preview statics circuits electricity and magnetism chapter 16 section 1 electric charge

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Preview Statics Circuits Electricity and Magnetism Chapter 16 Section 1 Electric Charge

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• Statics

• Circuits

• Electricity and Magnetism

Chapter 16 Section 1 Electric Charge

Section 1 Electric ChargeChapter 16

Objectives

• Understand the basic properties of electric charge.

• Differentiate between conductors and insulators.

• Distinguish between charging by contact, charging by induction, and charging by polarization.

Chapter 16 Section 1 Electric Charge

Properties of Electric Charge

• There are two kinds of electric charge.– like charges repel– unlike charges attract

• Electric charge is conserved.– Positively charged particles are called protons.– Uncharged particles are called neutrons.– Negatively charged particles are called electrons.

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Visual Concept

Chapter 16 Section 1 Electric Charge

Electric Charge

Chapter 16 Section 1 Electric Charge

Properties of Electric Charge, continued

• Electric charge is quantized. That is, when an object is charged, its charge is always a multiple of a fundamental unit of charge.

• Charge is measured in coulombs (C).

• The fundamental unit of charge, e, is the magnitude of the charge of a single electron or proton.

e = 1.602 176 x 10–19 C

Chapter 16

The Milikan Experiment

Section 1 Electric Charge

Chapter 16 Section 1 Electric Charge

Transfer of Electric Charge, continued

• Insulators and conductors can be charged by contact.

• Conductors can be charged by induction.

• Induction is a process of charging a conductor by bringing it near another charged object and grounding the conductor.

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Visual Concepts

Visual Concept

Chapter 16

Charging by Induction

Chapter 16 Section 1 Electric Charge

Transfer of Electric Charge, continued

• A surface charge can be induced on insulators by polarization.

• With polarization, the charges within individual molecules are realigned such that the molecule has a slight charge separation.

Section 2 Electric ForceChapter 16

Objectives

• Calculate electric force using Coulomb’s law.

• Compare electric force with gravitational force.

• Apply the superposition principle to find the resultant force on a charge and to find the position at which the net force on a charge is zero.

Chapter 16

Coulomb’s Law

• Two charges near one another exert a force on one another called the electric force.

• Coulomb’s law states that the electric force is propor-tional to the magnitude of each charge and inversely proportional to the square of the distance between them.

Section 2 Electric Force

1 22

2

charge 1 charge 2electric force = Coulomb constant

distance

electric C

q qF k

r

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Visual Concept

Chapter 16 Section 2 Electric Force

Superposition Principle

Coulomb’s Law, continued

• The Coulomb force is a field force.

• A field force is a force that is exerted by one object on another even though there is no physical contact between the two objects.

Chapter 16 Section 2 Electric Force

Chapter 16 Section 3 The Electric Field

Electric Field Strength

• An electric field is a region where an electric force on a test charge can be detected.

• The SI units of the electric field, E, are newtons per coulomb (N/C).

• The direction of the electric field vector, E, is in the direction of the electric force that would be exerted on a small positive test charge.

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Visual Concept

Chapter 16 Section 3 The Electric Field

Electric Fields and Test Charges

Chapter 16 Section 3 The Electric Field

Electric Field Strength, continued

• Electric field strength depends on charge and distance. An electric field exists in the region around a charged object.

• Electric Field Strength Due to a Point Charge

2

2

charge producing the fieldelectric field strength = Coulomb constant

distance

C

qE k

r

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Visual Concept

Chapter 16 Section 3 The Electric Field

Calculating Net Electric Field

Chapter 16 Section 3 The Electric Field

Electric Field Lines

• The number of electric field lines is proportional to the electric field strength.

• Electric field lines are tangent to the electric field vector at any point.

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Visual Concept

Chapter 16 Section 3 The Electric Field

Rules for Drawing Electric Field Lines

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Visual Concept

Chapter 16 Section 3 The Electric Field

Rules for Sketching Fields Created by Several Charges

Section 1 Electric PotentialChapter 17

Electrical Potential Energy

• Electrical potential energy is potential energy associated with a charge due to its position in an electric field.

• Electrical potential energy is a component of mechanical energy.

ME = KE + PEgrav + PEelastic + PEelectric

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Visual Concept

Chapter 17 Section 1 Electric Potential

Electrical Potential Energy

Section 1 Electric PotentialChapter 17

Potential Difference

• Electric Potential equals the work that must be performed against electric forces to move a charge from a reference point to the point in question, divided by the charge.

• The electric potential associated with a charge is the electric energy divided by the charge:

V

PEelectric

q

Section 1 Electric PotentialChapter 17

Potential Difference, continued

• Potential Difference equals the work that must be performed against electric forces to move a charge between the two points in question, divided by the charge.

• Potential difference is a change in electric potential.

change in electric potential energy

potential differenceelectric charge

electricPEV

q

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Visual Concept

Chapter 17 Section 1 Electric Potential

Potential Difference

Section 1 Electric PotentialChapter 17

Potential Difference, continued

• The potential difference in a uniform field varies with the displacement from a reference point.

• Potential Difference in a Uniform Electric Field

∆V = –Ed

potential difference = –(magnitude of the electric field displacement)

Section 2 CapacitanceChapter 17

Capacitors and Charge Storage

• A capacitor is a device that is used to store electrical potential energy.

• Capacitance is the ability of a conductor to store energy in the form of electrically separated charges.

• The SI units for capacitance is the farad, F, which equals a coulomb per volt (C/V)

Section 2 CapacitanceChapter 17

Capacitors and Charge Storage, continued

• Capacitance is the ratio of charge to potential difference.

magnitude of charge on each platecapacitance =

potential difference

QC

V

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Visual Concept

Chapter 17 Section 2 Capacitance

Capacitance

Section 2 CapacitanceChapter 17

Capacitors and Charge Storage, continued

• Capacitance depends on the size and shape of a capacitor.

• Capacitance for a Parallel-Plate Capacitor in a Vacuum

–12 2

0

0

area of one of the platescapacitance = permittivity of a vacuum

distance between the plates

of the medium 8.85 10 C /N mpermittivity

AC

d

Chapter 17

Capacitors in Keyboards

Section 2 Capacitance

Click below to watch the Visual Concept.

Visual Concept

Chapter 17 Section 2 Capacitance

Parallel-Plate Capacitor