chapter 32 electrostatics. electric charge and electric field static electricity – unmoving charge...

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Chapter 32 Electrostatics

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Page 1: Chapter 32 Electrostatics. Electric Charge and Electric Field Static Electricity – Unmoving charge Two types Positive – lack of electrons Negative – excess

Chapter 32

Electrostatics

Page 2: Chapter 32 Electrostatics. Electric Charge and Electric Field Static Electricity – Unmoving charge Two types Positive – lack of electrons Negative – excess

Electric Charge and Electric Field

Static Electricity – Unmoving charge Two types

Positive – lack of electrons Negative – excess electrons

Like charges - Repel Opposite Charges - Attract

Page 3: Chapter 32 Electrostatics. Electric Charge and Electric Field Static Electricity – Unmoving charge Two types Positive – lack of electrons Negative – excess

Electric Charges

Charge can be induced by rubbing an object – View demonstrations

Charge is detected using an electroscope.

Charge can travel via a conductor. Poor conductors are insulators.

Page 4: Chapter 32 Electrostatics. Electric Charge and Electric Field Static Electricity – Unmoving charge Two types Positive – lack of electrons Negative – excess

Force Exerted by Charges

Coulomb’s Law F = kQ1Q2/r2

k = 9 x 109 N•m2/C2

Positive solution – repulsion Negative solution - attraction

Page 5: Chapter 32 Electrostatics. Electric Charge and Electric Field Static Electricity – Unmoving charge Two types Positive – lack of electrons Negative – excess

Sample Problem

Two charges, Q1 = +10 µC, and Q2 = -15 µC, are separated by 1.5 meters.

What is the electrostatic force acting between them?

SolutionF = kQ1Q2/r2 =

(9 x 109 N•m2/C2)(+10 x 10-6 C)(-15 x 10-6 C)/(1.5 m)2

= -0.6 N

Page 6: Chapter 32 Electrostatics. Electric Charge and Electric Field Static Electricity – Unmoving charge Two types Positive – lack of electrons Negative – excess

Conductors and Insulators

A good conductor transfers charge easily.

A good insulator inhibits the transfer of charge.

A good conductor is a poor insulator and a good insulator is a poor conductor.

Page 7: Chapter 32 Electrostatics. Electric Charge and Electric Field Static Electricity – Unmoving charge Two types Positive – lack of electrons Negative – excess

Creation of Static Charges

Two ways to create a static charge are: Charging by contact (friction) – when

electrons are transferred from one object to another by touching.

Induction – when a charge is transferred by bringing one object near another without actually touching

Page 8: Chapter 32 Electrostatics. Electric Charge and Electric Field Static Electricity – Unmoving charge Two types Positive – lack of electrons Negative – excess

Chapter 33

Electric Fields and Potential

Page 9: Chapter 32 Electrostatics. Electric Charge and Electric Field Static Electricity – Unmoving charge Two types Positive – lack of electrons Negative – excess

Electric Field

Field – Affect that acts at a distance, without contact Examples

Electric Field Gravitational Field

Electric Field Strength – E = F/q = kQ/r2

Page 10: Chapter 32 Electrostatics. Electric Charge and Electric Field Static Electricity – Unmoving charge Two types Positive – lack of electrons Negative – excess
Page 11: Chapter 32 Electrostatics. Electric Charge and Electric Field Static Electricity – Unmoving charge Two types Positive – lack of electrons Negative – excess

Sample Problem

Calculate the strength of an electric field at a point 30 cm

from a point charge Q = +3 µC

SolutionE = kQ/r2 =

(9 x 109 N•m2/C2)(+3 x 10-6 C)/(0.3 m)2

= 300000 N/C

Page 12: Chapter 32 Electrostatics. Electric Charge and Electric Field Static Electricity – Unmoving charge Two types Positive – lack of electrons Negative – excess

Electrical Energy Electrical Energy is generated from other

forms of energy and transmitted over power lines and/or stored in batteries

Vocabulary Voltage (V)

Force in an electrical system; Volt = Work/Charge = W/q = Joule/Coloumb

Current (I) Rate in an electrical system = Charge/time = q/t

=Coloumb/sec = 1 Ampere

Page 13: Chapter 32 Electrostatics. Electric Charge and Electric Field Static Electricity – Unmoving charge Two types Positive – lack of electrons Negative – excess

Energy in Electrical System

Volts =Work/charge = V =W/q Work is measured in joules (the same

as energy) Charge is measured in Coloumbs (C) The charge on an electron is 1.6 x 10-

19 C 1 V = 1 Joule/1 Coloumb

Work = Volts * Charge = Vq

Page 14: Chapter 32 Electrostatics. Electric Charge and Electric Field Static Electricity – Unmoving charge Two types Positive – lack of electrons Negative – excess

Sample Problem

How much work is needed to move a 10 μC charge to a point where the potential is 70 V?

W = Vq = (70 V)(10 x 10-6 C) = 7 x 10-4 J

Page 15: Chapter 32 Electrostatics. Electric Charge and Electric Field Static Electricity – Unmoving charge Two types Positive – lack of electrons Negative – excess

Electrical Energy Storage Electrical Energy can be stored in two

ways: Batteries

Long term storage, even flow of charge Storage ability measured in Volts

Capacitors Short term storage, releases charge all at once (boost

in charge) Storage capacity measured in Farads (F) 1 Farad = 1 Coloumb/Volt Mathematically Charge = Capacitance * Voltage = q

= CV

Page 16: Chapter 32 Electrostatics. Electric Charge and Electric Field Static Electricity – Unmoving charge Two types Positive – lack of electrons Negative – excess

Chapter 34

Electric Current

Page 17: Chapter 32 Electrostatics. Electric Charge and Electric Field Static Electricity – Unmoving charge Two types Positive – lack of electrons Negative – excess

Electric Current

Circuit – A continuous path connected between the terminals of a power source.

Current – Flow of Charge I = ΔQ/Δt Current is measured in

Coloumbs/Sec which is called an Ampere.

Page 18: Chapter 32 Electrostatics. Electric Charge and Electric Field Static Electricity – Unmoving charge Two types Positive – lack of electrons Negative – excess

Electric Current

Electron Flow is from – terminal to + terminal.

Conventional Current is from + terminal to – terminal.

Page 19: Chapter 32 Electrostatics. Electric Charge and Electric Field Static Electricity – Unmoving charge Two types Positive – lack of electrons Negative – excess

Sample Problem

A steady current of 2.5 Amps passes through a wire for 4 minutes. How much charge passed through any point in

the circuit?Solution

Q = IΔt (2.5 C/s)(240 s) = 600 C

Page 20: Chapter 32 Electrostatics. Electric Charge and Electric Field Static Electricity – Unmoving charge Two types Positive – lack of electrons Negative – excess

Ohm’s Law

Resistance – how much the conductor slows down the flow of electrons through it.

Resistance is measured in Ohms (Ω)

Ohm’s law -In any Circuit:V = IR or R = V/I

Page 21: Chapter 32 Electrostatics. Electric Charge and Electric Field Static Electricity – Unmoving charge Two types Positive – lack of electrons Negative – excess

Sample Problem

A small flashlight bulb draws a current of 300 mA from a 1.5 V battery. What is the resistance

of the bulb?SolutionR = V/I =

(1.5 V)/(0.3 A) = 5 Ω

Page 22: Chapter 32 Electrostatics. Electric Charge and Electric Field Static Electricity – Unmoving charge Two types Positive – lack of electrons Negative – excess

Resistor Color Code Resistors are banded in order to

describe the amount of resistance they provide. Each resistor is banded with 4 stripes.

Band Represents

1 First Digit

2 Second Digit

3 Multiplier

4 Tolerance

Page 23: Chapter 32 Electrostatics. Electric Charge and Electric Field Static Electricity – Unmoving charge Two types Positive – lack of electrons Negative – excess

Bright Black 0

Boys Brown 1

Remember Red 2

Our Orange 3

Young Yellow 4

Girls Green 5

Become Blue 6

Very Violet 7

Good Grey 8

Wives White 9

Gold 5%

Silver 10%

None 20%

Resistor Color Code

Page 24: Chapter 32 Electrostatics. Electric Charge and Electric Field Static Electricity – Unmoving charge Two types Positive – lack of electrons Negative – excess

Sample Problem

Calculate the resistance of a resistor which is banded with the

following colors: Red, Green, Blue, Silver.Solution

Red = 2, Green = 5, Blue = 6 and Silver = 10% R = 25000000 ± 10%

OrR = 25 MΩ ± 10%

Page 25: Chapter 32 Electrostatics. Electric Charge and Electric Field Static Electricity – Unmoving charge Two types Positive – lack of electrons Negative – excess

Electrical Power

Electrical Power is measured in Watts.

Power = current x voltageP = IV or P = I2R or P = V2/R

Since Energy is Power x Time electrical energy is often measured in Kilowatt•hours or power x time.

Page 26: Chapter 32 Electrostatics. Electric Charge and Electric Field Static Electricity – Unmoving charge Two types Positive – lack of electrons Negative – excess

Chapter 35

DC Circuits

Page 27: Chapter 32 Electrostatics. Electric Charge and Electric Field Static Electricity – Unmoving charge Two types Positive – lack of electrons Negative – excess

DC Circuits Batteries Connected in Series

Increase Voltage Et= E1 + E2 + E3. . .

Produce the Same Current It= I1 = I2 = I3. . .

Batteries Connected in Parallel Produce the Same Voltage

Et= E1 = E2 = E3. . . Increase Current

It= I1 + I2 + I3. . .

Page 28: Chapter 32 Electrostatics. Electric Charge and Electric Field Static Electricity – Unmoving charge Two types Positive – lack of electrons Negative – excess

Sample Problem

Calculate the voltage and current when 3 batteries (1.5 V, 0.25 A are connected in

A) SeriesB) Parallel

Solutiona) Et= E1 + E2 + E3 =1.5 V + 1.5 V + 1.5 V = 4.5 V

It= I1 + I2 + I3= 0.25 A

b) Et= E1 = E2 = E3=1.5 V

It= I1 + I2 + I3=0.25 A + 0.25 A + 0.25 A = 0.75 A

Page 29: Chapter 32 Electrostatics. Electric Charge and Electric Field Static Electricity – Unmoving charge Two types Positive – lack of electrons Negative – excess

DC Circuits

Resistance in SeriesRt=R1+R2+R3. . .

Resistance in Parallel

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Page 30: Chapter 32 Electrostatics. Electric Charge and Electric Field Static Electricity – Unmoving charge Two types Positive – lack of electrons Negative – excess

Sample Problem

Calculate the resistance when a 5 Ω, 6 Ω, and 3 Ω resistor are connected in

A) SeriesB) Parallel

Solution

a) Rt=R1+R2+R3 = 5 Ω+ 6 Ω+ 3 Ω = 14 Ωb)

Rt= 1.43 Ω

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321 RRRRt