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General Physics (PHYS101). Acceleration 1D motion with Constant Acceleration Free Fall Lecture 04 (Chap. 2, Sec. 6-10 ). Sections 30 and 33 are canceled and became section 27. Lightning Review. Last lecture:. Displacement - change of position
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General Physics (PHYS101) Acceleration 1D motion with Constant Acceleration Free Fall Lecture 04 (Chap. 2, Sec. 6-10 ) Sections 30 and 33 are canceled and became section 27
Lightning Review Last lecture: • Displacement - change of position • Average velocity - displacement over time interval • Instantaneous velocity - the same but for very small time interval
Average Acceleration • Average acceleration is the rate of change of the velocity SI unit: m/s2 • Changing velocity (non-uniform) means an acceleration is present • Average acceleration is a vector quantity (i.e described by both magnitude and direction)
Instantaneous Acceleration • Instantaneous acceleration is the limiting case of the average acceleration as the time interval goes to zero.
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
1D motion: uniform velocity • Uniform velocity (shown by red arrows maintaining the same size) • Acceleration equals zero
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)
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)
1D motion: constant acceleration Our job:to find the equation for the position and velocity of the object to make predictions!
v x x0 t t 1D motion with constant acceleration • Recall that • We know that v0 • We find • Since
acceleration is constant velocity as a function of time velocity as a function of displacement displacement as a function of velocity and time Displacement as a function of velocity average velocity displacement as a function of time Summary of kinematic equations: 1D motion
0 y x 0 2 1 3 1 2 3 y Free fall - 1D motion with constant acceleration • All objects moving under the influence of only gravity are said to be in free fall • All objects falling near the earth’s surface fall with a constant acceleration • This acceleration is called gravitations acceleration, indicated by g and always points perpendicular to the earth’s surface
acceleration displacement vs velocity and time displacement vs time displacement vs velocity velocity vs time velocity vs displacement average velocity Free fall - 1D motion with constant acceleration
y Case 1:zero initial velocity
Case 1 y y Case 2:NONzero initial velocity Case 2
Free fall • Mass does not matter, if the air resistance is neglected
1D motion with constant acceleration • Example 1: A car is traveling with a constant speed v0. 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 tf, before it stops completely. • low long does it travel if the stopping distance is xf. Given: v0=v0 a=-a x0=0 t0=0 v=0 Find: 1) xf=?, knowing tf. 2) tf=?, knowing xf.