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Page 1: 1. 2 PHYSICS 632 SUMMER 2008 9:00 – 10:50 Room 203 Electricity, Magnetism and Light Richard A. Lindgren, Office Room 302 Text: Halliday, Resnick, and

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Page 2: 1. 2 PHYSICS 632 SUMMER 2008 9:00 – 10:50 Room 203 Electricity, Magnetism and Light Richard A. Lindgren, Office Room 302 Text: Halliday, Resnick, and

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PHYSICS 632 SUMMER 20089:00 – 10:50 Room 203Electricity, Magnetism

and Light

Richard A. Lindgren, Office Room 302

Text: Halliday, Resnick, and Walker, 7’th edition, Extended Version,

Starting with Chapter 21 on Charge.

Page 3: 1. 2 PHYSICS 632 SUMMER 2008 9:00 – 10:50 Room 203 Electricity, Magnetism and Light Richard A. Lindgren, Office Room 302 Text: Halliday, Resnick, and

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Your Goals and Interest• get a degree• crossover teaching• fill in knowledge gaps• review, learn new teaching ideas• peer learning• modeling• inquiry learning• group learning• new experiments and demos• computer technology• solidify concepts• learn how to do problems.

Page 4: 1. 2 PHYSICS 632 SUMMER 2008 9:00 – 10:50 Room 203 Electricity, Magnetism and Light Richard A. Lindgren, Office Room 302 Text: Halliday, Resnick, and

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Assignments• See syllabus for daily homework assignments using WebAssign.• Work on problems in recitation after lecture.

• Discuss with TA’s and others in the apartments at night. Due at 8:00 am next day.

• Algebra, trigonometry, unit vectors and vectors, derivatives and integration review.

• How do you improve problem-solving skills. Lots of practice and more practice.

• Quizzes on second three Tuesdays and final on WebAssign, 30% conceptual questions, 70% problem oriented.

• There will also be 4 homework assignments due in August and September.

• Final exam at the end of September on WebAssign.

Page 5: 1. 2 PHYSICS 632 SUMMER 2008 9:00 – 10:50 Room 203 Electricity, Magnetism and Light Richard A. Lindgren, Office Room 302 Text: Halliday, Resnick, and

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Class Organization

• Cartoon• Demonstrations• Lecture and discussion• Experiments and demos with explanations• Hand-worked problems on Elmo• Clicker/Polling problems

Page 6: 1. 2 PHYSICS 632 SUMMER 2008 9:00 – 10:50 Room 203 Electricity, Magnetism and Light Richard A. Lindgren, Office Room 302 Text: Halliday, Resnick, and

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References and other Texts

• Calculus-Based Physics II (download)– Schnick– http://www.anselm.edu/internet/physics/cbphysics/downloadsII.html

• Physics for Scientists and Engineers, 6th Edition– Serway, Jewett

• Physics for Scientists and Engineers, 3rd Edition– Fishbane, Gasiorowicz, Thornton

• Physics for Scientists & Engineers, 4th Edition– Giancoli

• Principals of Electricity – Page, Adams

Page 7: 1. 2 PHYSICS 632 SUMMER 2008 9:00 – 10:50 Room 203 Electricity, Magnetism and Light Richard A. Lindgren, Office Room 302 Text: Halliday, Resnick, and

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Lecture 1 Charge Ch. 21• Electrostatics: study of electricity when the charges are not in motion. Good place to start studying E&M because there are lots of demonstrations.

• Cartoon - Charge is analogous to mass• Demo - Large Van de Graaff

• Math Review and Tooling up

• Topics–What is electric charge? Point objects, Size. Atomic model–Methods of charging objects. Friction,Contact, Induction, Machines–Instruments to measure charge–Quantization of charge and conservation of charge–Coulombs Law and examples–Principle of superposition and examples

• Demos• Elmo

–Two pennies–Three charges in a plane–Hanging path ball

• Polling

Page 8: 1. 2 PHYSICS 632 SUMMER 2008 9:00 – 10:50 Room 203 Electricity, Magnetism and Light Richard A. Lindgren, Office Room 302 Text: Halliday, Resnick, and

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Charged Hair Van de Graaff Demo

• How does this gadget produce a mini-lightning bolt?• What upward forces are keeping your hair up?• How are these forces produced?• Why do the hair strands spread out from each other?• Why do they spread out radially from the head?• Is hair a conductor or insulator? How can we find out? Does it depend if

is wet or dry.• To understand what is going on we need to know about charge and we

need a model of electricity.

• Need a female teacher to come forward.

Page 9: 1. 2 PHYSICS 632 SUMMER 2008 9:00 – 10:50 Room 203 Electricity, Magnetism and Light Richard A. Lindgren, Office Room 302 Text: Halliday, Resnick, and

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• “In the matter of physics, the first lessons should contain nothing but what is experimental and interesting to see. A pretty experiment is in itself more valuable than 20 formulae.” Albert Einstein

Page 10: 1. 2 PHYSICS 632 SUMMER 2008 9:00 – 10:50 Room 203 Electricity, Magnetism and Light Richard A. Lindgren, Office Room 302 Text: Halliday, Resnick, and

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Charge• What is charge?• How do we visualize it.• We only know charge exists because in experiments electric forces cause objects to move. • Charge is analogous to mass in mechanics. We know how it behaves, but we don’t know what it really is. The same is true for charge..• Need more experiments to get the point across.

• UVa Electrostatics Kit (http://people.virginia.edu/~ral5q/classes/phys632/summer08/lecture_1.html)• Rub a Balloon• 2 x 4 on glass.

• Need a model

Page 11: 1. 2 PHYSICS 632 SUMMER 2008 9:00 – 10:50 Room 203 Electricity, Magnetism and Light Richard A. Lindgren, Office Room 302 Text: Halliday, Resnick, and

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More on charging using the UVa Electrostatic Kit

Page 12: 1. 2 PHYSICS 632 SUMMER 2008 9:00 – 10:50 Room 203 Electricity, Magnetism and Light Richard A. Lindgren, Office Room 302 Text: Halliday, Resnick, and

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QuickTime™ and aTIFF (Uncompressed) decompressor

are needed to see this picture.

Bohr Model

Page 13: 1. 2 PHYSICS 632 SUMMER 2008 9:00 – 10:50 Room 203 Electricity, Magnetism and Light Richard A. Lindgren, Office Room 302 Text: Halliday, Resnick, and

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QuickTime™ and aTIFF (Uncompressed) decompressor

are needed to see this picture.

3 protons, 3 neutrons

Page 14: 1. 2 PHYSICS 632 SUMMER 2008 9:00 – 10:50 Room 203 Electricity, Magnetism and Light Richard A. Lindgren, Office Room 302 Text: Halliday, Resnick, and

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More complicated than just protons, neutrons, and electrons, but this will

suffice.• Electron: Considered a point object with radius less than 10-18 meters with electric

charge e= -1.6 x 10 -19 Coulombs (SI units) and mass me= 9.11 x 10 - 31 kg

• Proton: It has a finite size with charge +e, mass mp= 1.67 x 10-27 kg and with radius– 0.805 +/-0.011 x 10-15 m scattering experiment– 0.890 +/-0.014 x 10-15 m Lamb shift experiment

• Neutron: Similar size as proton, but with total charge = 0 and mass mn=– Positive and negative charges exists inside the neutron

• Pions: Smaller than proton. Three types: + e, - e, 0 charge and radius– 0.66 +/- 0.01 x 10-15 m

• Quarks: Point objects. Confined to the proton and neutron,– Not free– Proton (uud) charge = 2/3e + 2/3e -1/3e = +e– Neutron (udd) charge = 2/3e -1/3e -1/3e = 0

– An isolated quark has never been found

Page 15: 1. 2 PHYSICS 632 SUMMER 2008 9:00 – 10:50 Room 203 Electricity, Magnetism and Light Richard A. Lindgren, Office Room 302 Text: Halliday, Resnick, and

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• Normally atoms are in the lowest energy state. This means that the material is electrically neutral. You have the same number of electrons as protons in the material.

• How do we change this?

• How do we add more electrons than protons or remove electrons?

• There are several different ways.

Page 16: 1. 2 PHYSICS 632 SUMMER 2008 9:00 – 10:50 Room 203 Electricity, Magnetism and Light Richard A. Lindgren, Office Room 302 Text: Halliday, Resnick, and

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QuickTime™ and aTIFF (Uncompressed) decompressor

are needed to see this picture.

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Page 17: 1. 2 PHYSICS 632 SUMMER 2008 9:00 – 10:50 Room 203 Electricity, Magnetism and Light Richard A. Lindgren, Office Room 302 Text: Halliday, Resnick, and

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More on our Model of electricity

1cm long and a radius of 0,005 cm1cm long and a radius of 0,005 cm

Copper atom:Copper atom:

Z=29(protons), N= 34(neutrons),Z=29(protons), N= 34(neutrons),

29 Electrons29 Electrons

Carbon or diamond - poor conductor

Copper (Face Centered Cube) - good conductor

Consider solid material like a piece of copper wire. The proton core is fixed in position in a lattice like structure. In a conductor, the valence electrons are free to move about. How many electrons are free to move about?

Page 18: 1. 2 PHYSICS 632 SUMMER 2008 9:00 – 10:50 Room 203 Electricity, Magnetism and Light Richard A. Lindgren, Office Room 302 Text: Halliday, Resnick, and

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Summary Comments

•Silk(+) on teflon(-)

•Silk (-) on acrylic (+)

•Wood doesn’t charge

•Charged objects always attract neutral objects

•Show Triboelectric series

•Not only chemical composition important, structure of surface is important - monolayer of molecules involved, quantum effect.(nanotechnology)

Page 19: 1. 2 PHYSICS 632 SUMMER 2008 9:00 – 10:50 Room 203 Electricity, Magnetism and Light Richard A. Lindgren, Office Room 302 Text: Halliday, Resnick, and

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Triboelectric serieshttp://www.sciencejoywagon.com/physicszone/lesson/07elecst/static/triboele.htm

SteelWoodAmberSealing WaxHard RubberNickel, CopperBrass, SilverGold, PlatinumSulfurAcetate, RayonPolyesterStyreneOrlonSaranBalloonPolyurethanePolypropyleneVinyl (PVC)SiliconTeflonNegative (Gains electrons easily)

Page 20: 1. 2 PHYSICS 632 SUMMER 2008 9:00 – 10:50 Room 203 Electricity, Magnetism and Light Richard A. Lindgren, Office Room 302 Text: Halliday, Resnick, and

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Electrostatics is based on 4 four empirical facts

• Conservation of charge

• Quantization of charge

• Coulombs Law

• The principle of superposition

Page 21: 1. 2 PHYSICS 632 SUMMER 2008 9:00 – 10:50 Room 203 Electricity, Magnetism and Light Richard A. Lindgren, Office Room 302 Text: Halliday, Resnick, and

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Conservation of charge

• Rubbing does not create charge, it is transferred from object to another

• Teflon negative - silk positive• Acrylic positive - silk negative Demo: Show electronic electroscope with cage: gives magnitude and sign of charge. Use teflon and silk to show + and -.

• Nuclear reactions 0 = e+ + e-

• Radioactive decay 238U92 = 234Th90 + 4He2

• High energy particle reactions e- + p+ = e- + + n0

Page 22: 1. 2 PHYSICS 632 SUMMER 2008 9:00 – 10:50 Room 203 Electricity, Magnetism and Light Richard A. Lindgren, Office Room 302 Text: Halliday, Resnick, and

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What is meant by quantization of charge?

• Discovered in 1911 by Robert A. Millikan in the oil drop experiment

• The unit of charge is so tiny that we will never notice it comes in indivisible lumps.

• Example: Suppose in a typical experiment we charge an object up with a nanoCoulomb of charge (Q = 10-9 C). How many elementary units, N, of charge is this?

N =

Qe=

10−9C

+1.6 ×10−19C=0.625 ×1010 =6.25 ×109

Six billion units of charge

e =+1.6 ×10−19CElementary unit of charge

Page 23: 1. 2 PHYSICS 632 SUMMER 2008 9:00 – 10:50 Room 203 Electricity, Magnetism and Light Richard A. Lindgren, Office Room 302 Text: Halliday, Resnick, and

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Coulombs Law

In 1785 Charles Augustin Coulomb reported in the Royal Academy Memoires using a torsion balance two charged mulberry pithballs repelled each other with a force that is inversely proportional to the distance.

q2q1 r RepulsionRepulsion

RepulsionRepulsion

AttractionAttraction

++ ++

++

-- --

Lab ExperimentLab Experiment

Spheres sameSpheres same as pointsas points

F=kq1q2

r2 where k = 8.99 ×109Nm2 /C2

--Point chargesPoint charges

Also F=1

4ε0

q1q2

r2 where ε0= 8.85 ×10

-12 C2 / N. m2

Electrical Permittivity of vacuum

F=Gm1m2

r2

Page 24: 1. 2 PHYSICS 632 SUMMER 2008 9:00 – 10:50 Room 203 Electricity, Magnetism and Light Richard A. Lindgren, Office Room 302 Text: Halliday, Resnick, and

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Coulombs Law Two Positive Charges

(Equivalent to the weight

of a long strand of hair)

F=kq1q2

r2

1 nC1 nC 1 cmq2q1 r

• What is the magnitude of the force between two positive charges, each 1 nanoCoulomb, and 1cm apart in a typical demo?

RepulsionRepulsion

F =8.99 ×109 Nm2

C2( ) 10−9c( )2

10−2m( )2 =9×10−5 N

• What is the direction of the force?1 nC1 nC 1 cm

What is the direction of the force in unit vector notation?

Page 25: 1. 2 PHYSICS 632 SUMMER 2008 9:00 – 10:50 Room 203 Electricity, Magnetism and Light Richard A. Lindgren, Office Room 302 Text: Halliday, Resnick, and

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F =8.99 ×109 Nm2

C2( ) 10−9c( )2

10−2m( )2 =9×10−5 N

1 nC1 nC 1 cm

• What is the direction of the force in unit vector notation?

x

y

j

i

F1 =−9×10−5 N i

1 2

F2 =+9 ×10−5 N i

Page 26: 1. 2 PHYSICS 632 SUMMER 2008 9:00 – 10:50 Room 203 Electricity, Magnetism and Light Richard A. Lindgren, Office Room 302 Text: Halliday, Resnick, and

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Coulombs Law in vector notation.

vF12 =k

q1 q2

r 2 r12

where: 12Fv is the force exerted by particle 1 on particle 2,

12r is a unit vector in the direction “from 1 to 2”, and k, q1, and q2 are defined as before (the Coulomb constant, the charge on particle 1, and the

charge on particle 2 respectively).

rF12 =

8.99 ×109 Nm2

C2( ) 10−9c( ) 10−9c( )

10−2m( )2 r12 =+9×10−5 N r12

The positive sign means the force on q2 is in the same direction as the unit vector

.q1 . q2

r

r12

rF12

Page 27: 1. 2 PHYSICS 632 SUMMER 2008 9:00 – 10:50 Room 203 Electricity, Magnetism and Light Richard A. Lindgren, Office Room 302 Text: Halliday, Resnick, and

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How do you write the Force on q1

vF21 =k

q1 q2

r 2 r21

where: vF21 is the force exerted by particle 2 on particle 1,

r21 is a unit vector in the direction “from 2 to 1”, and k, q1, and q2 are defined as before (the Coulomb constant, the charge on particle 1, and the

charge on particle 2 respectively).

rF21 =

8.99 ×109 Nm2

C2( ) 10−9c( ) 10−9c( )

10−2m( )2 r12 =+9×10−5 N r21

The positive sign means the force on q1 is in the same direction as the unit vector.

.q1 .q2

r

r21

rF21

Page 28: 1. 2 PHYSICS 632 SUMMER 2008 9:00 – 10:50 Room 203 Electricity, Magnetism and Light Richard A. Lindgren, Office Room 302 Text: Halliday, Resnick, and

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Principle of SuperpositionThree charges In a line

Example Three charges lie on the x axis: q1=+25 nC at the origin, q2= -12 nC at x = 2m, q3=+18 nC at x=3 m. What is the net force on q1 and the direction

of the force? We simply add the two forces keeping track of their directions.

1 2

x3

= 8.99 ×109 Nm2

C2( )(25 ×10−9C)−12 ×10−9C

(2m)2r21 +

18 ×10−9C

(3m)2r31

⎝⎜⎞

⎠⎟

= 8.99 × 109 Nm2

C2( )(25 × 10−9C) −3 × 10−9C r21 + 2 × 10−9C r31( )

=−2.25 ×10−7N r21 (Directed in the positive x direction)

rFnet ,1 =

rF21 +

rF31

rFnet ,1 =k

q1 q2

r212 r21 + k

q1 q3

r312 r31 =kq1

q2

r212 r21 +

q3

r312 r31

⎝⎜⎞

⎠⎟

r21 r31

Page 29: 1. 2 PHYSICS 632 SUMMER 2008 9:00 – 10:50 Room 203 Electricity, Magnetism and Light Richard A. Lindgren, Office Room 302 Text: Halliday, Resnick, and

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Uniformly charged metal spheres of Radius R

F=kq2

(r)2

F≈kq2

(r+2R)2

Demo: Show uniformity of charge around sphere using electrometer. Demo: Show charging spheres by induction using electrometer

Page 30: 1. 2 PHYSICS 632 SUMMER 2008 9:00 – 10:50 Room 203 Electricity, Magnetism and Light Richard A. Lindgren, Office Room 302 Text: Halliday, Resnick, and

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Coulombs Law Two Pennies without electrons

What is the force between two 3 gm pennies one meter apart if we remove all the electrons from the copper atoms?

(Use Elmo)

Page 31: 1. 2 PHYSICS 632 SUMMER 2008 9:00 – 10:50 Room 203 Electricity, Magnetism and Light Richard A. Lindgren, Office Room 302 Text: Halliday, Resnick, and

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What is the force on charge q1 due to many other charges lying in a plane. I would like to show you

another notation.

-q3

+q2+q1

r13

r12

r12

r13

-q3

+q2+q1

rF13

rF12

rFnet

rFnet =

rF12 +

rF13

rF12 =

kq1q2

(r12 )2 r12

rF13 =

kq1q3

(r13)2 r13

rFnet =

rF1i

i=2

N

rFnet

rF13

rF12

In practice you find the x and y comonents of all the vectors and add them up

Page 32: 1. 2 PHYSICS 632 SUMMER 2008 9:00 – 10:50 Room 203 Electricity, Magnetism and Light Richard A. Lindgren, Office Room 302 Text: Halliday, Resnick, and

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Question: What is the net force on q1 and in what direction?

Hint : Find x and y components of force on q1 due to q2 and q3 and add them up.

q1= + 1 nC q2= + 1 nC

+y

+x

5 cm

2 cm

1 cm

q3= - 2 nC

Example: Three point charges in a plane (Use Elmo)

Page 33: 1. 2 PHYSICS 632 SUMMER 2008 9:00 – 10:50 Room 203 Electricity, Magnetism and Light Richard A. Lindgren, Office Room 302 Text: Halliday, Resnick, and

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In an atom can we neglect the gravitational force between the electrons and protons? What is the ratio of Coulomb’s electric force to Newton’s gravity force for 2 electrons separated by a

distance r ?

Fc

Fg

=ke2

Gm2

qq r mm r

Fg =Gmm

r2Fc =kee

r2

Fc

Fg

=8.99 ×109 Nm2

C2( ) 1.6 ×10−19C( )2

6.67 ×10−11 Nm2

kg2( ) 9.1×10−31kg( )2

=4.2 ×1042

Huge number - pure number - no units

Page 34: 1. 2 PHYSICS 632 SUMMER 2008 9:00 – 10:50 Room 203 Electricity, Magnetism and Light Richard A. Lindgren, Office Room 302 Text: Halliday, Resnick, and

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Why are neutral objects always attracted to positive or negative charged objects.

For example:•Rubbed balloon is attracted to wall•Comb is attracted to small bits of paper•Clothes in the dryer stick together.

Demo: Put wood on the spinner and place charged teflon and plastic rods near it.

What is the explanation of all of these phenomena?

Page 35: 1. 2 PHYSICS 632 SUMMER 2008 9:00 – 10:50 Room 203 Electricity, Magnetism and Light Richard A. Lindgren, Office Room 302 Text: Halliday, Resnick, and

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Explanation: The neutral objects atoms and molecules orientthemselves in the following way so that the Coulomb forces due to attraction are greater than those due to repulsion because the latter are further away. (Inverse square Law)

++++++

Acrylic Rod Wooden block

++++++

------

++++++

Acrylic Rod Wooden block

AttractionRepulsion

Attractive forces >> Repulsive Forces

221

r

qkqF =

Page 36: 1. 2 PHYSICS 632 SUMMER 2008 9:00 – 10:50 Room 203 Electricity, Magnetism and Light Richard A. Lindgren, Office Room 302 Text: Halliday, Resnick, and

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Problem: Two equally charged hanging pith balls (Use Elmo)

• Show induction: Click on http://people.virginia.edu/~ral5q/classes/phys632/summer08/lecture_1.html

-- Demo: Using conducting spheres and electrometer– Demo: Electrophorus– Demo: Electroscope

– Demo: hanging charged/conducting pith ball- first attraction by induction, then contact, then conduction of charge, then repulsion

Page 37: 1. 2 PHYSICS 632 SUMMER 2008 9:00 – 10:50 Room 203 Electricity, Magnetism and Light Richard A. Lindgren, Office Room 302 Text: Halliday, Resnick, and

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Chapter 21 Problem 29In crystals of a certain salt, singly charged cations form the eight corners of a cube and a singly charged anion is at the cube's center (Figure 21-32). The edge length of the cube is x = 0.32 nm. The cations are each deficient by one electron (and thus each has a charge of +e), and the anion has one excess electron (and thus has a charge of -e).

Fig. 21-32

(a) What is the magnitude of the net electrostatic force exerted on the anion by the eight cations at the corners of the cube?(b) If one of the cations is missing, the crystal is said to have a defect. What is the magnitude of the net electrostatic force exerted on the anion by the seven remaining cations?

Page 38: 1. 2 PHYSICS 632 SUMMER 2008 9:00 – 10:50 Room 203 Electricity, Magnetism and Light Richard A. Lindgren, Office Room 302 Text: Halliday, Resnick, and

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Chapter 21 Problem 68

In Figure 21-23 particles 1 and 2 are fixed in place, but particle 3 is free to move. If the net electrostatic force on particle 3 due to particles 1 and 2 is zero and L23 =2.00 L12, what is the ratio q1/q2?

Figure 21-23