+ + + + + + + + + + + + + + + + + + + + ++ + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + +

Slides:



Advertisements
Similar presentations
Chapter 22 Electrostatics.
Advertisements

Physics 2415 Lecture 6 Michael Fowler, UVa
Electrostatics and Electricity. ELECTRIC CHARGE Static Electricity: electric charge at rest due to electron transfer (usually by friction) + – + – + –
Electric Potential AP Physics Montwood High School R. Casao.
Coulomb’s Law Coulomb’s law states that the force of a charged object on another charged object is directly proportional to the product of their charge(s)
When an object is dropped on earth, the work done by the gravitational force is equal to the change in gravitational potential energy: W = mgh initial.
ELECTRIC FIELDS… Field diagrams, properties of conductors, and the superposition principle.
Capacitors Physics 2415 Lecture 8 Michael Fowler, UVa.
Electrostatics …the branch of physics that studies the nature of charges that’s not moving.
Hw: All Chapter 5 problems and exercises. Test 1 results Average 75 Median 78 >90>80>70>60>50
Charge is invisibly small but sparks are visible! What are they made of? Why can we see them?
Triple Gun Assembly (R,B,G beams) of a color television tube.
Electric Charge and Electric Field
Norah Ali Al-moneef king saud university
If the effective field is E =800,000 N/C over a gap length of 2.5 cm, what is the electron’s final velocity, v ? Electron Gun Heated filamentPositively.
Summary: Coulomb’s Law describes the force between two charges Coulomb’s Law is identical in form to Newton’s Gravitational Law, but force is much stronger.
AP Physics: Electricity & Magnetism
Electricity and Magnetism ISCI Electricity is a Force – Vector – Electric charges (attract and repel) – Comb and Ball Example 2.Atoms – Protons.
ELECTRIC ENERGY AND ELECTRIC POTENTIAL. ENERGY REVIEW When we studied energy a couple of months ago there were a few major points of interest: Work is.
Chapter 33: Electric Fields and Potential I. Electric Fields (33.1) A. Gravitational Field- the force field that surrounds a mass 1. Idea that things.
9.3.1Define electric potential and electric potential energy State and apply the expression for electric potential due to a point charge State.
Electric Potential and Electric Energy Chapter 17.
Two different things that sound alike! Electrical Energy and Electrical Potential In order to bring two like charges together work must be done. In order.
Electric Potential and Capacitance What’s a volt anyway? Presentation 2001 Dr. Phil Dauber as modified by R. McDermott.
Electrical Energy and Potential IB Physics. Electric Fields and WORK In order to bring two like charges near each other work must be done. In order to.
Chapter 18 Electrical Energy and Capacitance. Chapter 18 Objectives Electrical potential Electric Potential from a Point Charge Capacitance Parallel Plate.
33 Electric Fields and Potential The electrical potential energy of a charged particle is increased when work is done to push it against the electric field.
Electric Energy and Capacitance
Weds., Jan. 29, 2014PHYS , Dr. Andrew Brandt 1 PHYS 1442 – Section 004 Lecture #5 Wednesday January 29, 2014 Dr. Andrew Brandt CH 17 Electric Potential.
Static Electricity Chapter 16 and 24. Review: The 4 Fundamental Forces Strong Force – The force that is involved in holding the nucleus of an atom together.
Capacitanc e and Dielectrics AP Physics C Montwood High School R. Casao.
Copyright © 2009 Pearson Education, Inc. Chapter 23 Electric Potential.
Chapter 16 Electrical Energy and Capacitance. Objectives Electrical potential Electric Potential from a Point Charge Electron Volt Capacitance Parallel.
Chapter 16 Electrical Energy and Capacitance Conceptual Quiz Questions.
Electrical Energy And Capacitance
Lecture A Fundamentals and Background. Charge “Charge” is the basic quantity in electrical circuit analysis Fundamental charge quantity is the charge.
Electrical Energy and Potential
It’s what we see… Static Electricity Charges Rubbing plastic or glass makes them attractive to bits of paper or dust Benjamin Franklin decided to call.
Electrostatics laboratory of the 1700s 
Wednesday, Sep. 14, PHYS Dr. Andrew Brandt PHYS 1444 – Section 04 Lecture #5 Chapter 21: E-field examples Chapter 22: Gauss’ Law Examples.
Electric Potential.
Electric Charge (1) Evidence for electric charges is everywhere, e.g.
Work and Voltage We studied electric force and electric field…now we can expand our discussion to include WORK and POTENTIAL ENERGY just as we did with.
Uniform Electric Field between Parallel Charged Plates Constant force on a charged particle Constant force on a charged particle.
Electric Potential 2 q A C B r A B r path independence a a Rr VQ 4   r Q 4   R.
Monday, Sept. 19, 2005PHYS , Fall 2005 Dr. Jaehoon Yu 1 PHYS 1444 – Section 003 Lecture #6 Monday, Sept. 19, 2005 Dr. Jaehoon Yu Electric Potential.
1) Electric Charge I 1) one is positive, the other is negative 2) both are positive 3) both are negative 4) both are positive or both are negative Two.
Oct. 4, From last time(s)… Work, energy, and (electric) potential Electric potential and charge Electric potential and electric field. Electric charges,
Electric Fields and Potential Chapter 33. Electric Fields Electric Field – a force field that fills the space around every electric charge or group of.
Monday, Sep. 19, PHYS Dr. Andrew Brandt PHYS 1444 – Section 004 Lecture #6 Chapter 23: Monday Sep. 19, 2011 Dr. Andrew Brandt Electric.
AP Electrostatics The force between two isolated charges is governed by Coulomb’s Law: F e = k q 1 q 2 r2r2 q 1 and q 2 are charges r = distance k = 9.
Static Electricity, Electric Forces, Electric Fields.
Static Electricity, Electric Forces, Electric Fields.
 What is the term for electricity at rest?  For a neutral atom, the amount of electrons equals…
Chapter 18 Electrical Energy and Capacitance Electrical Potential Energy Objectives 1. Define electrical potential energy 2. Compare the electrical.
Static Electricity / Electrostatics Where have you experienced this? –Shocked a friend? (or yourself) –Clothes in the dryer stick together –Stroke a cat.
Physics 30 Unit 2 Review Electrical Forces and Fields.
Electric Force and Electric FieldS
A proton and an electron are in a constant electric field created by oppositely charged plates. You release the proton from the positive side and the.
Electric Potential Energy and The Electric Potential
ConcepTest 17.1a Electric Potential Energy I
Electric Potential Between Charged Plates
PHYS 1444 – Section 02 Lecture #5
Chapter 33 ELECTRIC FIELDS AND POTENTIAL.
Unit 2.2 Static Electricity – Part 2
PHYS 1444 – Section 003 Lecture #6
Electric Potential Physics 1220 Lecture 6.
Electrical Potential Voltage.
PHYS 1444 – Section 003 Lecture #6
Objectives Define work in terms of energy.
Presentation transcript:

What is the electric field at the very CENTER of this spherical conductor? E = 0!!

The electric field at this off-CENTER point within the spherical conductor Nearby charges create a strong electric field. Much farther away, individual charges have a much smaller effect, but there are much more of them! All of this balances beautifully and the electric field even at off-center points (in fact, EVERYWHERE ) within the conductor is zero!

That’s why fan motors or transformers (which can produce fluctuating electric fields) are often shielded from the more sensitive parts of circuits by “cans” of conducting metal.

Conducting panels when screwed in place provide a surrounding shield against stray electric fields!

Concept Review h = 1 m A man lifts a 5 kg rock 1 meter off the ground. The potential energy of the rock is about A) (5 kg)  ( 1 m) = 5 J B) (5 kg)  g  1m  50 J C) 2(5 kg)  (1 m) = 100 J D) (5 kg)  g 2  500 J About how much work did he do? A) 5 J C) 50 J B) 100 J D) 500 J E) cannot be determined from the information given Gravitational potential energy = mgh

Concept Review Test The balls in the figure are identical. When released from rest, which has a greater kinetic energy when it gets to the bottom of its ramp? A) B) C) both the same

Electric Energy Which experiences the greater acceleration? (1) proton (2) electron (3) both have equal acceleration (4) neither will accelerate at all. A proton and an electron are each accelerated by moving the same distance across a region of constant electric field, E.

Electric Energy Which experiences the bigger increase in Kinetic Energy ? (1) proton (2) electron (3) both receive the same increase in KE increase in KE (4) neither --  KE = 0 for both A proton and an electron are each accelerated by moving the same distance across a region of constant electric field, E.

h Recall the work done in elevating a bag of fluids W = mgh results in added pressure P =  gh in this I.V. tube:

Just like the work done mgh in lifting (pumping water) creates added pressure P =  gh which can be exchanged as fluid kinetic energy = ½  v 2. in separating unlike charge and/or building concentrations of like charge. Electric Potential Difference Work q voltage is related to the work done (by a generator or even chemically by a battery) V =

Work q  PE q Electric Potential Difference V = = Notice the amount of potential energy stored by any charge in a potential V is charge  voltage = ENERGY

       + Separating clinging fabrics is doing work (W = Fd) against the electric fields that try to hold them together.      Prying your shoe from carpet involves a tiny bit more work than just lifting the weight of your foot.

m  PE = work required to move an object against a “restoring” force (F avg )(x ) moved against that force g d Work = mgd depends on m, g, d

m g d Work = mgd depends on m, g, d E +q+q Work = Fd +q+q d = (qE)d(qE)d Work q =EdEd V = Ed depends on q, E, d

E +q+q +q+q d V = Ed Work = (qE)d For a uniform E-field But moving toward a tightly concentrated charge Q +q+q

But for a tightly concentrated charge Q +q+q V = EdWork = (qE)d Since the E-field keeps changing so fast! Instead : Work = k  k qQ R stop qQ R start

Q and the voltage of a concentration of charge Q build up across the surface of a spherical conductor of radius, R:

            

MIT’s Van de Graff Generator 1935 Robert Jamison Van de Graff

750 keV = 750,000 eV Fermi National Laboratory

1.5 MeV electron accelerator Basel, Switzerland

Two identical conducting spheres (with insulated handles) are charged to different voltages, V 1 >V 2. The two spheres must be a. charged with Q 1 >Q 2. b. charged identically with Q 1 = Q 2. c. charged with Q 1 <Q 2.

Two identical conducting spheres (with insulated handles) are charged to different voltages, V 1 >V 2. When touched together a. charge flows from 1  2. b. all charge stays in place. c. charge flows from 2  1.

Two identical conducting spheres (with insulated handles) are charged to different voltages, V 1 >V 2. Having been touched together a. both spheres are now at V 1. b. both spheres are now at V 2. c. both spheres are now at a voltage in between V 1 and V 2.

A large conducting sphere of radius R initially carries an initial charge. When touched to a smaller, uncharged conducting sphere of radius r < R charge flows to the smaller sphere until 1. each sphere carries half the total charge. 2. each sphere carries the same density of charge. 3. charge is divided between them in proportion to their radii: q/Q = r/R.

Two conducting spheres (radius R and r), after touching, are at the same potential. = or

But check out a comparison of the charge DENSITY across the surface of each: If then And how do these compare: 1. > 2. = 3. <

But check out a comparison of the charge DENSITY across the surface of each: Although Q > q The charge density across the surface of the smaller sphere is HIGHER! Charge is crowded together much more tightly on the smaller sphere!

7. is zero QUESTION 1 As explained in slide 2! 7. is zero QUESTION 2 As argued in slides 4-5! (B) (5 kg)  g  1m  50 J QUESTION 3 Gravitational potential energy = mgh (C) 50 J QUESTION 4 Work done = change in energy it produces (2) electron QUESTION 5 q electron =q proton so since F=qE both proton and electron experience the same sized force! However, since m electron << m proton, they respond differently! The electron will move with an acceleration ~2000  greater than the proton (since the proton is almost 2000  heavier! both receive the same (3) both receive the same increase in KE increase in KE QUESTION 6 Both experience the same F=qE and travel the same distance d under its influence. So the same amount of work W=Fd is done on each. QUESTION 7 We’ll discuss this one on Wednesday!