont
  • The direction of the instantaneous velocity vector at any point in a particle’s path is along a line tangent to the path at that point and in the direction of motion
  • The magnitude of the instantaneous velocity vector is the speed
average acceleration
Average Acceleration
  • The average acceleration of a particle as it moves is defined as the change in the instantaneous velocity vector divided by the time interval during which that change occurs.
average acceleration cont
Average Acceleration, cont
  • As a particle moves, can be found in different ways
  • The average acceleration is a vector quantity directed along

Fig 3.3

instantaneous acceleration
Instantaneous Acceleration
  • The instantaneous acceleration is the limit of the average acceleration as approaches zero
producing an acceleration
Producing An Acceleration
  • Various changes in a particle’s motion may produce an acceleration
    • The magnitude of the velocity vector may change
    • The direction of the velocity vector may change
      • Even if the magnitude remains constant
    • Both may change simultaneously
3 2 kinematic equations for two dimensional motion
3.2 Kinematic Equations for Two-Dimensional Motion
  • When the two-dimensional motion has a constant acceleration, a series of equations can be developed that describe the motion
  • These equations will be a generlization of those of one-dimensional kinematics to the vector form.
kinematic equations 2
Kinematic Equations, 2
  • Position vector
  • Velocity
    • Since acceleration is constant, we can also find an expression for the velocity as a function of time:
kinematic equations 3
Kinematic Equations, 3
  • The velocity vector can be represented by its components
  • is generally not along the direction of either or

Fig 3.4(a)

kinematic equations 4
Kinematic Equations, 4
  • The position vector can also be expressed as a function of time:
    • This indicates that the position vector is the sum of three other vectors:
      • The initial position vector
      • Thedisplacement resulting from
      • The displacement resulting from
kinematic equations 5
Kinematic Equations, 5
  • The vector representation of the position vector
  • is generally not in the same direction as or as
  • and are generally not in the same direction

Fig 3.4(b)

kinematic equations components
Kinematic Equations, Components
  • The equations for final velocity and final position are vector equations, therefore they may also be written in component form
  • This shows that two-dimensional motion at constant acceleration is equivalent to two independent motions
    • One motion in the x-direction and the other in the y-direction
kinematic equations component equations
Kinematic Equations, Component Equations
  • becomes
    • vxf = vxi + axt and
    • vyf = vyi + ayt
  • becomes
    • xf = xi + vxit + 1/2 axt2 and
    • yf = yi + vyit + 1/2 ayt2
3 3 projectile motion
3.3 Projectile Motion
  • The motion of an object under the influence of gravity only
  • The form of two-dimensional motion
assumptions of projectile motion
Assumptions of Projectile Motion
  • The free-fall acceleration is constant over the range of motion
    • And is directed downward
  • The effect of air friction is negligible
  • With these assumptions, the motion of the object will follow
projectile motion vectors
Projectile Motion Vectors
  • The final position is the vector sum of the initial position, the displacement resulting from the initial velocity and that resulting from the acceleration
  • This path of the object is called the trajectory

Fig 3.6

analyzing projectile motion
Analyzing Projectile Motion
  • Consider the motion as the superposition of the motions in the x- and y-directions
  • Constant-velocity motion in the x direction
    • ax = 0
  • A free-fall motion in the y direction
    • ay = -g
verifying the parabolic trajectory
Verifying the Parabolic Trajectory
  • Reference frame chosen
    • y is vertical with upward positive
  • Acceleration components
    • ay = -g and ax = 0
  • Initial velocity components
    • vxi = vi cos qi and vyi = vi sin qi
projectile motion velocity at any instant
Projectile Motion – Velocity at any instant
  • The velocity components for the projectile at any time t are:
    • vxf = vxi = vi cos qi = constant
    • vyf = vyi – g t = vi sin qi – g t
projectile motion position
Projectile Motion – Position
  • Displacements
    • xf = vxit = (vi cos qi)t
    • yf = vyit + 1/2ay t2 = (vi sinqi)t - 1/2 gt2
  • Combining the equations gives:
    • This is in the form of y = ax – bx2 which is the standard form of a parabola
what are the range and the maximum height of a projectile
What are the range and the maximum height of a projectile
  • The range, R, is the maximum horizontal distance of the projectile
  • The maximum height, h, is the vertical distance above the initial position that the projectile can reaches.

Fig 3.7

projectile motion implications
Projectile Motion – Implications
  • The y-component of the velocity is zero at the maximum height of the trajectory
  • The accleration stays the same throughout the trajectory
height of a projectile equation
Height of a Projectile, equation
  • The maximum height of the projectile can be found in terms of the initial velocity vector:
  • The time to reach the maximum:
range of a projectile equation
Range of a Projectile, equation
  • The range of a projectile can be expressed in terms of the initial velocity vector:
  • The time of flight = 2tm
  • This is valid only for symmetric trajectory
range of a projectile final
Range of a Projectile, final
  • The maximum range occurs at qi = 45o
  • Complementary angles will produce the same range
    • The maximum height will be different for the two angles
    • The times of the flight will be different for the two angles