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(1)

Catapult Engineering

Pilot Workshop

LA Tech STEP

2007 - 2008

(2)

Some Background Info

• Galileo Galilei (1564-1642) did

experiments regarding Acceleration.

• He realized that the change in velocity of balls rolling down inclined planes and

falling objects were accelerated by the

same phenomenon and followed the same

mathematical rules.

(3)

Galileo observed that the final velocity of an object starting from rest and accelerating at a constant rate equals the

product of the acceleration and the elapsed time. If it had an initial velocity, the final velocity will equal the sum of the initial velocity and the increase in

velocity caused by the acceleration.

From rest w/ initial velocity

V

f

= aDt V

f

= V

o

+ aDt

(4)

Objects fall toward Earth because of a force called gravity. Acceleration due to gravity (g) is

9.8 m/s

2

1 sec 9.8 m/s 2 sec 19.6 m/s

If a bowling ball

dropped from the roof, after the 1st second, it would be traveling 9.8 m/s.

A second later its velocity is 19.6 m/s.

After falling for 10 seconds, its velocity is 98 m/s or about 219 miles per hour!

0 m/s

(5)

Isaac Newton (1642-1727)

•Newton pondered Galileo’s work and motion in general

•He realized that the force (gravity) that

caused the acceleration noted by Galileo was the same force that kept the planets in their orbits

•Newton formulated three laws of motion

• Two are important right now for us

(6)

What exactly is a force?

• A force is a push or a pull

• A force can act though contact

– Spring, rope, chain, friction, etc

• A force can act a distance

– Gravity, magnetism, electrical

(7)

Newton’s First Law

• The Law of Inertia

An object at rest will remain at rest, or an object in motion will remain in motion with

constant velocity when the

net force acting on the object

is zero

(8)

Newton’s Second Law The Law of Acceleration

• The effect of an applied force is to

accelerate a body in the direction of the force.

•The acceleration is proportional to the applied force and the mass of the object.

F=ma

(9)

What does this have to do with a catapult?

Hang on, I’m getting there.

• Consider,

– A bullet is fired horizontally from a rifle

– A second bullet is dropped from the rifle’s height at the exact instant the bullet leaves the rifle’s barrel.

•Which bullet

strikes the ground first? Justify your answer.

Ignore Air resistance

(10)

What force is acting on the bullet flying horizontally? Which of Newton’s Laws applies to this bullet?

What force is acting on the bullet that was dropped? Which law applies to this one?

How many “components of motion are applied to the dropped bullet?

How many “components of motion are applied to the fired bullet?

(11)

That is right. They strike the ground at the same time. Why? Because the only force being applied to each of them in the vertical direction was

gravity. Therefore they fell to the ground at the same rate.

However, their flight paths (trajectories) are different.

The bullet that was dropped had a path that was straight down. What kind of path did the other one follow?

(12)

Yes, A curved one. This is PROJECTILE

MOTION.

Look at the next slide for an animation of

these concepts.

(13)
(14)

A diagram showing the “components” of motion for the projectile launched with horizontal velocity, for

(15)

Note, For Projectile Motion:

• In these illustrations there was an independence of horizontal and vertical motions.

– Horizontal motion is under Newton’s first law;

therefore, it is at constant horizontal velocity – Vertical motion is under Newton’s second law;

therefore, it is at constant downwards acceleration

• The combination of these two motions results in the observed parabolic path of a projectile.

(16)

Now, lets launch the projectile at an upward angle.

• Again, What forces act vertically? Horizontally?

• As a result, what type of flight path is taken?

• What components of velocity are involved?

(17)

Diagram of a projectile launched at an

upwards angle with an initial velocity of Vo.

(18)

A few formulas

From rest w/ initial velocity V

f

= aDt V

f

= V

o

+ aDt

Dd = ½ aDt

2

Dd = V

o

Dt + ½ aDt

2

Vf = 2aDd

2

+ 2aDd

Speed: V=Dd/Dt

The following acceleration formulas are based

on or can be derived from Galileo's work:

(19)

How might this apply to a Catapult?

(20)

Projectile Motion

(Motion in 2 Dimensions)

distance (s), time (t)

Launch Angle ()

height (h)

Oh, yeah. An object launched from a catapult is a projectile.

•It is launched with

•an initial velocity, Vo

•An initial horizontal velocity, Vox

v0y

v0x

(21)

distance (s), time (t)

Launch Angle ()

height (h)

v0y

v0x

A projectile is launched with an initial velocity of 22.0 m/s at an angle of 40.0o. Calculate the range of the projectile.

To calculate range, you need to use this formula: Ddx = VxDt Therefore, we need to calculate Dt, Vx

But, to calculate Dt, we need to calculate Vy So let’s get at it.

(22)

distance (s), time (t)

Launch Angle ()

height (h)

v0y

v0x

Sin  = Voy / Vo Voy = Vo Sin 

= 22.0 m/s x Sin 40.0o

= 14.1 m/s

Cosin  = Vox / Vo Vox = Vo cosin 

= 22.0 m/s x cosin 40.0o

= 16.9 m/s

First calculate horizontal and vertical components of Vo:

(23)

distance (s), time (t)

Launch

Angle () height (h) Ddy

v0y

v0x

Now let’s calculate Dt

Ddy =VoyDt + ½ aDt2

= Dt (Voy + ½ aDt) since projectile goes up and back down Ddy = 0 0 = Dt (Voy + ½ aDt)

0 = (Voy + ½ aDt) & 0 = Dt

Dt =- [(2)(Voy)] / g a = g = -9.8m/s2

= -[(2) (14.1 m/s)] /-9.8 m/s2

=2.88 s flight time

(24)

distance (Ddx), time (t)

Launch

Angle () height (h) Ddy

v0y

v0x

Now we can finally calculate range.

Range = Ddx Vox = Ddx / Dt Ddx = Vox Dt

= (16.9 m/s)(2.88s)

= 48.67 m

= 49 m

(25)

Wait

How to you get the projectile up to it’s initial velocity, Vo?

Right, a force has to be applied to accelerate the projectile

.

That is where the spring comes in.

(26)

What’s Next?

In order to design and build a catapult to

accomplish certain tasks, you are going to have to apply kinematic (motion) formulas and solve for the variables concerning projectile motion,

angular acceleration, potential energy of springs, and other such stuff..

Fortunately for me, that is someone else’s job to show you.

(27)

Thank heavens for that

References

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