Test Repair, Thursday before school (7:20) or
Lunch
Inuit Yoyo lab (circular motion) due Wednesday,
9/9
My Solar System Phet Lab due Friday, 9/11
Unit 3 “exam” and HW due Friday, 9/11
Rocket Lab III Monday 9/14- need more bottles!!!
Circular Motion and Gravitation
Part 2: Universal Gravitation and G
Newton, Newton, Newton, Newton… Arrrgggghhhh!!!
actually stars the moon.
Newton realized that the force that attracted the apple to the Earth was the same as the force that attracted the Moon.
He set up the problem and…….
it didn’t work!!! Ha Ha!!
20 years later he gave it another try:
1680, with Edmund Halley
Gravitational Force, F
G
, depends directly on the product of the masses of the two objects and inversely with the square of the distance between them.
Let’s write that more neatly using math:
F
G a m
1 x m
2
F
G a
1/d 2
So…
F
G a m
1 x m
2 d 2
Still can’t find the a button so let’s change it to =
In order to make the equation work we need a constant, G
G = the universal gravitational constant.
G = 6.67 x 10 -11 Nm 2 /kg 2
This value was determined by a
British physicist, Henry Cavendish, in 1798 in a very slick experiment called “Weighing Earth”
F
G
=
Gm
1 m
2 d 2
CARD!!
This was used to “Weigh Earth”
The force Earth exerts on a 1 kg object at Earth’s surface is
9.8 N.
The distance between the object and Earth’s center is
Earth’s radius, 6.4 x 10 6 m.
So, plug all this in……..
9.8 N = 6.67 x 10 -11 Nm 2 /kg 2
1kg x m
E
(6.4 x 10 6 m) 2
E
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