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It’s what we see… Circuits

Circuits

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Circuits. It’s what we see…. Simple Circuits. A basic circuit contains 3 parts : A source of electric potential ( voltage ) gives charge an electric potential ex. battery, solar panel. Simple Circuits. A resistance load uses up energ y 3 ways: converts to - PowerPoint PPT Presentation

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Page 1: Circuits

It’s what we see…Circuits

Page 2: Circuits

Simple Circuits•A basic circuit contains 3 parts:

① A source of electric potential (voltage)

•gives charge an electric potential•ex. battery, solar panel

Page 3: Circuits

Simple Circuits② A resistance load• uses up energy•3 ways: converts to• light (ex. lightbulb)•heat (toaster)•motion (motor)

Page 4: Circuits

Simple Circuitsmost loads do more than one

•ex. lightbulbs also give off heat•ex. toaster wires glow (light)

Page 5: Circuits

Simple Circuits③ Conductors• provides path for

flow between source and load

•ex. wire

Page 6: Circuits

Resistance

•All materials give some resistance to flow of charge•exception. superconductors•Materials with high resistance• insulators•ex. rubber, plastic•Materials with low resistance•conductors•ex. metals

Page 7: Circuits

ResistanceAmount of resistance depends on:•material•length of wire•thickness of wire (cross-sectional area)•imagine a straw•easier to blow through:•shorter• thicker

Page 8: Circuits

Calculating Resistance

•R•L•A•ρ

R = ρ LA

º resistance (Ω = Ohm) º length of wire (m)º cross sectional area of wire (m2)º resistivity (depends on material Ω•m)

Page 9: Circuits

Calculating Resistance

R = ρ LA

semiconductor

Page 10: Circuits

ExampleHow much resistance is in the graphite of a 20. cm long pencil if the graphite has a diameter of 4.0 mm?Given:

L = 20cm

Want:

R€

D = 4.0mm

A = πr2 = (3.14)(.0020m)2 =1.26 ×10−5 m2

1m100 cm( ) = 0.20m

1m1,000 mm( ) = .0040m

ρ =1×10−4 Ω ⋅m (from table)

Page 11: Circuits

Example

solve for R

R = ρ LA

R = (1×10−4 Ω ⋅ / m ) .20 / m 1.26 ×10−5 / m 2 ⎛ ⎝ ⎜

⎞ ⎠ ⎟

R = 1.59Ω

Page 12: Circuits

Current

rate of electric flow (of charge)

current = chargetime

⇒ I = qt

•q• t• I

º charge (C) º time (s)º current (A)

1 Ampere (A) = 1Coulombsecond

Page 13: Circuits

Current Flow•Conventional Current is the direction positive charges move

•Actual electron flow is the other way!

Page 14: Circuits

Ohm’s Law• Current depends on two things:

1. the potential difference, V

2. the resistance, R

Together, they make Ohm’s Law:€

I ∝ V

I = VR

also, V = IR

or R = VI

I ∝ 1R

Page 15: Circuits

Ohm’s LawWater Circuit AnalogyPotential Difference•amount of water (pressure)

Page 16: Circuits

Ohm’s LawWater Circuit Analogy

Switch• turns flow on and off

Page 17: Circuits

Ohm’s LawWater Circuit Analogy

Resistance• thickness & length of hose

Page 18: Circuits

Ohm’s LawWater Circuit Analogy

Current• rate of flow

Page 19: Circuits

Electric Shocks•1 mA •10 mA •100 mA

= pain= release current= death

Page 20: Circuits

Inside a Lightbulb•Each wire of filament goes to a different part•This allows for the current to flow through

Page 21: Circuits

Power and Energy

•Power = rate of energy useage•P = Energy/timeNew unit Watts

1Watt (W ) = 1Joulesecond

volt (V ) = JouleCoulomb

current (I) = Coulombsecond

and

VI = J/ C ⎛ ⎝ ⎜

⎞ ⎠ ⎟

/ C s ⎛ ⎝ ⎜

⎞ ⎠ ⎟= J

s

P = VIso,

Page 22: Circuits

Combining Equations

P = VI

⇒ P = V VR ⎛ ⎝ ⎜

⎞ ⎠ ⎟

⇒ P = V 2

R

P = VI

⇒ P = (IR)I

⇒ P = I2R

twinkle, twinkle…

Page 23: Circuits
Page 24: Circuits

Power and Energy

Energy Equations

E = Pt or E = VIt

E = Pt

⇒ E = V 2

Rt

⇒ E = I2Rt

Page 25: Circuits

Units and Variables

Variable UnitqtVRIEP

coulombs (C)seconds (s)

volts (V)ohms (Ω)

amperes (A)joules (J)Watts (W)

Page 26: Circuits

ExampleIn 3.0 minutes an electric pot delivers 48,000 J of energy to the water inside it. The coffee pot is connected to a standard 120-volt source. What is the resistance of the coffee pot?Given:

t = 3min

Want:

R€

E = 48,000J

V = 120V€

60 sec1min( ) = 180 s

Page 27: Circuits

Example

pick an equation

E = V 2

Rt

R = (120V )2

(48,000 J)180 s

R = 54Ω€

⇒ R = V 2

Et

Page 28: Circuits

Example1 kW-hr costs $.50:Let’s find the cost of running a 60 W lightbulb for 24 hours

Given:

t = 24 hr

Want:

cost€

P = 60W

3,600 sec1hr( ) = 86,400 s

Problem: what is a kW-hr?

Page 29: Circuits

Example Let’s take a close look at the kilowatt-hour:

1kW− hr

1,000W1 / k / W ( )

3,600 sec1 / h r( ) = 3.6 ×106 W ⋅ s

• kW = P•hr = t• Pt = E• kW-hr is a unit of energy

=3.6 ×106 J/ s / s = 3.6 ×106 J

Page 30: Circuits

Example1 kW-hr costs $.50:Let’s find the cost of running a 60 W lightbulb for 24 hours

• Let’s solve for energy

1kW − hr = 3.6 ×106 J

E = Pt

E = (60W )(86,400 s)

E = 5,184,000J

1kW − hr3.6 ×106 J ⎛ ⎝ ⎜

⎞ ⎠ ⎟=

1.44 kW− hr

Page 31: Circuits

Example1 kW-hr costs $.50:Let’s find the cost of running a 60 W lightbulb for 24 hours

1.44 kW− hr

$.501kW − hr

⎛ ⎝ ⎜

⎞ ⎠ ⎟= .$72

Page 32: Circuits

Time to Practice

go to pg. 260

Page 33: Circuits

Measuring Resistance

•Symbol• Isolate from circuit•Place leads on each side• Ohmmeter

Page 34: Circuits

Measuring Voltage

•Symbol•Voltage source must be connected to circuit•Place leads on each side• Voltmeter

Page 35: Circuits

Measuring Current

•Need to break open circuit•Force current through meter• ammeter

Page 36: Circuits

Electrical Circuits Lab

Time for lab!Go to page 264

Page 37: Circuits

Series CircuitLet’s start with Current• In order for all of the current to make it around the loop, they all have to flow at the same rate!

So,

IT

=I1

=I2

=I3

Page 38: Circuits

Series CircuitResistance•The current is forced to pass through each resistor.

So,

RT

=R1 + R2 + R3

Page 39: Circuits

Series CircuitVoltage•The voltage drops a constant amount•The voltage drops are spread out proportionately between each resistor so they add up to the total

So,

VT

=V1 + V2 + V3

Page 40: Circuits

Parallel CircuitLet’s start with Voltage• Imagine parallel as separate serial circuits connected•Circuit 1•Circuit 2•Circuit 3•Each uses the whole voltageSo,

VT

=V1

=V2

=V3

Page 41: Circuits

Parallel CircuitCurrent•The total flow is split into each branch-off loop

So,

IT

=I1 + I2 + I3

Page 42: Circuits

Parallel CircuitResistance• Let’s start with the current

•now substitute I=V/R

• since VT = V1 = V2 = V3€

IT = I1 + I2 + I3

VT

RT

= V1

R1

+ V2

R2

+ V3

R3

VRT

= VR1

+ VR2

+ VR3

Page 43: Circuits

Parallel Circuit

Resistance•Now divide each side by V

1RT

= 1R1

+ 1R2

+ 1R3

Page 44: Circuits

Parallel CircuitLooks weird you say?• let’s try an example:• Find total resistance if a 100 Ω, 200 Ω and a 300 Ω

resistor are all in parallel.

1RT

= 1R1

+ 1R2

+ 1R3

1RT

= 1100Ω

+ 1200Ω

+ 1300Ω

1RT

= 6600Ω

+ 3600Ω

+ 2600Ω

Page 45: Circuits

Parallel CircuitLooks weird you say?• let’s try an example:• Find total resistance if a 100 Ω, 200 Ω and a 300 Ω

resistor are all in parallel.

=11

600Ω

1RT

= 6600Ω

+ 3600Ω

+ 2600Ω

RT = 600Ω11

= 55Ω

Page 46: Circuits