galilean relativity projectile motion the principle of relativity

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GALILEAN RELATIVITY Projectile motion The Principle of Relativity

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Page 1: GALILEAN RELATIVITY Projectile motion The Principle of Relativity

GALILEAN RELATIVITY

Projectile motion

The Principle of Relativity

Page 2: GALILEAN RELATIVITY Projectile motion The Principle of Relativity

NON-ZERO INITIAL SPEED

v

t

v0

v0 + at

v = v0 + at x = vAVt = ½(v0 + v)t

x = ½(v0 + v0 + at)t = v0t + 1/2at2

Page 3: GALILEAN RELATIVITY Projectile motion The Principle of Relativity

EXAMPLE: THROW ROCK UP

Then v = v0 -gt

Choose upward to be positive displacement and speed.(This choice is arbitrary)

Let v0 = 5m/s and g = 10m/s2

When does the rock get to the top of its motion?

v = 0 = 5 – 10t so 5 = 10t and t = 0.5s

How high did it go?

y = v0t – 1/2gt2 = 5(0.5) – 5(0.5)2 = 2.5 – 1.25 = 1.25m

Page 4: GALILEAN RELATIVITY Projectile motion The Principle of Relativity

QUESTION

For the rock just thrown, what was its accelerationat the very top of its motion?

A. + 10 m/s2

B. + 5 m/s2

C. 0 m/s2

D. - 5 m/s2

E. - 10 m/s2

Page 5: GALILEAN RELATIVITY Projectile motion The Principle of Relativity

SAME QUESTION USING INCLINED PLANE

Cart on track with motion sensor.

Start it initially moving upwards. This is analogous to throwing the rock up.

v0

Page 6: GALILEAN RELATIVITY Projectile motion The Principle of Relativity

DROP ROCK FROM TOP OF BUILDING

Here we extend our earlier equations by adding an initial displacement

y = y0 – 1/2gt2

Let y0 = 50m.

y = 50 – 5t2

When does it hit? Answer: when y = 0

0 = 50 – 5t2 so 5t2 = 50 and t2 = 10 so t = 3.2 s

Page 7: GALILEAN RELATIVITY Projectile motion The Principle of Relativity

SHOOT AND DROP

v

Page 8: GALILEAN RELATIVITY Projectile motion The Principle of Relativity

ROLL AND FALL

Page 9: GALILEAN RELATIVITY Projectile motion The Principle of Relativity

SUPERPOSITION

x = v0ty = y0 – 1/2gt2

y = y0 – [g/2v02]x2

Parabola

This is called projectile motion.

Page 10: GALILEAN RELATIVITY Projectile motion The Principle of Relativity

EXAMPLE

A building is 20m high.A rock is thrown off it horizontally with speed15 m/s. How far away doesthe rock land?

Time in the air:y = y0 – 1/2gt2

= 20 – 5t2 = 0t2 = 4, t = 2 seconds.

x = v0t = 15*2 = 30m

Page 11: GALILEAN RELATIVITY Projectile motion The Principle of Relativity

GALILEAN RELATIVITYPerson on a moving ship drops a rock. They see it fall straightdown to land at their feet.

Someone on shore sees the rock continue to move horizontallyas it falls, and says the trajectory is parabolic.

Another observer on another ship sees it move horizontally witha different speed and sees a different parabola.

They all see it land at the same time. Galileo concluded that thehorizontal motion cannot influence the vertical motion, and thatwhat takes place on the ship is independent of the ship’s motion. He argued this applies to all physical and biological processes.

The same principle applies to what takes place on a moving Earth.

Page 12: GALILEAN RELATIVITY Projectile motion The Principle of Relativity

RELATIVITY CAR

v0

v

Page 13: GALILEAN RELATIVITY Projectile motion The Principle of Relativity

Target is released when dart is fired

x

h

DART AND TARGET