6. Old: )yy(gm)y(U 0g
New:
r
MmG
)r(Ug
How could these be the same?
Consider a location near the surface of the earth, y0
= R, y = R+h.
The only thing that matters is U, not U itself.
Old: hgm)RhR(gmUg +
New:
+
+
hR
1
R
1
MmG
R
MmG
hR
MmG
Ug
+
+
hRR
h
MGm
hR
1
R
1
MGm 2
(h << R)
hgmh
R
MG
m
R
h
MGm 22
8. Newton’s 2nd law force (F) is acting on
falling ball (mass = m)
All masses have same acceleration
. . . so more mass means more force
needed:
mF
F
m
Ball
Earth
9. F
Newton’s 3rd law ball pulls on Earth
Ball
F
Does Earth accelerate?
Earth
10. All bits of matter attract all other bits of matter . . .
M1 M2
d
F F
“Inverse square law”
d
1
F2.
MMF1.
2
21
11. 1. Increase one or both masses, and force increases.
2. Force decreases as distance increases.
Force Distance
400 N 10 m
100 N 20 m
25 N 40 m
16 N 50 m
4 N 100 m
d
M1 M2F F
4
400
2
400
100 2
13. Putting the two parts of the force law together . . .
2
21
d
MGM
F (G = gravitational constant)
Acts through empty space
“action at a distance”
Explains how gravity behaves – but not why
15. Weight
Measure of gravitational attraction of Earth
(or any other planet) for you.
Earth
R
F
m
M
Weight
2
R
GMm
FW
16. Other planets: M and R change, so your
weight must change
Mars: R = 0.53 x Earth’s radius
M = 0.11 x Earth’s mass
Earth Mars
Weight 150 lbs 59 lbs
A real planet . . .
20. By 1915, Einstein had worked through all the math (with some help)
to show that his postulates led to a new theory of gravity based on
the effect of mass and energy to curve the structure of space and
time. His theory has some startling implications, one being the
existence of “black holes” – regions of space where the gravity field
is so high that even light cannot escape. The predictions of General
Relativity, including the existence of black holes, have been
confirmed by all experiments to date.
21. Any motion controlled only by gravity is an orbit
Without gravity
With gravity
NEWTON: Gravity explains how planets (and
moons & satellites & etc.) go.
Sun