Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

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Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin

Transcript of Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Page 1: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Lesson 17

Electric Fields and Potential

Eleanor Roosevelt High School

Chin-Sung Lin

Page 2: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Electric Fields

Page 3: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Law of Universal Gravitation

Coulomb’s Law

Gravitational & Electric Forces

What are the formulas for the following physics laws?

Page 4: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Gravitational & Electric Forces

Fg = G m1 m2

r2

Law of Universal Gravitation

Coulomb’s Law

Fe = k q1 q2

r2

Page 5: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Gravitational Field What’s the definition of gravitational field?

Page 6: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Gravitational Field

• Fg: gravitational force (N)

• m: mass (kg)

• g: gravitational field strength (N/kg, or m/s2)

g = Fg

m

Gravitational Field: Force per unit mass

Page 7: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Electric Field

• Fe: electric force (N)

• q: charge (C)

• E: electric field strength (N/C)

E = Fe

q

Electric Field: Force per unit charge

Page 8: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Gravitational & Electric Fields

E = Fe

q

Electric Field

g = Fg

m

Gravitational Field

Page 9: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Electric Field

Source Charge

+q+QFe

Fe

qE =

Test Charge

r

Page 10: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Electric Field

Source Charge

Fe

qE =

Test Charge

+q–Q Fer

Page 11: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Electric Field Electric field is a vector

A vector includes ___________ and ____________

Source Charge

Test Charge

+q+QFe

r Fe

qE =

+q–Q Fer

Page 12: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Electric Field Electric field is a vector

A vector includes direction and magnitude

Source Charge

Test Charge

+q+QFe

r Fe

qE =

+q–Q Fer

Page 13: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Electric Field

E = Fe

q

Can you apply Coulomb’s law to this formula and then simplify it?

Source Charge

+q+QFe

Test Charge

r

= ???

Page 14: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Electric Field

• Fe: electric force (N)

• q: test charge (C)

• Q: source charge (C)

• E: electric field strength (N/C)

• r: distance between charges (m)

• k: electrostatic constant (N m2/C2)

Electric Field: Force per unit charge

E = Fe

q= k

q Q

r2 q= k

Q

r2

Page 15: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Electric Field Example

What is the magnitude of the electric field strength when an electron experiences a 5.0N force?

Page 16: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Electric Field Example

E = Fe / q

E = 5 N / (1.6 x 10-19 C)

= 3.13 x 1019 N/C

What is the magnitude of the electric field strength when an electron experiences a 5.0N force?

Page 17: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Electric Field Example

What are the magnitude and direction of the electric field 1.5 m away from a positive charge of 2.1*10-9 C?

Page 18: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Electric Field Example

What are the magnitude and direction of the electric field 1.5 m away from a positive charge of 2.1*10-9 C?

E = k Q / r2

E = (8.99 x 109 N m2/C2) (2.1 x 10-9 C) / (1.5 m)2

= 8.4 N/C

Direction: away from the positive charge

Page 19: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Electric Field Exercise

There is a negative charged particle of 0.32 C in the free space. (a) What are the magnitude and direction of the electric field 2.0 m away from the particle? (b) What are the magnitude and direction of the electric force when an electron is placed 2.0 m away from this particle?

[3 minutes] e –– 0.32 C2.0 m

Page 20: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Electric Field Exercise

There is a negative charged particle of 0.32 C in the free space. (a) What are the magnitude and direction of the electric field 2.0 m away from the particle?

E = k Q / r2

E = (8.99 x 109 N m2/C2) (0.32 C) / (2.0 m)2

= 7.2 x 108 N/C

Direction: toward the negative charge

Page 21: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Electric Field Exercise

There is a negative charged particle of 0.32 C in the free space. (b) What are the magnitude and direction of the electric force when an electron is placed 2.0 m away from this particle? E = Fe / q Fe = q E

Fe = (1.6 x 10-19 C) (7.2 x 108 N/C)

= 1.15 x 10-10 N

Page 22: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Aim: Electric Field

DoNow: (4 minutes)

Write down the definition of Electric Field in words

Write down the formulas of Electric Field in two different forms

Define every symbol in the formula and identify their units

Identify the relationships between Electric Field and other variables

Page 23: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Aim: Electric Field

Page 24: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Electric Field

• Fe: electric force (N)

• q: test charge (C)

• Q: source charge (C)

• E: electric field strength (N/C)

• r: distance between charges (m)

• k: electrostatic constant (N m2/C2)

Electric Field: Force per unit charge

E = Fe

q= k

Q

r2

Page 25: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Electric Field

• Fe: electric force (N)

• q: test charge (C)

• Q: source charge (C)

• E: electric field strength (N/C)

• r: distance between charges (m)

• k: electrostatic constant (N m2/C2)

Electric Field: Force per unit charge

E ~ Fe E ~ 1r2

E ~ Q 1qE ~

Page 26: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Electric Field

Source Charge

+q+QFe

Fe

qE =

Test Charge

If you shift the test charge around, where can you find the electric field with the same magnitude?

Page 27: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Electric Field

Source Charge

+q+QFe

Test Charge

Fe

Fe

Fe

E

E

E

E

Page 28: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Electric Field

Source Charge

Test Charge

+q+QFe

Fe

Fe

Fe

E

E

E

E

What will happen if you move the test charges away from the source charge?

Page 29: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Electric Field

Source Charge

+q+QFe

Test Charge

Fe

Fe

Fe

E

E

E

E

Page 30: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Electric Field

Fe

Fe

Source Charge

+q+QFe

Test Charge

Fe

Fe

E

E

E

E

Fe

Fe

Fe

E

E

E

E

Page 31: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Electric Field

Source Charge

+q+QFe

Test Charge

Fe

Fe

Fe

E

E

E

E

Fe

Fe

Fe

Fe

E

E

E

E

Test Charge

+q

Page 32: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Vector representation

-+

Electric Field Representation

Page 33: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Line-of-Force representation

-+

Electric Field Representation

Page 34: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Electric Field Representation

-+

How do you decide the strength of electric field?

Page 35: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Electric Field Representation

-+

When the field lines are denser, the field is stronger

Page 36: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Electric Field Representation Where can you find the the strongest

electric field?

A

B

C

D

E

Page 37: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Electric Field: Point Charge

Line-of-Force representation

-+

Page 38: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Electric Field: Pair of Charges

Line-of-Force representation

Page 39: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Electric Field: Pair of Charges

Sketch the electric field for like charges?

++

Page 40: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Electric Field: Pair of Charges

Line-of-Force representation

++

Page 41: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Electric Field: Pair of Charges

Line-of-Force representation

Page 42: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Electric Field: Parallel Plates

Line-of-Force representation

Page 43: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Electric Field: Parallel Plates

Anything special for the electric field between the parallel plates charged with opposite charges?

Page 44: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Electric Field: Parallel Plates

The electric field between the parallel plates is uniform except at both ends

Page 45: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Electric Field Example

A charged droplet of mass 5.87 x 10-10 kg is hovering motionless between two parallel plates. The parallel plates have a electric field of 1.2 x 107 N/C and are 2.00 mm apart. (a) What is the charge on the particle? (b) By how many electrons is the particle deficient?

Page 46: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Electric Field Example

A charged droplet of mass 5.87 x 10-10 kg is hovering motionless between two parallel plates. The parallel plates have a electric field of 1.2 x 107 N/C and are 2.00 mm apart. (a) What is the charge on the particle? E = Fe / q Fe = E q Fg = m g Fe = Fg

E q = m g

(1.2 x 107 N/C) q = (5.87 x 10-10 kg) (9.81 m/s2)

q = 4.80 x 10-16 C

Page 47: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Electric Field Example

A charged droplet of mass 5.87 x 10-10 kg is hovering motionless between two parallel plates. The parallel plates have a electric field of 1.2 x 107 N/C and are 2.00 mm apart. (b) By how many electrons is the particle deficient?e - = 1.6 x 10-19 C

number of e - = 4.80 x 10-16 C / 1.6 x 10-19 C = 3000 e –

Page 48: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Electric Field Exercise

A charged droplet of mass 5.87 x 10-10 kg is hovering motionless between two parallel plates. The parallel plates have a electric field of 9.6 x 106 N/C and are 2.00 mm apart. What is the charge on the particle?

Page 49: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Electric Field Exercise

A charged droplet of mass 5.87 x 10-10 kg is hovering motionless between two parallel plates. The parallel plates have a electric field of 9.6 x 106 N/C and are 2.00 mm apart. What is the charge on the particle? E = Fe / q Fe = E q Fg = m g Fe = Fg

E q = m g

(9.6 x 106 N/C) q = (5.87 x 10-10 kg) (9.81 m/s2)

q = 6.0 x 10-16 C

Page 50: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Electric Field Exercise

A positively charged ball with mass 20 g is hanging between two charged parallel plates from the ceiling through an insulating wire with length 0.1 m. The electric field strength of the charged parallel plates is 4.2 x 109 N/C. When the ball is in balance, the wire and the vertical line form an angle of 60o. What is the charge of the ball?

Page 51: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Electric Fields

Page 52: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Electric Fields

Page 53: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Electric Fields

Page 54: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Electric Fields

Page 55: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Electric Fields

Page 56: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Electric Fields and Shielding

E = 0Electric Shielding

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Electric Fields and Shielding

Cancellation of electric force

The electric forces of area A and area B on P completely cancel out

A BP

Page 58: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Electric Potential

Page 59: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Aim: Electric PotentialDoNow: (3 minutes)

Write down the formulas of Electric Field

Draw the electric field surrounding a pair of opposite charge

Draw the electric field surrounding a pair of charged parallel plates

Page 60: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Aim: Electric Potential

Page 61: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Electric Field

• Fe: electric force (N)

• q: test charge (C)

• Q: source charge (C)

• E: electric field strength (N/C)

• r: distance between charges (m)

• k: electrostatic constant (N m2/C2)

Electric Field: Force per unit charge

E = Fe

q= k

Q

r2

Page 62: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Electric Field: Pair of Charges

Line-of-Force representation

Page 63: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Electric Field: Parallel Plates

Line-of-Force representation

Page 64: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Gravitational Potential Energy (GPE)

Page 65: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Gravitational Potential Energy (GPE)

What happens in the picture?

What types of energy have been converted?

Page 66: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Gravitational Potential Energy (GPE)

What happens in the picture?

What types of energy have been converted?

If we want to pull the weight up back to its original position, what should we do?

Page 67: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Gravitational Potential Energy (GPE)

What happens in the picture?

What types of energy have been converted?

If we want to pull the weight up back to its original position, what should we do?

How much work do we need?

Page 68: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Electric Potential Energy (EPE)

++

++

-----

What are they in common?

Page 69: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Electric Potential Energy (EPE)

++

++

-----

What happens in the picture?

What types of energy have been converted?

If we want to pull the weight up back to its original position, what should we do?

How much work do we need?

Page 70: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Electric Potential Energy (EPE)

++

++

-----

What are they different?

Page 71: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Electric Potential Energy

What did the monkey do in order to bring a positively charged ball toward a

positively charged object?

Page 72: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Electric Potential Energy

What did the monkey do in order to bring a positively charged ball toward a

positively charged object?

When the ball was released, what happened to the ball? Why?

Page 73: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Gravitational Potential Energy

The work performed in taking a mass from height A to height B does not depend on the path

B

A A

Page 74: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Electric Potential Energy

B

A

The work performed in taking a charge from A to B does not depend on the path

Page 75: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Gravitational Potential Energy

x2

What happens when we double the mass?

Page 76: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Gravitational Potential Energy

x2

When mass is doubled, the gravitational potential energy is also doubled

PE2 = (2m)gh = 2(mgh) = 2PE1

Page 77: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Electric Potential Energy

++

++

---

x2

What did we double here?

Page 78: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Electric Potential Energy

++

++

---

x2

We doubled the charge.

What happens when we double the charge?

Page 79: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Electric Potential Energy

++

++

---

x2

When charge is doubled, the electric potential energy is also doubled

Page 80: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Electric Potential Energy

• W: electric (potential) energy aka work (J)

W is a scalar (not a vector)

W or EPE

Potential Energy – Capability to Do Work

Page 81: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Electric Potential Energy

• W: electric (potential) energy aka work (J)

W or EPE

Potential Energy – Capability to Do Work

W ~ q

Page 82: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Electric Potential

• W: electric (potential) energy, aka work (J)

• V: electric potential, aka potential difference,

aka voltage (V, Volts)

• q: charge (C)

V = Wq

Electric potential energy per unit charge

Page 83: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Electric Potential

Electric potential (V) is based on a zero reference point

Only the potential difference matters Electric potential (Voltage, V) is the work

(W) required to bring a unit charge (1 C) from the zero reference point

V is a scalar (not a vector)

W = qV

Page 84: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Electric Potential Example

How much work is required to move 3.0 C of positive charge from the negative terminal of a 12-volt battery to the positive terminal?

Page 85: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Electric Potential Example

How much work is required to move 3.0 C of positive charge from the negative terminal of a 12-volt battery to the positive terminal?

V = W / q W = q V

W = (3.0 C) (12.0 V) = 36.0 J

Page 86: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Electric Potential Example

If an electron loses 1.4 x 10-15 J of energy in traveling from the cathode to the screen of a computer monitor, across what potential difference must it travel?

Page 87: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Electric Potential Example

If an electron loses 1.4 x 10-15 J of energy in traveling from the cathode to the screen of a computer monitor, across what potential difference must it travel?

V = W / q W = q V

V = (1.4 x 10-15 J) / (1.6 x 10-19 C) = 8750 V

Page 88: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Electric Potential Example

Can you make up a question using the definition of electric potential?

Page 89: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Electric Potential Example

Page 90: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Electric Potential: Parallel Plates

What is special about the electric field between the charged parallel plates?

Page 91: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Electric Potential: Parallel Plates

Electric Field (E): is uniform due to uniform density of the electric field lines

E E E

Page 92: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Electric Potential: Parallel Plates

If we place test charge at different locations between the charged parallel plates, compare the forces experienced by these test charges

E E E

Page 93: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Electric Potential: Parallel Plates

Electric Force (Fe): experienced by a test charge is constant due to Fe = qE

E E E

Fe

FeFe

Page 94: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Electric Potential: Parallel Plates

Compare the work required to move test charges from the negative plate to the positive plate

E E EFe dFeFe

Page 95: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Electric Potential: Parallel Plates

Electric potential energy / work (W): required to move a test charge from negative plate to positive plate is constant due to W = Fe d

E E EFe dFe Fe

Page 96: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Electric Potential: Parallel Plates

V = Wq

Given the following formulas, can you derive the formula for Electric potential (V) and Electric field (E)?

W = Fe d

Fe = q E

Page 97: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Electric Potential: Parallel Plates

V = Wq

Electric potential (V):

W = Fe d and Fe = q E

W = q E d

V = E d or

= q E dq = E d

E = Vd

Page 98: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Electric Potential: Parallel Plates

Electric potential (V): relative to the negative plate is proportional to the distance to it due to V = E d

E E E

dV

Page 99: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Equipotential Lines: Parallel Plates

Equipotential Lines: on an equipotential line, voltages are all the same

Equipotential lines are perpendicular to field lines

E E E

d1

V1V1V1

V2V2V2

d2

Page 100: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Equipotential Lines: Point Charge

Equipotential Lines for a point charge:

Page 101: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Equipotential Lines: Point Charge

Equipotential Lines for a charge pair

Page 102: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Electric Field and Potential

• E: electric field (N/C or V/m)• V: electric potential / potential difference /

voltage (V, Volts)• d: distance between parallel plates (m)• q: charge (C)

Electric field

E = Vd =

Fe

q

Page 103: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

Electric Potential Example

A charged droplet of mass 5.87x 10-10 kg is hovering motionless between two parallel plates. The parallel plates have a potential difference of 24000 V and are 2.00 mm apart. What is the charge on the particle?

Page 104: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

A charged droplet of mass 5.87x 10-10 kg is hovering motionless between two parallel plates. The parallel plates have a potential difference of 24000 V and are 2.00 mm apart. What is the charge on the particle?

E = Fe / q Fe = E q Fg = m g Fe = Fg

E q = m g E = V / d V q / d = m g

(24000 V) q / ((0.002 m) = (5.87 x 10-10 kg) (9.81 m/s2)

q = 4.80 x 10-16 C

Electric Potential Example

Page 105: Lesson 17 Electric Fields and Potential Eleanor Roosevelt High School Chin-Sung Lin.

The End