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Page 1: the flow of charged particles charged particles ; can be positive or negative, but usually negative (electrons) through a conducting metal
Page 2: the flow of charged particles charged particles ; can be positive or negative, but usually negative (electrons) through a conducting metal

the flow ofthe flow of charged particlescharged particles;

can be positive or negative,but usually negative (electrons)

through a conducting metal

Page 3: the flow of charged particles charged particles ; can be positive or negative, but usually negative (electrons) through a conducting metal

electric cell - a device thatconverts one form of energy

to electrical energy

Chemical cells convert chemicalenergy into electrical energy.

Chemical cells can be“wet” or “dry”.

Page 4: the flow of charged particles charged particles ; can be positive or negative, but usually negative (electrons) through a conducting metal

SolarSolar cellscells convert light energyinto electrical energy.

A generatorgenerator converts mechanicalenergy into electrical energy.

batterybattery - two or more cellsconnected in series or in parallel

Page 5: the flow of charged particles charged particles ; can be positive or negative, but usually negative (electrons) through a conducting metal

Electric current is measuredin Amperes, in honor ofAndre Marie Ampere.

One Ampere is the flow ofOne Ampere is the flow ofone Coulomb of charge per second.one Coulomb of charge per second.

1 Amp = 1 Coulomb per second = 1 C/s1 Amp = 1 Coulomb per second = 1 C/s

II = QQ/tt

Page 6: the flow of charged particles charged particles ; can be positive or negative, but usually negative (electrons) through a conducting metal

AmmeterAmmetera device that measures current

VoltmeterVoltmetera device that measures

electric potential difference

Page 7: the flow of charged particles charged particles ; can be positive or negative, but usually negative (electrons) through a conducting metal

powerpower = = workwork//timetime

= (= (workwork//chargecharge))..((chargecharge//timetime))

== electric potential differenceelectric potential difference ..

currentcurrent

PP ( (WattsWatts) = ) = VV ( (VoltsVolts))..II ( (AmpsAmps))

Page 8: the flow of charged particles charged particles ; can be positive or negative, but usually negative (electrons) through a conducting metal

Analogies of simple circuits are these links:Analogies of simple circuits are these links:

Water circuit analogy Water circuit analogy linkAir flow Air flow link

Page 9: the flow of charged particles charged particles ; can be positive or negative, but usually negative (electrons) through a conducting metal

ResistanceResistance

determines the amount of current flowdetermines the amount of current flow

= the ratio of potential difference to current= the ratio of potential difference to current

RR =VVII

The SI unit of resistance is the OhmOhm, , namedin honor of Georg Simon Ohm.

One OhmOne Ohm of resistance is the resistancesuch that one Voltone Volt of potential differenceis needed to obtain a current of one Ampone Amp.

Page 10: the flow of charged particles charged particles ; can be positive or negative, but usually negative (electrons) through a conducting metal

The resistance of a circuit element depends on:

1. the length of the conductorthe length of the conductoras length increases, resistance increases proportionally

2. the cross-sectional area of the conductorthe cross-sectional area of the conductoras area increases, resistance decreases proportionally

3. the resistivity of the conductorthe resistivity of the conductoras resistivity increases, resistance increases proportionally

Page 11: the flow of charged particles charged particles ; can be positive or negative, but usually negative (electrons) through a conducting metal

Ohm’s LawOhm’s LawThe ratio of potential difference to currentThe ratio of potential difference to current

is constant.is constant.

If R = V/I is a constant valueIf R = V/I is a constant valuefor a given resistor, then thatfor a given resistor, then that

resistor is said to obey Ohm’s Law.resistor is said to obey Ohm’s Law.

Click Click here and and here to link to pages describing resistor to link to pages describing resistorcolor codes.color codes.

Page 12: the flow of charged particles charged particles ; can be positive or negative, but usually negative (electrons) through a conducting metal

ResistivityResistivityThe resistivity, , of a conductor is equal to the

resistance of a wire 1 cm long and having a cross-sectional area of 1 cm2.

RR

RR = resistance, measured in Ohms = resistance, measured in Ohms

=

= resistivity, usually in units of = resistivity, usually in units of cmcm

ll

l = length, measured in cml = length, measured in cm

AA

AA = cross-sectional area, measured in cm = cross-sectional area, measured in cm22

Page 13: the flow of charged particles charged particles ; can be positive or negative, but usually negative (electrons) through a conducting metal

Click Click here and and here to run to runsimulations of Ohm’s Law.simulations of Ohm’s Law.

Many circuit elements do notMany circuit elements do notobey Ohm’s Law. Resistorsobey Ohm’s Law. Resistorsthat get hot, like light bulbsthat get hot, like light bulbsand heating elements, do notand heating elements, do notkeep a constant resistance. keep a constant resistance. Resistance generally Resistance generally increases as increases as objects become hotter.objects become hotter.

Page 14: the flow of charged particles charged particles ; can be positive or negative, but usually negative (electrons) through a conducting metal

Resistor CircuitsResistor CircuitsSeries

1. 1. total resistancetotal resistance is the sum of the is the sum of the separate resistorsseparate resistors

RRTT = R = R11 + R + R22 + R + R33 + ... + ...

2. 2. currentcurrent is the same through each resistor is the same through each resistor

IITT = I = I11 = I = I22 = I = I33 = ... = ...

3. 3. total potential differencetotal potential difference is the sum of each is the sum of each

VVTT = V = V11 + V + V22 + V + V33 + ... + ...

In other words, in a series circuit,In other words, in a series circuit,resistance and voltage add,resistance and voltage add,but current stays the same.but current stays the same.

Page 15: the flow of charged particles charged particles ; can be positive or negative, but usually negative (electrons) through a conducting metal

RR11

RR22

RR33

EE = 12 V = 12 V

RRTT = =

VVTT = =

IITT = =

RR11

RR22

RR33

V,V,VV

PPTT = =

R,R,

I,I,AA

P,P,WW

8.0

5.0

2.0

Page 16: the flow of charged particles charged particles ; can be positive or negative, but usually negative (electrons) through a conducting metal

RR11

RR22

RR33

EE = 12 V = 12 V

RRTT = 15 = 15 ΩΩ

VVTT = 12 V = 12 V

IITT = 0.80 A = 0.80 A

RR11

RR22

RR33

V,V,VV

PPTT = 9.6 W = 9.6 W

R,R,

I,I,AA

P,P,WW

8.0

5.0

2.0

0.80

0.80

0.80

6.4

1.6

4.0

5.1

1.3

3.2

Page 17: the flow of charged particles charged particles ; can be positive or negative, but usually negative (electrons) through a conducting metal

Parallel 1.1. reciprocal of the total resistance reciprocal of the total resistance is is

the the sum of the reciprocals of the sum of the reciprocals of the

separate separate resistorsresistors

1/R1/RTT = 1/R = 1/R11 + 1/R + 1/R22 +1/R +1/R33 + ...+ ...2. 2. total currenttotal current is the sum of the current is the sum of the current

through each resistorthrough each resistorIITT = I = I11 + I + I22 + I + I33 + ... + ...

3. 3. potential differencepotential difference is the same is the same across across each resistoreach resistorVVTT = V = V11 = V = V22 = V = V33 = ... = ...

In other words, in a parallel circuit, resistance adds as reciprocals,

voltage stays the same, and current splits.

In other words, in a parallel circuit, resistance adds as reciprocals,

voltage stays the same, and current splits.

Page 18: the flow of charged particles charged particles ; can be positive or negative, but usually negative (electrons) through a conducting metal

EE = 12 V = 12 V

RRTT = =

VVTT = =

IITT = =

RR11

RR22

RR33

R,R,

V,V,VV

I,I,

PPTT = =

RR33

RR11

RR22

P,P,WW

12

8.0

12

Page 19: the flow of charged particles charged particles ; can be positive or negative, but usually negative (electrons) through a conducting metal

EE = 12 V = 12 V

RRTT = 3.42 = 3.42 ΩΩ

VVTT = 12 V = 12 V

IITT = 3.50 A = 3.50 A

RR11

RR22

RR33

R,R,

V,V,VV

I,I,

PPTT = 42 W = 42 W

RR33

RR11

RR22

P,P,WW

12

8.0

12

12

12

12

1.0

1.5

1.0

12

12

18

Page 20: the flow of charged particles charged particles ; can be positive or negative, but usually negative (electrons) through a conducting metal

Go to Go to link1, , link2, , link3, , link4, link5, and link6 to view, link5, and link6 to viewpages and simulations examining pages and simulations examining

Kirchhoff’s Loop and Junction Rules.Kirchhoff’s Loop and Junction Rules.

Kirchhoff’s RulesKirchhoff’s Rules

Loop Rule: Loop Rule: The sum of the potential differencesThe sum of the potential differencesaround any closed circuit loop is zero.around any closed circuit loop is zero.

Junction Rule: Junction Rule: The sum of the currentsThe sum of the currentsinto any circuit junction is zero.into any circuit junction is zero.

Page 21: the flow of charged particles charged particles ; can be positive or negative, but usually negative (electrons) through a conducting metal

The site linkedThe site linkedhere allows youhere allows youto build and test to build and test your own series,your own series,parallel, and/orparallel, and/orcombination circuits.combination circuits.

For a complete interactive tutorial onFor a complete interactive tutorial onelectricity and magnetism, go here.electricity and magnetism, go here.