acceleration 1d motion with constant acceleration free fall lecture 04 (chap. 2, sec. 6-10 ) general...

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Acceleration 1D motion with Constant Acceleration Free Fall Lecture 04 (Chap. 2, Sec. 6-10 ) General Physics (PHYS101) ections 30 and 33 are canceled and became section 2

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  • Slide 1
  • Acceleration 1D motion with Constant Acceleration Free Fall Lecture 04 (Chap. 2, Sec. 6-10 ) General Physics (PHYS101) Sections 30 and 33 are canceled and became section 27
  • Slide 2
  • Lightning Review Displacement - change of position Average velocity - displacement over time interval Instantaneous velocity - the same but for very small time interval Last lecture:
  • Slide 3
  • Average Acceleration Average acceleration is the rate of change of the velocity Changing velocity (non-uniform) means an acceleration is present Average acceleration is a vector quantity (i.e described by both magnitude and direction) SI unit: m/s 2
  • Slide 4
  • Instantaneous Acceleration Instantaneous acceleration is the limiting case of the average acceleration as the time interval goes to zero.
  • Slide 5
  • Graphical Interpretation of Acceleration Average acceleration is the slope of the line connecting the initial and final velocities on the velocity-time graph Instantaneous acceleration is the slope of the tangent to the curve of the velocity-time graph for the given value of time
  • Slide 6
  • 1D motion: uniform velocity Uniform velocity (shown by red arrows maintaining the same size) Acceleration equals zero
  • Slide 7
  • 1D motion: constant (positive) acceleration Velocity and acceleration are in the same direction Acceleration is uniform (blue arrows maintain the same length) Velocity is increasing in time (red arrows are getting longer)
  • Slide 8
  • 1D motion: constant (negative) acceleration Velocity and acceleration are in opposite directions Acceleration is uniform (blue arrows maintain the same length) Velocity is decreasing (red arrows are getting longer)
  • Slide 9
  • 1D motion: constant acceleration Our job: to find the equation for the position and velocity of the object to make predictions!
  • Slide 10
  • 10 1D motion with constant acceleration Recall that We know that We find v t v0v0 Since x t x0x0
  • Slide 11
  • 11 1D motion with constant acceleration
  • Slide 12
  • 12 Summary of kinematic equations: 1D motion acceleration is constant displacement as a function of velocity and time displacement as a function of time velocity as a function of time velocity as a function of displacement average velocity Displacement as a function of velocity
  • Slide 13
  • 13 Free fall - 1D motion with constant acceleration
  • Slide 14
  • 14 Free fall - 1D motion with constant acceleration 0 x 1 2 3 0 y 1 2 3 All objects moving under the influence of only gravity are said to be in free fall All objects falling near the earths surface fall with a constant acceleration This acceleration is called gravitations acceleration, indicated by g and always points perpendicular to the earths surface y
  • Slide 15
  • 15 acceleration displacement vs velocity and time displacement vs time velocity vs time velocity vs displacement average velocity displacement vs velocity Free fall - 1D motion with constant acceleration
  • Slide 16
  • 16 Case 1: zero initial velocity y
  • Slide 17
  • 17 Case 2: NONzero initial velocity y y Case 1 Case 2
  • Slide 18
  • 18 Case 3: object thrown upward
  • Slide 19
  • 19 Case 4: object thrown upward
  • Slide 20
  • Free fall Mass does not matter, if the air resistance is neglected
  • Slide 21
  • 21 Positive acceleration
  • Slide 22
  • 22 Negative acceleration
  • Slide 23
  • 23 1D motion with constant acceleration Example 1: A car is traveling with a constant speed v 0. At some time, the driver puts on the brakes, which slows the car down at a rate of a. Find: how much farther does the car travel for time t f, before it stops completely. low long does it travel if the stopping distance is x f. Given: v 0 =v 0 a=-a x 0 =0 t 0 =0 v=0 Find: 1) x f =?, knowing t f. 2) t f =?, knowing x f.