Astronomy 101 The Solar System Tuesday, Thursday 2:30-3:45 pm Hasbrouck 20 Tom Burbine

Slides:



Advertisements
Similar presentations
Section 2: Newton’s Law of Gravitation
Advertisements

The Beginning of Modern Astronomy
Chapter 4 Making Sense of the Universe Understanding Motion, Energy, and Gravity.
Gravity. Review Question What are Kepler’s laws of planetary motion?
Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display. Fix Astronomy Chapter 5.
Astronomy 101 The Solar System Tuesday, Thursday 2:30-3:45 pm Hasbrouck 20 Tom Burbine
Survey of the Universe Tom Burbine
© 2004 Pearson Education Inc., publishing as Addison-Wesley 5.1 Describing Motion: Examples from Daily Life Distinguish between speed, velocity, and acceleration.
Astronomy 100 Tuesday, Thursday 2:30 - 3:45 pm Tom Burbine
Newton’s Law of Universal Gravitation By: Heather Britton.
Gravity, Projectiles, and Satellites Physics Click HERE if the web page above does not open. In this lesson, we will discuss the following: Newton’s Law.
Astronomy 101 The Solar System Tuesday, Thursday Tom Burbine
Today’s APODAPOD  Start Reading NASA website (Oncourse)  2 nd Homework due TODAY  IN-CLASS QUIZ NEXT FRIDAY!! The Sun Today A100 Solar System.
Astronomy 101 The Solar System Tuesday, Thursday 2:30-3:45 pm Hasbrouck 20 Tom Burbine
Ms. Mitchell’s 6th Grade Greenbriar West Elementary Matter.
Earth and Moon I 1) the Earth pulls harder on the Moon
Physics I Honors 1 Specific Forces Fundamental Forces Universal Gravitation.
Universal Gravitation
Gravity Chapter 7. Newton  Noticed the moon followed a curved path  Knew a force was required to allow an object to follow a curved path  Therefore,
Part 4 Newton’s Second Law of Motion Newton’s Second Law Acceleration is the rate at which your velocity (speed with direction) changes.
Newton’s Law of Universal Gravitation
Ms. Mitchell’s 6th Grade Greenbriar West Elementary TEACHER VERSION Matter.
Kepler’s first law of planetary motion says that the paths of the planets are A. Parabolas B. Hyperbolas C. Ellipses D. Circles Ans: C.
Universal Gravitation Chapter 8. Isaac Newton and Gravity Newton realized an apple falls because of force Moon follows circular path, force needed Newton.
In order to stay in a closed orbit, an object has to be within a certain range of velocities: Too slow  Object falls back down to Earth Too fast  Object.
Astronomy 101 The Solar System Tuesday, Thursday Tom Burbine
Universal Gravitation Physics Mr. Padilla. Falling Apple hits Newton on the head. According to the law of inertia, it would not fall unless acted upon.
Chapter 5 Circular Motion; Gravitation. © 2004 Pearson Education Inc., publishing as Addison- Wesley The Force of Gravity What is the universal law of.
Astronomy 101 The Solar System Tuesday, Thursday Tom Burbine
Newton believed that every object ___attracts_____ every other object. The force of the attraction depends on the __mass___ and _distance__ of the two.
GRAVITY What goes up, must come down??. Gravity Is it possible for some basketball players to “hang” in the air during a dunk? Give your opinion
Universal Gravitation.
Astronomy 101 The Solar System Tuesday, Thursday Tom Burbine
Astronomy 101 The Solar System Tuesday, Thursday 2:30-3:45 pm Hasbrouck 20 Tom Burbine
Describing Motion: Examples from Daily Life Distinguish between speed, velocity, and acceleration. What is the acceleration of gravity? How does the acceleration.
Introduction to Physical Science Monday, Wednesday, Thursday Tom Burbine
Gravity and Orbits   Newton’s Law of Gravitation   The attractive force of gravity between two particles   G = 6.67 x Nm 2 /kg 2 Why is this.
SPH3U – Unit 2 Gravitational Force Near the Earth.
Getting Off the Earth Focus 2 Part 2.
Find the gravitational attraction of the moon to the Earth using the regents reference tables. What would the gravitational attraction of the Earth to.
Copyright © 2010 Pearson Education, Inc. Lecture Outline Chapter 12 Physics, 4 th Edition James S. Walker.
Copyright © 2012 Pearson Education Inc. Gravitation Physics 7C lecture 17 Tuesday December 3, 8:00 AM – 9:20 AM Engineering Hall 1200.
Newton’s Universal Law of Gravitation Chapter 8. Gravity What is it? The force of attraction between any two masses in the universe. It decreases with.
Newton’s Law of Universal Gravitation
Notes: Forces Big “G” and little “g” Newton’s Law of Universal Gravity -F g, the force of attraction between two objects is directly proportional to the.
Astronomy 101 The Solar System Tuesday, Thursday 2:30-3:45 pm Hasbrouck 20 Tom Burbine
If it is known that A is directly proportional to B, how would A change if B is increased by a factor of 2? 1. Increase by a factor of 2 2. Increase by.
Units are covered. Galileo Galilei ( ) Using a Dutch-designed telescope that he built himself, he made several startling observations that.
Astronomy 101 The Solar System Tuesday, Thursday 2:30-3:45 pm Hasbrouck 20 Tom Burbine
4.4 & 4.5 Gravity, Tides and Orbits. Newton discovered that gravity is universal. Everything pulls on everything else in a way that involves only mass.
Gravity 1.Gravity requires air/atmosphere. 2.The strength of a gravitational force depends on the mass of objects. 3.ALL objects in the Universe attract.
Astronomy 101 The Solar System Tuesday, Thursday 2:30-3:45 pm Hasbrouck 20 Tom Burbine
Universal Gravitation Ptolemy (150AD) theorized that since all objects fall towards Earth, the Earth must be the center of the universe. This is known.
What holds us together? Gravity. Gravity is a force Force: a push or pull exerted on an object Gravity: the attractive force between objects; force that.
Which is stronger, Earth’s pull on the Moon, or the Moon’s pull on Earth? 1) the Earth pulls harder on the Moon 2) the Moon pulls harder on the Earth 3)
FgFg agag mg g W Do you know the difference?? Newton’s Law of Universal Gravitation Every body in the universe attracts every other body with a force.
Newton Anything with mass attracts anything else with mass. The size of that attraction is given by my Law of Gravitation: Fg = Gm 1 m 2 r 2.
Gravity and Motion. Kepler’s Theory of Planetary Motion 1. Paths are ellipses and sun at the focus 2. Planets move faster when closer 3. Relationship.
The story of the apple When Newton observed the apple fall, he wondered if the force that caused the apple to fall to the ground was the same force that.
Centripetal force Acceleration Mass Contact force momentum
Gravitation: Forces and Escape Velocity
Gravitation.
GRAVITY.
Newton’s Laws of Motion
Gravity.
Gravity and Motion.
The story of the apple When Newton observed the apple fall, he wondered if the force that caused the apple to fall to the ground was the same force that.
Newton’s Law of Universal Gravitation
Newton’s Law of Universal Gravitation
Presentation transcript:

Astronomy 101 The Solar System Tuesday, Thursday 2:30-3:45 pm Hasbrouck 20 Tom Burbine

Course Course Website: – Textbook: –Pathways to Astronomy (2nd Edition) by Stephen Schneider and Thomas Arny. You also will need a calculator.

Office Hours Mine Tuesday, Thursday - 1:15-2:15pm Lederle Graduate Research Tower C 632 Neil Tuesday, Thursday - 11 am-noon Lederle Graduate Research Tower B 619-O

Homework We will use Spark owebcthttps://spark.oit.umass.edu/webct/logonDisplay.d owebct Homework will be due approximately twice a week

Exam #1 Average was 85 Grades ranged from 40s to 100s

HW #5 Due Thursday

A hypothesis is an educated guess, based on observation. Usually, a hypothesis can be supported or refuted through experimentation or more observation. A hypothesis can be disproven, but not proven to be true. A scientific theory summarizes a hypothesis or group of hypotheses that have been supported with repeated testing. A theory is valid as long as there is no evidence to dispute it. Therefore, theories can be disproven. A law generalizes a body of observations. At the time it is made, no exceptions have been found to a law.

assume all mass is concentrated in the center of a body

F = G M 1 M 2 r 2 The value of G was determined by Henry Cavendish between G = 6.67 x m 3 /(kg  s 2 ) calculate-the-gravitational-constant-like-cavendish- did/ calculate-the-gravitational-constant-like-cavendish- did/

What is the attraction of two people in this room? F = G M 1 M 2 r 2 Say their masses are both 100 kg Their distances are 10 meters apart F = 6.67 x m 3 /(kg  s 2 ) * 100*100 kg 2 /(10*10 m 2 ) F = 6.67 x N = N Remember the person weighs 980 N

F = G M 1 M 2 r 2 How would the force between the two people change if they were only 5 meters apart instead of 10 meters? A) Stay the same B) Double (Increase by a Factor of 2) C) Quadrupul (Increase by a Factor of 4) D) halve (decrease by a factor of 2)

F = G M 1 M 2 = G M 1 M 2 = 4 G M 1 M 2 (r/2) 2 r 2 /4 r 2 How would the force between the two people change if they were only 5 meters apart instead of 10 meters? A) Stay the same B) Double (Increase by a Factor of 2) C) Quadrupul (Increase by a Factor of 4) D) halve (decrease by a factor of 2)

Acceleration of gravity (g) M is the Earth’s mass F = ma = G Mm r is the Earth’s radius r 2 m is the mass of an object F is the force a is the acceleration a = G M r 2 g = a = G M r 2

Acceleration of gravity (g) M is the Earth’s mass g = G M r is the Earth’s radius r 2 g = 6.67 x m 3 /(kg  s 2 ) * (6.0 x kg) (6.4 x 10 6 m) * (6.4 x 10 6 m) g = 9.8 m/s 2

Gravitational acceleration Gravitational acceleration is different on different planets because they have different sizes and masses Gravitational acceleration (on Moon) = 1.6 m/s² (0.165 g) Gravitational acceleration (on Jupiter) = 24.8 m/s² (2.53 g)

Experiment on the Moon

How things fall Heavy and light objects fall at the same rate The heavy object does not fall faster (as long as there is no air resistance) g = G M (does not depend on mass of object) r 2

How does gravity work? Gravity distort space-time einsteins-messengershttp:// einsteins-messengers

Escape velocity Velocity above this will allow an object to escape a planet’s gravity For Earth: v = square root[(2 x 6.67 x m 3 /(kg  s 2 ) x (6.0 x kg)] (6.4 x 10 6 m) v = square root [1.25 x 10 8 m 2 /s 2 ] v = 11.2 x 10 3 m/s = 11.2 km/s v

Escape velocity Escape velocity is different on different planets because they have different sizes and masses Escape velocity (on Moon) = 2.4 km/s Escape velocity (on Jupiter) = 59.5 km/s

What causes tides on earth? Moon pulls on different parts of the Earth with different strengths khttp:// k

Forces on Water Average Force on 1 kg water on Earth from Moon F = G M m = 6.67 x m 3 /(kg  s 2 ) * (7.35 x kg) * (1 kg) r 2 (3.84 x 10 8 m) 2 F = 3.33 x N Force of 1 kg on water on near-side of Earth from Sun F = G M m = 6.67 x m 3 /(kg  s 2 ) * (7.35 x kg) * (1 kg) r 2 (3.84 x 10 8 m x 10 6 m) 2 F = 3.44 x N Difference in forces is 1.1 x N Called Tidal Force

Tidal force arises because the gravitational force exerted on one body by a second body is not constant across its diameter Water flows so this tidal force causes the tides that are seen on Earth

Effects on tides due to Sun Sun exerts a stronger gravitational force on the Earth But since farther away, the differential force from one side of the Earth to the other is smaller Sun’s tidal effect is about one-half that of the Moon

Forces on Water Average Force on 1 kg water on Earth from Sun F = G M m = 6.67 x m 3 /(kg  s 2 ) * (2 x kg) * (1 kg) r 2 (1.5 x m) 2 F = x N Force of 1 kg on water on near-side of Earth from Sun F = G M m = 6.67 x m 3 /(kg  s 2 ) * (2 x kg) * (1 kg) r 2 (1.5 x m x 10 6 m) 2 F = x N Difference in forces is 5.0 x N due to Sun Difference in forces is 1.1 x N due to Moon

Remember Force downwards is 9 Newtons on 1 kg of water Water won’t be pulled off Earth Water can flow

Shoemaker-Levy 9 Comet that hit Jupiter Jupiter-orbiting comet Broken apart by tidal forces Discovered in 1993 Hit Jupiter in 1994

Roche Limit The smallest distance at which a natural satellite can orbit a celestial body without being torn apart by the larger body's gravitational force (tidal forces). The distance depends on the densities of the two bodies and the orbit of the satellite. If a planet and a satellite have identical densities, then the Roche limit is times the radius of the planet. Jupiter's moon Metis and Saturn's moon Pan are examples of natural satellites that survive despite being within their Roche limits

Why is the Roche Limit important? Comet Shoemaker-Levy 9's decaying orbit around Jupiter passed within its Roche limit in July, 1992, causing it to break into a number of smaller pieces. All known planetary rings are located within the Roche limit

The first impact occurred at 20:15 UTC on July 16, 1994 Fragment A of the nucleus slammed into Jupiter's southern hemisphere at a speed of about 60 km/s. Instruments on Galileo detected a fireball which reached a peak temperature of about 24,000 K, compared to the typical Jovian cloudtop temperature of about 130 K, before expanding and cooling rapidly to about 1500 K after 40 s.

Has this happened before? Ganymede

Any Questions?