HOMEWORK 2 SOLUTIONS COSMOLOGY PHYSICS 20B

Size: px
Start display at page:

Download "HOMEWORK 2 SOLUTIONS COSMOLOGY PHYSICS 20B"

Transcription

1 HOMEWORK S COSMOOGY PHYSICS 0B (5pts) 1. If it takes Venus 5 days to orbit the Sun, roughly how far is Venus from the Sun? et us define the period of Venus orbit around the Sun as P V the semi-major axis distance from the Sun as A V. and Venus Since the eccentricity of Venus orbit is very close to zero (e 0.007) the semi-major axis distance is approximately the distance between the Sun and Venus. We can then use the following relation to solve for the distance between Venus and the Sun. P V P E = A3 V A 3 E where P E is the period of the Earth s orbit around the Sun and A E is the Earth s semi-major axis distance from the Sun. Converting 5 days to years and plugging in the values we get the following: (0.616 yr) (1 yr) = A3 V (1 AU) 3 () (0.616 yr) A V = 3 (1 yr) AU 0.74 AU (3) The distance between the Sun and Venus is approximately 0.74 AU. (1) (5pts). Rigel is the brightest star in the Orion constellation. Its spectrum peaks at a wavelength of approximately 77 Å. What is the temperature at the surface of Rigel? We can use the following relation to solve for the temperature of Rigel given its mas wavelength. λ MAX = 600 nm 5000 K T First we must convert 77 Åto nm. Note: 1 Å= m (4) m 109 nm 1 m = 7.7 nm (5) 1

2 Rearranging equation 4 we can solve for the temperature of Rigel. T = 5000 k 600 nm λ MAX = 5000 K 600 nm 7.7 nm K (6) The temperature at the surface of the star Rigel is K. (5pts) 3. If the Earth orbited the Sun at a distance of 8 AU, how much fainter would the Sun appear to be in the daytime sky? For this question we use the apparent brightness equation. b = 4πR (7) where b is the apparent brightness, is the luminosity, and R is the distance from the source. We want to compare the apparent brightness of the Sun when the Earth is 8 AU away and when its 1 AU away. When the Earth is 1 AU away we have the following: b 1 = 1 4π(1 AU) (8) where b 1 and 1 is the apparent brightness and luminosity of the Sun at 1 AU away. And for the Earth at 8 AU from the Sun we have b 8 = 8 4π(8 AU) (9) where b 8 and 8 is the apparent brightness and luminosity of the Sun at 8 AU away. Since the source aka the Sun is the same in both set ups the luminosity is the same. 1 = 8 = We can then rearrange equation 8 and 9 to be in terms of b and R. 4π = b 8(8 AU) = b 1 (1 AU) (10) b 8 = 1 64 b 1 = b 1 (11) If the Earth was 8 AU away it would be 64 times fainter than if it was at 1 AU or 1.6 % the brightness at 1 AU.

3 (10pts) 4. How much weaker ( or stronger ) is the force of gravity on the surface of Pluto versus that on the surface of the Earth? [ The mass and radius of the Earth and Pluto are M E = kg, R E = 6400 km, M P = kg, R P = 100 km. ] In this problem we want to solve for the force of gravity at the surface of the Earth and Pluto. We first start with the force due to gravity equation F = Gm 1m d (1) where G is the gravitational constant, m 1 and m are the masses of objects 1 and, respectively, and d is the distance between the objects. To solve for the force of gravity at the surface we need to place an object at the surface and calculate the force on it for both planets. et s assume we place a person on the surface of the Earth with mass, m. Therefore F will be the force of gravity on the person at the surface. Solving for the force of gravity on a person at the surface of the Earth we get F E = GmM E R E (13) Doing the same process for a person on the surface of Pluto we get F P = GmM P R P (14) What we have done here is solved for the force of a person on the surface of the Earth and Pluto due to the individual Planet s gravitational pull. We then now equate the two equations using the fact that Gm is the same in both equations. Solving for F P Gm = F P R P M P = F E R E M E (15) F P = R E M P M E RP F E = (6400 km)( kg ) ( kg)(100 km) F E 1 16 F E 0.06 F E (16) The force on the surface of Pluto is 6.% or 16 times weaker than the force on the surface of the Earth. 3

4 (5pts) 5. You are 10 meters away from a candle and 100 meters away from a 150 Watt light bulb, but both the candle and the bulb look to be the same brightness to you. How uminous is the candle ( in Watts )? Again we use the apparent brightness equation b = 4πR (17) For the candle and the light bulb we have the following equations c b c = 4πRc (18) b b b = 4πRb (19) where b c, b b, R c, R b, c and b is the apparent brightness, distance and luminosity of the candle and light bulb, respectively. We are given the values of R c, R b and b are given values in the problem question as well as the understanding that b c = b b. We can then solve for the luminosity of the candle, c. c 4πR c = b 4πR b c = b Rb Rc (150 W atts)(10 m) = (100 m) = 1.5 W atts (0) The uminosity of the candle is 1.5 Watts. (5pts) 6. Neptune is approximately km from the Sun and takes roughly 165 years to complete one trip around the Sun. How quickly is Neptune moving along its orbit? We want to solve for Neptune s speed. ike from HW 1 the speed is T otal Distance Speed = (1) T otal T ime et s confine ourselves to one orbit around the Sun with radius R N. In one orbit, the total distance traveled is given by the circumference. T otal Distance T raveled = πr N = π ( km ) = km () 4

5 Converting kilometers to meters and years to seconds we can solve for the speed. Speed = T otal Distance T otal T ime = m s = 544 m s or 19, 59km hr (3) Neptune s speed as it orbits the Sun is 544 m s km or 19,59 hr. 5

Assignment 1. Due Jan. 31, 2017

Assignment 1. Due Jan. 31, 2017 Assignment 1 Due Jan. 31, 2017 Show all work and turn in answers on separate pages, not on these pages. Circle your final answers for clarity. Be sure to show/explain all of your reasoning and that your

More information

Properties of Stars. 1.1 Brightnesses of Stars

Properties of Stars. 1.1 Brightnesses of Stars Properties of Stars 1.1 Brightnesses of Stars I m sure you have noticed that some stars are very bright, others less bright, and some are quite dim. There is a true brightness of a star and an apparent

More information

Astro 1050 Mon. Apr. 3, 2017

Astro 1050 Mon. Apr. 3, 2017 Astro 1050 Mon. Apr. 3, 017 Today: Chapter 15, Surveying the Stars Reading in Bennett: For Monday: Ch. 15 Surveying the Stars Reminders: HW CH. 14, 14 due next monday. 1 Chapter 1: Properties of Stars

More information

5. A particular star has an angle of parallax of 0.2 arcsecond. What is the distance to this star? A) 50 pc B) 2 pc C) 5 pc D) 0.

5. A particular star has an angle of parallax of 0.2 arcsecond. What is the distance to this star? A) 50 pc B) 2 pc C) 5 pc D) 0. Name: Date: 1. How far away is the nearest star beyond the Sun, in parsecs? A) between 1 and 2 pc B) about 12 pc C) about 4 pc D) between 1/2 and 1 pc 2. Parallax of a nearby star is used to estimate its

More information

Stellar Composition. How do we determine what a star is made of?

Stellar Composition. How do we determine what a star is made of? Stars Essential Questions What are stars? What is the apparent visual magnitude of a star? How do we locate stars? How are star classified? How has the telescope changed our understanding of stars? What

More information

AP Physics C Textbook Problems

AP Physics C Textbook Problems AP Physics C Textbook Problems Chapter 13 Pages 412 416 HW-16: 03. A 200-kg object and a 500-kg object are separated by 0.400 m. Find the net gravitational force exerted by these objects on a 50.0-kg object

More information

A1101, Lab 5: The Hertzsprung- Russell Diagram Laboratory Worksheet

A1101, Lab 5: The Hertzsprung- Russell Diagram Laboratory Worksheet Student Name: Lab TA Name: A1101, Lab 5: The Hertzsprung- Russell Diagram Laboratory Worksheet One of the most basic physical properties of a star is its luminosity, the rate at which it radiates energy

More information

+ (38 yr) 1 yr. = 742 mo. 1 yr The number of days in 742 months is

+ (38 yr) 1 yr. = 742 mo. 1 yr The number of days in 742 months is ASTR 101 Homework 2 Solutions 3-44 Chinese Calendar The traditional Chinese lunar calendar has 12 months in most years but adds a thirteenth month to 22 of every 60 years. How many days does this give

More information

Solution for Homework# 3. Chapter 5 : Review & Discussion

Solution for Homework# 3. Chapter 5 : Review & Discussion Solution for Homework# 3 Chapter 5 : Review & Discussion. The largest telescopes are reflecting telescopes, primarily because of 3 distinct disadvantages of the refracting telescope. When light passes

More information

Space Science Jeopardy!

Space Science Jeopardy! Space Science Jeopardy! Structure of the Universe Stars & HR Diagram Seasons, Tides, Phases, Eclipses Astronomical Bodies The Sun & Gravity 10 10 10 10 10 20 20 20 20 20 30 30 30 30 30 40 40 40 40 40 50

More information

Astronomy 111 Review Problems Solutions

Astronomy 111 Review Problems Solutions Astronomy 111 Review Problems Solutions Problem 1: Venus has an equatorial radius of 6052 km. Its semi-major axis is 0.72 AU. The Sun has a radius of cm. a) During a Venus transit (such as occurred June

More information

Part I Multiple Choice (4 points. ea.)

Part I Multiple Choice (4 points. ea.) ach xam usually consists of 10 ultiple choice questions which are conceptual in nature. They are often based upon the assigned thought questions from the homework. There are also 4 problems in each exam,

More information

The Sun. How are these quantities measured? Properties of the Sun. Chapter 14

The Sun. How are these quantities measured? Properties of the Sun. Chapter 14 The Sun Chapter 14 The Role of the Sun in the Solar System > 99.9% of the mass Its mass is responsible for the orderly orbits of the planets Its heat is responsible for warming the planets It is the source

More information

Twin Sun Calculations mtlk 7/18/03

Twin Sun Calculations mtlk 7/18/03 Twin Sun Calculations mtlk 7/18/03 This is a short report containing my mathematical analysis of the data provided by the Cassiopaea session transcripts on the subject of the twin sun and associated effects.

More information

Gravity and the Orbits of Planets

Gravity and the Orbits of Planets Gravity and the Orbits of Planets 1. Gravity Galileo Newton Earth s Gravity Mass v. Weight Einstein and General Relativity Round and irregular shaped objects 2. Orbits and Kepler s Laws ESO Galileo, Gravity,

More information

Chapter 9. Gravitation

Chapter 9. Gravitation Chapter 9 Gravitation 9.1 The Gravitational Force For two particles that have masses m 1 and m 2 and are separated by a distance r, the force has a magnitude given by the same magnitude of force acts on

More information

ASTRONOMY QUIZ NUMBER 1

ASTRONOMY QUIZ NUMBER 1 ASTRONOMY QUIZ NUMBER. You read in an astronomy atlas that an object has a negative right ascension. You immediately conclude that A) the object is located in the Southern Sky. B) the object is located

More information

Characteristics of Stars

Characteristics of Stars Characteristics of Stars Mass of a Star The mass of a star is the hardest for astronomers to determine and it can only be found based on the gravitational forces and interactions with nearby stars. We

More information

Question number Answer Notes Marks 1 correctly; (ii) Sun X should be left of the imaginary 5-7 line, reject X placed outside the orbit

Question number Answer Notes Marks 1 correctly; (ii) Sun X should be left of the imaginary 5-7 line, reject X placed outside the orbit ( a) (i) omet orbit behind Sun completed Dashed or solid correctly; curved line X marked anywhere in grey area; No need to label X as Sun X should be left of the imaginary 5-7 line, reject X placed outside

More information

Astronomical Measurements: Brightness-Luminosity-Distance-Radius- Temperature-Mass. Dr. Ugur GUVEN

Astronomical Measurements: Brightness-Luminosity-Distance-Radius- Temperature-Mass. Dr. Ugur GUVEN Astronomical Measurements: Brightness-Luminosity-Distance-Radius- Temperature-Mass Dr. Ugur GUVEN Space Science Distance Definitions One Astronomical Unit (AU), is the distance from the Sun to the Earth.

More information

AY2 Winter 2017 Midterm Exam Prof. C. Rockosi February 14, Name and Student ID Section Day/Time

AY2 Winter 2017 Midterm Exam Prof. C. Rockosi February 14, Name and Student ID Section Day/Time AY2 Winter 2017 Midterm Exam Prof. C. Rockosi February 14, 2017 Name and Student ID Section Day/Time Write your name and student ID number on this printed exam, and fill them in on your Scantron form.

More information

AST111 PROBLEM SET 4 SOLUTIONS. Ordinarily the binary has a magnitude of 10 and this is due to the brightness of both stars.

AST111 PROBLEM SET 4 SOLUTIONS. Ordinarily the binary has a magnitude of 10 and this is due to the brightness of both stars. AST111 PROBLEM SET 4 SOLUTIONS Homework problems 1. On Astronomical Magnitudes You observe a binary star. Ordinarily the binary has a magnitude of 10 and this is due to the brightness of both stars. The

More information

Constellations In ancient times, constellations only referred to the brightest stars that appeared to form groups, representing mythological figures.

Constellations In ancient times, constellations only referred to the brightest stars that appeared to form groups, representing mythological figures. Chapter 2: The Sky Constellations In ancient times, constellations only referred to the brightest stars that appeared to form groups, representing mythological figures. Constellations Today, constellations

More information

Guidepost. Chapter 2 A User s Guide to the Sky. Constellations Constellations (2) 8/27/2015. Outline. Outline (continued)

Guidepost. Chapter 2 A User s Guide to the Sky. Constellations Constellations (2) 8/27/2015. Outline. Outline (continued) Chapter 2 A User s Guide to the Sky Guidepost Astronomy is about us. As we learn about astronomy, we learn about ourselves. We search for an answer to the question What are we? The quick answer is that

More information

Evaluate numerical expressions

Evaluate numerical expressions EXAMPLE 1 Evaluate numerical expressions a. ( 4 2 5 ) 2 ( 4) 2 (2 5 ) 2 16 2 5 2 16 2 10 16,384 Power of a product property Power of a power property Simplify and evaluate power. b. 11 5 11 8 1 11 8 11

More information

Chapter 11 Surveying the Stars

Chapter 11 Surveying the Stars Chapter 11 Surveying the Stars Luminosity Luminosity: Rate of energy emitted by star every second. Apparent brightness (flux): Amount of energy passing through every second per unit area. Luninosity =

More information

Patterns in the Solar System (Chapter 18)

Patterns in the Solar System (Chapter 18) GEOLOGY 306 Laboratory Instructor: TERRY J. BOROUGHS NAME: Patterns in the Solar System (Chapter 18) For this assignment you will require: a calculator, colored pencils, a metric ruler, and meter stick.

More information

18 An Eclipsing Extrasolar Planet

18 An Eclipsing Extrasolar Planet Name: Date: 18 An Eclipsing Extrasolar Planet 18.1 Introduction One of the more recent new fields in astronomy is the search for (and discovery of) planets orbiting around stars other than our Sun, or

More information

Homework #2, AST 203, Spring 2012

Homework #2, AST 203, Spring 2012 Homework #2, AST 203, Spring 2012 Due in class (i.e. by 4:20 pm), Tuesday February 28 General grading rules: One point off per question (e.g., 1a or 1b) for egregiously ignoring the admonition to set the

More information

Overview of the Solar System

Overview of the Solar System The Solar System Overview of the Solar System Basics Source: Nine Planets - A Multimedia Tour of the Solar System * By Bill Arnett The solar system consists of the Sun, the nine planets, about 90 satellites

More information

Gravity & The Distances to Stars. Lecture 8. Homework 2 open Exam on Tuesday in class bring ID and #2 pencil

Gravity & The Distances to Stars. Lecture 8. Homework 2 open Exam on Tuesday in class bring ID and #2 pencil 1 Gravity & The Distances to Stars Lecture 8 Homework 2 open Exam on Tuesday in class bring ID and #2 pencil 2 Preparing for the Exam 1 Exams in this class are multiple choice, but the questions can be

More information

ASTRO 1050 Scientific Notation, Model Scales, and Calculations

ASTRO 1050 Scientific Notation, Model Scales, and Calculations ASTRO 1050 Scientific Notation, Model Scales, and Calculations The simple truth is, interstellar distances will not fit into the human imagination. - Douglas Adams Materials: Ping pong balls, meter sticks,

More information

I. Introduction. II. An Introduction to Starry Night NAME: ORBITAL MOTION

I. Introduction. II. An Introduction to Starry Night NAME: ORBITAL MOTION NAME: ORBITAL MOTION What will you learn in this Lab? You will be using some special software to simulate the motion of planets in our Solar System and across the night sky. You will be asked to try and

More information

PTYS/ASTR 206 Section 2 Spring 2007 Homework #1 (Page 1/4)

PTYS/ASTR 206 Section 2 Spring 2007 Homework #1 (Page 1/4) PTYS/ASTR 206 Section 2 Spring 2007 Homework #1 (Page 1/4) NAME: KEY Due Date: start of class 1/25/2007 5 pts extra credit if turned in before 9:00AM (early!) (To get the extra credit, the assignment must

More information

Physical Data Mass = 2x10 30 kg (333,000 time more massive than the Earth) Diameter: 7x10 5 km (about 100 Earth radii) Volume: you can fit about 1.3 m

Physical Data Mass = 2x10 30 kg (333,000 time more massive than the Earth) Diameter: 7x10 5 km (about 100 Earth radii) Volume: you can fit about 1.3 m The Sun Physical Data Mass = 2x10 30 kg (333,000 time more massive than the Earth) Diameter: 7x10 5 km (about 100 Earth radii) Volume: you can fit about 1.3 million earths inside the sun! 70% Hydrogen,

More information

Useful Formulas and Values

Useful Formulas and Values Name Test 1 Planetary and Stellar Astronomy 2017 (Last, First) The exam has 20 multiple choice questions (3 points each) and 8 short answer questions (5 points each). This is a closed-book, closed-notes

More information

Astronomy, Astrophysics, and Cosmology

Astronomy, Astrophysics, and Cosmology Astronomy, Astrophysics, and Cosmology Luis A. Anchordoqui Department of Physics and Astronomy Lehman College, City University of New York Lesson I February 2, 2016 arxiv:0706.1988 L. A. Anchordoqui (CUNY)

More information

Patterns in the Solar System (Chapter 18)

Patterns in the Solar System (Chapter 18) GEOLOGY 306 Laboratory Instructor: TERRY J. BOROUGHS NAME: Patterns in the Solar System (Chapter 18) For this assignment you will require: a calculator, colored pencils, a metric ruler, and meter stick.

More information

Questions. theonlinephysicstutor.com. facebook.com/theonlinephysicstutor. Name: Edexce Black Body. Date: Time: Total marks available:

Questions. theonlinephysicstutor.com. facebook.com/theonlinephysicstutor. Name: Edexce Black Body. Date: Time: Total marks available: Name: Edexce Black Body Date: Time: Total marks available: Total marks achieved: Questions Q1. A lamp consists of a filament in a vacuum. Under normal working conditions the filament has a temperature

More information

Johannes Kepler ( ) German Mathematician and Astronomer Passionately convinced of the rightness of the Copernican view. Set out to prove it!

Johannes Kepler ( ) German Mathematician and Astronomer Passionately convinced of the rightness of the Copernican view. Set out to prove it! Johannes Kepler (1571-1630) German Mathematician and Astronomer Passionately convinced of the rightness of the Copernican view. Set out to prove it! Kepler s Life Work Kepler sought a unifying principle

More information

Homework 2 AST 301, Sections and 46850, Spring NAME Student EID Score: on last page. Due Tuesday, March 1, 2016

Homework 2 AST 301, Sections and 46850, Spring NAME Student EID Score: on last page. Due Tuesday, March 1, 2016 Homework 2 AST 301, Sections 46845 and 46850, Spring 2016 NAME Student EID Score: on last page Due Tuesday, March 1, 2016 Questions A C should help you to understand the properties of light. Show your

More information

PSI AP Physics C Universal Gravity Multiple Choice Questions

PSI AP Physics C Universal Gravity Multiple Choice Questions PSI AP Physics C Universal Gravity Multiple Choice Questions 1. Who determined the value of the gravitational constant (G)? (A) Newton (B) Galileo (C) Einstein (D) Schrödinger (E) Cavendish 2. Who came

More information

Observational Astronomy - Lecture 4 Orbits, Motions, Kepler s and Newton s Laws

Observational Astronomy - Lecture 4 Orbits, Motions, Kepler s and Newton s Laws Observational Astronomy - Lecture 4 Orbits, Motions, Kepler s and Newton s Laws Craig Lage New York University - Department of Physics craig.lage@nyu.edu February 24, 2014 1 / 21 Tycho Brahe s Equatorial

More information

Nm kg. The magnitude of a gravitational field is known as the gravitational field strength, g. This is defined as the GM

Nm kg. The magnitude of a gravitational field is known as the gravitational field strength, g. This is defined as the GM Copyright FIST EDUCATION 011 0430 860 810 Nick Zhang Lecture 7 Gravity and satellites Newton's Law of Universal Gravitation Gravitation is a force of attraction that acts between any two masses. The gravitation

More information

II. Universal Gravitation - Newton 4th Law

II. Universal Gravitation - Newton 4th Law Periodic Motion I. Circular Motion - kinematics & centripetal acceleration - dynamics & centripetal force - centrifugal force II. Universal Gravitation - Newton s 4 th Law - force fields & orbits III.

More information

AST 301 Cosmic Collisions (AKA Collisions)

AST 301 Cosmic Collisions (AKA Collisions) AST 301 Cosmic Collisions (AKA Collisions) James Lattimer lattimer@astro.sunysb.edu Department of Physics & Astronomy 461 ESS Bldg. Stony Brook University Lattimer, AST 301, Lecture 1 p.1/11 Course Components

More information

Welcome to Environmental Science!!!

Welcome to Environmental Science!!! Welcome to Environmental Science!!! The Sun Physical Data Mass = 2x10 30 kg (333,000 time more massive than the Earth) Diameter: 7x10 5 km (about 100 Earth radii) Volume: you can fit about 1.3 million

More information

Putting Earth In Its Place

Putting Earth In Its Place Teacher Instructions Overview: During this activity, students build a model of our Solar System to gain insight into the relative sizes and distances involved. ives: The student will: create a scale model

More information

Astronomy 111 Exam Review Problems (Real exam will be Tuesday Oct 25, 2016)

Astronomy 111 Exam Review Problems (Real exam will be Tuesday Oct 25, 2016) Astronomy 111 Exam Review Problems (Real exam will be Tuesday Oct 25, 2016) Actual Exam rules: you may consult only one page of formulas and constants and a calculator while taking this test. You may not

More information

LEARNING ABOUT THE OUTER PLANETS. NASA's Cassini spacecraft. Io Above Jupiter s Clouds on New Year's Day, Credit: NASA/JPL/University of Arizona

LEARNING ABOUT THE OUTER PLANETS. NASA's Cassini spacecraft. Io Above Jupiter s Clouds on New Year's Day, Credit: NASA/JPL/University of Arizona LEARNING ABOUT THE OUTER PLANETS Can see basic features through Earth-based telescopes. Hubble Space Telescope especially useful because of sharp imaging. Distances from Kepler s 3 rd law, diameters from

More information

AST Section 2: Test 1

AST Section 2: Test 1 AST1002 - Section 2: Test 1 Date: 10/06/2009 Name: Equations: c = λ f, λ peak = Question 1: A star with a declination of +40.0 degrees will be 1. east of the vernal equinox. 2. west of the vernal equinox.

More information

Name and Student ID Section Day/Time:

Name and Student ID Section Day/Time: AY2 - Overview of the Universe - Midterm #1 - Instructor: Maria F. Duran Name and Student ID Section Day/Time: 1) Imagine we ve discovered a planet orbiting another star at 1 AU every 6 months. The planet

More information

Chapter 14 Satellite Motion

Chapter 14 Satellite Motion 1 Academic Physics Mechanics Chapter 14 Satellite Motion The Mechanical Universe Kepler's Three Laws (Episode 21) The Kepler Problem (Episode 22) Energy and Eccentricity (Episode 23) Navigating in Space

More information

By; Jarrick Serdar, Michael Broberg, Trevor Grey, Cameron Kearl, Claire DeCoste, and Kristian Fors

By; Jarrick Serdar, Michael Broberg, Trevor Grey, Cameron Kearl, Claire DeCoste, and Kristian Fors By; Jarrick Serdar, Michael Broberg, Trevor Grey, Cameron Kearl, Claire DeCoste, and Kristian Fors What is gravity? Gravity is defined as the force of attraction by which terrestrial bodies tend to fall

More information

KNOWLEDGE TO GET FROM TODAY S CLASS MEETING

KNOWLEDGE TO GET FROM TODAY S CLASS MEETING KNOWLEDGE TO GET FROM TODAY S CLASS MEETING Class Meeting #6, Monday, February 1 st, 2016 1) GRAVITY: finish up from Fri, Jan 29 th (pages 111-112, 123) 2) Isaac Newton s LAWS of MOTION (briefly) (pages

More information

Laws describing the planetary motion. Weight and acceleration due to gravity. Calculating the mass of Earth (6378 M G

Laws describing the planetary motion. Weight and acceleration due to gravity. Calculating the mass of Earth (6378 M G Laws describing the planetary motion Kepler s Laws a Newton s Laws Speed, velocity, acceleration, force, inertia, mass, balanced and unbalanced forces Weight and acceleration due to gravity 1. Weight gravitational

More information

Observational Astronomy - Lecture 8 Stars I - Distances, Magnitudes, Spectra, HR Diagram

Observational Astronomy - Lecture 8 Stars I - Distances, Magnitudes, Spectra, HR Diagram Observational Astronomy - Lecture 8 Stars I - Distances, Magnitudes, Spectra, HR Diagram Craig Lage New York University - Department of Physics craig.lage@nyu.edu April 7, 2014 1 / 36 JPL Horizons Database.

More information

The Hertzprung-Russell Diagram. The Hertzprung-Russell Diagram. Question

The Hertzprung-Russell Diagram. The Hertzprung-Russell Diagram. Question Key Concepts: Lecture 21: Measuring the properties of stars (cont.) The Hertzsprung-Russell (HR) Diagram (L versus T) The Hertzprung-Russell Diagram The Stefan-Boltzmann Law: flux emitted by a black body

More information

Newton's Law of Universal Gravitation

Newton's Law of Universal Gravitation Section 2.17: Newton's Law of Universal Gravitation Gravity is an attractive force that exists between all objects that have mass. It is the force that keeps us stuck to the earth and the moon orbiting

More information

Physics Unit 7: Circular Motion, Universal Gravitation, and Satellite Orbits. Planetary Motion

Physics Unit 7: Circular Motion, Universal Gravitation, and Satellite Orbits. Planetary Motion Physics Unit 7: Circular Motion, Universal Gravitation, and Satellite Orbits Planetary Motion Geocentric Models --Many people prior to the 1500 s viewed the! Earth and the solar system using a! geocentric

More information

Chapter 13: universal gravitation

Chapter 13: universal gravitation Chapter 13: universal gravitation Newton s Law of Gravitation Weight Gravitational Potential Energy The Motion of Satellites Kepler s Laws and the Motion of Planets Spherical Mass Distributions Apparent

More information

Stars, Galaxies & the Universe Announcements. Stars, Galaxies & the Universe Observing Highlights. Stars, Galaxies & the Universe Lecture Outline

Stars, Galaxies & the Universe Announcements. Stars, Galaxies & the Universe Observing Highlights. Stars, Galaxies & the Universe Lecture Outline Stars, Galaxies & the Universe Announcements HW#3 due Tuesday (Tomorrow) at 3 pm Lab Observing Trip Tues (9/28) & Thurs (9/30) First Exam next Wed. (9/22) in class - will post review sheet, practice exam

More information

Planetary Mechanics:

Planetary Mechanics: Planetary Mechanics: Satellites A satellite is an object or a body that revolves around another body due to the gravitational attraction to the greater mass. Ex: The planets are natural satellites of the

More information

The Magnitude Scale. The Color Index.

The Magnitude Scale. The Color Index. The Magnitude Scale The Color Index. The Magnitude Scale Measuring the brightness of astronomical objects While cataloging stars in the sky, the Greek Astronomer Hipparchus developed the magnitude system,

More information

The Sun s center is much hotter than the surface. The Sun looks large and bright in the sky. Other stars look much smaller.

The Sun s center is much hotter than the surface. The Sun looks large and bright in the sky. Other stars look much smaller. The Sun A star is a huge ball of hot, glowing gases. The Sun is a star. The width of the Sun is equal to the width of 100 Earths placed side by side. The Sun is extremely hot. The surface of the Sun has

More information

A. What is Energy? B. Kinetic Energy. 6.1: Energy of all shapes and sizes. 1 Define: (a) Watt (b) Joule (c) Erg

A. What is Energy? B. Kinetic Energy. 6.1: Energy of all shapes and sizes. 1 Define: (a) Watt (b) Joule (c) Erg 6.1: Energy of all shapes and sizes A. What is Energy? (a) Watt (b) Joule (c) Erg 2 Why does an electric bill have W-hrs listed on it? 3 What is the speed of light in centimeter-gram-second units? 4 Organize

More information

Key Points: Learn the relationship between gravitational attractive force, mass and distance. Understand that gravity can act as a centripetal force.

Key Points: Learn the relationship between gravitational attractive force, mass and distance. Understand that gravity can act as a centripetal force. Lesson 9: Universal Gravitation and Circular Motion Key Points: Learn the relationship between gravitational attractive force, mass and distance. Understand that gravity can act as a centripetal force.

More information

ASTR 497 / ESS 490, Planetary Sciences and Astrobiology Prof. David Catling

ASTR 497 / ESS 490, Planetary Sciences and Astrobiology Prof. David Catling HOMEWORK: PROBLEM SET 3 Qu. 1) In the core of the Sun, all atoms are ionized. The Sun shines by virtue of nuclear fusion, with the energy source being the fusion of hydrogen nuclei (protons) to helium

More information

Reading and Announcements. Read Chapters 9.5, 9.6, and 11.4 Quiz #4, Thursday, March 7 Homework #5 due Tuesday, March 19

Reading and Announcements. Read Chapters 9.5, 9.6, and 11.4 Quiz #4, Thursday, March 7 Homework #5 due Tuesday, March 19 Reading and Announcements Read Chapters 9.5, 9.6, and 11.4 Quiz #4, Thursday, March 7 Homework #5 due Tuesday, March 19 Stars The stars are distant and unobtrusive, but bright and enduring as our fairest

More information

Name Period Date. Record all givens, draw a picture, arrow all vectors, write the formula, substitute and solve. units

Name Period Date. Record all givens, draw a picture, arrow all vectors, write the formula, substitute and solve. units Example Problems 12.1 E1. Doc Fizzix, whose mass is 65.0 kg, is doing a physics demonstration at the front of the classroom. How much gravitational force does Doc Fizzix exert on Rob, whose mass is 55

More information

Equation of orbital velocity: v 2 =GM(2/r 1/a) where: G is the gravitational constant (G=6.67x10 11 N/m 3 kg), M is the mass of the sun (or central

Equation of orbital velocity: v 2 =GM(2/r 1/a) where: G is the gravitational constant (G=6.67x10 11 N/m 3 kg), M is the mass of the sun (or central Everything in Orbit Orbital Velocity Orbital velocity is the speed at which a planetary body moves in its orbit around another body. If orbits were circular, this velocity would be constant. However, from

More information

Which of the following planets are all made up of gas? When a planets orbit around the Sun looks like an oval, it s called a(n)

Which of the following planets are all made up of gas? When a planets orbit around the Sun looks like an oval, it s called a(n) When a planets orbit around the Sun looks like an oval, it s called a(n) - ellipse - circle - axis - rotation Which of the following planets are all made up of gas? - Venus, Mars, Saturn and Pluto - Jupiter,

More information

Lecture 8: What we can learn via light

Lecture 8: What we can learn via light Lecture 8: What we can learn via light As with all course material (including homework, exams), these lecture notes are not be reproduced, redistributed, or sold in any form. Lecture 8: What we can learn

More information

The Mass of Jupiter Student Guide

The Mass of Jupiter Student Guide The Mass of Jupiter Student Guide Introduction: In this lab, you will use astronomical observations of Jupiter and its satellites to measure the mass of Jupiter. We will use the program Stellarium to simulate

More information

The sun then falls below the horizon, and it is nighttime for our little person:

The sun then falls below the horizon, and it is nighttime for our little person: Venus Update! Problem 6 on Homework 1 in Physics 2A last September asked you to find the distance from Earth to Venus at that time. I gave you the angle between the sun and Venus at that time; you drew

More information

Lecture 16. Gravitation

Lecture 16. Gravitation Lecture 16 Gravitation Today s Topics: The Gravitational Force Satellites in Circular Orbits Apparent Weightlessness lliptical Orbits and angular momentum Kepler s Laws of Orbital Motion Gravitational

More information

Physics 12. Unit 5 Circular Motion and Gravitation Part 2

Physics 12. Unit 5 Circular Motion and Gravitation Part 2 Physics 12 Unit 5 Circular Motion and Gravitation Part 2 1. Newton s law of gravitation We have seen in Physics 11 that the force acting on an object due to gravity is given by a well known formula: F

More information

= 4,462K T eff (B) =

= 4,462K T eff (B) = Homework 1 Solutions Problem 1: Star A emits most of its light in the orange, Star B in the gre en and Star C in the blue color range. What wavelengths are these most likely to be, and what effective temperature

More information

Lecture 19: The Moon & Mercury. The Moon & Mercury. The Moon & Mercury

Lecture 19: The Moon & Mercury. The Moon & Mercury. The Moon & Mercury Lecture 19: The Moon & Mercury The Moon & Mercury The Moon and Mercury are similar in some ways They both have: Heavily cratered Dark colored surfaces No atmosphere No water They also have some interesting

More information

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

Astronomy 101 The Solar System Tuesday, Thursday 2:30-3:45 pm Hasbrouck 20. Tom Burbine Astronomy 101 The Solar System Tuesday, Thursday 2:30-3:45 pm Hasbrouck 20 Tom Burbine tomburbine@astro.umass.edu Course Course Website: http://blogs.umass.edu/astron101-tburbine/ Textbook: Pathways to

More information

Basic Properties of the Stars

Basic Properties of the Stars Basic Properties of the Stars The Sun-centered model of the solar system laid out by Copernicus in De Revolutionibus (1543) made a very specific prediction: that the nearby stars should exhibit parallax

More information

AST 248, Lecture 2. James Lattimer. Department of Physics & Astronomy 449 ESS Bldg. Stony Brook University. January 28, 2015

AST 248, Lecture 2. James Lattimer. Department of Physics & Astronomy 449 ESS Bldg. Stony Brook University. January 28, 2015 AST 248, Lecture 2 James Lattimer Department of Physics & Astronomy 449 ESS Bldg. Stony Brook University January 28, 2015 The Search for Life in the Universe james.lattimer@stonybrook.edu Distances in

More information

PH 2213 : Chapter 06 Homework Solutions. Problem 6.08 :

PH 2213 : Chapter 06 Homework Solutions. Problem 6.08 : PH 2213 : Chapter 06 Homework Solutions Problem 6.08 : Every few hundred years most of the planets line up on the same side of the Sun. Calculate the total force on the Earth due to Venus, Jupiter, and

More information

Physics 111. Tuesday, November 9, Universal Law Potential Energy Kepler s Laws. density hydrostatic equilibrium Pascal s Principle

Physics 111. Tuesday, November 9, Universal Law Potential Energy Kepler s Laws. density hydrostatic equilibrium Pascal s Principle ics Tuesday, ember 9, 2004 Ch 12: Ch 15: Gravity Universal Law Potential Energy Kepler s Laws Fluids density hydrostatic equilibrium Pascal s Principle Announcements Wednesday, 8-9 pm in NSC 118/119 Sunday,

More information

F = ma P 2 = a 3 (M + m) P 2 = a 3. max T = 2900 K m

F = ma P 2 = a 3 (M + m) P 2 = a 3. max T = 2900 K m Summer 2013 Astronomy - Test 1 Test form A Name Do not forget to write your name and fill in the bubbles with your student number, and fill in test form A on the answer sheet. Write your name above as

More information

PH104 Descriptive Astronomy Learning Objectives

PH104 Descriptive Astronomy Learning Objectives PH104 Descriptive Astronomy Learning Objectives April 6, 2008 1 Introduction This list of questions are questions that will need to be answered in order for students to be successful in the course. Each

More information

AST 101 INTRODUCTION TO ASTRONOMY SPRING MIDTERM EXAM 2 TEST VERSION 1 ANSWERS

AST 101 INTRODUCTION TO ASTRONOMY SPRING MIDTERM EXAM 2 TEST VERSION 1 ANSWERS AST 101 INTRODUCTION TO ASTRONOMY SPRING 2008 - MIDTERM EXAM 2 TEST VERSION 1 ANSWERS Multiple Choice. In the blanks provided before each question write the letter for the phrase that best answers the

More information

9J Gravity and Space ILU

9J Gravity and Space ILU 9J Gravity and Space ILU Level 3 4 5 6 7 no. of qu.s 0 1 3 5 0. Level 4 1. Lisa drew a picture of herself standing at four different positions on the Earth, A D B C not to scale (a) (i) Draw an arrow at

More information

Name. Topic. K: What I Know. W: What I Want to Know. L: What I Learned. S: What I Still Want to Know

Name. Topic. K: What I Know. W: What I Want to Know. L: What I Learned. S: What I Still Want to Know Instructions: Write the Solar System topic you are studying on the line provided. In the first section, write what you already know about the topic. In the second section, write what you would like to

More information

OPTION E, ASTROPHYSICS TEST REVIEW

OPTION E, ASTROPHYSICS TEST REVIEW IB PHYSICS Name: DEVIL PHYSICS Period: Date: BADDEST CLASS ON CAMPUS OPTION E, ASTROPHYSICS TEST REVIEW S1. This question is about the nature of certain stars on the Hertzsprung-Russell diagram and determining

More information

Astronomy 102: Stars and Galaxies Exam 2

Astronomy 102: Stars and Galaxies Exam 2 October 13, 2004 Name: Astronomy 102: Stars and Galaxies Exam 2 Instructions: Write your answers in the space provided; indicate clearly if you continue on the back of a page. No books, notes, or assistance

More information

KNOWLEDGE TO GET FROM TODAY S CLASS MEETING

KNOWLEDGE TO GET FROM TODAY S CLASS MEETING KNOWLEDGE TO GET FROM TODAY S CLASS MEETING Class Meeting #5, Friday, January 29 th, 2016 1) GRAVITY: (text pages 111-112, 123) 2) Isaac Newton s LAWS of MOTION (briefly) (text pages 115-117) 3) Distances

More information

OPEN CLUSTER PRELAB The first place to look for answers is in the lab script!

OPEN CLUSTER PRELAB The first place to look for answers is in the lab script! NAME: 1. Define using complete sentences: Globular Cluster: OPEN CLUSTER PRELAB The first place to look for answers is in the lab script! Open Cluster: Main Sequence: Turnoff point: Answer the following

More information

AST 301, Lecture 1. James Lattimer. Department of Physics & Astronomy 449 ESS Bldg. Stony Brook University. January 23, 2017

AST 301, Lecture 1. James Lattimer. Department of Physics & Astronomy 449 ESS Bldg. Stony Brook University. January 23, 2017 AST 301, Lecture 1 James Lattimer Department of Physics & Astronomy 449 ESS Bldg. Stony Brook University January 23, 2017 Cosmic Catastrophes (AKA Collisions) james.lattimer@stonybrook.edu Course Components

More information

Gravitation. Makes the World Go Round

Gravitation. Makes the World Go Round Gravitation Makes the World Go Round Gravitational Force The Force of gravity is an attractive force felt between all objects that have mass. G=6.67x10-11 N m 2 /kg 2 Example 1: What is the Force of Gravity

More information

Name: Earth and Space Assessment Study Guide. Assessment Date : Term Rotation Revolution

Name: Earth and Space Assessment Study Guide. Assessment Date : Term Rotation Revolution Name: Earth and Space Assessment Study Guide Assessment Date : Earth s Rotation and Revolution Term Rotation Revolution Brief Definition Earth s Time to Complete One complete spin on an axis 24 hours (or

More information

Solutions to Homework #3, AST 203, Spring 2009

Solutions to Homework #3, AST 203, Spring 2009 Solutions to Homework #3, AST 203, Spring 2009 Due on March 5, 2009 General grading rules: One point off per question (e.g., 1a or 2c) for egregiously ignoring the admonition to set the context of your

More information

Worlds in Points of Light. What to Expect

Worlds in Points of Light. What to Expect Worlds in Points of Light What to Expect Vision and Intellect Week Path of the planets 1 Learning from light 2 Planet diversity 3 Remote sensing 4 Planetary evolution 5 Extra-solar planets 6 (Naked-eye

More information

KNOWLEDGE TO GET FROM TODAY S CLASS MEETING Class Meeting #11, Friday, February 12 th

KNOWLEDGE TO GET FROM TODAY S CLASS MEETING Class Meeting #11, Friday, February 12 th KNOWLEDGE TO GET FROM TODAY S CLASS MEETING Class Meeting #11, Friday, February 12 th 1) RADIANT ENERGY (Stefan-Boltzmann Law & Wien s Law) Pgs 154-156 Pgs 154-156 - an in-class exercise 2) Earn a good

More information

Assignment 1. Due Feb. 11, 2019

Assignment 1. Due Feb. 11, 2019 Assignment 1 Due Feb. 11, 2019 Show all work and turn in answers on separate pages, not on these pages. Circle your final answers for clarity. Be sure to show/explain all of your reasoning and that your

More information