RE 6.d Electric and Rest Energy RE 6.e EP6, HW6: Ch 6 Pr s 58, 59, 91, 99(a-c), 105(a-c)

Similar documents
Physics 202, Lecture 2. Announcements

24-2: Electric Potential Energy. 24-1: What is physics

LINEAR MOMENTUM. product of the mass m and the velocity v r of an object r r

Physics 2A Chapter 11 - Universal Gravitation Fall 2017

One-dimensional kinematics

a v2 r a' (4v) 2 16 v2 mg mg (2.4kg)(9.8m / s 2 ) 23.52N 23.52N N

PHY126 Summer Session I, 2008

Energy and Energy Transfer

Remember: When an object falls due to gravity its potential energy decreases.

Rotational Kinematics. Rigid Object about a Fixed Axis Western HS AP Physics 1

COLLEGE OF FOUNDATION AND GENERAL STUDIES PUTRAJAYA CAMPUS FINAL EXAMINATION TRIMESTER /2017

PHYS Week 5. Reading Journals today from tables. WebAssign due Wed nite

v c motion is neither created nor destroyed, but transferred via interactions. Fri. Wed (.18,.19) Introducing Potential Energy RE 6.

Chapter 3 and Chapter 4

Chapter 5 Circular Motion

Description Linear Angular position x displacement x rate of change of position v x x v average rate of change of position

Chapter 8. Linear Momentum, Impulse, and Collisions

10/23/2003 PHY Lecture 14R 1

3.1 Electrostatic Potential Energy and Potential Difference

Energy in Closed Systems

9/19/2013. PHY 113 C General Physics I 11 AM-12:15 PM MWF Olin 101

EMU Physics Department

Page 1. Physics 131: Lecture 14. Today s Agenda. Things that stay the same. Impulse and Momentum Non-constant forces

Spring Force and Power

Chapter 23: Electric Potential

Review. Physics 231 fall 2007

Chapter 07: Kinetic Energy and Work

Week 6, Chapter 7 Sect 1-5

Physics Exam II Chapters 25-29

Physics for Scientists and Engineers. Chapter 9 Impulse and Momentum

Conservation of Angular Momentum = "Spin"

Physics 181. Particle Systems

Physics 207 Lecture 13. Lecture 13

CHAPTER 8 Potential Energy and Conservation of Energy

PHYS 705: Classical Mechanics. Derivation of Lagrange Equations from D Alembert s Principle

CSU ATS601 Fall Other reading: Vallis 2.1, 2.2; Marshall and Plumb Ch. 6; Holton Ch. 2; Schubert Ch r or v i = v r + r (3.

Physics 1: Mechanics

Lecture 16. Chapter 11. Energy Dissipation Linear Momentum. Physics I. Department of Physics and Applied Physics

Fri Angular Momentum Quiz 10 RE 11.a; HW10: 13*, 21, 30, 39 Mon , (.12) Rotational + Translational RE 11.b Tues.

Physics 201 Lecture 4

Study Guide For Exam Two

So far: simple (planar) geometries

Physics 1501 Lecture 19

Chapter I Matrices, Vectors, & Vector Calculus 1-1, 1-9, 1-10, 1-11, 1-17, 1-18, 1-25, 1-27, 1-36, 1-37, 1-41.

Physics 207 Lecture 16

Ch04 Work, Energy and Power What is work in physics?

ALL QUESTIONS ARE WORTH 20 POINTS. WORK OUT FIVE PROBLEMS.

Linear Momentum. Center of Mass.

PHYS 2421 Fields and Waves

Scalars and Vectors Scalar

Dynamics of Rigid Bodies

in state i at t i, Initial State E = E i

First Law: A body at rest remains at rest, a body in motion continues to move at constant velocity, unless acted upon by an external force.

Mechanics Physics 151

Integral Vector Operations and Related Theorems Applications in Mechanics and E&M

1. A body will remain in a state of rest, or of uniform motion in a straight line unless it

Electron density: Properties of electron density (non-negative): => exchange-correlation functionals should respect these conditions.

Physics 111 Lecture 11

Physics 106 Lecture 6 Conservation of Angular Momentum SJ 7 th Ed.: Chap 11.4

Week 11: Chapter 11. The Vector Product. The Vector Product Defined. The Vector Product and Torque. More About the Vector Product

You will analyze the motion of the block at different moments using the law of conservation of energy.

Chapter 3. r r. Position, Velocity, and Acceleration Revisited

Period & Frequency. Work and Energy. Methods of Energy Transfer: Energy. Work-KE Theorem 3/4/16. Ranking: Which has the greatest kinetic energy?

AP-C WEP. h. Students should be able to recognize and solve problems that call for application both of conservation of energy and Newton s Laws.

Physics 207: Lecture 20. Today s Agenda Homework for Monday

Lesson 8: Work, Energy, Power (Sections ) Chapter 6 Conservation of Energy

iclicker Quiz a) True b) False Theoretical physics: the eternal quest for a missing minus sign and/or a factor of two. Which will be an issue today?

PHYS 1443 Section 004 Lecture #12 Thursday, Oct. 2, 2014

Mon , (.12) Rotational + Translational RE 11.b Tues.

Problem While being compressed, A) What is the work done on it by gravity? B) What is the work done on it by the spring force?

Rigid Bodies: Equivalent Systems of Forces

Chapter 12 Equilibrium & Elasticity

Physics 114 Exam 2 Spring Name:

10/15/2013. PHY 113 C General Physics I 11 AM-12:15 PM MWF Olin 101

UNIVERSITÀ DI PISA. Math thbackground

Physics 2A Chapter 3 HW Solutions

Physics 131: Lecture 16. Today s Agenda

Capítulo. Three Dimensions

Chapter 8: Potential Energy and The Conservation of Total Energy

Conservation of Energy

HW 7 Help. 60 s t. (4.0 rev/s)(1 min) 240 rev 1 min Solving for the distance traveled, we ll need to convert to radians:

Physics 11b Lecture #2. Electric Field Electric Flux Gauss s Law

Test 1 phy What mass of a material with density ρ is required to make a hollow spherical shell having inner radius r i and outer radius r o?

Week 9 Chapter 10 Section 1-5

Lecture 1a: Satellite Orbits

Conflict Exam Issue. Sorry, Can t do it. Please see Kevin Pitts if you have any additional questions or concerns about this. Office is 231 Loomis

PHYSICS 231 Review problems for midterm 2

PHYS 1441 Section 002 Lecture #16

TEST-03 TOPIC: MAGNETISM AND MAGNETIC EFFECT OF CURRENT Q.1 Find the magnetic field intensity due to a thin wire carrying current I in the Fig.

Page 1. Clicker Question 9: Physics 131: Lecture 15. Today s Agenda. Clicker Question 9: Energy. Energy is Conserved.

( ) ( ) Review of Force. Review of Force. r = =... Example 1. What is the dot product for F r. Solution: Example 2 ( )

PHYS 705: Classical Mechanics. Newtonian Mechanics

Dynamics of Rotational Motion

Slide 1. Quantum Mechanics: the Practice

Lecture 1a: Satellite Orbits

11. Dynamics in Rotating Frames of Reference

DYNAMICS VECTOR MECHANICS FOR ENGINEERS: Kinematics of Rigid Bodies in Three Dimensions. Seventh Edition CHAPTER

Review of Vector Algebra and Vector Calculus Operations

Engineering Mechanics. Force resultants, Torques, Scalar Products, Equivalent Force systems

Physics 2A Chapters 6 - Work & Energy Fall 2017

Transcription:

ed. Lab., Mon. Tues. ed. Lab. Mon. Tues. 6.1-.4 (.1) Intoducng Enegy & ok Quz 5 L5: Buoyancy, Ccles & Pendulums 6.5-.7 (.) Rest Mass,ok by Changng oces tudy Day tudy Day 6.8-.9(.18,.19) Intoducng Potental Enegy The Thngs Physcsts & Engnees Do 6.1-.13 (.) Gavtatonal P.E. & Vsualzng RE 6.a laptop RE 6.b tudy Day tudy Day RE 6.c (last day to dop) RE 6.d 6.14-.17 Electc and Rest Enegy RE 6.e EP6, H6: Ch 6 P s 58, 59, 91, 99(a-c), 15(a-c) moton s nethe ceated no destoyed, but tanseed va nteactons. Momentum p mv v 1 c Enegy dt dt d E all all all dt d Impulse ok

Undestandng ok: cala o Dot Poduct as sum o poducts o components y z ŷ y z y y ˆ

ŷ' ˆ y' ' Undestandng ok: cala o Dot Poduct as pojecton o one vecto onto anothe poduct o magntudes and cosne ŷ ˆ z y z y cos z y z y

Undestandng ok: conceptual non-physcst de Teache tudents ok E = E = Teaches Physcs Lean Physcs T

Undestandng ok: conceptual non-physcst de Teache tudents ok E = Zzzz Teaches Physcs Lean Physcs T Teaches Physcs Lean Nothng

Undestandng ok: conceptual non-physcst de Teache tudents ok Zzzz E = Teaches Physcs Lean Physcs T Teaches Physcs Teaches Nothng Lean Nothng Lean Physcs

Undestandng ok: conceptual non-physcst de E = B=NC 3 Teache tudents ok T?? Teaches Physcs Lean Physcs Teaches Physcs Teaches Nothng Lean Nothng Lean Physcs Teaches Physcs Unlean Physcs

Undestandng ok: conceptual non-physcst de E = C est un Gand Chen! Teache tudents ok Teaches Physcs Lean Physcs T Teaches Physcs Lean Nothng Teaches Nothng Lean Physcs Teaches Physcs Unlean Physcs Teaches Physcs Lean ench

Undestandng ok: conceptual non-physcst de E = C est un Gand Chen! Teache tudents ok Teaches Physcs Lean Physcs T Teaches Physcs Lean Nothng Teaches Nothng Lean Physcs Teaches Physcs Unlean Physcs Teaches Physcs Lean ench ok s the poduct o eot and achevement Both n the same decton, t s good (+) wok Both opposte dectons, t s bad (-) wok Both unelated dectons, t s no () wok One non-estent, t s no () wok

ŷ ˆ ysphus Pushes ock uphll z s y z y... Rock goes up hll. + wok Rock stays put. wok Rock olls down hll. - wok Rock sldes sdeways. z wok Undestandng ok: conceptual physcst de

ŷ ˆ ysphus Pushes ock uphll z s y z y.... + wok. wok. - wok. z wok ok s the poduct o oce and Dsplacement Both n the same decton, t s good (+) wok Both opposte dectons, t s bad (-) wok Both unelated dectons, t s no () wok One non-estent, t s no () wok Undestandng ok: conceptual physcst de

On a space staton, you pushed a bo that was at est at locaton <,, 1 > m to locaton <,,14 > m, applyng a oce <,, 5 > N. How much wok dd you do on the bo? 1) = J ) = 5 J 3) = 7 J 4) = 14 J 5) Not enough nomaton Assumng no othe oces appled to the bo hat happened? 1) The bo slowed down. ) The bo sped up. 3) The bo moved at constant speed. Net you patne pushed back on the movng bo wth a oce <,, -3 > N. Ate the bo had moved om <,, 14 > m to <,, 16 > m. hat happened? 1) The bo slowed down. ) The bo sped up. 3) The bo moved at constant speed.

You move an object om < 3, 7, 4 > m to <, 1, 1 > m, applyng a oce < 1, -, 3 > N. How much wok do you do? 1) 1 J ) 17 J 3) < -1, -6, 4 > J 4) < 3, -14, 1 > J 5)

Enegy E ok Enegy Relaton You won t have to do anythng lke ths o a ew yeas E v om o dt dt sub.-ng back n E 1 d d p / m p d 1 1 all d v 1 c ok d v dt mv p / m v whee p so v c 1 1 1 d v c d p E 1 1 p 1 / p p

Q6..d: Consde an electon (mass 9e-31 kg) movng wth speed v =.9c. hat s ts total (patcle) enegy? 1) 7.3e-31 J ) 8.1e-14 J 3) 1.5e-13 J 4) 1.86e-13 J 5).7e8 m/s

Enegy E ok Enegy Relaton dt dt I v<<c d d p all mv d dt d v ok E v m dv v 1 mv 1 1 mv mv (appomate) Knetc Enegy

Q6..a: A ball whose mass s kg tavels at a velocty o <, 3, 4> m/s. hat s the knetc enegy o the ball? 1) <, 6, 8 > J ) <, 3, 4 > J 3) J 4) 1 J 5) 5 J

ed. Lab., Mon. Tues. ed. Lab. Mon. Tues. 6.1-.4 (.1) Intoducng Enegy & ok Quz 5 L5: Buoyancy, Ccles & Pendulums 6.5-.7 (.) Rest Mass,ok by Changng oces tudy Day tudy Day 6.8-.9(.18,.19) Intoducng Potental Enegy The Thngs Physcsts & Engnees Do 6.1-.13 (.) Gavtatonal P.E. & Vsualzng RE 6.a laptop RE 6.b tudy Day tudy Day RE 6.c (last day to dop) RE 6.d 6.14-.17 Electc and Rest Enegy RE 6.e EP6, H6: Ch 6 P s 58, 59, 91, 99(a-c), 15(a-c) moton s nethe ceated no destoyed, but tanseed va nteactons. Enegy E all d ok

Eample. An electon (mass 9e-31 kg) s tavelng at a speed o.95c (so v/c =.95)n an electon acceleato. An electc oce o 1.6e-13 N s appled n the decton o moton whle the electon tavels a dstance o m. e want to detemne the new value o v/c o the electon, usng the enegy pncple. Eample 1: The acat cae Nmtz has a ully loaded mass o 8.35 1 7 kg. It tavels a dstance o 8 1 3 m n 3.5 h (1.6 1 3 s). hat s the aveage knetc enegy (n joules) o the Nmtz?