Medical Physics General Physics Chapter 15 Electric Forces and Electric Fields.

Slides:



Advertisements
Similar presentations
Announcements Monday guest lecturer: Dr. Fred Salsbury. Solutions now available online. Will strive to post lecture notes before class. May be different.
Advertisements

Chapter 22: The Electric Field II: Continuous Charge Distributions
Lecture 6 Problems.
Continuous Charge Distributions
Gauss’s law and its applications
THE ELECTRIC FIELD Chapter Field Force Electric force, just like gravitational force is a field force. A field force is capable of acting through.
Physics 2113 Lecture 12: WED 11 FEB Gauss’ Law III Physics 2113 Jonathan Dowling Carl Friedrich Gauss 1777 – 1855 Flux Capacitor (Operational)
Chapter 24 Gauss’s Law.
Chapter 23 Gauss’ Law.
Gauss’s Law PH 203 Professor Lee Carkner Lecture 5.
Chapter 24 Gauss’s Law.
Hw: All Chapter 5 problems and exercises. Test 1 results Average 75 Median 78 >90>80>70>60>50
Chapter 22 Gauss’s Law Electric charge and flux (sec & .3)
Chapter 24 Gauss’s Law.
Chapter 22 Gauss’s Law Electric charge and flux (sec &.3) Gauss’s Law (sec &.5) Charges on conductors(sec. 22.6) C 2012 J. Becker.
Norah Ali Al-moneef King Saud university
Chapter 23 Gauss’s Law.
Nadiah Alanazi Gauss’s Law 24.3 Application of Gauss’s Law to Various Charge Distributions.
Electric Forces and Electric Fields
Electric Forces and Electric Fields
From Chapter 23 – Coulomb’s Law
Chapter 24 Gauss’s Law.
Bright Storm on Electric Field (Start to minute 6:18)
Chapter 23 Gauss’ Law Key contents Electric flux Gauss’ law and Coulomb’s law Applications of Gauss’ law.
Physics.
Electric Field Lines - a “map” of the strength of the electric field. The electric field is force per unit charge, so the field lines are sometimes called.
Fig 24-CO, p.737 Chapter 24: Gauss’s Law قانون جاوس 1- Electric Flux 2- Gauss’s Law 3-Application of Gauss’s law 4- Conductors in Electrostatic Equilibrium.
Chapter 22 Gauss’s Law.
Gauss’s Law The electric flux through a closed surface is proportional to the charge enclosed The electric flux through a closed surface is proportional.
Physics Lecture 3 Electrostatics Electric field (cont.)
Physics 213 General Physics Lecture 3. 2 Last Meeting: Electric Field, Conductors Today: Gauss’s Law, Electric Energy and Potential.
Lecture 3 Electric Field Electric Field Lines Conductors in Electrostatic Equilibrium Millikan’s Oil-Drop Experiment Van de Graff Generator Electric Flux.
Chapter 16 Electric Forces and Electric Fields. Fundamental Forces of Nature.
Definitions Flux—The rate of flow through an area or volume. It can also be viewed as the product of an area and the vector field across the area Electric.
Chapter 21 Gauss’s Law. Electric Field Lines Electric field lines (convenient for visualizing electric field patterns) – lines pointing in the direction.
Lecture 4 Van de Graff Generator Millikan’s Oil-Drop Experiment Electric Flux and Gauss’s Law Potential Difference Capacitance.
Electric Flux and Gauss Law
Chapter 23 Gauss’s Law Summer Chapter 23 Gauss’ law In this chapter we will introduce the following new concepts: The flux (symbol Φ ) of the electric.
Chapter 15 Electric Forces and Electric Fields. First Studies – Greeks Observed electric and magnetic phenomena as early as 700 BC – Found that amber,
Faculty of Engineering Sciences Department of Basic Science 5/26/20161W3.
Chapter 24 Gauss’s Law. Let’s return to the field lines and consider the flux through a surface. The number of lines per unit area is proportional to.
Lecture 2 The Electric Field. Chapter 15.4  15.9 Outline The Concept of an Electric Field Electric Field Lines Electrostatic Equilibrium Electric Flux.
Chapter 27. A uniformly charged rod has a finite length L. The rod is symmetric under rotations about the axis and under reflection in any plane containing.
1 CHAPTER-23 Gauss’ Law. 2 CHAPTER-23 Gauss’ Law Topics to be covered  The flux (symbol Φ ) of the electric field  Gauss’ law  Application of Gauss’
CHAPTER 24 : GAUSS’S LAW 24.1) ELECTRIC FLUX
Application of Gauss’ Law to calculate Electric field:
ELECTRICITY PHY1013S GAUSS’S LAW Gregor Leigh
Electrostatics.
Introduction: what do we want to get out of chapter 24?
Tue. Feb. 3 – Physics Lecture #26 Gauss’s Law II: Gauss’s Law, Symmetry, and Conductors 1. Electric Field Vectors and Electric Field Lines 2. Electric.
Chapter 28 Gauss’s Law 28.1 to 28.4.
Physics 2113 Lecture 10: WED 16 SEP Gauss’ Law III Physics 2113 Jonathan Dowling Carl Friedrich Gauss 1777 – 1855 Flux Capacitor (Operational)
3/21/20161 ELECTRICITY AND MAGNETISM Phy 220 Chapter2: Gauss’s Law.
Fig 24-CO, p.737 Chapter 24: Gauss’s Law قانون جاوس 1- Electric Flux 2- Gauss’s Law 3-Application of Gauss’s law 4- Conductors in Electrostatic Equilibrium.
Chapter 15 Electric Forces and Electric Fields. First Studies – Greeks Observed electric and magnetic phenomena as early as 700 BC – Found that amber,
Copyright © 2012 Pearson Education Inc. PowerPoint ® Lectures for University Physics, Thirteenth Edition – Hugh D. Young and Roger A. Freedman Lectures.
24.2 Gauss’s Law.
Chapter 23 Gauss’s Law Spring 2008.
Electric Flux & Gauss Law
15.6 Conductors in Electrostatic Equilibrium
Flux Capacitor (Operational)
Chapter 21 Gauss’s Law.
Chapter 23 Gauss’s Law.
Chapter 24 - Summary Gauss’s Law.
Norah Ali Al-moneef King Saud university
Phys102 Lecture 3 Gauss’s Law
Chapter 23 Gauss’s Law.
Electric Fields of Conductors
Areas and Stuff January 29, 2010.
Chapter 23 Gauss’s Law.
Presentation transcript:

Medical Physics General Physics Chapter 15 Electric Forces and Electric Fields

Medical Physics General Physics Gauss’s Law Sections 7-9

Medical Physics General Physics What is the difference between Electric Field (E) and Force (F)? E factors out the magnitude of the test charge, it only depends on the other charges 2.E is defined everywhere, F only at one point 3.Both 1) and 2) 4.Neither 1) or 2)

Medical Physics General Physics Review Corn Field: corn at regularly space intervals Vector Field: a vector at each point in space Scalar Field: a number at each point in space –Eg: Temperature

Medical Physics General Physics Review Electric Field Field lines: an easy way to visualize fields –Tangent to E –Density of lines proportional to E field begin at (+), end at (-) # of lines proportional to q lines don’t cross

Medical Physics General Physics Review Conductors & Electrostatic equilibrium – E=0 inside a conductor – excess charge lies on outer surface – E is perpendicular to surface – charge is greatest at highest curvature

Medical Physics General Physics Why are you safe inside a car during a thunder storm? The rubber tires insulate the car from the ground 2.Charge cannot come inside the metal shell of the car 3.The rounded car has a lower charge density 4.It’s not safe!

Medical Physics General Physics Millikan Oil-Drop Experiment –Found every charge had an integral multiple of e (q = n e) –Measured the elementary charge, e = 1.6  C Active Figure: The Millikan Oil-Drop ExperimentThe Millikan Oil-Drop Experiment EquilibriumDrag -- Terminal velocity

Medical Physics General Physics Van de Graaff Generator An electrostatic generator designed and built by Robert J. Van de Graaff in 1929 Charge is transferred to the dome by means of a rotating belt Limited by ionization of air, which carries charge away Eventually an electrostatic discharge takes place MU28T33

Medical Physics General Physics Museum of Science, Boston

Medical Physics General Physics Holifield Radioactive Ion Beam Facility Oak Ridge National Laboratory 25.5 MeV

Medical Physics General Physics Electric Flux Field lines penetrating an area A perpendicular to the field The product of EA is the flux, Φ (the number of field lines!) In general: Φ E = E A cos θ

Medical Physics General Physics Electric Flux, cont. –When the area is constructed such that a closed surface is formed, use the convention that flux lines passing into the interior of the volume are negative and those passing out of the interior of the volume are positive Φ E = E A cos θ –The perpendicular to the area A is at an angle θ to the field

Medical Physics General Physics Gauss’ Law Gauss’ Law: the electric flux through any closed surface is proportional to the net charge Q inside the surface –ε o =8.85 x C 2 /Nm 2 is the permittivity of free space –The area in Φ is an imaginary surface, a Gaussian surface, it does not have to coincide with the surface of a physical object Active Figure: Electric Flux Through an Arbitrary Closed SurfaceElectric Flux Through an Arbitrary Closed Surface MU29T17

Medical Physics General Physics Electric Field of a Charged Thin Spherical Shell The calculation of the field outside the shell is identical to that of a point charge The electric field inside the shell is E = 0 MU29T23

Medical Physics General Physics Electric Field of a Nonconducting Plane Sheet of Charge Total charge Q is uniformly distributed over surface A Charge density σ = Q/A Use a cylindrical Gaussian surface The flux through the ends is EA, no field through the curved part of the surface Note, the field is uniform

Medical Physics General Physics Electric Field of a Nonconducting Plane Sheet of Charge, cont. The field must be perpendicular to the sheet The field is directed either toward or away from the sheet

Medical Physics General Physics Parallel Plate Capacitor The device consists of plates of positive and negative charge The total electric field between the plates is given by The field outside the plates is zero

Medical Physics General Physics What is the total electric flux through the surface of the cube in a constant electric field E? E L E L E L E

Medical Physics General Physics Maxwell’s Equation #1 or They all mean the same thing. or SPACE TIME