T.Merfat Al-Zumia بسم هللا الرحمن الرحيم Chapter (2) :Motion in one dimension 8- Motion under a constant velocity: Velocity = ∆x/∆t X (m) ( ) * But we know the line equation: Y= slop X + Co ** By comparing equation * with **: T.Merfat Al-Zumia -The condition when the particle moves under a constant velocity: So a Motion under a constant : 1- Velocity means 2- Speed means A constant speed (magnitude) A constant speed (magnitude) And on a straight line (direction) And even on a straight or a curved line (no direction) T.Merfat Al-Zumia 9- Motion under a constant acceleration: 1- A First motion’s law : From the average acceleration ( ) (1) We know the line equation is Y= slop X + co = slop T.Merfat Al-Zumia 2- A second motion’s law: From the average velocity equation ( ) ( ( ) ) ( ) From equation (1) ( ) ( ( ) ) T.Merfat Al-Zumia ( ) ( ( ( ) ) ( ) ) (2) 3- A Third motion’s law : From the average velocity equation From and the average acceleration equation From T.Merfat Al-Zumia From two columns ( ) ( ) (3) We now have all the equations we need to solve constant-acceleration problems. ( ) (1) ( ) (2) (3) T.Merfat Al-Zumia Galileo dropped two balls of different weights from the top of building the two balls will reach the ground at the same time. He proved that when objects of different weights are dropped at the same height and time, they take the same amount of time to fall to the ground (ignoring air resistance). T.Merfat Al-Zumia Example (2.7) : A jet lands on an aircraft carrier at (63 =m/s). 1-What is its acceleration (assumed constant) if it stops in 2.0 s ? 2-If the plane touches down at position xi = 0, what is the final position of the plane? 3-if the displacement is 75m find the maximum initial speed with which the plane can land and still come to rest T.Merfat Al-Zumia 10- The thrown up and freely falling: 1-Means Acceleration Due to Gravity 2-The acceleration of a freely falling body is called the acceleration due to gravity, g= 9.80 m/s2 3-The acceleration due to gravity is directed downward, toward the center of the earth. Maximum height Note : Vyf = 0 yf= value Vyi = 0 yi = value Vy,falling = -Vy,thrown ay,falling = - ay,thrown (9.8) (-9.8) tfalling = tthrown Thrown up t = t thrown ay= - 9.8 Freely falling t = t falling ay= 9.8 Vyi = value yi = 0 Vyf = value yf= 0 yi,falling = -yf,thrown T.Merfat Al-Zumia The equation for motion in one dimension: In x-axis Xi ≠ 0 ( Thrown up a = -g Vyf = 0 yi = 0 Freely falling a = g Vyi = 0 yf = 0 ) ( ) ) Also In x-axis But Xi = 0 ( ) ( ) T.Merfat Al-Zumia Example (2.12): A stone thrown from the top of a building is given an initial velocity of 20.0 m/s straight upward. The building is 50.0 m high, and the stone just misses the edge of the roof on its way down, as shown. Using tA = 0 as the time the stone leaves the thrower’s hand at position (A) T.Merfat Al-Zumia determine: 1- the time at which the stone reaches its maximum height? 2-the maximum height T.Merfat Al-Zumia 3-the time at which the stone returns to the height from which it was thrown, 4- the velocity of the stone at this instant T.Merfat Al-Zumia 6- the velocity of the stone at t = 5.00s 5- the position of the stone at t = 5.00s Best wishes , T.Merfat Al-Zumia, T.Merfat Al-Zumia
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