chapter ix gravitation a. newtons law of gravitation b. weight c. gravitational potential energy d....

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Chapter IX Gravitation A. Newton’s Law of Gravitation B. Weight C. Gravitational Potential Energy D. Orbits E. Blach Hole

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Page 1: Chapter IX Gravitation A. Newtons Law of Gravitation B. Weight C. Gravitational Potential Energy D. Orbits E. Blach Hole

Chapter IXGravitationA. Newton’s Law of GravitationB. WeightC. Gravitational Potential EnergyD. OrbitsE. Blach Hole

Page 2: Chapter IX Gravitation A. Newtons Law of Gravitation B. Weight C. Gravitational Potential Energy D. Orbits E. Blach Hole

Every particle or matter in the universe attracts every other particle with a force that is directly proportional to the product of the masses of the particles and inversely proportional to the square of the distance between them.

A. Newton’s Law of Gravitation

Gavitational Constant =

Page 3: Chapter IX Gravitation A. Newtons Law of Gravitation B. Weight C. Gravitational Potential Energy D. Orbits E. Blach Hole

B. Weight

w = mg

Page 4: Chapter IX Gravitation A. Newtons Law of Gravitation B. Weight C. Gravitational Potential Energy D. Orbits E. Blach Hole

C. Gravitational Potential Energy

work is given by,

where Fr is the radial component of the gravitational force F that is, the component in the direction outward from the center of the earth.

Because F points directly inward toward the center of the earth, F, is negative. The magnitude of the gravitational force, by a minus sign,

Page 5: Chapter IX Gravitation A. Newtons Law of Gravitation B. Weight C. Gravitational Potential Energy D. Orbits E. Blach Hole

Wgrav = - (U2 – U1)Gravitational Potential Energy

Page 6: Chapter IX Gravitation A. Newtons Law of Gravitation B. Weight C. Gravitational Potential Energy D. Orbits E. Blach Hole

D. Orbits

Page 7: Chapter IX Gravitation A. Newtons Law of Gravitation B. Weight C. Gravitational Potential Energy D. Orbits E. Blach Hole
Page 8: Chapter IX Gravitation A. Newtons Law of Gravitation B. Weight C. Gravitational Potential Energy D. Orbits E. Blach Hole

E. BLACK HOLE The concept of a black hole is one of the

most interesting and startling products of modern gravitational theory, yet the basic idea can be understood on the basis of Newtonian principles.

Page 9: Chapter IX Gravitation A. Newtons Law of Gravitation B. Weight C. Gravitational Potential Energy D. Orbits E. Blach Hole

The Escape Speed from a StarThink first about the properties of our own sun. Its mass M = 1.99 X 1030 kg and radius R = 6.96 X 108 m are much larger than those of any planet, but compared to other stars, our sun is not exceptionally massive. The sun's average density ,

Page 10: Chapter IX Gravitation A. Newtons Law of Gravitation B. Weight C. Gravitational Potential Energy D. Orbits E. Blach Hole

The sun's temperatures range from 5800 K at the surface up to 1.5 X 107 K in the interior, so it surely contains no solids or liquids.

Yet gravitational attraction pulls the sun's gas atoms together until the sun is, on average, 41 % denser than water and about 1200 times as dense as the air we breathe.

Page 11: Chapter IX Gravitation A. Newtons Law of Gravitation B. Weight C. Gravitational Potential Energy D. Orbits E. Blach Hole

From the earth to the moon. Three men were sent to the moon in a shell fired from a giant cannon sunk in the earth in Florida. Find the escape speed-that is, the muzzle speed that would allow the shell to escape from the earth completely. Neglect air resistance, the earth's rotation, and the gravitational pull of the moon. The earth's radius is RE = 6380 km = 6.38 X 106 m, and its mass is mE = 5.97 X 1024 kg.

Page 12: Chapter IX Gravitation A. Newtons Law of Gravitation B. Weight C. Gravitational Potential Energy D. Orbits E. Blach Hole

Solution:

This result does not depend on the mass of the shell, nor does it depend on the direction in which the shell is launched

Page 13: Chapter IX Gravitation A. Newtons Law of Gravitation B. Weight C. Gravitational Potential Energy D. Orbits E. Blach Hole

To generalize our result, the initial speed v, needed for a body to escape from the surface of a spherical mass M with radius R (ignoring air resistance) is

Substituting M = V = (4/3 R3) into

Using either form of this equation, you can show that the escape speed for a body at the surface of our sun is

v = 6.18 X 105 m/ s. This value, roughly 1/500 the speed of light.

Page 14: Chapter IX Gravitation A. Newtons Law of Gravitation B. Weight C. Gravitational Potential Energy D. Orbits E. Blach Hole

Noted that if a body with the same average density as the sun had about 500 times the radius of the sun, its escape speed would be greater than the speed of light c. With his statement that "all light emitted from such a body would be made to return toward it," Mitchell became the first person to suggest the existence of what we now call a black hole.

Page 15: Chapter IX Gravitation A. Newtons Law of Gravitation B. Weight C. Gravitational Potential Energy D. Orbits E. Blach Hole

The first expression for escape speed suggests that a body of mass M will act as a black hole if its radius R is less than or equal to a certain critical radius. by simply setting v = c

For sun,

radius of sun R = 6.96 X 108 m