Walker3 Lecture Ch12

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2007 Pearson Prentice Hall

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Lecture Outlines

Chapter 12

Phys ics, 3rdEdit ion

James S. Walker


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Chapter 12

Gravity


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Units of Chapter 12

Newtons Law of Universal Gravitation Gravitational Attraction of Spherical

Bodies

Keplers Laws of Orbital Motion

Gravitational Potential Energy

Energy Conservation

Tides


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12-1 Newtons Law of Universal Gravitation

Newtons insight:

The force accelerating an apple downward is

the same force that keeps the Moon in its orbit.

Hence, Universal Gravitation.


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The gravitational force is always attractive, and

points along the line connecting the two

masses:

The two forces shown are an action-reaction

pair.


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Gis a very small number; this means that theforce of gravity is negligible unless there is a

very large mass involved (such as the Earth).

If an object is being acted upon by several

different gravitational forces, the net force on it

is the vector sum of the individual forces.

This is called the principle of superposition.


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12-2 Gravitational Attraction of Spherical

Bodies

Gravitational force between a point mass and a

sphere: the force is the same as if all the mass

of the sphere were concentrated at its center.


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Bodies

What about the gravitational force on objects atthe surface of the Earth? The center of the Earth is

one Earth radius away, so this is the distance we

use:

Therefore,


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Bodies

The acceleration of gravity decreases slowly withaltitude:


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Bodies

Once the altitude becomes comparable to the

radius of the Earth, the decrease in the

acceleration of gravity is much larger:


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Bodies

The Cavendish experiment allows us to measurethe universal gravitation constant:


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Bodies

Even though the gravitational force is very small,the mirror allows measurement of tiny deflections.

Measuring G also allowed the mass of the Earth tobe calculated, as the local acceleration of gravity

and the radius of the Earth were known.


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12-3 Keplers Laws of Orbital Motion

Johannes Kepler made detailed studies of the

apparent motions of the planets over many years,and was able to formulate three empirical laws:

1. Planets follow elliptical orbits, with the Sun at

one focus of the ellipse.


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2. As a planet moves in its orbit, it sweeps out an

equal amount of area in an equal amount of time.


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3. The period,T

, of a planet increases as itsmean distance from the Sun, r, raised to the 3/2

power.

This can be shown to be a consequence of the

inverse square form of the gravitational force.


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A geosynchronous satellite is one whose orbital

period is equal to one day. If such a satellite is

orbiting above the equator, it will be in a fixed

position with respect to the ground.

These satellites are used for communications and

and weather forecasting.


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GPS satellites are not in geosynchronous orbits;

their orbit period is 12 hours. Triangulation of

signals from several satellites allows preciselocation of objects on Earth.


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Keplers laws also give us an insight into

possible orbital maneuvers.


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12-4 Gravitational Potential Energy

Gravitational potential energy of an object of

mass m a distance rfrom the Earths center:

12 4 G


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12-4 Gravitational Potential Energy

Very close to the Earths surface, the

gravitational potential increases linearly withaltitude:

Gravitational potential energy, just like all

other forms of energy, is a scalar. Ittherefore has no components; just a sign.


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12-5 Energy Conservation

Total mechanical energy of an object of mass m

a distance r from the center of the Earth:

This confirms what we already know as an

object approaches the Earth, it moves fasterand faster.

12 5 E C ti


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12 5 E C ti


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Another way of visualizing the gravitational

potential well:

12 5 E C ti


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Escape speed: the initial upward speed a

projectile must have in order to escape

from the Earths gravity

12 5 E C ti


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Speed of a projectile as it leaves the Earth,

for various launch speeds

12 5 E C ti


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Black holes:

If an object is sufficiently massive and

sufficiently small, the escape speed will

equal or exceed the speed of light

light itself will not be able to escape the

surface.

This is a black hole.

12 5 E C ti


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Light will be bent by any

gravitational field; this canbe seen when we view a

distant galaxy beyond a

closer galaxy cluster. This is

called gravitational lensing,and many examples have

been found.

12 6 Tid


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12-6 Tides

Usually we can treat planets, moons, and stars

as though they were point objects, but in factthey are not.

When two large objects exert gravitational

forces on each other, the force on the near sideis larger than the force on the far side, because

the near side is closer to the other object.

This difference in gravitational force across an

object due to its size is called a tidal force.

12 6 Tides


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12-6 Tides

This figure illustrates a general tidal force on

the left, and the result of lunar tidal forces on

the Earth on the right.

12 6 Tides


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12-6 Tides

Tidal forces can result in orbital locking,

where the moon always has the same facetowards the planetas does Earths Moon.

If a moon gets too close to a large planet, the

tidal forces can be strong enough to tear the

moon apart. This occurs inside the Roche

limit; closer to the planet we have rings, notmoons.

Summary of Chapter 12


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Force of gravity between two point masses:

G is the universal gravitational constant:

In calculating gravitational forces,spherically symmetric bodies can be replaced

by point masses.



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Acceleration of gravity:

Mass of the Earth:

Keplers laws:1. Planetary orbits are ellipses, Sun at one

focus

2. Planets sweep out equal area in equal time

3. Square of orbital period is proportional to

cube of distance from Sun



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Orbital period:

Gravitational potential energy:

U is a scalar, and goes to zero as the

masses become infinitely far apart



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Total mechanical energy:

Escape speed:

Tidal forces are due to the variations ingravitational force across an extended body

Walker3 Lecture Ch12

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