Transcript
Page 1: Current Electricity. Current Electricity – what have we discussed static electricity Properties of Conductors & Insulators. Transfer of charge through

Current Electricity

Page 2: Current Electricity. Current Electricity – what have we discussed static electricity Properties of Conductors & Insulators. Transfer of charge through

Current Electricity –what have we discussed static electricity

• Properties of Conductors & Insulators.

• Transfer of charge through various methods.

• Calculation of Forces between charged objects.

• Calculation of Forces exerted by electric fields.

• Energy of charges at positions electric fields (voltage)

Page 3: Current Electricity. Current Electricity – what have we discussed static electricity Properties of Conductors & Insulators. Transfer of charge through

We’ll apply what we know to current electricity.

What does current mean?

What does electric current mean?

Flow or motion.

Flow or motion of electric charge.

Page 4: Current Electricity. Current Electricity – what have we discussed static electricity Properties of Conductors & Insulators. Transfer of charge through

What will happen if two oppositely charged metal plates touch?

Until the plates have equal charge.

How long?

Hint: RememberThe conducting spheres.

Page 6: Current Electricity. Current Electricity – what have we discussed static electricity Properties of Conductors & Insulators. Transfer of charge through

With static I can charge an object, & transfer the electric charge to do work.

Static electricity is quick transfer of charge but charge stops when equilibrium reached.

Demo with bulb

We often want continuous flow of charge because we want continuous work.

Page 7: Current Electricity. Current Electricity – what have we discussed static electricity Properties of Conductors & Insulators. Transfer of charge through

Current Electricity provides continuous motion or flow of charges.

Page 8: Current Electricity. Current Electricity – what have we discussed static electricity Properties of Conductors & Insulators. Transfer of charge through

Current still needs a potential difference/voltage to push charges to move.

Each volt does work on each coulomb of charge & each charge changing q’s Energy:

The van der Graff & sphere set up p.d.

The vdg is not continuous enough for constant work.

V = W/q. V = E/q.

Page 9: Current Electricity. Current Electricity – what have we discussed static electricity Properties of Conductors & Insulators. Transfer of charge through

Current Electricity requires constant source of potential difference or

voltage.

• Battery

• Wall outlet

• Generator

• Solar Cell

Page 10: Current Electricity. Current Electricity – what have we discussed static electricity Properties of Conductors & Insulators. Transfer of charge through

Constant Potential Dif/Voltage induces charges to move continuously.

Page 11: Current Electricity. Current Electricity – what have we discussed static electricity Properties of Conductors & Insulators. Transfer of charge through

Voltage/p.d. provides the “push” or “pressure” to charges. Think of 1 side as more + and 1 side more neg

The higher the voltage/p.d., the more push or pressure each charge gets, the more E each q

has, the more W each q can do.

+-

Page 12: Current Electricity. Current Electricity – what have we discussed static electricity Properties of Conductors & Insulators. Transfer of charge through

An electric circuit allows current to flow an to do continuous work. Circuits need the following components:

• A source of continuous voltage.

• A pathway made of conducting materials.

• Appliance(s) to convert electric E to some other form (heat, light, sound etc.)

Page 13: Current Electricity. Current Electricity – what have we discussed static electricity Properties of Conductors & Insulators. Transfer of charge through

Solids only e- flow.

Liquids any charged particles or ions can flow.

Which type of charges can move?

Page 14: Current Electricity. Current Electricity – what have we discussed static electricity Properties of Conductors & Insulators. Transfer of charge through

Measuring Current

• Rate of flow of charge.

Page 15: Current Electricity. Current Electricity – what have we discussed static electricity Properties of Conductors & Insulators. Transfer of charge through

Amperes (A) measures rate of coulombs passing a point in a wire.

1 A = 1 C/s

passing a point or cross section of wire.

# charges per sec or# Coulombs per sec.

Page 16: Current Electricity. Current Electricity – what have we discussed static electricity Properties of Conductors & Insulators. Transfer of charge through

I = q/t

I = current C/s or AQ = charge in Coulombs

t = time in seconds

Page 17: Current Electricity. Current Electricity – what have we discussed static electricity Properties of Conductors & Insulators. Transfer of charge through

Ex 1: 100 C pass a section of wire every 5 sec. How much current flows in the wire?

I = q 100C 20 C/s or 20 A. t 5 s

Page 18: Current Electricity. Current Electricity – what have we discussed static electricity Properties of Conductors & Insulators. Transfer of charge through

Ex 2: The current in a light bulb is 0.835 A. How long does it take for a total charge of 1.67 C to pass a point in the wire?

I = Q/t t = Q/I

t = 1.67C = 2.00 s

0.835 C/s

Page 19: Current Electricity. Current Electricity – what have we discussed static electricity Properties of Conductors & Insulators. Transfer of charge through

Ex 3: If, in 1 second 6.25 billion billion (6.25 x 10 18) electrons pass through a point in a wire, what is the current?

1 A

Page 20: Current Electricity. Current Electricity – what have we discussed static electricity Properties of Conductors & Insulators. Transfer of charge through

Hwk read text 19-1

• Do page 695 # 3 – 5 & pg 717 #1 – 6 neatly on lined in full sentences! Show work.

Page 21: Current Electricity. Current Electricity – what have we discussed static electricity Properties of Conductors & Insulators. Transfer of charge through

How many ways can you set up a circuit of 1 battery, 2 bulbs, 3 wires to li

• Use all the components for each circuit, but no extra components allowed.

• Sketch all the arrangements that light the bulbs.

• Sketch all the arrangements that did not light the bulbs.

• Look at your sketches. Explain what you think is happening physically. Why do the bulbs light with certain arrangements? Why won’t they light with others? Write your hypothesis under your sketches.

• For a circuit that worked, list the E transformations.

• Write down any questions you have about the circuit.

• If time allows, find the circuit symbols in your reference table. Re-sketch your circuits using proper symbols.

Page 22: Current Electricity. Current Electricity – what have we discussed static electricity Properties of Conductors & Insulators. Transfer of charge through

Electric Current Clip 9 minutes

• http://www.youtube.com/watch?v=5laTkjINHrg

http://www.youtube.com/watch?v=IpaEGhjpZgc

Battery clip old but nice. 10 min.

Page 23: Current Electricity. Current Electricity – what have we discussed static electricity Properties of Conductors & Insulators. Transfer of charge through

To get continuous flow of charge we need:

1. voltage (p.d.) to push charges.

2. Charge Pump = do work on charge which gains PE. Pumps are batteries, generators.

3. Closed Circuit – continuous pathway for charges to flow –metal wire.

Page 24: Current Electricity. Current Electricity – what have we discussed static electricity Properties of Conductors & Insulators. Transfer of charge through

Outlet has p.d. = 120V.Don’t stick a fork in it!!

Page 25: Current Electricity. Current Electricity – what have we discussed static electricity Properties of Conductors & Insulators. Transfer of charge through

How does p.d. make charge flow??

Page 26: Current Electricity. Current Electricity – what have we discussed static electricity Properties of Conductors & Insulators. Transfer of charge through

Pot. Dif. Causes electric field to spread through wire at near light speed.

e- in wire respond by moving in field & colliding with neighboring e- starting to flow.

Page 27: Current Electricity. Current Electricity – what have we discussed static electricity Properties of Conductors & Insulators. Transfer of charge through

Electric field in wire caused by voltage source induces all

e- to move.

Each e- moves slowly but all begin at once.

Page 28: Current Electricity. Current Electricity – what have we discussed static electricity Properties of Conductors & Insulators. Transfer of charge through

Circuit – Closed pathway for charges. All components need p.d. to move.

Potential Dif/ VoltageGives the push

Conducting path (wire). Easy to move current through very little p.d. needed.

Resistors – (bulbs)Difficult for current to flow. Larger p.d. needed.

Page 29: Current Electricity. Current Electricity – what have we discussed static electricity Properties of Conductors & Insulators. Transfer of charge through

Work & Energy on Charges (q) in circuit.

Battery does work on q.

Q pushed into Conducting path (wire).

Resistors – (bulbs)

PEchm – PEelc

Q in motion. PEelc - KE

Work on q, PEelc &KE – heat, light.

PEelc used up, PEchm, starts cycle again.

Page 30: Current Electricity. Current Electricity – what have we discussed static electricity Properties of Conductors & Insulators. Transfer of charge through

Voltage E transformations as skiiers. 9.5 min.

• http://www.youtube.com/watch?v=F1p3fgbDnkY

Page 31: Current Electricity. Current Electricity – what have we discussed static electricity Properties of Conductors & Insulators. Transfer of charge through

Bulbs, toasters, computers... convert KE of e- to other forms of E – heat, light etc.

Devices are called resistors or loads. They slow down the e- so they resist current flow. (Like paddle wheel in river).

A Closer Look at Resistors

Page 32: Current Electricity. Current Electricity – what have we discussed static electricity Properties of Conductors & Insulators. Transfer of charge through

As e- flow through filament, KE lost to heat & light.

What must be around the bulb to push e- through it?

p. d.

Page 33: Current Electricity. Current Electricity – what have we discussed static electricity Properties of Conductors & Insulators. Transfer of charge through

Ohm’s Law The resistance of a conductor

R = V/I

V = volts J/C

I = current A, C/s

R = resistance ohm’s or V/A.

Resistance (R) unit = ohm’s .

Page 34: Current Electricity. Current Electricity – what have we discussed static electricity Properties of Conductors & Insulators. Transfer of charge through

Ex A: A 120-V potential difference is applied to a toaster which draws a current of 4 A. What is the toaster’s resistance?

• R – V/I

• = 120-V/4 A

• =30 .

Page 35: Current Electricity. Current Electricity – what have we discussed static electricity Properties of Conductors & Insulators. Transfer of charge through

Resistance in Wires

Occurs in wires as well as appliances. Certain factors affect how much resistance a wire will offer to current flow.

Page 36: Current Electricity. Current Electricity – what have we discussed static electricity Properties of Conductors & Insulators. Transfer of charge through

Factors affecting wire resistance.

1. Length2. Area3. Temperature4. Type of material

Page 37: Current Electricity. Current Electricity – what have we discussed static electricity Properties of Conductors & Insulators. Transfer of charge through

Length – longer wire offers more resistance. More chances for friction in wire.

More resistance

Less resistance

Page 38: Current Electricity. Current Electricity – what have we discussed static electricity Properties of Conductors & Insulators. Transfer of charge through

Cross Sectional AreaThick wires offer less resistance.

Page 39: Current Electricity. Current Electricity – what have we discussed static electricity Properties of Conductors & Insulators. Transfer of charge through

TemperatureHot offers more RCold offers less R

Page 40: Current Electricity. Current Electricity – what have we discussed static electricity Properties of Conductors & Insulators. Transfer of charge through

R = resistance () = constant of resistivity (m)l = length (m) A = cross sectional area (m2) See table

At a given temperature,

Page 41: Current Electricity. Current Electricity – what have we discussed static electricity Properties of Conductors & Insulators. Transfer of charge through

Ex 1: A 9.5 cm length of copper wire has a cross sectional area of 2.5 x 10-3 m2. What is the resistance of the wire at 20oC?

Page 42: Current Electricity. Current Electricity – what have we discussed static electricity Properties of Conductors & Insulators. Transfer of charge through

From table = 1.72 x 10-8 m.

So R = (1.72 x 10-8 m)(.095 m ) 2.5 x 10-3 m2

= 6.5 x 10-7 .

Page 43: Current Electricity. Current Electricity – what have we discussed static electricity Properties of Conductors & Insulators. Transfer of charge through

Ex 2: Find the resistance of a copper wire 10 m long and 1.2 x 10-9 m2 in area.

.

Page 44: Current Electricity. Current Electricity – what have we discussed static electricity Properties of Conductors & Insulators. Transfer of charge through

For wire with known p and length use:

R = L/A

for R with known V and I use

R = V/I.

Resistance

Page 45: Current Electricity. Current Electricity – what have we discussed static electricity Properties of Conductors & Insulators. Transfer of charge through

Resistance

Film clip with questions. 9:30 minutes.

Page 46: Current Electricity. Current Electricity – what have we discussed static electricity Properties of Conductors & Insulators. Transfer of charge through

6 V

Name _______________________________

After Film: Given the circuit connected with copper wires to a 6V battery, what should each voltage (p.d.) read at position 1 and 2? Write the voltages in the space.

• If the potential difference around the bulb is actually measured as 5.5V, what might you conclude happened ?

• _____________________________

1. _____V

2. _____V

Page 47: Current Electricity. Current Electricity – what have we discussed static electricity Properties of Conductors & Insulators. Transfer of charge through

Ex: A spool of gold wire with area 1.2 x 10-7 m2, has a resistance of 1.5 . What is its length?

• 7.4 m

Page 48: Current Electricity. Current Electricity – what have we discussed static electricity Properties of Conductors & Insulators. Transfer of charge through

Hwk Read tx. 19 – 1 & 19 - 2Do text text p 717 #15,19, 20

AND

do review book pg 225 #2 - 7

Page 49: Current Electricity. Current Electricity – what have we discussed static electricity Properties of Conductors & Insulators. Transfer of charge through
Page 50: Current Electricity. Current Electricity – what have we discussed static electricity Properties of Conductors & Insulators. Transfer of charge through

Ohm’s LawResistance, Current, Voltage

Page 51: Current Electricity. Current Electricity – what have we discussed static electricity Properties of Conductors & Insulators. Transfer of charge through

Potential DropIf a current flows in a resistor or appliance, there must be a pd across the ends of the resistor.

The voltage pushes the charge.

The resistor “drops” or lowers the PEelc of the charge. So is sometimes called potential or voltage drop.

- +R

e- current

Page 52: Current Electricity. Current Electricity – what have we discussed static electricity Properties of Conductors & Insulators. Transfer of charge through

Current (flow rate) increases w/ increased pd

& decreases with increased resistance.

• R = V/I

• I = V units V/ R

Or V = IR

Page 53: Current Electricity. Current Electricity – what have we discussed static electricity Properties of Conductors & Insulators. Transfer of charge through

Ohm’s LawWhen T across a metallic resistor is constant, the current is directly proportional to pd across it.

V = RI V/I = R = constant.

V = volts J/C

I = current A, C/s

R = total resistance

ohm’s .

Page 54: Current Electricity. Current Electricity – what have we discussed static electricity Properties of Conductors & Insulators. Transfer of charge through

What is the graph of Ohm’s Law? Usu V on y-axis, I on x-axis, R is slope of direct linear.

Page 55: Current Electricity. Current Electricity – what have we discussed static electricity Properties of Conductors & Insulators. Transfer of charge through

V = RI yield direct linear relationship.V on Y axis. I on x axis. R is slope of straight line. R = constant.

Page 56: Current Electricity. Current Electricity – what have we discussed static electricity Properties of Conductors & Insulators. Transfer of charge through

What would the slope represent if current was placed on the Y axis?

1/R

Page 57: Current Electricity. Current Electricity – what have we discussed static electricity Properties of Conductors & Insulators. Transfer of charge through

Ex 1: A 30-V battery maintains a current through a 10- resistor. Find the current in the circuit.

Page 58: Current Electricity. Current Electricity – what have we discussed static electricity Properties of Conductors & Insulators. Transfer of charge through

V = IR

I = V/R

30 V/10 = 3.0 A

Page 59: Current Electricity. Current Electricity – what have we discussed static electricity Properties of Conductors & Insulators. Transfer of charge through

Ex 2: What is the current flow through an 80- coil when it is connected to a generator supplying 120-V?

V = IR I = V/R

120V/80 = 1.5 A

Page 60: Current Electricity. Current Electricity – what have we discussed static electricity Properties of Conductors & Insulators. Transfer of charge through

Ex 3: What is the rate of electron flow through the coil above?

Page 61: Current Electricity. Current Electricity – what have we discussed static electricity Properties of Conductors & Insulators. Transfer of charge through

Need to convert coulombs of charge from current equation to electrons so use equivalence of e- in 1 C:

1.5 C/s x (6.25 x 1018 e-/C) =

9.4 x 1018 e-/s pass through a point in the coil.

Page 62: Current Electricity. Current Electricity – what have we discussed static electricity Properties of Conductors & Insulators. Transfer of charge through

Ex 4. A 1 – m long copper wire has a cross sectional area of 0.0002 m2. If the current flow is 0.5-A, what is the potential difference?

Page 63: Current Electricity. Current Electricity – what have we discussed static electricity Properties of Conductors & Insulators. Transfer of charge through

Find R using.

R = 8.6 x 10-5 .

Page 64: Current Electricity. Current Electricity – what have we discussed static electricity Properties of Conductors & Insulators. Transfer of charge through

Find V using:V = IR

V = (8.6 x 10-5 .)(0.5 A) = 4.3 x 10-5V

Page 65: Current Electricity. Current Electricity – what have we discussed static electricity Properties of Conductors & Insulators. Transfer of charge through

5. A light bulb heats up as it’s in use. Which best represents the V-I graph of a bulb filament.

Page 66: Current Electricity. Current Electricity – what have we discussed static electricity Properties of Conductors & Insulators. Transfer of charge through

Hwk read txt 19.2 do pg 703 prb #1 – 6

Page 67: Current Electricity. Current Electricity – what have we discussed static electricity Properties of Conductors & Insulators. Transfer of charge through

Power in Resistors

• Resistors convert KE & EElc to other forms.

• They do work on q.

• P rate work gets done or E used/ converted/ dissipated or supplied J/s or Watts.

• Power rating of 500 W means Eelc converted to other kinds at rate 500 J/s.

Page 68: Current Electricity. Current Electricity – what have we discussed static electricity Properties of Conductors & Insulators. Transfer of charge through

Derive some equations relating power, voltage, resistance, and

current.

Page 69: Current Electricity. Current Electricity – what have we discussed static electricity Properties of Conductors & Insulators. Transfer of charge through

P = W t

• qV q = I t t

• VI

• P = VI

• The power dissipated is thermal energy and work done in resistor.

Page 70: Current Electricity. Current Electricity – what have we discussed static electricity Properties of Conductors & Insulators. Transfer of charge through

Other Power Equations

From Ohm’s Law we use R = V/I to derive other equations for power.

P = I2R = V2.

R

Page 71: Current Electricity. Current Electricity – what have we discussed static electricity Properties of Conductors & Insulators. Transfer of charge through

Ex 1. A toaster draws a current of 2.0-A from a 120-V source. What is its power rating?

P = VI

P = (120V)(2.0 A)

240 VA or 240 W.

Page 72: Current Electricity. Current Electricity – what have we discussed static electricity Properties of Conductors & Insulators. Transfer of charge through

For bulbs, power = brightness.

• Rate bulb converts Peelc & KE to heat & light.

Page 73: Current Electricity. Current Electricity – what have we discussed static electricity Properties of Conductors & Insulators. Transfer of charge through

Work done

Since Power is Work/Time,

Power x Time = Work or Energy

Page 74: Current Electricity. Current Electricity – what have we discussed static electricity Properties of Conductors & Insulators. Transfer of charge through

Ex 2: A resistor of 12 has a current of 2.0-A flowing through it. How much energy is generated in the resistor in one minute?I = 2A R = 12 t = 60-s E = ? J

• Work = Energy

• W = I2Rt

=(2-A)2(12)(60s) = 2880 J.

Page 75: Current Electricity. Current Electricity – what have we discussed static electricity Properties of Conductors & Insulators. Transfer of charge through

Graphs P=VI

Pow

er

Current

Slope =Voltage

Page 76: Current Electricity. Current Electricity – what have we discussed static electricity Properties of Conductors & Insulators. Transfer of charge through

Power Ratings for Appliances

Devices are rated by the power they use. A bulb rated 60 W 220 V means:

the bulb will dissipate 60 W when attached to a 220 p.d.

If a different p.d. is used, then it won’t dissipate 60 W.

Page 77: Current Electricity. Current Electricity – what have we discussed static electricity Properties of Conductors & Insulators. Transfer of charge through

Fuses

As current flows, wires heat up.

Fuses designed to break circuit if current becomes to high for the wires.

Fuse should be rated just above the ideal operating current for a circuit.

Page 78: Current Electricity. Current Electricity – what have we discussed static electricity Properties of Conductors & Insulators. Transfer of charge through

Story of Electricity BBC 2 hours

• http://www.youtube.com/watch?v=mJnc79MHSs4

Page 79: Current Electricity. Current Electricity – what have we discussed static electricity Properties of Conductors & Insulators. Transfer of charge through

Finish Power Examples

Hwk Read 19.3 Text

do p 710 1 – 4,

p713 #1 – 3 and prac set

Page 80: Current Electricity. Current Electricity – what have we discussed static electricity Properties of Conductors & Insulators. Transfer of charge through

Kilowatt hours kWh.

• Power is a rate of energy use.

• Electric sold in kWh which is Pt.

• 1 kWh is energy delivered to home in 1hour.

• 1 kWh (1000 W/kW)(60 min/h)(60s/min) = 3.6 x 106 Ws = 3.6 x 106 J


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