Projectile Motion CCHS Physics. Projectile Properties?

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Projectile Motion CCHS Physics

Transcript of Projectile Motion CCHS Physics. Projectile Properties?

Page 1: Projectile Motion CCHS Physics. Projectile Properties?

Projectile Motion

CCHS Physics

Page 2: Projectile Motion CCHS Physics. Projectile Properties?

Projectile Properties?

Page 3: Projectile Motion CCHS Physics. Projectile Properties?

Projectile Motion

• Describe the motion of an object in TWO dimensions

• Keep it simple by considering motion close to the surface of the earth for the time being (g = -9.8 m/s2 = constant in y direction)

• Neglect air resistance to make it simpler• Assume the rotation of the Earth has no effect

Page 4: Projectile Motion CCHS Physics. Projectile Properties?

Projectile Motion

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Launch speed = Return Speed. Speed is minimum at apex of parabolic trajectory.

Horizonal component

Net velocity

vx

vertical component

vy v

Above: Vectors areadded in geometricFashion.

Velocity Components at various points of the Trajectory

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Projectile Motion

The ball is in free fall vertically and moves at constant speed horizontally!!!

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Projectile Motion

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Video

Page 9: Projectile Motion CCHS Physics. Projectile Properties?

What’s wrong with this picture ?

Answer: It never happens ! Only whenthere is no gravity.

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Projectile Motion

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A History of Projectile Motion

Aristotle:The canon ball travels in a straight line until it lost its ‘impetus’.

Galileo: a result of Free Fall Motionalong y-axis and Uniform Motion along x-axis.

Page 12: Projectile Motion CCHS Physics. Projectile Properties?

What’s the similarity between a freely-falling ball and a projectile ?

A dropped ball falls in the same time as a ball shot horizontally.Along the vertical, their motions are identical (uniformly accelerated motion (free-fall).

Along the horizontal, notice the ball fired horizontally covers the Same distance in the same unit time intervals (uniform motion along x)

x

yuniform motion

verticalmotion

Projectilemotion

Page 13: Projectile Motion CCHS Physics. Projectile Properties?

Projectile Motion EquationsHorizontal (x)

x =vxt

Vertical (y)

y=y0 + v0yt−

12

gt2 or dy =12

gt2 + viyt

vy =v0y −gt or g=vfy

−viy

t

Page 14: Projectile Motion CCHS Physics. Projectile Properties?

1. Along x, the projectile travels with constant velocity. vx=vxo x = vxot

2. Along y, the projectile travels in free-fall fashion.vy = vyo – gt y = vyot – (1/2) gt2 , g= 9.8 m/s2

Projectile motion = a combination of uniform motion along x and uniformly accelerated motion (free fall) along y.

Projectile Motion = Sum of 2 Independent Motions

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Everyday Examples of Projectile Motion

1.Baseball being thrown2.Water fountains3.Fireworks Displays4.Soccer ball being kicked5.Ballistics Testing

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QuickTime™ and aTIFF (Uncompressed) decompressor

are needed to see this picture.Type IA ball is kicked off a 125 m cliff with a horizontal velocity of 50 m/s. What is the range of the ball?

V = 50 m/s

125

m

Horizontal Verticald = d = vi = vi = a = a = t = t =

-125 m

0 m/s50 m/s

0 m/s2 -9.8 m/s2

5.1 s5.1 s

255 m

d =12

at2 +vit

−125 =1

2−9.8( ) t 2 + 0

d =12

at2 +vit

d =0+50(5.1)d =255 m

t =5.1s

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Type IIA ball is kicked of a with a velocity of 50 m/s at an angle of 37° from the horizontal. What is the range of the ball?

Horizontal Verticald = d = vi = vi = a = a = t = t =

0 m

30 m/s40 m/s

0 m/s2 -9.8 m/s2

6.1 s6.1 s

244 m

d =12

at2 +vit

0 =12

−9.8( )t2 + 30t

d =12

at2 +vit

d =0+40(6.1)d =244 m

t =0 or 6.1s

v = 50 m/s37°

v = 50 m/svy = 50sin37 = 30 m/s

37°

vx = 50cos37 = 40 m/s

QuickTime™ and aTIFF (Uncompressed) decompressor

are needed to see this picture.

Page 18: Projectile Motion CCHS Physics. Projectile Properties?

Type IIIA ball is kicked off a 125 m cliff with a velocity of 50 m/s at an angle of 37° from the horizontal. What is the range of the ball?

Horizontal Verticald = d = vi = vi = a = a = t = t =

-125 m

30 m/s40 m/s

0 m/s2 -9.8 m/s2

9.0 s9.0 s

360 m

d =12

at2 +vit

−125 =1

2−9.8( ) t 2 + 30t

d =12

at2 +vit

d =0+40(9.0)d = 360 m

t =9.0 or -2.8s

v = 50 m/s37°

125

mNote, this type

requires the use of the quadratic

equation

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Horizontal Range

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Maximum Range

• How to maximize horizontal range:– keep the object off the ground for as long

as possible.– This allows the horizontal motion to be a

maximum since x = vxt

– Make range longer by having a greater initial velocity velocity

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QuickTime™ and aTIFF (Uncompressed) decompressor

are needed to see this picture.

vi

R

x =R=vxt

R=vi cos ( )t

Range Equation

d =12

at2 + vit

0 =12

gt2 + viyt ⇒ t=

2viy

g=2vi sin

g

What is total t? To solve, set vertical displacement = 0.

R =vi cos ( )2vi sin

g⎛⎝⎜

⎞⎠⎟=

vi2

g2sin cos( )

Trig Identity: 2sincos = sin(2)

R =vi2

gsin 2( ) REMEMBER: ONLY VALID WHEN VERTICAL

DISPLACEMENT IS ZERO (Type II problems).

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Projectile Motion• We can see that complementary angles have

the same range because sin = sin2

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At what angle do I launch for Maximum Range ?

Need to stay in air for the longest time, and with the fastest horizontal velocity componentAnswer: 45°

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Projectile Motion

• What happens when we add air resistance?• Adds a new force on the ball• The force is in the opposite direction to the

ball’s velocity vector and is proportional to the velocity at relatively low speeds

• Need calculus to sort out the resulting motion• Lowers the angle for maximum range

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Projectile Motion