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Newton’s Law of Universal Gravitation states that gravity is an attractive force acting between all pairs of massive objects.
Gravity depends on: Masses of the two objects Distance between the objects
Universal Gravitation
Newton’s question:
Can gravity be the force keeping the Moon in its orbit?
Newton’s approximation: Moon is on a circular orbit
Even if its orbit were perfectly circular, the Moon would still be accelerated
v
v
v
v
Universal Gravitation
The Moon’s Orbital Speed
radius of orbit: r = 3.8 x 108 m
Circumference: 2r = ???? m
orbital period: T = 27.3 days = ???? sec
orbital speed: v = (2r)/T = ??? m/sec
The Moon’s Orbital Speed
radius of orbit: r = 3.8 x 108 m
Circumference: 2r = 2.4 x 109 m
orbital period: T = 27.3 days = 2.4 x 106 sec
orbital speed: v = (2r)/T = 103 m/sec = 1 km/s
The Moon’s Centripetal Acceleration
The centripetal acceleration of the moon:
orbital speed: v = 103 m/s
orbital radius: r = 3.8 x 108 m
centripetal acceleration: Ac = v2 / r = ???? m/s2
The Moon’s Centripetal Acceleration
The centripetal acceleration of the moon:
orbital speed: v = 103 m/s
orbital radius: r = 3.8 x 108 m
centripetal acceleration: Ac = v2 / r
Ac = (103 m/s)2 / (3.8 x 108 m) = 0.00272 m/s2
At the surface of Earth (r = radius of Earth)
a = 9.8 m/s2
At the orbit of the Moon (r = 60x radius of Earth)
a =0.00272 m/s2
What’s relation between them?
The Moon’s Centripetal Acceleration
At the surface of Earth (r = radius of Earth)
a = 9.8 m/s2
At the orbit of the Moon (r = 60x radius of Earth)
a =0.00272 m/s2
9.8 m/s2 / 0.00272 m/s2 = 3600 / 1 = 602 / 1
The Moon’s Centripetal Acceleration
r 2r 3r 4r 5r 6r 60r
g g g g g g g1 4 9 16 25 36 3600
Bottom LineThe Moon’s Centripetal Acceleration
Bottom LineGravity’s Inverse Square Law
r 2r 3r 4r 5r 6r 60r
Fg Fg Fg Fg Fg Fg Fg
1 4 9 16 25 36 3600
Bottom LineGravity’s Inverse Square Law
Gravity decreases with altitude, since greater altitude means greater distance from the Earth's centre
If all other things being equal, on the top of Mount Everest (8,850 metres), weight decreases about 0.28%
Bottom LineGravity’s Inverse Square Law
Astronauts in orbit are NOT weightless
At an altitude of 400 km, a typical orbit of the Space Shuttle, gravity is still nearly 90% as strong as at the Earth's surface
LocationDistance fromEarth's center
(m)
Value of g(m/s2)
Earth's surface
6.38 x 106 m 9.8
1000 km above
7.38 x 106 m 7.33
2000 km above
8.38 x 106 m 5.68
3000 km above
9.38 x 106 m 4.53
4000 km above
1.04 x 107 m 3.70
5000 km above
1.14 x 107 m 3.08
6000 km above
1.24 x 107 m 2.60
7000 km above
1.34 x 107 m 2.23
8000 km above
1.44 x 107 m 1.93
9000 km above
1.54 x 107 m 1.69
10000 km above
1.64 x 107 m 1.49
50000 km above
5.64 x 107 m 0.13
Bottom LineGravity’s Inverse Square Law
Bottom LineLaw of Universal Gravitation
Newton’s discovery
Newton didn’t discover gravity. In stead, he discovered that the gravity is universal
Everything pulls everything in a beautifully simple way that involves only mass and distance
Bottom LineLaw of Universal Gravitation
Universal gravitation formula
Fg = G m1 m2 / d2
Fg: gravitational force between objects
G: universal gravitational constant
m1: mass of one object
m2: mass of the other object
d: distance between their centers of mass
Bottom LineLaw of Universal Gravitation
Fg = G m1 m2 / d2
Gravity is always there
Though the gravity decreases rapidly with the distance, it never drop to zero
The gravitational influence of every object, however small or far, is exerted through all space
Bottom LineLaw of Universal Gravitation Example
Mass 1 Mass 2 Distance Relative Force
m1 m2 d F
2m1 m2 d
m1 3m2 d
2m1 3m2 d
m1 m2 2d
m1 m2 3d
2m1 2m2 2d
Law of Universal Gravitation Example
Mass 1 Mass 2 Distance Relative Force
m1 m2 d F
2m1 m2 d 2F
m1 3m2 d 3F
2m1 3m2 d 6F
m1 m2 2d F/4
m1 m2 3d F/9
2m1 2m2 2d F
Universal Gravitational Constant
The Universal Gravitational Constant (G) was first measured by Henry Cavendish 150 years after Newton’s discovery of universal gravitation
Universal Gravitational Constant
Cavendish’s experiment
Use Torsion balance (Metal thread, 6-foot wooden rod and 2” diameter lead sphere)
Two 12”, 350 lb lead spheres
The reason why Cavendish measuring the G is to “Weight the Earth”
The measurement is accurate to 1% and his data was lasting for a century
Universal Gravitational Force
Force StrongElectro-
magneticWeak Gravity
Strength 1 1/137 10-6 6x10-39
Range 10-15 m ∞ 10-18 m ∞
Universal Gravitation Example
Calculate the force of gravity between two students with mass 55 kg and 45kg, and they are 1 meter away from each other
Universal Gravitation Example
Calculate the force of gravity between two students with mass 55 kg and 45kg, and they are 1 meter away from each other
Fg = G m1 m2 / d2
Fg = (6.67 x 10-11 N·m2/kg2)(55 kg)(45 kg)/(1 m)2
= 1.65 x 10-7 N
Universal Gravitation Example
Calculate the force of gravity between Earth (mass = 6.0 x 1024 kg) and the moon (mass = 7.4 x 1022 kg). The Earth-moon distance is 3.8 x 108 m
Universal Gravitation Example
Calculate the force of gravity between Earth (mass = 6.0 x 1024 kg) and the moon (mass = 7.4 x 1022 kg). The Earth-moon distance is 3.8 x 108 m
Fg = G m1 m2 / d2
Fg = (6.67 x 10-11 N·m2/kg2)(6.0 x 1024 kg)
(7.4 x 1022 kg)/(3.8 x 108 m)2
= 2.1 x 1020 N
Acceleration Due to Gravity
Law of Universal Gravitation:
Fg = G m M / r2
Weight
Fg = m g
Acceleration due to gravity
g = G M / r2
Fg: gravitational force / weight
G: univ. gravitational constant
M: mass of Earth
m: mass of the object
r: radius of Earth
g: acceleration due to gravity
Universal Gravitation Example
Calculate the acceleration due to gravity of Earth (mass = 6.0 x 1024 kg, radius = 6.37 × 106 m )
Universal Gravitation Example
Calculate the acceleration due to gravity of Earth (mass = 6.0 x 1024 kg, radius = 6.37 × 106 m )
g = G M / r2
g = (6.67 x 10-11 N·m2/kg2)(5.98 x 1024 kg)/(6.37 x 106 m)2
= 9.83 m/s2
Universal Gravitation Example
In The Little Prince, the Prince visits a small asteroid called B612. If asteroid B612 has a radius of only 20.0 m and a mass of 1.00 x 104 kg, what is the acceleration due to gravity on asteroid B612?
Universal Gravitation Example
In The Little Prince, the Prince visits a small asteroid called B612. If asteroid B612 has a radius of only 20.0 m and a mass of 1.00 x 104 kg, what is the acceleration due to gravity on asteroid B612?
g = G M / r2
g = (6.67 x 10-11 N·m2/kg2)(1.00 x 104 kg)/(20.0 m)2
= 1.67 x 10-9 m/s2
Universal Gravitation Example
The planet Saturn has a mass that is 95 times as massive as Earth and a radius that is 9.4 times Earth’s radius. If an object is 1000 N on the surface of Earth, what is the weight of the same object on the surface of Saturn?
Universal Gravitation Example
The planet Saturn has a mass that is 95 times as massive as Earth and a radius that is 9.4 times Earth’s radius. If an object is 1000 N on the surface of Earth, what is the weight of the same object on the surface of Saturn?
Fg = G m M / r2 Fg ~ M / r2
Fg = 1000 N x 95 / (9.4)2 = 1075 N
Isaac Newton’s Influence
People could uncover the workings of the physical universe
Moons, planets, stars, and galaxies have such a beautifully simple rule to govern them
Phenomena of the world might also be described by equally simple and universal laws
Summary
• Isaac Newton• Universal gravitation – Apple and Moon? • Moon’s centripetal acceleration• Gravity’s inverse square law• Law of universal gravitation• Universal gravitational constant – Henry Cavendish• Calculate the mass of Earth• Weak gravitational force• Acceleration due to gravity• Newton’s influence
Force Field
A force field exerts a force on objects in its vicinity
Magnetic Field
A magnetic field is a force field that surrounds a magnet and exerts a magnetic force on magnetic substances
Electric Field
An electric field is a force field surrounding electric charges
Gravitational Field
Gravitational Field
A gravitational field is a force field that surrounds massive objects
Gravitational Field
Earth’s gravitational field is represented by imaginary field lines
Where the field lines are closer together, the gravitational field is stronger
The direction of the field at any point is along the line the point lies on
Arrows show the field direction
Any mass in the vicinity of Earth will be accelerated in the direction of the field line at that location
Earth’s Gravitational Field
Strength of the gravitational field is the force per unit mass exerted by Earth on any object
Gravitational Field
g = Fg / m = (G m M / r2) / m = G M / r2
F: weight of the objectG: universal gravitational constant (6.67 x 10-11 N·m2/kg2) m: mass of the objectM: mass of Earth (5.98 x 1024 kg)r: Earth’s radius (6.37 x 106 m)
Strength of Gravitational Field
Gravitational Field Inside a Planet
Cancellation of gravitational force
If Earth were of uniform density, the gravity of the entire surrounding shell of inner radius equal to your radial distance from the center will completely cancel out
P
Cr
Gravitational Field Inside a Planet
A BP
Cancellation of gravitational force
The gravity of area A and area B on P completely cancel out
Gravitational Field Inside a Planet
Cancellation of gravitational force
You are pulled only by the mass within this shell – below you
At Earth’s center, the whole Earth is the shell and complete cancellation occurs
P
Cr
Gravitational Field Inside a Planet
Strength of the gravitational field is proportional to M / r2
g = GM/r2 = GDV/r2 = GD(4/3)πr3/r2 = (4/3)GDπr
g ~ r
G: universal gravitational constant (6.67 x 10-11 N·m2/kg2) M: mass of Earth (5.98 x 1024 kg)D: density of EarthV: volume of Earthr: distance to the Earth’s center
Gravitational Field Inside a Planet
Without air drag, the trip would take nearly 45 minutes. The gravitational field strength is steadily decreasing as you continue toward the center
At the center of Earth, you are pulled in every direction equally, so that the net force is zero and the gravitational field is zero