Electric Circuits LCHS Physics Mark Ewoldsen, Ph.D.

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Electric Electric Circuits Circuits LCHS Physics LCHS Physics Mark Ewoldsen, Ph.D. Mark Ewoldsen, Ph.D.

Transcript of Electric Circuits LCHS Physics Mark Ewoldsen, Ph.D.

Page 1: Electric Circuits LCHS Physics Mark Ewoldsen, Ph.D.

Electric CircuitsElectric CircuitsLCHS PhysicsLCHS Physics

Mark Ewoldsen, Ph.D.Mark Ewoldsen, Ph.D.

Page 2: Electric Circuits LCHS Physics Mark Ewoldsen, Ph.D.

DefinitionsDefinitions

• VoltageVoltage: Electric Potential or Potential : Electric Potential or Potential Difference (Energy added or used)Difference (Energy added or used)– V (volts) = Joules/Coulomb V (volts) = Joules/Coulomb

– One volt = one coulomb of charge gains One volt = one coulomb of charge gains or loses one joule of energyor loses one joule of energy

Page 3: Electric Circuits LCHS Physics Mark Ewoldsen, Ph.D.

What is the difference between E and V?What is the difference between E and V?

• E is the voltage supplied by a batteryE is the voltage supplied by a battery

• V is the voltage measured across a resistorV is the voltage measured across a resistor

Page 4: Electric Circuits LCHS Physics Mark Ewoldsen, Ph.D.

BatteriesBatteries• Positive and Negative terminals Positive and Negative terminals

– electrons leave negative terminalelectrons leave negative terminal

• Batteries use a chemical reaction to create Batteries use a chemical reaction to create voltagevoltage

• Construction: Two different metals and AcidConstruction: Two different metals and Acid– e.g. Copper, Zinc, and Citrus Acide.g. Copper, Zinc, and Citrus Acid

– e.g. Lead, Lead Oxide, Sulfuric Acide.g. Lead, Lead Oxide, Sulfuric Acid

– e.g. Nickel, Cadmium, Acid Pastee.g. Nickel, Cadmium, Acid Paste

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CapacitorsCapacitors• Both batteries and capacitors store electrical Both batteries and capacitors store electrical

energyenergy

• The difference between a capacitor and a battery The difference between a capacitor and a battery is that a capacitor can dump its entire charge in a is that a capacitor can dump its entire charge in a tiny fraction of a second, where a battery would tiny fraction of a second, where a battery would take minutes to completely discharge itselftake minutes to completely discharge itself – Sometimes, capacitors are used to store charge for Sometimes, capacitors are used to store charge for

high-speed use. high-speed use. • a camera flash or a TVa camera flash or a TV

Page 6: Electric Circuits LCHS Physics Mark Ewoldsen, Ph.D.

capacitorcapacitor

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DefinitionsDefinitions

• CurrentCurrent: Flow of electric charge: Flow of electric charge– I (amps) = Q/t = Coulombs/secondI (amps) = Q/t = Coulombs/second

– Higher current increases heat due to more Higher current increases heat due to more collisions of ‘free’ electrons with atomscollisions of ‘free’ electrons with atoms

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Effect of Currents on the BodyEffect of Currents on the Body

• 0.001 A can be felt0.001 A can be felt

• 0.005 A is painful0.005 A is painful

• 0.010 A0.010 A causes involuntary muscle causes involuntary muscle contractionscontractions

• 0.015 A causes loss of muscle control0.015 A causes loss of muscle control

• 0.070 A can be fatal if the current last for more 0.070 A can be fatal if the current last for more than 1 second than 1 second

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Speed of Electrons in CircuitSpeed of Electrons in Circuit

• Light goes on ‘instantly’ when switch turned onLight goes on ‘instantly’ when switch turned on– Electrons do not move at speed of lightElectrons do not move at speed of light

• c = 3 x 10c = 3 x 108 8

• Electrons – 6 x 10Electrons – 6 x 1055 m/s in random directions m/s in random directions

– Signal (energy) moves at speed of light due to electric Signal (energy) moves at speed of light due to electric energy fieldenergy field

• Wire acts as pipe to guide electric fieldWire acts as pipe to guide electric field

• Electrons in circuit do not come from battery but Electrons in circuit do not come from battery but are from the wireare from the wire

Page 10: Electric Circuits LCHS Physics Mark Ewoldsen, Ph.D.

DefinitionsDefinitions• ResistanceResistance: : measure of a material’s ability measure of a material’s ability

to resist the flow of of electronsto resist the flow of of electrons– ΩΩ (ohms) = J-s/C (ohms) = J-s/C22

– Conductor – low resistanceConductor – low resistance• materials with free electronsmaterials with free electrons• e.g. copper, aluminum, gold, most metalse.g. copper, aluminum, gold, most metals

– Insulator – high resistanceInsulator – high resistance• materials with no free electronsmaterials with no free electrons• e.g. glass, plastics, ceramics, woode.g. glass, plastics, ceramics, wood

Page 11: Electric Circuits LCHS Physics Mark Ewoldsen, Ph.D.

DefinitionsDefinitions• ResistanceResistance

– Increases with length Increases with length – L– L – Decreases with cross area Decreases with cross area – A – A – ResistivityResistivity – – ρρ

• material material dependentdependent • temperature dependenttemperature dependent

R = R = ρLρL AA

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DefinitionsDefinitions

• PowerPower is the rate energy is converted is the rate energy is converted into another forminto another form– Resistors transform electrical energy into Resistors transform electrical energy into

light, mechanical or heat energylight, mechanical or heat energy

• Equation for Power:Equation for Power:P = I V P = I V

(Watts) – Joules/second(Watts) – Joules/second

Page 13: Electric Circuits LCHS Physics Mark Ewoldsen, Ph.D.

DefinitionsDefinitions

AAmmeterAmmeter: measures amp(ere)s: measures amp(ere)s

BatteryBattery: Source of energy: Source of energy

ResistorResistor: Removes energy: Removes energy

VVoltmeterVoltmeter: measures volt(age): measures volt(age)

WiresWires::

Page 14: Electric Circuits LCHS Physics Mark Ewoldsen, Ph.D.

Ohm’s Law:Ohm’s Law:V = I RV = I R

V = voltage, I = current, R = resistanceV = voltage, I = current, R = resistance

For a given voltage, as the resistance goes up, For a given voltage, as the resistance goes up, the current will go downthe current will go down

OR

If the resistance is less, the current is moreIf the resistance is less, the current is more

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Ohm’s LawOhm’s Law

V

A

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Ohm’s LawOhm’s Law

V

A

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Constant VoltageConstant Voltage• For a given pressure on a car’s acceleratorFor a given pressure on a car’s accelerator

– Voltage or energy inputVoltage or energy input

• By increasing the steepness of a hillBy increasing the steepness of a hill– Changing resistanceChanging resistance

• The car’s speed will go downThe car’s speed will go down– Decrease the current or ampsDecrease the current or amps

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Turned on

When light is first turned onWhen light is first turned on• Filament is coldFilament is cold

– The resistance is low andThe resistance is low and– since V = IR, current is highsince V = IR, current is high

• High current means filament is more likely High current means filament is more likely to burn outto burn out

Page 20: Electric Circuits LCHS Physics Mark Ewoldsen, Ph.D.

Ohm’s Law:Ohm’s Law:V/I = RV/I = R

V = voltage, I = current, R = resistanceV = voltage, I = current, R = resistance

For a given resistance, as the voltage For a given resistance, as the voltage goes up, the current goes upgoes up, the current goes up

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Ohm’s Law – Set ResistanceOhm’s Law – Set Resistance

A

V

A

V

A

V

A

V

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http://www.physics.udel.edu/wwwusers/watson/scen103/98w/note0105.html

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Series CircuitSeries Circuit

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Finding V, I & R for a Finding V, I & R for a Series CircuitSeries Circuit

1.1. Determine total E (V from battery)Determine total E (V from battery)2.2. Find the total Resistance Find the total Resistance

RRT T = R= R11 + R + R2 2 + R+ R33 … …

3.3. Determine IDetermine ITT by by

I = VI = VTT/R/RTT

3.3. Since I is constant in a series circuit, find Since I is constant in a series circuit, find V (energy used) by each resistor using V (energy used) by each resistor using

V = IV = ITTRR

Page 25: Electric Circuits LCHS Physics Mark Ewoldsen, Ph.D.

Finding V, I & R for a Finding V, I & R for a Series CircuitSeries Circuit

1.1. Determine E (V from battery)Determine E (V from battery)

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12 V12 V

1 Ω2 Ω

3 Ω

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Finding V, I & R for a Finding V, I & R for a Series CircuitSeries Circuit

1.1. Determine E (V from battery)Determine E (V from battery) - 12V- 12V2.2. Find the total ResistanceFind the total Resistance

RRT T = R= R11 + R + R2 2 + R+ R33 … …

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12 V

1 1 ΩΩ2 2 ΩΩ

3 3 ΩΩ

6 6 ΩΩ = = 3 3 ΩΩ + + 2 2 ΩΩ + + 1 1 ΩΩ

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Finding V, I & R for a Finding V, I & R for a Series CircuitSeries Circuit

1.1. Determine E (V from battery)Determine E (V from battery) - 12V- 12V

2.2. Find the total Resistance - Find the total Resistance - 6 6 ΩΩ

Page 30: Electric Circuits LCHS Physics Mark Ewoldsen, Ph.D.

Finding V, I & R for a Finding V, I & R for a Series CircuitSeries Circuit

1.1. Determine E (V from battery)Determine E (V from battery) - 12V- 12V

2.2. Find the total Resistance Find the total Resistance - - 6 6 ΩΩ

3.3. Determine IDetermine ITT by I by ITT = V = VTT/R/RTT

2 A2 A = 12 V/ 6 = 12 V/ 6 ΩΩ

Page 31: Electric Circuits LCHS Physics Mark Ewoldsen, Ph.D.

Finding V, I & R for a Finding V, I & R for a Series CircuitSeries Circuit

1.1. Determine E (V from battery)Determine E (V from battery) - 12V- 12V

2.2. Find the total Resistance Find the total Resistance - - 6 6 ΩΩ

3.3. Determine that IDetermine that IT T = = 2 A2 A

4.4. Since I is constant in a series circuit, find Since I is constant in a series circuit, find V (energy used ) for each resistor using V (energy used ) for each resistor using V = IV = ITTRR

Page 32: Electric Circuits LCHS Physics Mark Ewoldsen, Ph.D.

12 V

1 Ω2 Ω

3 Ω

2V2V = 2A * 1 = 2A * 1ΩΩ4V4V = 2A * 2 = 2A * 2ΩΩ

6V6V = 2A * 3 = 2A * 3ΩΩ

1212V = V = 6V6V + + 4V4V + + 2V2V

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Series CircuitSeries Circuit• Current is the same at all points Current is the same at all points

I = II = I11 = I = I22 = I = I33 = I = I44

• Volt is divided among all the resistorVolt is divided among all the resistor

E = VE = V11 + V + V22 + V + V33

• Resistance accumulatesResistance accumulates

R = RR = R11 + R + R22 + R + R33

Page 34: Electric Circuits LCHS Physics Mark Ewoldsen, Ph.D.

Parallel CircuitParallel Circuit

Page 35: Electric Circuits LCHS Physics Mark Ewoldsen, Ph.D.

Finding V, I & R for a Finding V, I & R for a Parallel CircuitParallel Circuit

1.1. Determine EDetermine E2.2. Find the total Resistance Find the total Resistance

1/R1/RT T = 1/R= 1/R11 + 1/R + 1/R2 2 + 1/R+ 1/R33 … …

3.3. Determine IDetermine ITT leaving battery by leaving battery by

IITT = V = VTT/R/RTT

4.4. Since V is constant for each part of a parallel circuit, Since V is constant for each part of a parallel circuit, find I through each resistor using find I through each resistor using

I = V/RI = V/R

5.5. Check to verify that Kirchhoff’s Law is trueCheck to verify that Kirchhoff’s Law is true

Page 36: Electric Circuits LCHS Physics Mark Ewoldsen, Ph.D.

1 Ω

2 Ω

12 V

Page 37: Electric Circuits LCHS Physics Mark Ewoldsen, Ph.D.

Finding V, I & R for a Finding V, I & R for a Parallel CircuitParallel Circuit

1.1. Determine EDetermine E 12 V12 V

Page 38: Electric Circuits LCHS Physics Mark Ewoldsen, Ph.D.

Finding V, I & R for a Finding V, I & R for a Parallel CircuitParallel Circuit

1.1. Determine EDetermine E

2.2. Find the total Resistance Find the total Resistance

1/R1/RT T = 1/R= 1/R11 + 1/R + 1/R2 2 + 1/R+ 1/R33 … …

Page 39: Electric Circuits LCHS Physics Mark Ewoldsen, Ph.D.

1 Ω

2 Ω

1/R1/RT T = 1/1= 1/1ΩΩ + 1/2 + 1/2ΩΩ1/R1/RT T = 3/2= 3/2ΩΩ

12 V

RRT T = = 22ΩΩ/3/3

Page 40: Electric Circuits LCHS Physics Mark Ewoldsen, Ph.D.

Finding V, I & R for a Finding V, I & R for a Parallel CircuitParallel Circuit

1.1. Determine EDetermine E

2.2. Find the total Resistance Find the total Resistance

1/R1/RT T = 1/R= 1/R11 + 1/R + 1/R2 2 + 1/R+ 1/R33 … …

RRT T = 2= 2ΩΩ/3/3

Page 41: Electric Circuits LCHS Physics Mark Ewoldsen, Ph.D.

Finding V, I & R for a Finding V, I & R for a Parallel CircuitParallel Circuit

1.1. Determine EDetermine E

2.2. Find the total Resistance Find the total Resistance

1/R1/RT T = 1/R= 1/R11 + 1/R + 1/R2 2 + 1/R+ 1/R33 … …

3.3. Determine IDetermine IBB leaving battery by leaving battery by

IIBB = V = VBB/R/RTT

IIBB = 12V / 2 = 12V / 2ΩΩ/3 /3 oror 12V x 3/2 12V x 3/2ΩΩ

IIBB = 18A = 18A

Page 42: Electric Circuits LCHS Physics Mark Ewoldsen, Ph.D.

1 Ω

2 Ω

12 V

IIBB = 18A = 18A

Page 43: Electric Circuits LCHS Physics Mark Ewoldsen, Ph.D.

Finding V, I & R for a Finding V, I & R for a Parallel CircuitParallel Circuit

1.1. Determine EDetermine E

2.2. Find the total Resistance Find the total Resistance

1/R1/RT T = 1/R= 1/R11 + 1/R + 1/R2 2 + 1/R+ 1/R33 … …

3.3. Determine IDetermine ITT leaving battery by leaving battery by

IITT = V = VTT/R/RTT

4.4. Since V is constant for each part of a parallel Since V is constant for each part of a parallel circuit, find I through each resistor using circuit, find I through each resistor using

I = V/RI = V/R

Page 44: Electric Circuits LCHS Physics Mark Ewoldsen, Ph.D.

1 Ω

2 Ω

12 V

I = 12V / 1I = 12V / 1Ω = 12AΩ = 12A

I = 12V / 2I = 12V / 2Ω = 6AΩ = 6A

Page 45: Electric Circuits LCHS Physics Mark Ewoldsen, Ph.D.

Finding V, I & R for a Finding V, I & R for a Parallel CircuitParallel Circuit

1.1. Determine EDetermine E

2.2. Find the total Resistance Find the total Resistance

1/R1/RT T = 1/R= 1/R11 + 1/R + 1/R2 2 + 1/R+ 1/R33 … …

3.3. Determine IDetermine ITT leaving battery by leaving battery by

IITT = V = VTT/R/RTT

4.4. Since V is constant for each part of a parallel circuit, Since V is constant for each part of a parallel circuit, find I through each resistor using find I through each resistor using

I = V/RI = V/R

5.5. Check to verify that Kirchhoff’s Rule is trueCheck to verify that Kirchhoff’s Rule is true

Page 46: Electric Circuits LCHS Physics Mark Ewoldsen, Ph.D.

1 Ω

2 Ω

12 V

18A18A

12A12A

6A6A

18A18A

IIBB = 18A = 18A

Page 47: Electric Circuits LCHS Physics Mark Ewoldsen, Ph.D.

Parallel CircuitParallel Circuit

Volt is the same at all points Volt is the same at all points

E = VE = V11 = V = V22 = V = V33

ResistanceResistance 1 1 1 11 1 1 1--- = --- + --- + ------ = --- + --- + --- R RR R11 R R22 R R33

Current accumulatesCurrent accumulates

I = II = I11 + I + I22 + I + I33

Page 48: Electric Circuits LCHS Physics Mark Ewoldsen, Ph.D.

Complex CircuitsComplex Circuits

Page 49: Electric Circuits LCHS Physics Mark Ewoldsen, Ph.D.

2 Ω

12 V

2 Ω

2 Ω

Page 50: Electric Circuits LCHS Physics Mark Ewoldsen, Ph.D.

Finding V, I & R for a Finding V, I & R for a Complex CircuitComplex Circuit

1.1. Find the most complex portion of the Circuit – usually Find the most complex portion of the Circuit – usually part of the Parallelpart of the Parallel

2.2. Find the Total Resistance for that portionFind the Total Resistance for that portion3.3. Continue until the Total Resistance for the Circuit is Continue until the Total Resistance for the Circuit is

knownknown4.4. Starting with the least complex resistor, find the Starting with the least complex resistor, find the

voltage it usesvoltage it uses5.5. Continue until the parallel portion where the Continue until the parallel portion where the

remaining voltage will used on both sides will be remaining voltage will used on both sides will be identical, Find Iidentical, Find I

6.6. Make sure Kirchhoff's Rule is followedMake sure Kirchhoff's Rule is followed

Page 51: Electric Circuits LCHS Physics Mark Ewoldsen, Ph.D.

Finding V, I & R for a Finding V, I & R for a Complex CircuitComplex Circuit

1.1. Find the most complex portion of the Find the most complex portion of the Circuit – usually part of the ParallelCircuit – usually part of the Parallel

Page 52: Electric Circuits LCHS Physics Mark Ewoldsen, Ph.D.

2 2 ΩΩ

12 V

2 2 ΩΩ

2 Ω

Page 53: Electric Circuits LCHS Physics Mark Ewoldsen, Ph.D.

Finding V, I & R for a Finding V, I & R for a Complex CircuitComplex Circuit

1.1. Find the most complex portion of the Circuit – usually Find the most complex portion of the Circuit – usually part of the Parallelpart of the Parallel

2.2. Find the Total Resistance for that portionFind the Total Resistance for that portion

Page 54: Electric Circuits LCHS Physics Mark Ewoldsen, Ph.D.

12 V

2 2 ΩΩ

2 2 ΩΩ

2 Ω

1/R1/RT T = 1/2= 1/2ΩΩ + 1/2 + 1/2ΩΩ1/R1/RT T = 2/2= 2/2ΩΩ

RRT T = 1= 1ΩΩ

Page 55: Electric Circuits LCHS Physics Mark Ewoldsen, Ph.D.

Finding V, I & R for a Finding V, I & R for a Complex CircuitComplex Circuit

1.1. Find the most complex portion of the Circuit – usually Find the most complex portion of the Circuit – usually part of the Parallelpart of the Parallel

2.2. Find the Total Resistance for that portionFind the Total Resistance for that portion

3.3. Continue until the Total Resistance for the Continue until the Total Resistance for the Circuit is knownCircuit is known

Page 56: Electric Circuits LCHS Physics Mark Ewoldsen, Ph.D.

12 V

2 2 ΩΩ

2 2 ΩΩ

2 Ω

RRT T = 2= 2ΩΩ + 1 + 1ΩΩRRT T = 3= 3ΩΩ

Page 57: Electric Circuits LCHS Physics Mark Ewoldsen, Ph.D.

Finding V, I & R for a Finding V, I & R for a Complex CircuitComplex Circuit

1.1. Find the most complex portion of the Circuit – usually Find the most complex portion of the Circuit – usually part of the Parallelpart of the Parallel

2.2. Find the Total Resistance for that portionFind the Total Resistance for that portion

3.3. Continue until the Total Resistance for the Circuit is Continue until the Total Resistance for the Circuit is knownknown

4.4. Find the Current that leaves the batteryFind the Current that leaves the battery

Page 58: Electric Circuits LCHS Physics Mark Ewoldsen, Ph.D.

12 V

2 2 ΩΩ

2 2 ΩΩ

2 Ω

V = IR or I = V/RV = IR or I = V/RI = 12V / 3I = 12V / 3ΩΩ

I = 4AI = 4A

, 4A, 4A

Page 59: Electric Circuits LCHS Physics Mark Ewoldsen, Ph.D.

Finding V, I & R for a Finding V, I & R for a Complex CircuitComplex Circuit

1.1. Find the most complex portion of the Circuit – usually Find the most complex portion of the Circuit – usually part of the Parallelpart of the Parallel

2.2. Find the Total Resistance for that portionFind the Total Resistance for that portion

3.3. Continue until the Total Resistance for the Circuit is Continue until the Total Resistance for the Circuit is knownknown

4.4. Starting with the least complex resistor, Starting with the least complex resistor, find the voltage it usesfind the voltage it uses

Page 60: Electric Circuits LCHS Physics Mark Ewoldsen, Ph.D.

2 2 ΩΩ

12 V, 4A

2 2 ΩΩ

V = IRV = IRSince it is series, I = 4ASince it is series, I = 4A

V = 4A x 2 V = 4A x 2 ΩΩ

V = 8V V = 8V 2 2 ΩΩ8V8V

Page 61: Electric Circuits LCHS Physics Mark Ewoldsen, Ph.D.

Finding V, I & R for a Finding V, I & R for a Complex CircuitComplex Circuit

1.1. Find the most complex portion of the Circuit – usually Find the most complex portion of the Circuit – usually part of the Parallelpart of the Parallel

2.2. Find the Total Resistance for that portionFind the Total Resistance for that portion3.3. Continue until the Total Resistance for the Circuit is Continue until the Total Resistance for the Circuit is

knownknown4.4. Starting with the least complex resistor, find the Starting with the least complex resistor, find the

voltage it usesvoltage it uses

5.5. Continue until the parallel portion where Continue until the parallel portion where the remaining voltage will used on both the remaining voltage will used on both sides will be identical, Find Isides will be identical, Find I

Page 62: Electric Circuits LCHS Physics Mark Ewoldsen, Ph.D.

12 V, 4A

22Ω Ω

22Ω Ω

2 Ω8V

12V – 8V = 4V12V – 8V = 4V

I = 4V / 2I = 4V / 2Ω = 2AΩ = 2A

I = 4V/2I = 4V/2Ω = 2AΩ = 2A

4V 4V

4V4V

Page 63: Electric Circuits LCHS Physics Mark Ewoldsen, Ph.D.

Finding V, I & R for a Finding V, I & R for a Complex CircuitComplex Circuit

1.1. Find the most complex portion of the Circuit – usually Find the most complex portion of the Circuit – usually part of the Parallelpart of the Parallel

2.2. Find the Total Resistance for that portionFind the Total Resistance for that portion3.3. Continue until the Total Resistance for the Circuit is Continue until the Total Resistance for the Circuit is

knownknown4.4. Starting with the least complex resistor, find the Starting with the least complex resistor, find the

voltage it usesvoltage it uses5.5. Continue until the parallel portion where the Continue until the parallel portion where the

remaining voltage will used on both sides will be remaining voltage will used on both sides will be identical, Find Iidentical, Find I

6.6. Make sure Kirchhoff's Rule is followedMake sure Kirchhoff's Rule is followed

Page 64: Electric Circuits LCHS Physics Mark Ewoldsen, Ph.D.

12 V, 4A

2 2 Ω, 4VΩ, 4V

2A + 2A = 4A2A + 2A = 4A

2A2A

2A2A

4A4A

4A4A

4A4A

2 Ω8V

2 2 Ω, 4VΩ, 4V

Page 65: Electric Circuits LCHS Physics Mark Ewoldsen, Ph.D.

PowerPower• Power is the amount of energy that is transferred Power is the amount of energy that is transferred

every secondevery second

• Power is measured in wattsPower is measured in watts

P = I x VP = I x V

• PP = The power transferred by the component = The power transferred by the componentII = The current going through a component = The current going through a componentVV = The voltage across a component = The voltage across a component

• Remember that a kilowatt = 1,000 wattsRemember that a kilowatt = 1,000 watts

Page 66: Electric Circuits LCHS Physics Mark Ewoldsen, Ph.D.

PracticePractice

An electric iron draws a current of 4A at An electric iron draws a current of 4A at 250V. What is its power usage?250V. What is its power usage?

A.A. 0.0166W 0.0166W

B.B. 60W 60W

C.C. 1000W1000W

Page 67: Electric Circuits LCHS Physics Mark Ewoldsen, Ph.D.

PracticePractice

A common lightbulb reads 60W, 120V. How A common lightbulb reads 60W, 120V. How much current in amperes will flow through much current in amperes will flow through the bulb?the bulb?

A.A. 7200 amps 7200 amps

B.B. 0.5 amps0.5 amps

C.C. 2.0 amps2.0 amps

Page 68: Electric Circuits LCHS Physics Mark Ewoldsen, Ph.D.

PracticePracticeDetermine the cost of using the following appliances for the time indicated if the average cost is 9 cents/kWh.Determine the cost of using the following appliances for the time indicated if the average cost is 9 cents/kWh.

(a) 1200W iron for 2 hours(a) 1200W iron for 2 hours

(b) 160W color TV for 3 hours and 30 minutes(b) 160W color TV for 3 hours and 30 minutes

(c) Six 60W bulbs for 7 hours.(c) Six 60W bulbs for 7 hours.

1.2 kW x (2h) x 9 cents = kWh

12.2 cents

0.16 kW x (3.5h) x 9 cents = kWh

5.04 cents

6 x .06 kW x (7h) x 9 cents = kWh

22.68 cents

Page 69: Electric Circuits LCHS Physics Mark Ewoldsen, Ph.D.

Concept TestConcept Test• For resistors in For resistors in seriesseries, what is the same , what is the same

for every resistor? R, V or I?for every resistor? R, V or I?• Answer: IAnswer: I

• For resistors in parallel, what is the For resistors in parallel, what is the same for every resistor? R, V or I?same for every resistor? R, V or I?

• Answer: VAnswer: V

Page 70: Electric Circuits LCHS Physics Mark Ewoldsen, Ph.D.

Try this!Try this!

‘Some Electrical Circuit Components and Circuits’ by Michael Condren, Professor of Chemistry, Christian Brothers University, Memphis,  TN  @ http://www.cbu.edu/~mcondren/chem415/c415_ele.ppt, 4/17/04

R6=5

R1= 5

R2=10

R5=6

R3=6R4=12

Page 71: Electric Circuits LCHS Physics Mark Ewoldsen, Ph.D.

Series-Parallel CircuitSeries-Parallel Circuit

R6=5

R1= 5

R2=10R5=6

R3=6R4=12

EXAMPLE: What is the equivalent resistanceand current for the following circuit?

Page 72: Electric Circuits LCHS Physics Mark Ewoldsen, Ph.D.

Series-Parallel CircuitSeries-Parallel Circuit

R6=5

R1= 5

R2=10R5=6

R3=6R4=12

R7

EXAMPLE: What is the equivalent resistanceand current for the following circuit?

Page 73: Electric Circuits LCHS Physics Mark Ewoldsen, Ph.D.

Series-Parallel CircuitSeries-Parallel Circuit

resistors 3 and 4 are in parallelresistors 3 and 4 are in parallel

1 1 1 1 1 1 1 1 1 1 --- = --- + --- = ----- + ---------- = --- + --- = ----- + -------

RR77 R R33 R R44 66 1212

= 0.25= 0.25 -1-1

RR77 = 4 = 4

EXAMPLE: What is the equivalent resistanceand current for the following circuit?

Page 74: Electric Circuits LCHS Physics Mark Ewoldsen, Ph.D.

Series-Parallel CircuitSeries-Parallel Circuit

R6=5

R1= 5

R2=10R5=6

R7=4

EXAMPLE: What is the equivalent resistanceand current for the following circuit?

Page 75: Electric Circuits LCHS Physics Mark Ewoldsen, Ph.D.

R6=5

R1= 5

R2=10R5=6

R7=4R8

Series-Parallel CircuitSeries-Parallel Circuit

EXAMPLE: What is the equivalent resistanceand current for the following circuit?

Page 76: Electric Circuits LCHS Physics Mark Ewoldsen, Ph.D.

Series-Parallel CircuitSeries-Parallel Circuit

resistor 5 and equivalent resistance 7 are in resistor 5 and equivalent resistance 7 are in seriesseries

RR88 = R = R77 + R + R55 = (4 + 6) = (4 + 6) = = 1010

EXAMPLE: What is the equivalent resistanceand current for the following circuit?

Page 77: Electric Circuits LCHS Physics Mark Ewoldsen, Ph.D.

Series-Parallel CircuitSeries-Parallel Circuit

R6=5

R1= 5

R2=10 R8=10

EXAMPLE: What is the equivalent resistanceand current for the following circuit?

Page 78: Electric Circuits LCHS Physics Mark Ewoldsen, Ph.D.

Series-Parallel CircuitSeries-Parallel Circuit

R6=5

R1= 5

R2=10 R8=10R9

EXAMPLE: What is the equivalent resistanceand current for the following circuit?

Page 79: Electric Circuits LCHS Physics Mark Ewoldsen, Ph.D.

Series-Parallel CircuitSeries-Parallel Circuit

resistor 2 and equivalent resistance 8 in resistor 2 and equivalent resistance 8 in parallelparallel

1 1 1 1 11 1 1 1 1--- = ----- + ----- = ------- + ---------- = ----- + ----- = ------- + ------- RR99 R R22 R R88 10 10 1010

= 0= 0.2 .2 -1 -1 ; R ; R9 9 = 5= 5

EXAMPLE: What is the equivalent resistanceand current for the following circuit?

Page 80: Electric Circuits LCHS Physics Mark Ewoldsen, Ph.D.

Series-Parallel CircuitSeries-Parallel Circuit

R6=5

R1= 5

R9=5V=7.5v

EXAMPLE: What is the equivalent resistanceand current for the following circuit?

Page 81: Electric Circuits LCHS Physics Mark Ewoldsen, Ph.D.

Bibliography Bibliography 1. ‘Some Electrical Circuit Components and Circuits’ by Michael Condren,

Professor of Chemistry, Christian Brothers University, Memphis,  TN  @ http://www.cbu.edu/~mcondren/chem415/c415_ele.ppt, 4/17/04

2. ‘Fundamentals of Electronics,’ Dan Bruton, Professor of Astrophysics Stephen F. Austin State University @ observe.phy.sfasu.edu/courses/phy262/ lectures262, 4/17/04