General Physics (PHY 2130)

Similar documents
CHAPTER 8 Potential Energy and Conservation of Energy

Faraday's Law of Induction

Lecture 2 The First Law of Thermodynamics (Ch.1)

Experiment 5 Elastic and Inelastic Collisions

Review C: Work and Kinetic Energy

Homework: 49, 56, 67, 60, 64, 74 (p )

Chapter 11 Torque and Angular Momentum

Chapter 9. Linear Momentum and Collisions

NMT EE 589 & UNM ME 482/582 ROBOT ENGINEERING. Dr. Stephen Bruder NMT EE 589 & UNM ME 482/582

Rotation Kinematics, Moment of Inertia, and Torque

Lagrangian Dynamics: Virtual Work and Generalized Forces

1 What is a conservation law?

University Physics AI No. 11 Kinetic Theory

WORK DONE BY A CONSTANT FORCE

5.74 Introductory Quantum Mechanics II

Goals Rotational quantities as vectors. Math: Cross Product. Angular momentum

Shielding Equations and Buildup Factors Explained

Chapter 31B - Transient Currents and Inductance

Mean Molecular Weight

Rotation and Conservation of Angular Momentum

HALL EFFECT SENSORS AND COMMUTATION

Physics 110 Spring D Motion Problems: Projectile Motion Their Solutions

Damage detection in composite laminates using coin-tap method

Laws of Electromagnetism

AP Physics B 2009 Free-Response Questions

Risk-based Fatigue Estimate of Deep Water Risers -- Course Project for EM388F: Fracture Mechanics, Spring 2008

Ch. 9 Center of Mass Momentum. Question 6 Problems: 3, 19, 21, 27, 31, 35, 39, 49, 51, 55, 63, 69, 71, 77

8.5 UNITARY AND HERMITIAN MATRICES. The conjugate transpose of a complex matrix A, denoted by A*, is given by

Work, Energy and Power

8. Potential Energy and Conservation of Energy Potential Energy: When an object has potential to have work done on it, it is said to have potential

Recurrence. 1 Definitions and main statements

Section 2 Introduction to Statistical Mechanics

Effects of Extreme-Low Frequency Electromagnetic Fields on the Weight of the Hg at the Superconducting State.

Linear Circuits Analysis. Superposition, Thevenin /Norton Equivalent circuits

AP Physics - Chapter 8 Practice Test

Problem Set 5 Work and Kinetic Energy Solutions

Chapter 7 WORK, ENERGY, AND Power Work Done by a Constant Force Kinetic Energy and the Work-Energy Theorem Work Done by a Variable Force Power

Work, Energy & Power. AP Physics B

SPEE Recommended Evaluation Practice #6 Definition of Decline Curve Parameters Background:

Inner core mantle gravitational locking and the super-rotation of the inner core

This circuit than can be reduced to a planar circuit

Consider a 1-D stationary state diffusion-type equation, which we will call the generalized diffusion equation from now on:

Chapter 6 Work and Energy

Chapter 6 Inductance, Capacitance, and Mutual Inductance

Q3.8: A person trying to throw a ball as far as possible will run forward during the throw. Explain why this increases the distance of the throw.

7.5. Present Value of an Annuity. Investigate

Chapter 2. Lagrange s and Hamilton s Equations

Solution: Let i = 10% and d = 5%. By definition, the respective forces of interest on funds A and B are. i 1 + it. S A (t) = d (1 dt) 2 1. = d 1 dt.

"Research Note" APPLICATION OF CHARGE SIMULATION METHOD TO ELECTRIC FIELD CALCULATION IN THE POWER CABLES *

Implementation of Deutsch's Algorithm Using Mathcad

Answer: A). There is a flatter IS curve in the high MPC economy. Original LM LM after increase in M. IS curve for low MPC economy

Jet Engine. Figure 1 Jet engine

Support Vector Machines

Objective: Work Done by a Variable Force Work Done by a Spring. Homework: Assignment (1-25) Do PROBS # (64, 65) Ch. 6, + Do AP 1986 # 2 (handout)

CHAPTER 6 WORK AND ENERGY

Thursday, December 10, 2009 Noon - 1:50 pm Faraday 143

Quotes. Research Findings. The First Law of Thermodynamics. Introduction. Introduction. Thermodynamics Lecture Series

CHAPTER 14 MORE ABOUT REGRESSION

Section 5.4 Annuities, Present Value, and Amortization

An Alternative Way to Measure Private Equity Performance

What is Candidate Sampling

Section 5.3 Annuities, Future Value, and Sinking Funds

Calculation of Sampling Weights

How To Understand The Results Of The German Meris Cloud And Water Vapour Product

Rate Monotonic (RM) Disadvantages of cyclic. TDDB47 Real Time Systems. Lecture 2: RM & EDF. Priority-based scheduling. States of a process

- 573 A Possible Detector for the Study of Weak Interactions at Fermi Clash R. Singer Argonne National Laboratory

The circuit shown on Figure 1 is called the common emitter amplifier circuit. The important subsystems of this circuit are:

Section C2: BJT Structure and Operational Modes

The Development of Web Log Mining Based on Improve-K-Means Clustering Analysis

1. Math 210 Finite Mathematics

Unit 3 Work and Energy Suggested Time: 25 Hours

where the coordinates are related to those in the old frame as follows.

NON-CONSTANT SUM RED-AND-BLACK GAMES WITH BET-DEPENDENT WIN PROBABILITY FUNCTION LAURA PONTIGGIA, University of the Sciences in Philadelphia

The Cox-Ross-Rubinstein Option Pricing Model

Portfolio Loss Distribution

Solving Newton s Second Law Problems

CHAPTER 5 RELATIONSHIPS BETWEEN QUANTITATIVE VARIABLES

UPGRADE YOUR PHYSICS

PRO-CRIMPER* III Hand Crimping Tool Assembly with Die Assembly

SIMPLE LINEAR CORRELATION

Causal, Explanatory Forecasting. Analysis. Regression Analysis. Simple Linear Regression. Which is Independent? Forecasting

Work-Energy Bar Charts

THERMAL PROPERTIES OF MATTER 12

At the skate park on the ramp

Texas Instruments 30X IIS Calculator

Review D: Potential Energy and the Conservation of Mechanical Energy

Addendum to: Importing Skill-Biased Technology

The OC Curve of Attribute Acceptance Plans

Mechanical Properties of Evaporated Gold Films. Hard Substrate Effect Correction

Viscosity of Solutions of Macromolecules

Simulating injection moulding of microfeatured components

Analysis of Reactivity Induced Accident for Control Rods Ejection with Loss of Cooling

Introduction to Statistical Physics (2SP)

Work, Power, Energy Multiple Choice. PSI Physics. Multiple Choice Questions

9. The kinetic energy of the moving object is (1) 5 J (3) 15 J (2) 10 J (4) 50 J

Curso Física Básica Experimental I Cuestiones Tema IV. Trabajo y energía.

Lesson 3 - Understanding Energy (with a Pendulum)

21 Vectors: The Cross Product & Torque

Ch 8 Potential energy and Conservation of Energy. Question: 2, 3, 8, 9 Problems: 3, 9, 15, 21, 24, 25, 31, 32, 35, 41, 43, 47, 49, 53, 55, 63

Lecture #21. MOS Capacitor Structure

Transcription:

General Physcs (PHY 130) Lecture 15 Energy Knetc and potental energy Conservatve and non-conservatve orces http://www.physcs.wayne.edu/~apetrov/phy130/

Lghtnng Revew Last lecture: 1. Work and energy: work: connecton between orces and energy knetc energy Revew Problem:.

Potental Energy Potental energy s assocated wth the poston o the object wthn some system Potental energy s a property o the system, not the object A system s a collecton o objects or partcles nteractng va orces or processes that are nternal to the system Unts o Potental Energy are the same as those o Work and Knetc Energy

Gravtatonal Potental Energy Gravtatonal Potental Energy s the energy assocated wth the relatve poston o an object n space near the Earth s surace Objects nteract wth the earth through the gravtatonal orce Actually the potental energy o the earth-object system

Potental Energy: example

Work and Gravtatonal Potental Energy Consder block o mass m at ntal heght y Work done by the gravtatonal orce W grav Thus : W ( F cosθ ) s grav y y mg s ( mg cosθ ) s, but :, cosθ 1, ( y y ) mgy mgy. Ths quantty s called potental energy: PE mgy Note: W gravty PE PE Important: work s related to the derence n PE s!

Reerence Levels or Gravtatonal Potental Energy A locaton where the gravtatonal potental energy s zero must be chosen or each problem The choce s arbtrary snce the change n the potental energy s the mportant quantty Choose a convenent locaton or the zero reerence heght oten the Earth s surace may be some other pont suggested by the problem

Reerence Levels or Gravtatonal Potental Energy A locaton where the gravtatonal potental energy s zero must be chosen or each problem The choce s arbtrary snce the change n the potental energy gves the work done W W W W grav1 grav grav3 grav1 mgy W mgy mgy 1 3 grav mgy mgy mgy W 1 3, grav3,..

Example: What s the change n gravtatonal potental energy o the box t s placed on the table? The table s 1.0 m tall and the mass o the box s 1.0 kg. 9 Frst: Choose the reerence level at the loor. U 0 here. ΔU g mgδy mg ( y y ) ( )( 1.0 kg 9.8 m/s )( 1.0 m 0 m) + 9.8 J

10 Example contnued: Now take the reerence level (U 0) to be on top o the table so that y -1.0 m and y 0.0 m. ΔU g mgδy mg ( y y ) ( )( 1kg 9.8 m/s ) 0.0m ( 1.0 m) ( ) + 9.8 J The results or the energy derence do not depend on the locaton o U 0!

ConcepTest At the bowlng alley, the ball-eeder mechansm must exert a orce to push the bowlng balls up a 1.0-m long ramp. The ramp leads the balls to a chute 0.5 m above the base o the ramp. Approxmately how much orce must be exerted on a 5.0-kg bowlng ball? 1. 00 N. 50 N 3. 5 N 4. 5.0 N 5. mpossble to determne

ConcepTest At the bowlng alley, the ball-eeder mechansm must exert a orce to push the bowlng balls up a 1.0-m long ramp. The ramp leads the balls to a chute 0.5 m above the base o the ramp. Approxmately how much orce must be exerted on a 5.0-kg bowlng ball? 1. 00 N. 50 N 3. 5 N 4. 5.0 N 5. mpossble to determne Note: The orce exerted by the mechansm tmes the dstance o 1.0 m over whch the orce s exerted must equal the change n the potental energy o the ball.

13 More about Gravtatonal Potental Energy The general expresson or gravtatonal potental energy s: U ( r) GM 1M where r U r ( ) 0

14 Example: What s the gravtatonal potental energy o a body o mass m on the surace o the Earth? U ( r R ) GM M r 1 e GM em R e

Conservatve Forces A orce s conservatve the work t does on an object movng between two ponts s ndependent o the path the objects take between the ponts The work depends only upon the ntal and nal postons o the object Any conservatve orce can have a potental energy uncton assocated wth t Note: a orce s conservatve the work t does on an object movng through any closed path s zero.

Examples o Conservatve Forces: Examples o conservatve orces nclude: Gravty Sprng orce Electromagnetc orces Snce work s ndependent o the path: W : only ntal and nal ponts c PE PE

Nonconservatve Forces A orce s nonconservatve the work t does on an object depends on the path taken by the object between ts nal and startng ponts. Examples o nonconservatve orces knetc rcton, ar drag, propulsve orces

Example: Frcton as a Nonconservatve Force The rcton orce transorms knetc energy o the object nto a type o energy assocated wth temperature the objects are warmer than they were beore the movement Internal Energy s the term used or the energy assocated wth an object s temperature

Frcton Depends on the Path The blue path s shorter than the red path The work requred s less on the blue path than on the red path Frcton depends on the path and so s a nonconservatve orce

Conservaton o Mechancal Energy Conservaton n general To say a physcal quantty s conserved s to say that the numercal value o the quantty remans constant In Conservaton o Energy, the total mechancal energy remans constant In any solated system o objects that nteract only through conservatve orces, the total mechancal energy o the system remans constant.

Conservaton o Energy Total mechancal energy s the sum o the knetc and potental energes n the system E K +U KE + PE E E KE + PE KE + PE Whenever nonconservatve orces do no work, the mechancal energy o a system s conserved. That s E E or ΔK -ΔU. Other types o energy can be added to mody ths equaton

What do you do when there are nonconservatve orces? For example, rcton s present ΔE E E W rc The work done by rcton.

Problem Solvng wth Conservaton o Energy Dene the system Select the locaton o zero gravtatonal potental energy Do not change ths locaton whle solvng the problem Determne whether or not nonconservatve orces are present I only conservatve orces are present, apply conservaton o energy and solve or the unknown

Example: A roller coaster car s about to roll down a track. Ignore rcton and ar resstance. At what speed does the car reach the top o the loop? 4 m 988 kg 40 m 0 m y0 (a) Idea: use conservaton o energy: mechancal energy s the same! U mgy + E K + 0 v U E mgy + g K + 1 ( y y ) 19.8 m/s mv

ConcepTest A block ntally at rest s allowed to slde down a rctonless ramp and attans a speed v at the bottom.to acheve a speed v at the bottom, how many tmes as hgh must a new ramp be? 1. 1. 3. 3 4. 4 5. 5 6. 6

ConcepTest A block ntally at rest s allowed to slde down a rctonless ramp and attans a speed v at the bottom.to acheve a speed v at the bottom, how many tmes as hgh must a new ramp be? 1. 1. 3. 3 4. 4 5. 5 6. 6 Note: The gan n knetc energy, proportonal to the square o the block s speed at the bottom o the ramp, s equal to the loss n potental energy. Ths, n turn, s proportonal to the heght o the ramp.

Work Done by Varyng Forces The work done by a varable orce actng on an object that undergoes a dsplacement s equal to the area under the graph o F versus x

8 Example: What s the work done by the varable orce shown below? F x (N) F 3 F F 1 x 1 x x 3 x (m) The work done by F 1 s W F ( x 0) 1 1 1 The work done by F s W F ( x ) x1 3 F3 x3 x The work done by F 3 s W ( ) The net work s then W 1 +W +W 3.

Potental Energy Stored n a Sprng Involves the sprng constant (or orce constant), k Hooke s Law gves the orce F - k x F s the restorng orce F s n the opposte drecton o x k depends on how the sprng was ormed, the materal t s made rom, thckness o the wre, etc.

Example: (a) I orces o 5.0 N appled to each end o a sprng cause the sprng to stretch 3.5 cm rom ts relaxed length, how ar does a orce o 7.0 N cause the same sprng to stretch? (b) What s the sprng constant o ths sprng? 30 F F 1 1 (a) For sprngs F x. Ths allows us to wrte. F 7.0 N 5.0 N Solvng or x : x x ( 3.5 cm) 4.9 cm. 1 x x 1 F1 (b) What s the sprng constant o ths sprng? Use Hooke s law: k x F 5.0 N 3.5 cm 1 1.43 N/cm. Or k x F 7.0 N 4.9 cm 1.43 N/cm.

Example: An deal sprng has k 0.0 N/m. What s the amount o work done (by an external agent) to stretch the sprng 0.40 m rom ts relaxed length? 31 F x (N) kx 1 x 1 0.4 m x (m) W Area under curve 1 1 1 ( kx )( x ) kx ( 0.0 N/m)( 0.4 m) 1.6 J 1 1 1