current electricity & ohms law

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Discusses Ohm's Law and current electricity and related to energy transfer in circuits. **More good stuff available at: www.wsautter.com and http://www.youtube.com/results?search_query=wnsautter&aq=f

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Page 1: Current Electricity & Ohms Law
Page 2: Current Electricity & Ohms Law

The next slide is a quick promo for my books after which the presentation will begin

Thanks for your patience!Walt S.

[email protected] stuff at: www.wsautter.com

Page 3: Current Electricity & Ohms Law

Books available at:www.wsautter.com

www.smashwords.comwww.amazon.com

www.bibliotastic.comwww.goodreads.com

Walt’s Books for Free!

Page 4: Current Electricity & Ohms Law

(1) A source voltage, that is, an electron pump usually a battery or power supply.

[ ENERGY IN]

(2) A conductor to carry electrons from and to the voltagesource (pump). The conductor is often a wire.

[ENERGY TRANSFER]

(3) A load or resistance. A point where energy is extractedform the circuit in the form of heat, light, motion, etc.

[ENERGY OUT]

All electrical circuits require three elements.

Page 5: Current Electricity & Ohms Law

ELECTRON PUMP

(SOURCE VOLTAGE)[ENERGY IN]

LOAD(RESISTANCE)[ENERGY OUT]

CONDUCTOR

ELECTRONSOUT OF SOURCE

ELECTRONSOUT OF LOAD

ELECTRONSBACK TOSOURCE

ELECTRONSINTOLOAD

HIGHER ENERGY ELECTRONS LOWER ENERGY ELECTRONS

CONDUCTOR

Page 6: Current Electricity & Ohms Law

Voltage Source(Potential Rise)

Low Energycurrent

High Energycurrent

Resistance(Potential Drop)

Low Energycurrent

High Energycurrent

Page 7: Current Electricity & Ohms Law

volts

Battery current

Electrons haveLess Energy

Electrons haveMore Energy Electrons get

An energy boost

current

Page 8: Current Electricity & Ohms Law

volts

Resistor current

Electrons haveMore Energy

Electrons haveLess Energy Energy is lost

In the resistor

Page 9: Current Electricity & Ohms Law

(1) VOLTAGE RISE – MEASURES THE ENERGY GIVEN TO ELECTRONS ASTHEY LEAVE A VOLTAGE SOURCE. IT IS MEASURED IN VOLTS (+)

(2) VOLTAGE DROP – MEASURES THE ENERGY LOST BY TO ELECTRONS WHEN THEY LEAVE A RESISTANCE. IT IS MEASURED IN VOLTS (-)

(3) CURRENT – MEASURES THE FLOW RATE THROUGH A CONDUCTOR.IT IS MEASURED IN AMPERES (AMPS)

(4)RESISTANCE – MEASURES THE OPPOSITION TO CURRENT FLOW THROUGH A CONDUCTOR OR RESISTOR

IT IS MEASURED IN OHMS (ITS SYMBOL IS OMEGA )

Page 10: Current Electricity & Ohms Law

6.25 x 10 18electrons1 coulomb

1 coulomb 1 second1 amp = 1 coul / sec

1 joule

1 coulomb of charge

1 volt = 1 joule / coul

ELECTRICAL QUANTITIES

Page 11: Current Electricity & Ohms Law

AMPS

volts

Ammeters measurecurrent in amperes

and are alwayswired in series in

the circuit.

Voltmeters measurepotential in voltsand are always

wired in parallel in the circuit.

Page 12: Current Electricity & Ohms Law
Page 13: Current Electricity & Ohms Law
Page 14: Current Electricity & Ohms Law

wiring

battery

voltmeter

ammeter

resistance

capacitor

+ -

A

V

junction

terminal

AC generator

Variableresistance

Variablecapacitor

Page 15: Current Electricity & Ohms Law

Measure electrical quantities in an electrical Circuit are related to eachother by:

OHM’S LAW

OHM’S LAW says, if the source voltage remains constant,increasing the resistance in a circuit will cause a decrease

in current flow in that circuit.In mathematical terms it tells us that current flow is

inversely proportional to resistance.

In equation form it says:Voltage (V) = Current (I) x Resistance (R)

orV(in volts) = I (in amps) x R (in ohms)

Page 16: Current Electricity & Ohms Law

PotentialIn volts

(joules / coul)

CurrentIn amperes

(coul / second)

ResistanceIn ohms

(volts / amp)

Drop across a resistance

Current passingThrough the

resistor

Page 17: Current Electricity & Ohms Law

VOLTAGE

(volts)

Current (I) in amps

I

v

The slope of theLine gives the

resistance

R = v /Ior rearrangedv = I x R

Page 18: Current Electricity & Ohms Law

All voltage sources contain internal resistance, thatis resistance that is part of the voltage producing

device itself which cannot be eliminated.

The voltage that the device (battery for example)could produce if no internal resistance was present

is called its EMF.EMF stands for electromotive force – the force

that moves the electrons.

The useable voltage which is available to the circuitafter the internal resistance consumes its share

of the EMF is called The terminal voltage.

Page 19: Current Electricity & Ohms Law

EMFVoltage

riseVoltage

drop

EMF of Source Internal resistance

+ -

Terminal voltage

conventionalcurrent

flow

Page 20: Current Electricity & Ohms Law

Since voltage rise across a source or Voltage drop across a resistance can be

Calculated by Ohm’s LawV= IR

And the above equation becomes

V terminal = EMF – I x R internal

Note that if R internal is very small then a largePercentage of the EMF is available to the circuit.

Also note that if I, the current is very large then a large percentage of the EMF is consumed within

the battery itself which can cause overheating and failure. This is generally the result of a short circuit.

Page 21: Current Electricity & Ohms Law

volts

Battery current

Voltage riseDue to EMF

Voltage dropDue to internal

resistance

current EMFRi

+V-V

Net VoltageRise of cell

(Terminal Voltage

Page 22: Current Electricity & Ohms Law