3/30/15 oregon state university ph 213, class #11 physics 213 (welcome!) instructor: chris coffin...

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3/30/15 Oregon State University PH 213, Class #1 1 Physics 213 (welcome! ) Instructor : Chris Coffin Wngr 283 [email protected] u www.physics.oregonstate.edu/~coffinc/COURSES/ ph213

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Page 1: 3/30/15 Oregon State University PH 213, Class #11 Physics 213 (welcome!) Instructor: Chris Coffin Wngr 283 coffinc@physics.oregonstate.edu coffinc/COURSES/ph213

3/30/15 Oregon State University PH 213, Class #1 1

Physics 213(welcome!)

Instructor: Chris CoffinWngr 283

[email protected]

www.physics.oregonstate.edu/~coffinc/COURSES/ph213

Page 2: 3/30/15 Oregon State University PH 213, Class #11 Physics 213 (welcome!) Instructor: Chris Coffin Wngr 283 coffinc@physics.oregonstate.edu coffinc/COURSES/ph213

3/30/15 Oregon State University PH 213, Class #1 2

Announcements

・ For all registration issues, go to the Physics Dept office (Wngr 301). Do not attend any class/lab other than what you are registered for.

・ No labs meet this week. You’ll first meet your lab TA next week; names/schedules will be posted soon. There is a take-home Lab 1 —see the Course Calendar.

・ No PH 223 recitations will meet this week. The recitation TA (Brian Johnson) may have contacted you already (check your e-mail) to intro- duce that course. (See also the link on the PH 213 home page.)

・ Get your textbook. If you’re not using the full hard-cover (3rd ed.), you’ll need Volume 3 of the custom OSU edition. The author is Randy Knight; the publisher is Pearson. You don’t need to buy a lab manual—labs will be posted online again this term.

・ We will be using clickers starting this Wednesday. We use the TurningPoint clicker model.

Page 3: 3/30/15 Oregon State University PH 213, Class #11 Physics 213 (welcome!) Instructor: Chris Coffin Wngr 283 coffinc@physics.oregonstate.edu coffinc/COURSES/ph213

3/30/15 Oregon State University PH 213, Class #1 3

About This Course

Read the web site.

Start with the Announcements and go from there.

The HW sets are not handed in for points,

but the HW is NOT optional.

Strong suggestion: Stay caught up with the reading and HW schedule shown on the Course Calendar. Do at least a little of the suggested HW item as scheduled—then return to do the rest as you’re doing your studying before the exam.

Page 4: 3/30/15 Oregon State University PH 213, Class #11 Physics 213 (welcome!) Instructor: Chris Coffin Wngr 283 coffinc@physics.oregonstate.edu coffinc/COURSES/ph213

3/30/15 Oregon State University PH 213, Class #1 4

This term is challenging.

Because we will be dealing with the properties of space itself (properties you can’t see with your eyes), you will need your fullest range of visualization skills, physics unit analysis, and “sense-making” habits.

This term is math-intensive.

Some of the properties of space are vectors. We can do 2-D analysis on many occasions, but (especially when we get to magnetism), we must do 3-D analysis.

You will need to be able to construct integrals. You can look up the analytical solutions to various integral forms, but first you have to do the physics to see what forms you have to work with.

Page 5: 3/30/15 Oregon State University PH 213, Class #11 Physics 213 (welcome!) Instructor: Chris Coffin Wngr 283 coffinc@physics.oregonstate.edu coffinc/COURSES/ph213

3/30/15 Oregon State University PH 213, Class #1 5

Note: Slides 5-14 offer only a brief summary of our basic understanding of electric charge. For a fuller account of how we have arrived at these conclusions, continue on with slides 15-61 (and read likewise in the text).

Electric Charge

Like mass, charge is an intrinsic property of matter.

Like mass, charge is conserved.

Like mass, charge exerts force.

Unlike mass, charge has two types: positive and negative. And whereas mass always attracts other mass, the force exerted between two charges may be either attractive or repulsive, depending on whether the charges are positive or negative.

Like charges repel.

Opposite charges attract.

Page 6: 3/30/15 Oregon State University PH 213, Class #11 Physics 213 (welcome!) Instructor: Chris Coffin Wngr 283 coffinc@physics.oregonstate.edu coffinc/COURSES/ph213

3/30/15 Oregon State University PH 213, Class #1 6

One very common amount of charge is called e. It is the amount of charge found on an electron (-e) or on a proton (+e). The magnitude of the charge, e, is

e = 1.60 x 10-19 C

The SI unit of charge is the Coulomb (C).

Note that the Coulomb is a base, or fundamental, SI unit.Like length, time and mass, charge can be considered a fundamental dimension in the universe.

Page 7: 3/30/15 Oregon State University PH 213, Class #11 Physics 213 (welcome!) Instructor: Chris Coffin Wngr 283 coffinc@physics.oregonstate.edu coffinc/COURSES/ph213

3/30/15 Oregon State University PH 213, Class #1 7

Electrons are much more easily moved from substance to substance than are protons. Protons are more tightly bound—in the nucleus— of each atom.

Thus, electrons are the most common carriers of charge. To give an object a net negative charge, you generally add electrons to it. To give it a net positive charge you generally remove electrons from it.

The atoms of some substances release electrons much more easily than others. These are called electrical conductors. (The others are called electrical insulators.)

Page 8: 3/30/15 Oregon State University PH 213, Class #11 Physics 213 (welcome!) Instructor: Chris Coffin Wngr 283 coffinc@physics.oregonstate.edu coffinc/COURSES/ph213

3/30/15 Oregon State University PH 213, Class #1 8

Most objects are electrically neutral unless electrons have been added or removed (by force), in a process called charging.

When charging occurs, the extra charge (which is either positive or negative) distributes uniformly over the outside of the object— because all those extra “like” charges are all repelled by one another.

This happens very quickly in a conductor, such as metal; much more slowly in an insulator.

You can charge an object either through contact or through induction.

Page 9: 3/30/15 Oregon State University PH 213, Class #11 Physics 213 (welcome!) Instructor: Chris Coffin Wngr 283 coffinc@physics.oregonstate.edu coffinc/COURSES/ph213

3/30/15 Oregon State University PH 213, Class #1 9

Keep in mind that the electrons that carry charge are also particles, each with a mass.

Example: You rub a plastic rod against a wool rug. Then you touch each object to a different but identical metal sphere.

Which sphere then has more mass?

How about if you then touch the spheres together?

How could you then induce a charge difference between them once again?

Page 10: 3/30/15 Oregon State University PH 213, Class #11 Physics 213 (welcome!) Instructor: Chris Coffin Wngr 283 coffinc@physics.oregonstate.edu coffinc/COURSES/ph213

3/30/15 Oregon State University PH 213, Class #1 10

me = 9.11 x 10-31 kg

e = 1.60 x 10-19 C

Example: Two objects, formerly identical and electrically neutral, now have equal and opposite net charges of ±3.0 C. What’s the difference in their masses now?

A. 1.07 x 10-13 kg

B. 1.71 x 10-17 kg

C. 3.42 x 10-17 kg

D. 3.29 x 10-24 kg

E. None of the above.

Page 11: 3/30/15 Oregon State University PH 213, Class #11 Physics 213 (welcome!) Instructor: Chris Coffin Wngr 283 coffinc@physics.oregonstate.edu coffinc/COURSES/ph213

3/30/15 Oregon State University PH 213, Class #1 11

Example: Three metal spheres, A, B and C, are identical in all respects, except that A carries a net charge of +10q; B carries a net charge of –2q; and C carries no net charge.

(a)What is the total net charge of all three spheres?

(b)A and B are touched together, then separated. Next, A and C are touched together, then separated. Finally, B and C are touched together, then separated. What net charge does C now carry?

(c)What is the total net charge of all three spheres now?

Page 12: 3/30/15 Oregon State University PH 213, Class #11 Physics 213 (welcome!) Instructor: Chris Coffin Wngr 283 coffinc@physics.oregonstate.edu coffinc/COURSES/ph213

An electroscope is positively charged by touching it with a positive glass rod. The electroscope leaves spread apart and the glass rod is removed. Then a negatively charged plastic rod is brought close to the top of the electroscope, but it doesn’t touch. What happens to the leaves?

1. The leaves get closer together

2. The leaves spread further apart

3. The leaves don’t move

4. One leaf moves higher, the other lower

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Page 13: 3/30/15 Oregon State University PH 213, Class #11 Physics 213 (welcome!) Instructor: Chris Coffin Wngr 283 coffinc@physics.oregonstate.edu coffinc/COURSES/ph213

If a negative charged rod is held near a neutral metal ball, the ball is attracted to the rod. This happens because…

1. There are magnetic effects.

2. The rod polarizes the metal.

3. The rod and the ball have opposite net charges.

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Three balls are suspended from thin threads. Balls 1 and 2 repel each other and balls 2 and 3 attract each other. From this we can conclude that

1. 1 and 3 carry charges of opposite sign.

2. 1 and 3 carry charges of equal sign.

3. All three carry the charges of the same sign.

4. One of the balls carries no charge.

5. We need to do more experiments to determine

the sign of the charges.

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Discovering Electricity: Experiment 1

Take a plastic rod that has been undisturbed for a long period of time and hang it by a thread.

Pick up another undisturbed plastic rod and bring it close to the hanging rod.

Nothing happens to either rod.

No forces are observed.

We will say that the original objects are neutral.3/30/15 15Oregon State University PH 213, Class #1

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Discovering Electricity: Experiment 2

Rub both plastic rods with wool.

Now the hanging rod tries to move away from the handheld rod when you bring the two close together.

Two glass rods rubbed with silk also repel each other.

There is a long-range repulsive force, requiring no contact, between two identical objects that have been charged in the same way.

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Discovering Electricity: Experiment 3

Bring a glass rod that has been rubbed with silk close to a hanging plastic rod that has been rubbed with wool.

These two rods attract each other.

These particular two types of rods are different materials, charged in a somewhat different way, and they attract each other rather than repel.

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Discovering Electricity: Experiment 4

Rub rods with wool or silk and observe the forces between them.

These forces are greater for rods that have been rubbed more vigorously.

The strength of the forces decreases as the separation between the rods increases.

The force between two charged objects depends on the distance between them.

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Discovering Electricity: Experiment 5

Hold a charged (i.e., rubbed) plastic rod over small pieces of paper on the table.

The pieces of paper leap up and stick to the rod.

There is an attractive force between a charged object and a neutral (uncharged) object.

A charged glass rod does the same. However, a neutral rod has no effect on the pieces

of paper.

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Discovering Electricity: Experiment 6

Rub a plastic rod with wool and a glass rod with silk.

Hang both by threads, some distance apart.

Both rods are attracted to a neutral object that is held close.

There is an attractive force between a charged object and a neutral (uncharged) object.

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Page 21: 3/30/15 Oregon State University PH 213, Class #11 Physics 213 (welcome!) Instructor: Chris Coffin Wngr 283 coffinc@physics.oregonstate.edu coffinc/COURSES/ph213

Charged glass and plastic rods hang by threads. An object attracts the glass rod. If this object is then held near the plastic rod, it will

A. Attract the plastic rod.

B. Repel the plastic rod.

C. Not affect the plastic rod.

D. Either A or B. There’s not enough information to tell.

QuickCheck 25.1

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Page 22: 3/30/15 Oregon State University PH 213, Class #11 Physics 213 (welcome!) Instructor: Chris Coffin Wngr 283 coffinc@physics.oregonstate.edu coffinc/COURSES/ph213

Charged glass and plastic rods hang by threads. An object attracts the glass rod. If this object is then held near the plastic rod, it will

A. Attract the plastic rod.

B. Repel the plastic rod.

C. Not affect the plastic rod.

D. Either A or B. There’s not enough information to tell.

QuickCheck 25.1

The object could have plastic charge, which would repel the plastic rod. Or it could be neutral and attract both charged rods.

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Discovering Electricity: Experiment 7

Rub a hanging plastic rod with wool and then hold the wool close to the rod.

The rod is weakly attracted to the wool.

The plastic rod is repelled by a piece of silk that has been used to rub glass.

The silk starts out with equal amounts of “glass charge” and “plastic charge” and the rubbing somehow transfers “glass charge” from the silk to the rod.

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Page 24: 3/30/15 Oregon State University PH 213, Class #11 Physics 213 (welcome!) Instructor: Chris Coffin Wngr 283 coffinc@physics.oregonstate.edu coffinc/COURSES/ph213

Discovering Electricity: Experiment 8

Other objects, after being rubbed, attract one of the hanging charged rods (plastic or glass) and repel the other.

These objects always pick up small pieces of paper.

There appear to be no objects that, after being rubbed, pick up pieces of paper and attract both the charged plastic and glass rods.

There are only two types of charge: “like plastic” and “like glass”; there is no third kind of charge.

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Charge Model, Part I

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Discovering Electricity: Experiment 9

Charge can be transferred from one object to another, but only when the objects touch.

The metal sphere then picks up small pieces of paper and repels a charged, hanging plastic rod.

The metal sphere appears to have acquired “plastic charge”.

Charge a plastic rod by rubbing it with wool.

Touch a neutral metal sphere with the rubbed area of the rod.

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Page 27: 3/30/15 Oregon State University PH 213, Class #11 Physics 213 (welcome!) Instructor: Chris Coffin Wngr 283 coffinc@physics.oregonstate.edu coffinc/COURSES/ph213

Discovering Electricity: Experiment 10

Charge a plastic rod, then run your finger along it.

After you’ve done so, the rod no longer picks up small pieces of paper or repels a charged, hanging plastic rod.

Removing charge from an object, which you can do by touching it, is called discharging.

Similarly, the metal sphere of Experiment 9 no longer repels the plastic rod after you touch it with your finger.

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Discovering Electricity: Experiment 11

Place two metal spheres close together with a plastic rod connecting them.

Charge a second plastic rod, by rubbing, and touch it to one of the metal spheres.

Afterward, the metal sphere that was touched picks up small pieces of paper and repels a charged, hanging plastic rod.

The other metal sphere does neither.

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Discovering Electricity: Experiment 12

Repeat Experiment 11 with a metal rod connecting the two metal spheres.

Metal is a conductor: Charge moves easily through it. Glass and plastic are insulators: Charges remain immobile.

Touch one metal sphere with a charged plastic rod.

Afterward, both metal spheres pick up small pieces of paper and repel a charged, hanging plastic rod.

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Charge Model, Part II

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Example 25.1 Transferring Charge

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Example 25.1 Transferring Charge

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Charge

The modern names for the two types of charge, coined by Benjamin Franklin, are positive charge and negative charge.

Franklin established the convention that a glass rod that has been rubbed with silk is positively charged.

Any other object that repels a charged glass rod is also positively charged, and any charged object that attracts a charged glass rod is negatively charged.

Thus a plastic rod rubbed with wool is negative.

This convention was established long before the discovery of electrons and protons.

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A rod attracts a positively charged hanging ball. The rod is

A. Positive.

B. Negative.

C. Neutral.

D. Either A or C.

E. Either B or C.

QuickCheck 25.2

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A rod attracts a positively charged hanging ball. The rod is

A. Positive.

B. Negative.

C. Neutral.

D. Either A or C.

E. Either B or C.

QuickCheck 25.2

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Atoms and Electricity

An atom consists of a very small and dense nucleus, surrounded by much less massive orbiting electrons.

The nucleus contains both protons and neutrons.

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Atoms and Electricity

The atom is held together by the attractive electric force between the positive nucleus and the negative electrons.

Electrons and protons have charges of opposite sign but exactly equal magnitude.

This atomic-level unit of charge, called the fundamental unit of charge, is represented by the symbol e.

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Charge Quantization

Where Np and Ne are the number of protons and electrons contained in the object.

Most macroscopic objects have an equal number of protons and electrons and therefore have q = 0.

A charged object has an unequal number of protons and electrons.

Notice that an object’s charge is always an integer multiple of e.

This is called charge quantization.

A macroscopic object has net charge:

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Atoms and Electricity

The process of removing an electron from the electron cloud of an atom, or adding an electron to it, is called ionization.

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Atoms and Electricity

Molecular ions can be created when one of the bonds in a large molecule is broken.

This is the way in which a plastic rod is charged by rubbing with wool or a comb is charged by passing through your hair.

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Insulators

The electrons in an insulator are all tightly bound to the  positive nuclei and not free to move around.

Charging an insulator by friction leaves patches of molecular ions on the surface, but these patches are immobile.

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Conductors

In metals, the outer atomic electrons are only weakly bound to the nuclei.

These outer electrons become detached from their parent nuclei and are free to wander about through the entire solid.

The solid as a whole remains electrically neutral, but the electrons are now like a negatively charged liquid permeating an array of positively charged ion cores.

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Charging

The figure shows how a conductor is charged by contact with a charged plastic rod.

Electrons in a conductor are free to move.

Once charge is transferred to the metal, repulsive forces between the electrons cause them to move apart from each other.

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Discharging

The figure shows how touching a charged metal discharges it.

Any excess charge that was initially confined to the metal can now spread over the larger metal human conductor.

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Charge Polarization

The figure shows how a charged rod held close to an electroscope causes the leaves to repel each other.

How do charged objects of either sign exert an attractive force on a neutral object?

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Charge Polarization

Although the metal as a whole is still electrically neutral, we say that the object has been polarized.

Charge polarization is a slight separation of the positive and negative charges in a neutral object.

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Charge Polarization

Charge polarization produces an excess positive charge on the leaves of the electroscope, so they repel each other.

Because the electroscope has no net charge, the electron sea quickly readjusts once the rod is removed.

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Polarization Force

The figure below shows a positively charged rod near a neutral piece of metal.

Because the electric force decreases with distance, the attractive force on the electrons at the top surface is slightly greater than the repulsive force on the ions at the bottom.

The net force toward the charged rod is called a polarization force.

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The Electric Dipole

The figure below shows how a neutral atom is polarized by an external charge, forming an electric dipole.

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The Electric Dipole

When an insulator is brought near an external charge, all the individual atoms inside the insulator become polarized.

The polarization force acting on each atom produces a net polarization force toward the external charge.

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Charging by Induction, Step 1

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Charging by Induction, Step 2

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Charging by Induction, Step 3

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Metal spheres 1 and 2 are touching. Both are initially neutral.a. The charged rod is brought near.b. The charged rod is then removed.c. The spheres are separated.Afterward, the charges on the sphere are:

A. Q1 is + and Q2 is +.

B. Q1 is + and Q2 is –.

C. Q1 is – and Q2 is +.

D. Q1 is – and Q2 is –.

E. Q1 is 0 and Q2 is 0.

QuickCheck 25.3

3/30/15 54Oregon State University PH 213, Class #1

Page 55: 3/30/15 Oregon State University PH 213, Class #11 Physics 213 (welcome!) Instructor: Chris Coffin Wngr 283 coffinc@physics.oregonstate.edu coffinc/COURSES/ph213

Metal spheres 1 and 2 are touching. Both are initially neutral.a. The charged rod is brought near.b. The charged rod is then removed.c. The spheres are separated.Afterward, the charges on the sphere are:

A. Q1 is + and Q2 is +.

B. Q1 is + and Q2 is –.

C. Q1 is – and Q2 is +.

D. Q1 is – and Q2 is –.

E. Q1 is 0 and Q2 is 0.

QuickCheck 25.3

3/30/15 55Oregon State University PH 213, Class #1

Page 56: 3/30/15 Oregon State University PH 213, Class #11 Physics 213 (welcome!) Instructor: Chris Coffin Wngr 283 coffinc@physics.oregonstate.edu coffinc/COURSES/ph213

Metal spheres 1 and 2 are touching. Both are initially neutral.a. The charged rod is brought near.b. The spheres are separated.c. The charged rod is then removed.Afterward, the charges on the sphere are:

A. Q1 is + and Q2 is +.

B. Q1 is + and Q2 is –.

C. Q1 is – and Q2 is +.

D. Q1 is – and Q2 is –.

E. Q1 is 0 and Q2 is 0.

QuickCheck 25.4

3/30/15 56Oregon State University PH 213, Class #1

Page 57: 3/30/15 Oregon State University PH 213, Class #11 Physics 213 (welcome!) Instructor: Chris Coffin Wngr 283 coffinc@physics.oregonstate.edu coffinc/COURSES/ph213

Metal spheres 1 and 2 are touching. Both are initially neutral.a. The charged rod is brought near.b. The spheres are separated.c. The charged rod is then removed.Afterward, the charges on the sphere are:

A. Q1 is + and Q2 is +.

B. Q1 is + and Q2 is –.

C. Q1 is – and Q2 is +.

D. Q1 is – and Q2 is –.

E. Q1 is 0 and Q2 is 0.

QuickCheck 25.4

Net charge is obtained if contact is broken while the spheres are polarized.This is charging by induction.

3/30/15 57Oregon State University PH 213, Class #1

Page 58: 3/30/15 Oregon State University PH 213, Class #11 Physics 213 (welcome!) Instructor: Chris Coffin Wngr 283 coffinc@physics.oregonstate.edu coffinc/COURSES/ph213

Based on the last experiment, where two spheres were charged by induction, we can conclude that

A. Only the – charges move.

B. Only the + charges move.

C. Both the + and – charges move.

D. We can draw no conclusion about which charges move.

QuickCheck 25.5

3/30/15 58Oregon State University PH 213, Class #1

Page 59: 3/30/15 Oregon State University PH 213, Class #11 Physics 213 (welcome!) Instructor: Chris Coffin Wngr 283 coffinc@physics.oregonstate.edu coffinc/COURSES/ph213

Based on the last experiment, where two spheres were charged by induction, we can conclude that

A. Only the – charges move.

B. Only the + charges move.

C. Both the + and – charges move.

D. We can draw no conclusion about which charges move.

QuickCheck 25.5

3/30/15 59Oregon State University PH 213, Class #1

Page 60: 3/30/15 Oregon State University PH 213, Class #11 Physics 213 (welcome!) Instructor: Chris Coffin Wngr 283 coffinc@physics.oregonstate.edu coffinc/COURSES/ph213

Identical metal spheres are initially charged as shown.Spheres P and Q are touched together and then separated.Then spheres Q and R are touched together and separated.Afterward the charge on sphere R is

A. –1 nC or less.

B. –0.5 nC.

C. 0 nC.

D. +0.5 nC.

E. +1.0 nC or more.

QuickCheck 25.6

3/30/15 60Oregon State University PH 213, Class #1

Page 61: 3/30/15 Oregon State University PH 213, Class #11 Physics 213 (welcome!) Instructor: Chris Coffin Wngr 283 coffinc@physics.oregonstate.edu coffinc/COURSES/ph213

Identical metal spheres are initially charged as shown.Spheres P and Q are touched together and then separated.Then spheres Q and R are touched together and separated.Afterward the charge on sphere R is

A. –1 nC or less.

B. –0.5 nC.

C. 0 nC.

D. +0.5 nC.

E. +1.0 nC or more.

QuickCheck 25.6

3/30/15 61Oregon State University PH 213, Class #1