AP Physics Gravity and Circular Motion

Similar documents
Worked Examples. v max =?

G.GMD.1 STUDENT NOTES WS #5 1 REGULAR POLYGONS

Orbits and Kepler s Laws

GRAVITATION 1. BASIC FORCES IN NATURE

(Ch. 22.5) 2. What is the magnitude (in pc) of a point charge whose electric field 50 cm away has a magnitude of 2V/m?

VEHICLE PLANAR DYNAMICS BICYCLE MODEL

r (1+cos(θ)) sin(θ) C θ 2 r cos θ 2

Intro to Circle Geometry By Raymond Cheong

2.016 Hydrodynamics Prof. A.H. Techet

Summary: Vectors. This theorem is used to find any points (or position vectors) on a given line (direction vector). Two ways RT can be applied:

Determining solar characteristics using planetary data

(d) False. The orbital period of a planet is independent of the planet s mass.

32. The Tangency Problem of Apollonius.

Exam in physics, El-grunder (Electromagnetism), , kl

Formulas and Units. Transmission technical calculations Main Formulas. Size designations and units according to the SI-units.

10. Collisions. Before During After

Experiment 6: Centripetal Force

Basically, logarithmic transformations ask, a number, to what power equals another number?

N V V L. R a L I. Transformer Equation Notes

Voltage ( = Electric Potential )

Curvature. (Com S 477/577 Notes) Yan-Bin Jia. Oct 8, 2015

Cypress Creek High School IB Physics SL/AP Physics B MP2 Test 1 Newton s Laws. Name: SOLUTIONS Date: Period:

Chapter 4 Newton s Laws

Mechanics 1: Motion in a Central Force Field

Experiment 6: Friction

7 Circular Motion. 7-1 Centripetal Acceleration and Force. Period, Frequency, and Speed. Vocabulary

Chapter 30: Magnetic Fields Due to Currents

Version 001 Summer Review #03 tubman (IBII ) 1

Solution to Problem Set 1

Episode 401: Newton s law of universal gravitation

Chapter 23 Electrical Potential

Geometry 7-1 Geometric Mean and the Pythagorean Theorem

v T R x m Version PREVIEW Practice 7 carroll (11108) 1

1240 ev nm 2.5 ev. (4) r 2 or mv 2 = ke2

Gravitation. AP Physics C

2 r2 θ = r2 t. (3.59) The equal area law is the statement that the term in parentheses,

Voltage ( = Electric Potential )

Solution Derivations for Capa #8

5.2. LINE INTEGRALS 265. Let us quickly review the kind of integrals we have studied so far before we introduce a new one.

Magnetic Field and Magnetic Forces. Young and Freedman Chapter 27

Example 27.1 Draw a Venn diagram to show the relationship between counting numbers, whole numbers, integers, and rational numbers.

Mechanics 1: Work, Power and Kinetic Energy

Incline and Friction Examples

The force between electric charges. Comparing gravity and the interaction between charges. Coulomb s Law. Forces between two charges

(a) The centripetal acceleration of a point on the equator of the Earth is given by v2. The velocity of the earth can be found by taking the ratio of

Answer, Key Homework 6 David McIntyre Mar 25,

Use Geometry Expressions to create a more complex locus of points. Find evidence for equivalence using Geometry Expressions.

Figure 2. So it is very likely that the Babylonians attributed 60 units to each side of the hexagon. Its resulting perimeter would then be 360!

. At first sight a! b seems an unwieldy formula but use of the following mnemonic will possibly help. a 1 a 2 a 3 a 1 a 2

Polynomial Functions. Polynomial functions in one variable can be written in expanded form as ( )

The Casino Experience. Let us entertain you

Appendix D: Completing the Square and the Quadratic Formula. In Appendix A, two special cases of expanding brackets were considered:

10.6 Applications of Quadratic Equations

Displacement, Velocity And Acceleration

Mr. Kepple. Motion at Constant Acceleration 1D Kinematics HW#5. Name: Date: Period: (b) Distance traveled. (a) Acceleration.

Description: Conceptual questions about projectile motion and some easy calculations. (uses applets)

PROF. BOYAN KOSTADINOV NEW YORK CITY COLLEGE OF TECHNOLOGY, CUNY

Math 135 Circles and Completing the Square Examples

PHYSICS 111 HOMEWORK SOLUTION #13. May 1, 2013

FXA Candidates should be able to : Describe how a mass creates a gravitational field in the space around it.

The Role of Gravity in Orbital Motion

12. Rolling, Torque, and Angular Momentum

Integration by Substitution

Standardized Coefficients

Chapter 11 Relative Velocity

Econ 4721 Money and Banking Problem Set 2 Answer Key

Graphs on Logarithmic and Semilogarithmic Paper

Chapter 19: Electric Charges, Forces, and Fields ( ) ( 6 )( 6

AP Physics Electromagnetic Wrap Up

LINEAR TRANSFORMATIONS AND THEIR REPRESENTING MATRICES

Chapter 22 The Electric Field II: Continuous Charge Distributions

PY1052 Problem Set 8 Autumn 2004 Solutions

Exam 3: Equation Summary

Mathematics. Vectors. hsn.uk.net. Higher. Contents. Vectors 128 HSN23100

Unit 6: Exponents and Radicals

PHYSICS 151 Notes for Online Lecture #11

JFET AMPLIFIER CONFIGURATIONS

Brillouin Zones. Physics 3P41 Chris Wiebe

Physics 43 Homework Set 9 Chapter 40 Key


Physics 235 Chapter 5. Chapter 5 Gravitation

Controlling the Money Supply: Bond Purchases in the Open Market

Phys 2101 Gabriela González. cos. sin. sin

Regular Sets and Expressions

Random Variables and Distribution Functions

Maths Word Searches. List of Contents. Word Search 1. Word Search 2. Word Search 3. Word Search 4. Word Search 5. Word Search 6.

COMPONENTS: COMBINED LOADING

Firm Objectives. The Theory of the Firm II. Cost Minimization Mathematical Approach. First order conditions. Cost Minimization Graphical Approach

A) When two objects slide against one another, the magnitude of the frictional force is always equal to μ

Practice Test 2. a. 12 kn b. 17 kn c. 13 kn d. 5.0 kn e. 49 kn

Lesson 4.1 Triangle Sum Conjecture

Vectors Recap of vectors

EASY RECEPTION TASKS FOR USE IN THE LITERACY HOUR. S t e p h e n s t e. Jigsaw names of self and friends.

Multiple choice questions [60 points]

CURVES ANDRÉ NEVES. that is, the curve α has finite length. v = p q p q. a i.e., the curve of smallest length connecting p to q is a straight line.

Doppler Effect. wavelength

AAPT UNITED STATES PHYSICS TEAM AIP 2010

Operations with Polynomials

Moment and couple. In 3-D, because the determination of the distance can be tedious, a vector approach becomes advantageous. r r

Transcription:

AP Phyic Gity nd icul Motion Newton theoy i ey iple. Gity i foce of ttction between ny two object tht he. Two object itting on dektop ttct ech othe with foce tht we cll gity. They don t go flying togethe becue gity i ey wek foce nd i only ignificnt when one o the othe of the e i enoou plnet ize. Thi i why we en t ttcted to object tht we p on ou dily wndeing. The ize of the foce of gity i gien by thi eqution: G 1 Newton lw of gity! 11 N " G i the uniel gittionl contnt. G 6.67 x10 kg 1 i the of one of the bodie nd i the of the othe body. i the ditnce between the two bodie. The lue of G i the e eeywhee thoughout the uniee. On the old AP Phyic Tet the eqution i witten : G G! 1 Newton lw of gity i n inee-que Lw. Thi en tht the foce of gity get lle o lge by the que of the ditnce. The foce i diectly popotionl to the e, o if the of one of the object double, the foce of gity would double. But if the ditnce doubled, the foce of gity would decee by fcto of fou. Tht becue it decee by the que of the ditnce. Inee-que lw e ey coon in phyic. We ll ee oe of the in ou explotion. To gie the pticul of the theoy: Uniel Lw of Gittion 1. Gittionl foce i field foce between two pticle -- in ll ediu.. oce ie the inee que of the ditnce 3. oce i popotionl to of object. 4. The gity foce ct fo the cente of the two object. 5. The gittionl foce i lwy ttctie. 6. The gittionl foce cnnot be hielded o cnceled. Soling gity poble i quite iple. Let do one.

A gil, Bndy (4.5 kg), it 1.50 fo boy (63.0 kg), Geoge. Wht i the foce of gity between the? (Thi will tell u how ttcted they e to ech othe.) G 1 ( 4.5 kg )( 63.0 kg ) "! 11 N $ # 6.67 x10 % kg & ' ( ( 1.50 )! 11! 8 7940 x10 N 7.94 x10 N You cn ee tht thi i tiny foce, one o ll tht Bndy will nee notice it peence. Geoge ut genete oe othe ttctie foce if thee i to be eltionhip between the two of the. One ueful ppliction of Newton lw of gity w to weigh Eth thi llowed phyicit to ke n ccute deteintion of the eth. Let do tht. ind the of the eth. e 6.38 x 10 6. We will ue 10.0 kg in ou olution (not tht it tte), the othe will be tht of the eth. 1 G E Thi i the foce of gity uing Newton lw. But we know tht the foce of gity ut lo equl g, o we et the equl to one nothe: 1 Eth 1g G The of the object cncel out: g G E g Sole fo the of the eth E G 6 9.8 ( 6.38 x10 ) 3 4 59.8 x10 kg 5.98 x10 kg E "! 11 kg $ # % x $ & ( kg ) 6.67 10 10.0 ' kg ( 3 4 59.8 x10 kg 5.98 x10 kg E

oce nd icul Motion - In ode fo n object to undego cicul otion, foce ut ct. Pictue n object tht h oe elocity. Wht will hppen to it if no foce ct on it? Well, ccoding to the fit lw, it will continue to oe with contnt elocity. It will follow tight-line pth. To ke it chnge diection foce ut ct on it. In ode to ke it chnge diection contntly, foce ut ct on it contntly. Wht i the diection of the foce needed to do thi? Well, when you pin oething in cicle, wht do you he to do? You jut pull it towd the cente you go ound nd ound. The object get cceleted towd the cente. We cll thi the centipetl cceletion. The eqution fo the centipetl cceletion i: c c i the centipetl cceletion, i the line o tngentil peed, nd i the diu of the cicul pth. Thi eqution will be poided to you fo the AP Phyic Tet. The foce tht bing bout thi cceletion i clled the centipetl foce. It diection i lo towd the cente of the cicul pth. entipetl en "cente eeking". The centipetl foce chnge the diection of the object elocity ecto. Without it, thee would be no cicul pth. The centipetl foce i eely conenient ne fo the net foce tht i towd the cente. It i lwy cued by oething it could be cued by the foce of gity, the ection foce between the contol ufce of n iplne with the i, &tc. When you otte bll ound you hed in cicle, the centipetl foce i upplied by the tenion in the ting. Wht i the ouce of the centipetl foce tht cue cec to tel in cicul pth on the cetck? The foce i bought bout by the tie puhing on the cetck. The fiction between the od nd the tie i ey ipotnt, o ce tie e deigned to xiize fiction. Wht i the ouce of the centipetl foce equied to ke the eth eole ound the un? Thi i whee the pple flling on Newton toy fit in. Befoe Newton no one could explin the obit of the plnet nd oon. Newton, the toy goe, w elxing unde n pple tee pondeing the poble of the oon obit. He knew tht thee hd to be foce cting on the oon to cceleting it towd the eth, but hd no ide wht w the ouce of the foce. Then he w n pple fll nd the iple olution tuck hi like the old thundebolt. Jut the eth gity eched out nd de the pple fll, o it eched out nd de the oon fll. Thu, the foce tht keep the plnet nd oon following thei obitl pth i gity.

The AP Tet eqution heet will not gie you the eqution fo centipetl foce. It doe gie you the eqution fo centipetl cceletion. It lo gie you the eqution fo the econd lw. Uing thee two eqution you cn eily deie the foul fo centipetl foce. Hee how to do it: o plug in the lue of the centipetl cceletion:! " # $ % & Tht ll thee i to it. A c i teling t contnt peed nd ke tun with diu of 50.0. It peed i15.0 /. ind the iniu coefficient of fiction needed to keep the c teling long the pth. Let look t the BD: n The fictionl foce ut equl the centipetl foce. The centipetl foce i gien by: We know tht thi ut equl the fictionl foce. We lo know tht the fictionl foce i: c g f f µ N Aue the od i flt, o n g Set the two equl to ech othe nd ole fo the coefficient of fiction: µ g µ g µ! " 1 # 15.0 0.459 $ % &! " # 9.8 50.0 $ % &

A child twil yo yo. If ngle of the cod with the eticl i 30.0, find c. Look t the foce in the y diection: 0 g y 0 T co! " g 0 T co! The hoizontl coponent of T i the centipetl foce. T in! Plug into eqution fo T: g in! g tn! We know tht: co! T 0 o g tn! g tn! 9.8 tn 30.0 o 5.66 g entipetl oce nd Gity: You y he een illy deonttion inoling bucket of wte tht w pinning in eticl cicle. The wte tyed in the bucket nd did not fll out. So wht w the del? Doe pinning oething in eticl cicle oehow cncel out gity? Well, no, gity i foce tht cnnot be topped o cnceled. It i lwy thee, nytie you he the ppopite e. The wte doe fll, it fll but the bucket fll with it nd ctche it. Thi only wok if the bucket i oing ft enough to ctch the wte. If the bucket i too low, then the wte will fll out of it. The iniu line peed fo thi i clled the citicl elocity. iticl elocity iniu elocity fo n object to tel in eticl cicle nd intin it cicul pth gint the foce of gity.

The e thing i needed fo tellite in obit ound the eth o plnet in obit ound the un. They too ut tel t the citicl elocity. The citicl elocity foul i not poided on the AP Tet, but it i ey iple to figue out. You jut et the centipetl foce equl to the weight of the object tht i in cicul otion. If the two foce e equl, then the object won t be ble to fll out of the bucket. nd g Set the equl to ech othe: g g g So hee i the citicl elocity g Obitl Eqution: Let u ue tht the obit of tellite bout the eth (o ny othe ie body) i cicle. Mot obit e not ctully cicle but e inted ellipe. Thi w dicoeed by Johne Kepple in the 1600. But let keep it iple nd look t cicul obit. In ode to he cicul pth, centipetl foce i equied. Thi i upplied by the foce of gity between the two bodie. So we cn et the centipetl foce equl to Newton lw of gity: G 1 gity centipetl foce Set the equl to one nothe: 1 G Notice how the of the object cnceled out. 1 1 Thi gie u n eqution fo the obitl elocity: The,, in the eqution i the of the body being obited. If we e tlking bout plnet obiting the un, then the we would ue would be tht of the un. The of the tellite cncel out, o it i not inoled in the obitl elocity eqution t ll. The eqution fo the obitl elocity will not be gien you on the AP Phyic Tet. So be peped to deie it if you need it.

Peiod of tellite: Thi i nothe iple deition job. The peiod of tellite i T, the tie to ke one obit. Wht would be the peiod of the eth ound the un? Let deelop the eqution fo the peiod of tellite. We ll ue the eqution fo ditnce nd ole it fo the tie: x x t t d, the ditnce teled i the cicufeence of the obit. We know tht it would be: x! So we cn plug tht in to the eqution we oled fo tie:! t but i lo gien by the eqution we jut deied fo the obitl elocity: If we plug the obitl elocity into ou woking eqution, i.e., put the togethe, we get: t! Sque both ide: 4! t len up eeything up nice nd netlike uing ou potent lgeb kill: 3 4! t 4! t t 3 4! t! 3 And we end up with n eqution fo the peiod of tellite. Agin the in the thing i the of the body being obited: t! 3