astronomy 1010 planetary astronomy fall_2015 day-16

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Astronomy 1010 Fall_2015 Day-16 Planetary Astronomy

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Course Announcements Dark Sky nights – Mon. 10/5 & Wed. 10/7 starting at 7:30pm – at the Observatory. Exam-2 will be Friday, Oct. 9 SW-chapter 4 posted: due Mon. Oct. 5 First Thursday Art Walk 5-8pm tomorrow; downtown

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Page 1: Astronomy 1010 Planetary Astronomy Fall_2015 Day-16

Astronomy 1010Fall_2015Day-16

Planetary Astronomy

Page 3: Astronomy 1010 Planetary Astronomy Fall_2015 Day-16

Course Announcements• Dark Sky nights – Mon. 10/5 & Wed. 10/7 starting at

7:30pm – at the Observatory.

• Exam-2 will be Friday, Oct. 9

• SW-chapter 4 posted: due Mon. Oct. 5• First Thursday Art Walk 5-8pm tomorrow; downtown

Page 4: Astronomy 1010 Planetary Astronomy Fall_2015 Day-16

Definitions & Terms -1• Tide: (1) A laundry detergent

• (2) A gravitational interaction which goes as d3

Page 5: Astronomy 1010 Planetary Astronomy Fall_2015 Day-16

Lecture – TutorialNewton’s Law of Gravity: pg 29

Work with a partner!Read the instructions and questions carefully.Discuss the concepts and your answers with one

another.Come to a consensus answer you both agree on.If you get stuck or are not sure of your answer,

ask another group.If you get really stuck or don’t understand what

the Lecture Tutorial is asking, ask one of us for help.

Page 6: Astronomy 1010 Planetary Astronomy Fall_2015 Day-16

i-Clicker Question

Renaissance Astronomy: Gravity Calculations 1

Page 7: Astronomy 1010 Planetary Astronomy Fall_2015 Day-16

PROCESS OF SCIENCEPROCESS OF SCIENCE For a theory to be

“scientific”, it must be testable.

Old theories that are disproven lead to greater insight.

Page 8: Astronomy 1010 Planetary Astronomy Fall_2015 Day-16

Newton’s Law and Gravitation

• All my favorite Projectiles behave like this!!!

Force

Velocity

Acceleration

Page 9: Astronomy 1010 Planetary Astronomy Fall_2015 Day-16

Kepler’s laws of orbits and Newton’s laws of motion and gravity are only the beginning.

Gravity is very important for shaping objects and orbits.

Internal forces Tides Orbital resonances

Page 10: Astronomy 1010 Planetary Astronomy Fall_2015 Day-16

The gravitational force results in an acceleration.

All objects on Earth fall with the same acceleration known as g.

g = 9.8 m/s2

weightF m g

Page 11: Astronomy 1010 Planetary Astronomy Fall_2015 Day-16

Gravity is an attractive force between any two objects with mass, acting along the line between them.

It depends on the objects’ masses. It depends on the distance between them.

Page 12: Astronomy 1010 Planetary Astronomy Fall_2015 Day-16

G is the universal gravitational constant. The m terms are the two masses. More mass = more force.

Page 13: Astronomy 1010 Planetary Astronomy Fall_2015 Day-16

The distance between the objects is r. A greater r = smaller force. Gravity is governed by an inverse square

law.

Page 14: Astronomy 1010 Planetary Astronomy Fall_2015 Day-16

i-Clicker Question

Renaissance Astronomy: Gravity Calculations 4

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In the Earth-Moon system, the gravitational force of Earth on the Moon is equal to the gravitational force of the Moon on Earth.

The accelerations are different! Remember Newton’s second law: F = m a. The more massive object will have a smaller

acceleration, while the less massive object will have a larger acceleration.

It is the same in the Sun-Earth system.

Page 16: Astronomy 1010 Planetary Astronomy Fall_2015 Day-16

The gravitational interaction of three bodies leads to Lagrangian equilibrium points.

These are special orbital resonances where the object at that point orbits in lockstep.

SOHO is near L1.

CONNECTIONS 4.2

Page 17: Astronomy 1010 Planetary Astronomy Fall_2015 Day-16

Orbits describe one body falling around another.

The less massive object is a satellite of the more massive object.

The two bodies orbit a common center of mass.

For a much smaller satellite, the center of mass is inside the more massive body.

Page 18: Astronomy 1010 Planetary Astronomy Fall_2015 Day-16

An astronaut inside an orbiting space shuttle will experience free fall because he is falling around Earth at the same rate as the shuttle.

He is not weightless.

Page 19: Astronomy 1010 Planetary Astronomy Fall_2015 Day-16

Gravity provides the centripetal force that holds a satellite in its orbit.

Uniform circular motion: moving on a circular pathat constant speed.

Still experiencing an acceleration since the direction is constantly changing.

Page 20: Astronomy 1010 Planetary Astronomy Fall_2015 Day-16

Planets in real-world scenarios move on elliptical orbits.

The gravitational force changes both the direction and the speed of the planet as it moves in its orbit.

Results in Kepler’s law of equal areas.

Page 21: Astronomy 1010 Planetary Astronomy Fall_2015 Day-16

Circles and ellipses are bound orbits. Objects with higher orbital speeds can

escape bound orbits to be in unbound orbits. Parabolas and hyperbolas are examples.

Page 22: Astronomy 1010 Planetary Astronomy Fall_2015 Day-16

Newton derived Kepler’s laws from his law of gravity.

Physical laws explain Kepler’s empirical results:

Distant planets orbit more slowly; the harmonic law and the law of equal areas result.

Newton’s laws were tested by Kepler’s observations.

Page 23: Astronomy 1010 Planetary Astronomy Fall_2015 Day-16

i-Clicker Question

Renaissance Astronomy: Graph Orbital VelocitiesRenaissance Astronomy: Graph Kepler’s 3rd Law

Page 24: Astronomy 1010 Planetary Astronomy Fall_2015 Day-16

The velocity of an object traveling in a circular orbit can be found by equating the gravitational force and the resulting centripetal force.

This yields: You can solve for the period by noting that

This yields Kepler’s third law:

MATH TOOLS 4.2

Page 25: Astronomy 1010 Planetary Astronomy Fall_2015 Day-16
Page 26: Astronomy 1010 Planetary Astronomy Fall_2015 Day-16

Tides are a consequence of gravity.

Something closer to an object experiences a stronger gravitational pull than something else farther away.

Page 27: Astronomy 1010 Planetary Astronomy Fall_2015 Day-16

The centers of Earth and the Moon orbit like point masses.

Parts of Earth are closer to the Moon than other parts.

This produces a stretch on the Earth, called a tide.

Tides cause bulges to appear on either side.

Page 28: Astronomy 1010 Planetary Astronomy Fall_2015 Day-16

Earth’s oceans flow in response to the tidal forces.

The oceans have a tidal bulge: They are elongated in a direction that is nearly pointed at the Moon.

Page 29: Astronomy 1010 Planetary Astronomy Fall_2015 Day-16

Earth rotates under the tidal bulge.

We get two high and two low tides each day.

The behavior is complicated by Earth’s landmasses and solar tides.

Page 30: Astronomy 1010 Planetary Astronomy Fall_2015 Day-16

Tides can affect the solid part of Earth, too.

A gravitational pull can stretch and deform a solid body.

Results in friction, which generates heat. Friction also opposes the rotation of Earth,

causing Earth to very gradually slow its rotation.

Days lengthen by about 0.0015 seconds every century.