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Physics 2102 Physics 2102 Lecture 04: FRI 23 JAN Lecture 04: FRI 23 JAN Electric Charge I Electric Charge I Physics 2113 Jonathan Dowling Charles-Augustin de Coulomb (1736–1806) Version: 03/25/22 Benjamin Franklin (1705–1790)
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Physics 2102 Lecture 04: FRI 23 JAN Electric Charge I Physics 2113 Jonathan Dowling Charles-Augustin de Coulomb (1736–1806) Version: 10/7/2015 Benjamin.

Dec 30, 2015

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Page 1: Physics 2102 Lecture 04: FRI 23 JAN Electric Charge I Physics 2113 Jonathan Dowling Charles-Augustin de Coulomb (1736–1806) Version: 10/7/2015 Benjamin.

Physics 2102 Physics 2102 Lecture 04: FRI 23 JANLecture 04: FRI 23 JAN

Electric Charge IElectric Charge I

Physics 2113

Jonathan Dowling

Charles-Augustin de Coulomb

(1736–1806)Version: 04/19/23

Benjamin Franklin (1705–1790)

Page 2: Physics 2102 Lecture 04: FRI 23 JAN Electric Charge I Physics 2113 Jonathan Dowling Charles-Augustin de Coulomb (1736–1806) Version: 10/7/2015 Benjamin.

LetLet’’s Get Started!s Get Started!Electric Charges…Electric Charges…

• Two Types of Charges: Positive/Negative• Like Charges Repel• Opposite Charges Attract

Atomic StructureAtomic Structure: • Negative Electron Cloud• Nucleus of Positive Protons, Uncharged Neutrons The Unit of Electric Charge isthe “Coulomb” which is “C”.Proton Charge: e = 1.60 × 10–19 C

Page 3: Physics 2102 Lecture 04: FRI 23 JAN Electric Charge I Physics 2113 Jonathan Dowling Charles-Augustin de Coulomb (1736–1806) Version: 10/7/2015 Benjamin.

Benjamin Franklin (1705–1790)

Rules of Electric Attraction and Repulsion Rules of Electric Attraction and Repulsion Discovered by Benjamin Franklin:Discovered by Benjamin Franklin:

Electrical Insulators Electrical Insulators

Page 4: Physics 2102 Lecture 04: FRI 23 JAN Electric Charge I Physics 2113 Jonathan Dowling Charles-Augustin de Coulomb (1736–1806) Version: 10/7/2015 Benjamin.

Benjamin Franklin (1705–1790)

Rules of Electric Attraction and Repulsion Rules of Electric Attraction and Repulsion Discovered by Benjamin Franklin:Discovered by Benjamin Franklin:

Electric ConductorsElectric Conductors

Page 5: Physics 2102 Lecture 04: FRI 23 JAN Electric Charge I Physics 2113 Jonathan Dowling Charles-Augustin de Coulomb (1736–1806) Version: 10/7/2015 Benjamin.

Benjamin Franklin (1705–1790)

Rules of Electric Attraction and Repulsion: ICPPRules of Electric Attraction and Repulsion: ICPP

C and D attract

B and D attract

Page 6: Physics 2102 Lecture 04: FRI 23 JAN Electric Charge I Physics 2113 Jonathan Dowling Charles-Augustin de Coulomb (1736–1806) Version: 10/7/2015 Benjamin.

Force Between Pairs of Point Force Between Pairs of Point Charges: CoulombCharges: Coulomb’’s Laws Law

Coulomb’s Law — the Force Between Point Charges:

• Lies Along the Line Connecting the Charges.

• Is Proportional to the Product of the Magnitudes.

• Is Inversely Proportional to the Distance Squared.

• Note That Newton’s Third Law Says |F12| = |F21|!!

Charles-Augustin De Coulomb (1736–1806)

Page 7: Physics 2102 Lecture 04: FRI 23 JAN Electric Charge I Physics 2113 Jonathan Dowling Charles-Augustin de Coulomb (1736–1806) Version: 10/7/2015 Benjamin.

Force Between Pairs of Point Charges: ICPPForce Between Pairs of Point Charges: ICPP

(a)

(c)

(b)

Page 8: Physics 2102 Lecture 04: FRI 23 JAN Electric Charge I Physics 2113 Jonathan Dowling Charles-Augustin de Coulomb (1736–1806) Version: 10/7/2015 Benjamin.

CoulombCoulomb’’s Laws Law

The “k” is the electric constant of proportionality.

Usually, we write:

Units: F = [N] = [Newton]; r = [m] = [meter]; q = [C] = [Coulomb]

Page 9: Physics 2102 Lecture 04: FRI 23 JAN Electric Charge I Physics 2113 Jonathan Dowling Charles-Augustin de Coulomb (1736–1806) Version: 10/7/2015 Benjamin.

Coulomb’s Law: ICCPCoulomb’s Law: ICCP

(a)a > c > b (b) less

Page 10: Physics 2102 Lecture 04: FRI 23 JAN Electric Charge I Physics 2113 Jonathan Dowling Charles-Augustin de Coulomb (1736–1806) Version: 10/7/2015 Benjamin.

Coulomb’s Torsion Balance Experiment For Electric Coulomb’s Torsion Balance Experiment For Electric Force Identical to Cavendish’s Experiment For Force Identical to Cavendish’s Experiment For

Gravitational Force!Gravitational Force!

The experiment measures “k” the electric constant of proportionality and confirms inverse square law.

http://www.dnatube.com/video/11874/Application-Of-Coulombs-Torsion-Balance

Page 11: Physics 2102 Lecture 04: FRI 23 JAN Electric Charge I Physics 2113 Jonathan Dowling Charles-Augustin de Coulomb (1736–1806) Version: 10/7/2015 Benjamin.

Two Inverse Square LawsTwo Inverse Square Laws

Newton’s Law of Gravitational Force Coulomb’s Law of

Electrical Force

Area of Sphere = 4πr2

Number of Lines of Force is Constant.

Hence #Force Lines Per-Unit-Area is Proportional to 1/r2

Page 12: Physics 2102 Lecture 04: FRI 23 JAN Electric Charge I Physics 2113 Jonathan Dowling Charles-Augustin de Coulomb (1736–1806) Version: 10/7/2015 Benjamin.

SuperpositionSuperposition

• Question: How Do We Figure Out the Force

on a Point Charge Due to Many Other Point

Charges?

• Answer: Consider One Pair at a Time,

Calculate the Force (a Vector!) In Each Case

Using Coulomb’s Law and Finally Add All the

Vectors! (“Superposition”)

• Useful To Look Out for SYMMETRY to

Simplify Calculations!

Page 13: Physics 2102 Lecture 04: FRI 23 JAN Electric Charge I Physics 2113 Jonathan Dowling Charles-Augustin de Coulomb (1736–1806) Version: 10/7/2015 Benjamin.

Feel the Force! Feel the Force! ExampleExample

• Three Equal Charges Form

an Equilateral Triangle of

Side 1.5 m as Shown

• Compute the Force on q1

• ICPP: What are the Forces

on the Other Charges?

d

q1

d

dq2

q3

q1= q2= q3= 20 mCd = 1.0 cm

Solution: Set up a Coordinate System, Compute Vector Sum of F12 and F13

d

1

2

3

d

d

y

x

θ

Page 14: Physics 2102 Lecture 04: FRI 23 JAN Electric Charge I Physics 2113 Jonathan Dowling Charles-Augustin de Coulomb (1736–1806) Version: 10/7/2015 Benjamin.

Feel the Force! Feel the Force! ExampleExample

q1= q2= q3= 20 mCd = 1.0 cm

d

1

2

3

d

d

y

x

θ

ICPP: What are the magnitudes and directions of the forces on 2 and 3?

Page 15: Physics 2102 Lecture 04: FRI 23 JAN Electric Charge I Physics 2113 Jonathan Dowling Charles-Augustin de Coulomb (1736–1806) Version: 10/7/2015 Benjamin.

What is the Force on Central Particle?

Charge +qPlaced at Center

Another Example With Another Example With SymmetrySymmetry

+q

r

All Forces Cancel Except From +2q!

F

Page 16: Physics 2102 Lecture 04: FRI 23 JAN Electric Charge I Physics 2113 Jonathan Dowling Charles-Augustin de Coulomb (1736–1806) Version: 10/7/2015 Benjamin.