projectile motion

4
Projectile Motion: is a form of motion in which an object or particle (called a projectile) is thrown near the earth's surface, and it moves along a curved path under the action of gravity only. The only force of significance that acts on the object is gravity, which acts downward to cause a downward acceleration. There are no horizontal forces needed to maintain the horizontal motion. This motion is simplified in to two independent motions: Horizontal Motion in X-direction (a x =0) Vertical Motion in Y-direction (a y =-g) In projectile motion, gravity is the only force acting on the object Projectile motion could be handled in the same way as two- dimensional motion with constant acceleration analyzed: Equation 1 r f =r i +v i t +0.5at 2 x y x f =x i +v xi t y f =y i +v yi t -0.5*g*t 2 Since a x =0 a y =-g = -9.81 m/s 2 Equation 2 r f =r i +0.5(v i +v f )t x y x f =x i +0.5(v xi +v xf )t y f =y i +0.5(v yi +v yf )t Equation 3 V f 2 =V i 2 +2a(r f -r i ) X y V xf 2 =V xi 2 V yf 2 =V yi 2 -2g(y f -y i ) Since a x =0 a y =-g = -9.81 m/s 2

Upload: mohammad-khasawneh

Post on 26-Dec-2015

6 views

Category:

Documents


1 download

DESCRIPTION

Projectile Motion - physics

TRANSCRIPT

Page 1: Projectile Motion

Projectile Motion:

is a form of motion in which an object or particle (called a projectile) is

thrown near the earth's surface, and it moves

along a curved path under the action of

gravity only. The only force of significance

that acts on the object is gravity, which acts

downward to cause a downward

acceleration. There are no horizontal forces

needed to maintain the horizontal motion.

This motion is simplified in to two independent motions:

Horizontal Motion in X-direction (ax=0)

Vertical Motion in Y-direction (ay=-g)

In projectile motion, gravity is the only force acting on the object

Projectile motion could be handled in the same way as two-

dimensional motion with constant acceleration analyzed:

Equation 1

rf=ri+vit +0.5at2 x y xf=xi+vxit yf=yi+vyit -0.5*g*t2

Since ax=0 ay=-g = -9.81 m/s2

Equation 2

rf=ri+0.5(vi+vf)t x y

xf=xi+0.5(vxi+vxf)t yf=yi+0.5(vyi+vyf)t

Equation 3

Vf2=Vi

2+2a(rf-ri) X y Vxf

2=Vxi2 Vyf

2=Vyi2-2g(yf-yi)

Since ax=0 ay=-g = -9.81 m/s2

Page 2: Projectile Motion

Horizontal range

Xf - xi

= R = vxi t

yf – yi = v

yi t – ½ gt2 = 0 (this equation gives the required time for the

whole trip) Substitute the time into the first equation to evaluate the horizontal range.

Maximum Height

Note: the body reaches it's maximum height when Vy= ZERO; (a critical

point between decelerating when particle moves up and accelerating

when particle goes down)

Vyf=Vyi – gt = 0

t = Vyi/g (this equation gives the required time for particle to reach the

maximum height)

then substitute the time value into :

yf = yi + vyi – 0.5 gt2 => yf – yi = vyi – 0.5 gt2 = h

or substitute (vyf =0) directly in equation 3

h= vyi2/2g

Page 3: Projectile Motion
Page 4: Projectile Motion

Vya = 6.69