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Chapter 6 Uniform Circular Motion and Gravitation (1/5) -- x-Douglas College Physics 1107 Fall 2019...

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Chapter 6 Uniform Circular Motion and Gravitation

Chapter 6 Uniform Circular Motion and Gravitation 6.6 Satellites and Kepler’s Laws: An Argument for Simplicity Summary - State Kepler’s laws of planetary motion. - Derive the third Kepler’s law for circular orbits. - Discuss the Ptolemaic model of the universe. - Define a planet according to the I.A.U. the International Astronomical Union - Explain why Pluto is not a planet Examples of gravitational orbits abound. Hundreds of artificial satellites orbit Earth together with thousands of pieces of debris. The Moon’s orbit about Earth has intrigued humans from time immemorial. The orbits of planets, asteroids, meteors, and comets about the Sun are no less interesting. If we look further, we see almost unimaginable numbers of stars, galaxies, and other celestial objects orbiting one another and interacting through gravity. All these motions are governed by gravitational force, and it is possible to describe them to various degrees of precision. Precise descriptions of complex systems must be made with large computers. However, we can describe an important class of orbits without the use of computers, and we shall find it instructive to study them. These orbits have the following characteristics: - A small mass m1 orbits a much larger mass m2.This allows us to view the motion as if m2 were stationary—in fact, as if from an inertial frame of reference placed on m2—without significant error. Mass m1 is the satellite of m2, if the orbit is gravitationally bound. - The system is isolated from other masses. This allows us to neglect any small effects due to outside masses. The conditions are satisfied, to good approximation, by Earth’s satellites (including the Moon), by objects orbiting the Sun, and by the satellites of other planets. Historically, planets were studied first, and there is a classical set of three laws, called Kepler’s laws of planetary motion, that describe the orbits of all bodies satisfying the two previous conditions (not just planets in our solar system). These descriptive laws are named for the German astronomer Johannes Kepler (1571–1630), who devised them after careful study (over some 20 years) of a large amount of meticulously recorded observations of planetary motion done by Tycho Brahe (1546–1601). Such careful collection and detailed recording of methods and data are hallmarks of good science. Data constitute the evidence from which new interpretations and meanings can be constructed. Kepler’s Laws of Planetary Motion Kepler’s First Law The orbit of each planet about the Sun is an ellipse with the Sun at one focus. Kepler’s Second Law Each planet moves so that an imaginary line drawn from the Sun to the planet sweeps out equal areas in equal times (see Figure 2). Kepler’s Third Law The ratio of the squares of the periods of any two planets about the Sun is equal to the ratio of the cubes of their average distances from the Sun. In equation form, this is where T is the period (time for one orbit) and r is the average radius. Th
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