Transcript Slide 1

Lecture 5

Ch4. TWO- AND THREE-DIMENSIONAL MOTION

University Physics: Mechanics

Dr.-Ing. Erwin Sitompul

http://zitompul.wordpress.com

Homework 4: The Plane

A plane flies 483 km west from city

A

then 966 km south from city

B

to city to city

C B

in 45 min and in 1.5 h.

From the total trip of the plane, determine: (a) the magnitude of its displacement; (b) the direction of its displacement; (c) the magnitude of its average velocity; (d) the direction of its average velocity; (e) its average speed.

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B C

Δr 2 Δr 1

Solution of Homework 4: The Plane

483 km, 45 min

A

      

r

total 

t

1 2 total    

t

1 1

t r

2 2   1

t

2 45 min 1.5 h   483i ˆ     0.75 h 2.25 h

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(a) the magnitude of its displacement 

r

total  2 1080.021 km 2 243.435

B A

(b) the direction of its displacement 

r

total  tan  1     966  483     63.435

  243.435

 • •

Quadrant I Quadrant III

C

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Solution of Homework 4: The Plane

(c) the magnitude of its average velocity

v

avg  

r

total 

t

total   483i ˆ  2.25 h 

v

avg   2   2  480 km h (d) the direction of its average velocity 

v

avg  tan  1     429.333

 214.667

    243.435

 •

Quadrant III

(e) its average speed

s

avg  total distance traveled total time  2.25 h  644 km h

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Projectile Motion

   Projectile motion: a motion in a vertical plane, where the acceleration is always the free-fall acceleration →

g

, which is downward.

Many sports involve the projectile motion of a ball.

Besides sports, many acts also involve the projectile motion.

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Projectile Motion

 Projectile motion consists of horizontal motion and vertical motion, which are independent to each other.

 The horizontal motion has no acceleration (it has a constant velocity).

 The vertical motion is a free fall motion with constant acceleration due to gravitational force.

a x

0

g

9.81m s

2

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a y

 

g

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Projectile Motion

a x

0

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v

0

v

0

x v

0

y

  

v

0

v

0

v

0

x

ˆ i

cos

sin 

v

0  0 0

y

ˆ j

a y

 

g

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Two Golf Balls

v

0

x

 0

v

0

x

 0

Projectile Motion

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• •

The vertical motions are quasi identical.

The horizontal motions are different.

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Projectile Motion Analyzed

The Horizontal Motion

x

x

0 

v t

0

x x

x

0  (

v

0 cos  0 )

t

The Vertical Motion

y

y

0 

v t

0

y

 1 2

gt

2

v

2

y y

 

y

0

v y v

0   (

v

0

v

0  0 sin sin ) 2    0 0 )

t

 

gt

1 2 

gt

2

y

0 )

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v v x y

= v 0x = –v 0y Erwin Sitompul

Projectile Motion Analyzed

The Horizontal Range

R x

  (

v

0

x

0  cos

R

 0 )

t

0  (

v

0

y

 sin

y

0  0  )

t

0  1 2

gt

2 Eliminating

t

,

R

 2

v

0 2

g

sin  0 cos  0 •

This equation is valid if the landing height is identical with the launch height.

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Projectile Motion Analyzed

Further examining the equation, 2

R

 2

v g

0 sin  0 cos  0 Using the identity sin 2  0  2sin  0 cos  0 , we obtain 2

R

v g

0 sin 2  0

R

is maximum when sin2

θ

0 = 1 or

θ

0 =45 °. •

If the launch height and the landing height are the same, then the maximum horizontal range is achieved if the launch angle is 45 °. Erwin Sitompul University Physics: Mechanics 5/11

Symmetry of Position and Speed

v

0 = 29.4 m/s • •

If the initial elevation and final elevation are the same, the velocity of an object at each elevation will be the same in magnitude , but opposite in direction.

The object’s height and the speed will be symmetrical around the time when the peak position is reached.

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Projectile Motion Analyzed

• •

The launch height and the landing height differ.

The launch angle 45 ° does not yield the maximum horizontal distance.

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The Effects of the Air

Projectile Motion Analyzed

 Path I: Projectile movement if the air resistance is taken into account  Path II: Projectile movement if the air resistance is neglected (as in a vacuum)

Our calculation along this chapter is based on this assumption Erwin Sitompul University Physics: Mechanics 5/14

Example: Baseball Pitcher

A pitcher throws a baseball at speed 40 km/h and at angle

θ

= 30 °.

h

30  (a) Determine the maximum height

h

of the baseball above the ground.

v y

v

0

y

gt

0  5.56 9.8

t h t

   5.56

9.8

 

y

0 1.58 m   0.567 s

v t

0

y

 (5.56)(0.567)  2 1 1 2

gt

2 (9.8)(0.567) 2

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v

0

y v

0

x

     

v

0 sin  (11.11) sin 30 5.56 m s 

v

0 cos  (11.11) cos 30 9.62 m s 

v

2

y y

 

v x y

0  

x

0 

v t

0

y v t

0

x

 1 2

y

v

0

y

gt v

2 0

y

 

gt y

2 0 )

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Example: Baseball Pitcher

A pitcher throws a baseball at speed 40 km/h and at angle

θ

= 30 °. 30 

d

(b) Determine the duration when the baseball is on the air.

t

on air 

t

up 

t

down   1.134 s (c) Determine the horizontal distance

d

it travels.

d x x

0  

v t

0

x

(9.62)(1.134)  10.91 m

v

2

y y

 

v x y

0  

x

0 

v t

0

y v t

0

x

 1 2

y

v

0

y

gt v

2 0

y

 

gt y

2 0 )

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Simulation: How to Fire the Cannon?

θ v

0 9 m 16 m

A cannon is 1.20 m above the ground. You may adjust the initial speed and the angle of fire of the cannon.

If the target is horizontally 16 m away from the cannon and at 9 m above the ground, how do you set the cannon so that the projectile can hit the target?

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v

2

y y

 

v x y

0  

x

0 

v t

0

y v t

0

x

 1 2

y

v

0

y

gt v

2 0

y

 

gt y

2 0 )

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Example: Rescue Plane

A rescue plane flies at 198 km/h and constant height is to land.

h

= 500 m toward a point directly over a victim, where a rescue capsule (a) What should be the angle release is made?

Φ

of the pilot’s line of sight to the victim when the capsule

y

y

0  

v t

0 (0)

y t

  1 2 1 2

gt

2 (9.8)

t

2

t

2

t

  9.8

 10.102 s 102.041

x

x

0  

v t

0

x

(55)(10.102)  555.61 m

Released horizontally

h

d y

0

x

0     1

d

tan  1

h

555.61

tan 48.016

500 

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Example: Rescue Plane

Released horizontally

A rescue plane flies at 198 km/h and constant height is to land.

h

= 500 m toward a point directly over a victim, where a rescue capsule (b) As the capsule reaches the water, what is its velocity →

v

in unit-vector notation and in magnitude-angle notation?

v y v y

 

v

0

y

gt

  99 m s

v x

 

v

0

x

55 m s

h d y

0

x

0

v

 ˆ

Unit-vector notation

v

 113.252 m s  60.945

Magnitude-angle notation Erwin Sitompul University Physics: Mechanics 5/19

Example: Clever Stuntman

A stuntman plans a spectacular jump from a higher building to a lower one, as can be observed in the next figure. Can he make the jump and safely reach the lower building?

y

y

0   1 

v t

0

y

(0)

t

 2 1 2

gt

2 (9.8)

t

2

t

2

t

  0.98

9.8

 0.99 s

Time for the stuntman to fall 4.8 m

x

x

0  

v t

0

x

(4.5)(0.99)  4.46 m

Horizontal distance jumped by the stuntman in 0.99 s Erwin Sitompul He cannot make the jump

v

2

y y

 

v x y

0  

x

0 

v t

0

y v t

0

x

 1 2

y

v

0

y

gt v

2 0

y

 

gt y

2 0 )

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Homework 5A: Three Point Throw

A basketball player who is 2.00 m tall is standing on the floor 10.0 m from the basket. If he shoots the ball at a 40.0

° angle with the horizontal, at what initial speed must he throw so that it goes through the hoop without striking the backboard? The basket height is 3.05 m.

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Homework 5B: Docking the Ship

1. A dart player throws a dart horizontally at 12.4 m/s. The dart hits the board 0.32 m below the height from which it was thrown. How far away is the player from the board?

2. As a ship is approaching the dock at 45.0 cm/s, an important piece of landing equipment needs to be thrown to it before it can dock. This equipment is thrown at 15.0 m/s at 60.0

° above the horizontal from the top of a tower at the edge of the water, 8.75 m above the ship’s deck.

For this equipment to land at the front of the ship, at what distance

D

from the dock should the ship be when the equipment is thrown? Air resistance can be neglected.

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