Your Questions - UMD Department of Physics - UMD...

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Transcript of Your Questions - UMD Department of Physics - UMD...

Page 1: Your Questions - UMD Department of Physics - UMD …physics.umd.edu/courses/Phys132/spring2014/LecturesB/B...• We ignore the electrostatic potential energies of all other pairs (since
Page 2: Your Questions - UMD Department of Physics - UMD …physics.umd.edu/courses/Phys132/spring2014/LecturesB/B...• We ignore the electrostatic potential energies of all other pairs (since

Your QuestionsI do not think I understand the difference between the electric field and the electric potential. They seem to be the same equation to me. I see that electric field is derived using the force between the charges while the electric potential is derived using the electrical energy between the charges, however I do not understand what you mean when you say that electric field is the ?gradient? of the electric potential.

Since V is the change in potential energy, would another way to calculate it be V = delta PE = delta (ugh)?

What is the electron volt?

Does the model of a line for charge always apply? Can the charge move down the line and not be equally?

I know the electric field above the plane points up, but what does the electric field look like below the plane?

"A sheet of charge" is too theoretical for me. What's an actual example of this in nature?

Page 3: Your Questions - UMD Department of Physics - UMD …physics.umd.edu/courses/Phys132/spring2014/LecturesB/B...• We ignore the electrostatic potential energies of all other pairs (since

Electrostatic Potential

3/6/2014 3 Physics 131

Page 4: Your Questions - UMD Department of Physics - UMD …physics.umd.edu/courses/Phys132/spring2014/LecturesB/B...• We ignore the electrostatic potential energies of all other pairs (since

Foothold ideas:Electrostatic potential energy and potential

• The potential energy between two charges is

• The potential energy ofmany charges is

• The potential energy added by adding a test charge q is

2/22/13 4 Physics 132

Potentials

Page 5: Your Questions - UMD Department of Physics - UMD …physics.umd.edu/courses/Phys132/spring2014/LecturesB/B...• We ignore the electrostatic potential energies of all other pairs (since

Forces and Fields

1

Nelec C iq

i iq

k qQUr=

∆ =∑elecqU

Vq

∆=

qFE

q=

rr

Potential Energy and Potential

�⃗�𝐹𝑞𝑞 = �𝑖𝑖=1

𝑁𝑁𝑘𝑘𝐶𝐶𝑞𝑞𝑄𝑄𝑖𝑖𝑟𝑟𝑖𝑖𝑞𝑞2

�̂�𝑟𝑖𝑖𝑞𝑞𝐸𝐸 =

�⃗�𝐹𝑞𝑞𝑞𝑞

5

Page 6: Your Questions - UMD Department of Physics - UMD …physics.umd.edu/courses/Phys132/spring2014/LecturesB/B...• We ignore the electrostatic potential energies of all other pairs (since

Foothold ideas:Electrostatic Potential energy and Electrostatic Potential

• Again we focus our attention on a test charge!• Usual definition of “electrostatic potential energy”: How much

does the energy of our system change if we add the test charge

• We ignore the electrostatic potential energies of all other pairs (since we assume the other charges do not move)

• We can pull the test charge magnitude out of the equation and obtain en electrostatic potential

2/15/13 6 Physics 132

It’s really a change in potential energy!

Page 7: Your Questions - UMD Department of Physics - UMD …physics.umd.edu/courses/Phys132/spring2014/LecturesB/B...• We ignore the electrostatic potential energies of all other pairs (since

Positive test charge with positive source

Potential energy of a positive test chargenear a positive source.

Electric Potentialof a positive test chargenear a positive source.

Page 8: Your Questions - UMD Department of Physics - UMD …physics.umd.edu/courses/Phys132/spring2014/LecturesB/B...• We ignore the electrostatic potential energies of all other pairs (since

What happens when I change the sign of the test charge?A. Potential energy graph

changesB. Electrostatic potential

graph changesC. Both changeD. Neither of the graphs

changes

1/23/13 8Physics 132Potentia

l energ

y grap

h chan

ges

Electr

ostatic

potentia

l graph...

Both change

Neither o

f the gr

aphs chan

ges

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Page 9: Your Questions - UMD Department of Physics - UMD …physics.umd.edu/courses/Phys132/spring2014/LecturesB/B...• We ignore the electrostatic potential energies of all other pairs (since

Negative test chargePotential energy of a negative test chargenear a positive source.

Electric Potentialof a negative test chargenear a positive source.

Page 10: Your Questions - UMD Department of Physics - UMD …physics.umd.edu/courses/Phys132/spring2014/LecturesB/B...• We ignore the electrostatic potential energies of all other pairs (since

Two test charges are brought separately into the vicinity of a charge +Q. First, test charge +q is brought to point A a distance r from +Q. Next, +q is removed and a test charge +2q is brought to point B a distance 2r from +Q. Compared with the electrostatic potential energy of the charge at A, that of the charge at B is

A. greaterB. smallerC. the sameD. You can’t tell from the

information given

1/23/13 10Physics 132

greate

r

smalle

r

the same

You can’t t

ell fro

m the i

nfor...

25% 25%25%25%

Page 11: Your Questions - UMD Department of Physics - UMD …physics.umd.edu/courses/Phys132/spring2014/LecturesB/B...• We ignore the electrostatic potential energies of all other pairs (since

Two test charges are brought separately into the vicinity of a charge +Q. First, test charge +q is brought to point A a distance r from +Q. Next, +q is removed and a test charge +2q is brought to point B a distance 2r from +Q. Compared with the electrostatic potential of the charge at A, that of the charge at B is

A. greaterB. smallerC. the sameD. You can’t tell from the

information given

1/23/13 11Physics 132

greate

r

smalle

r

the same

You can’t t

ell fro

m the i

nfor...

25% 25%25%25%

Page 12: Your Questions - UMD Department of Physics - UMD …physics.umd.edu/courses/Phys132/spring2014/LecturesB/B...• We ignore the electrostatic potential energies of all other pairs (since

Your QuestionsWhere does π come from? kc is actually a combination of fundamental constants

𝑘𝑘𝐶𝐶 =1

4𝜋𝜋𝜖𝜖0π comes from spherical symmetry

Where does the ½ come from? From the relationship between electric potential and electric potential energy and capacitance:

𝑑𝑑𝑑𝑑 = 𝑑𝑑𝑞𝑞𝑑𝑑 = 𝑑𝑑𝑞𝑞𝑞𝑞𝐶𝐶

→ �0

𝑈𝑈𝑑𝑑𝑑𝑑 =

1𝐶𝐶�0

𝑄𝑄𝑞𝑞𝑑𝑑𝑞𝑞 → 𝑑𝑑 =

12𝑄𝑄2

𝐶𝐶=

12𝐶𝐶𝑑𝑑2 =

12𝑄𝑄𝑑𝑑

What are some examples of capacitors in biology?

Page 13: Your Questions - UMD Department of Physics - UMD …physics.umd.edu/courses/Phys132/spring2014/LecturesB/B...• We ignore the electrostatic potential energies of all other pairs (since

A massive object might be placed at one of three spots in a region where there is a uniform gravitational field. How do the gravitational potentials, V = gh, on the masses at positions 1, 2, and 3 compare?

A. V is greatest at 1B. V is greatest at 2C. V is greatest at 3D. V = 0 at all three spotsE. V ≠ 0 but same at all

three spotsF. Not enough information

1/23/13 13Physics 132

Page 14: Your Questions - UMD Department of Physics - UMD …physics.umd.edu/courses/Phys132/spring2014/LecturesB/B...• We ignore the electrostatic potential energies of all other pairs (since

A positive charge might be placed at one of three spots in a region. It feels the same force (pointing to the left) in each of the spots. How does the electric potential, Velec, on the charge at positions 1, 2, and 3 compare?A. V is greatest at 1B. V is greatest at 2C. V is greatest at 3D. V = 0 at all three spotsE. V ≠ 0 but same at all

three spotsF. Not enough information

1/23/13 14Physics 132

Page 15: Your Questions - UMD Department of Physics - UMD …physics.umd.edu/courses/Phys132/spring2014/LecturesB/B...• We ignore the electrostatic potential energies of all other pairs (since

Graphical representations of the Electric Field and Potential

3/6/2014 15 Physics 131

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E field

3/6/2014Physics

13216

Page 17: Your Questions - UMD Department of Physics - UMD …physics.umd.edu/courses/Phys132/spring2014/LecturesB/B...• We ignore the electrostatic potential energies of all other pairs (since

At which point is the force downhill strongest?

A. AB. BC. CD. none

A B Cnone

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A

B

C

Topography map = gravitational PE graph (2D)

Page 18: Your Questions - UMD Department of Physics - UMD …physics.umd.edu/courses/Phys132/spring2014/LecturesB/B...• We ignore the electrostatic potential energies of all other pairs (since

At which point is the force downhill pointing to the east? (North is up)

A. AB. BC. CD. none

A B Cnone

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A

B

C

Topography map = gravitational PE graph (2D)

Page 19: Your Questions - UMD Department of Physics - UMD …physics.umd.edu/courses/Phys132/spring2014/LecturesB/B...• We ignore the electrostatic potential energies of all other pairs (since

V

3/4/2014Physics

13219

Page 20: Your Questions - UMD Department of Physics - UMD …physics.umd.edu/courses/Phys132/spring2014/LecturesB/B...• We ignore the electrostatic potential energies of all other pairs (since

Model of PE for 2 line charges(3D)

Page 21: Your Questions - UMD Department of Physics - UMD …physics.umd.edu/courses/Phys132/spring2014/LecturesB/B...• We ignore the electrostatic potential energies of all other pairs (since

Where would a test charge feel the strongest electric force?

A. AB. BC. CD. A&B

A B CA&B

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Model of PE for 2 line charges

Page 22: Your Questions - UMD Department of Physics - UMD …physics.umd.edu/courses/Phys132/spring2014/LecturesB/B...• We ignore the electrostatic potential energies of all other pairs (since

Where would a test charge feel the strongest electric force?

A. AB. BC. CD. A&B

A B CA&B

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Model of PE for 2 line charges

Page 23: Your Questions - UMD Department of Physics - UMD …physics.umd.edu/courses/Phys132/spring2014/LecturesB/B...• We ignore the electrostatic potential energies of all other pairs (since

Where would a test charge feel the strongest electric field?

A. AB. BC. CD. A&B

A B CA&B

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Model of PE for 2 line charges

Page 24: Your Questions - UMD Department of Physics - UMD …physics.umd.edu/courses/Phys132/spring2014/LecturesB/B...• We ignore the electrostatic potential energies of all other pairs (since

Where would a test charge feel the largest potential energy?

A. AB. BC. CD. A&BE. Depends on whether

the test charge is positive or negative

A B CA&B

Depends on w

hether

the test

ch...

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Model of PE for 2 line charges

Page 25: Your Questions - UMD Department of Physics - UMD …physics.umd.edu/courses/Phys132/spring2014/LecturesB/B...• We ignore the electrostatic potential energies of all other pairs (since

Where would a test charge feel the strongest electric force?

A. AB. BC. CD. DE. EF. More than one

A B C D E

More th

an one

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Map of electric PE for 3 charges (water molecule) (3D)

Page 26: Your Questions - UMD Department of Physics - UMD …physics.umd.edu/courses/Phys132/spring2014/LecturesB/B...• We ignore the electrostatic potential energies of all other pairs (since

26 Physics 132

The sheet of charge

• Field is constant, pointing away from positive sheet, towards negative sheet.

• Constant!!?How can that be?

Page 27: Your Questions - UMD Department of Physics - UMD …physics.umd.edu/courses/Phys132/spring2014/LecturesB/B...• We ignore the electrostatic potential energies of all other pairs (since

27 Physics 132

Two sheets of charge

Page 28: Your Questions - UMD Department of Physics - UMD …physics.umd.edu/courses/Phys132/spring2014/LecturesB/B...• We ignore the electrostatic potential energies of all other pairs (since

28 Physics 132

Two sheets of charge

Page 29: Your Questions - UMD Department of Physics - UMD …physics.umd.edu/courses/Phys132/spring2014/LecturesB/B...• We ignore the electrostatic potential energies of all other pairs (since

2/22/13 29 Physics 132

Result

The fields of the two plates canceleach other on the outside.

The fields of the two plates canceleach other on the outside.

The fields of the two plates addon the inside, producing double the field of asingle plate.

Page 30: Your Questions - UMD Department of Physics - UMD …physics.umd.edu/courses/Phys132/spring2014/LecturesB/B...• We ignore the electrostatic potential energies of all other pairs (since

Capacitance and Capacitors

The figure shows a capacitor just after it has been connected to a battery.

Current will flow in this manner for a nanosecond or so until the capacitor is fully charged.

Page 31: Your Questions - UMD Department of Physics - UMD …physics.umd.edu/courses/Phys132/spring2014/LecturesB/B...• We ignore the electrostatic potential energies of all other pairs (since

The figure shows a fully charged capacitor.

Now the system is in electrostatic equilibrium.

Capacitance always refers to the charge per voltage on a fully charged capacitor.

Capacitance and Capacitors

Page 32: Your Questions - UMD Department of Physics - UMD …physics.umd.edu/courses/Phys132/spring2014/LecturesB/B...• We ignore the electrostatic potential energies of all other pairs (since

The ratio of the charge Q to the potential difference ∆VC is called the capacitance C:

Capacitance is a purely geometric property of two electrodes because it depends only on their surface area and spacing.

The SI unit of capacitance is the farad:

The charge on the capacitor plates is directly proportional to the potential difference between the plates:

Capacitance and Capacitors

𝐴𝐴4𝜋𝜋𝑘𝑘𝐶𝐶𝑑𝑑

Page 33: Your Questions - UMD Department of Physics - UMD …physics.umd.edu/courses/Phys132/spring2014/LecturesB/B...• We ignore the electrostatic potential energies of all other pairs (since

What is the capacitance of these two electrodes?

A. 8 nFB. 4 nFC. 2 nFD. 1 nFE. Some other value

8 nF4 nF

2 nF1 nF

Some oth

er va

lue

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Page 34: Your Questions - UMD Department of Physics - UMD …physics.umd.edu/courses/Phys132/spring2014/LecturesB/B...• We ignore the electrostatic potential energies of all other pairs (since

Capacitance and Capacitors

Capacitors are important elements in electric circuits. They come in a variety of sizes and shapes.

The keys on most computer keyboards are capacitor switches. Pressing the key pushes two capacitor plates closer together, increasing their capacitance.

Page 35: Your Questions - UMD Department of Physics - UMD …physics.umd.edu/courses/Phys132/spring2014/LecturesB/B...• We ignore the electrostatic potential energies of all other pairs (since

Example 29.6 Charging a Capacitor

𝐴𝐴 = 4𝜋𝜋𝑘𝑘𝐶𝐶𝑑𝑑𝐶𝐶

Whiteboard, TA & LA

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Forming a Capacitor

Consequently, the capacitance depends only on the geometry of the electrodes.

The figure shows two arbitrary electrodes charged to ±Q.

It might appear that the capacitance depends on the amount of charge, but the potential difference is proportional to Q.

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The Energy Stored in a Capacitor

The total energy transferred from the battery to the capacitor is:

The figure shows a capacitor being charged.

As a small charge dq is lifted to a higher potential, the potential energy of the capacitor increases by:

Page 38: Your Questions - UMD Department of Physics - UMD …physics.umd.edu/courses/Phys132/spring2014/LecturesB/B...• We ignore the electrostatic potential energies of all other pairs (since

Capacitors are important elements in electric circuits because of their ability to store energy.

The charge on the two plates is ±q and this charge separation establishes a potential difference ∆V = q/Cbetween the two electrodes.

In terms of the capacitor’s potential difference, the potential energy stored in a capacitor is:

The Energy Stored in a Capacitor

Page 39: Your Questions - UMD Department of Physics - UMD …physics.umd.edu/courses/Phys132/spring2014/LecturesB/B...• We ignore the electrostatic potential energies of all other pairs (since

A capacitor can be charged slowly but then can release the energy very quickly. An important medical

application of capacitors is the defibrillator.

A heart attack or a serious injury can cause the heart to enter a state known as fibrillation in which the heart muscles twitch randomly and cannot pump blood.

A strong electric shock through the chest completely stops the heart, giving the cells that control the heart’s rhythm a chance to restore the proper heartbeat.

The Energy Stored in a Capacitor

Page 40: Your Questions - UMD Department of Physics - UMD …physics.umd.edu/courses/Phys132/spring2014/LecturesB/B...• We ignore the electrostatic potential energies of all other pairs (since

A capacitor charged to 1.5 V stores 2.0 mJ of energy. If the capacitor is charged to 3.0 V, it will store

A. 1.0 mJB. 2.0 mJC. 4.0 mJD. 6.0 mJE. 8.0 mJ

1.0 mJ

2.0 mJ

4.0 mJ

6.0 mJ

8.0 mJ

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