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Electric Power Distribution, Generators and Motors

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Presentation on theme: "Electric Power Distribution, Generators and Motors"— Presentation transcript:

1 Electric Power Distribution, Generators and Motors
Benchmark Companies Inc PO Box Aurora CO 80047

2 Electric Power Distribution,

3 New ideas for today Magnetic induction Lenz’s law Transformers and power transmission Motors and Generators

4 Observations about Power Distribution
Household power is AC (alternating current) Power comes in voltages like 120V & 240V

5 Observations about Power Distribution
Power is transmitted at “high voltage” like 500KV

6 Observations about Power Distribution
Power transformers are visible everywhere

7 Observations about Power Distribution
Power substations are visible on occasion

8

9 Power Consumption in wires
Reminder: power consumption = current x voltage drop IxV voltage drop = resistance x current IxR power consumption = resistance x current I2xR Impact of the calculation: Wires waste power as heat Doubling current quadruples wasted power

10 Power Consumption in wires
Example: Resistance of 1 mile of power line is 10 Ohms. Determine the voltage drop across the power line if 200 Amps is transmitted at 240 Volts to power one typical house. The Power consumed across 1 mile is I2xR = 200A2x10 = 400KW is needed before we can begin to deliver power to a typical house.

11 DC AC Edison Tesla Westinghouse

12 DC vs AC a visual approach
DC can supply power . So can AC For transmission AC is superior DC= “direct current” AC=“alternating current”

13 AC = alternating current
Let’s explore why…… DC= “direct current” AC=“alternating current” Rotation Amplitude Amplitude/Time

14 AC = alternating current
As a conductor is rotated within a magnetic field alternating current is produced in that conductor Rotation within a magnetic field Amplitude Current Amplitude vs. time 0o 90o 180o 270o 360o 90o 0o 180o Positive Amplitude P N Negative Amplitude 360o 270o Time

15 Power Transmission For efficient power transmission:
Use low-resistance wires (thick, short copper) Use low current and high voltage drop Can accomplish this with AC (alternating current) power transmission.

16 Click for Bar Magnet And Pick-up coil example

17 Electromagnetic Induction
Changing magnetic field produces an electric field

18 Electromagnetic Induction
Current in a conductor produces a magnetic field

19 Electromagnetic Induction
An Induced magnetic field opposes the original magnetic field change (Lenz’s law)

20 Lenz’s Law

21 Electromagnet Transformer Example

22 Transformer Alternating current in one circuit induces an alternating current in a second circuit Transfers power between the two circuits Doesn’t transfer charge between the two circuits Demonstration: AC Electromagnet and Wire Loop with Lamp.

23 Transformer on fire

24 Transformers Power arriving in the primary circuit must equal power leaving the secondary circuit Power = current x voltage A transformer can change the voltage and current while keeping the power unchanged!

25 Step Down Transformer Fewer turns in secondary circuit so charge is pushed a shorter distance Smaller voltage rise A larger current at low voltage flows in the secondary circuit

26 Step Up Transformer More turns in secondary circuit so charge is pushed a longer distance Larger voltage rise A smaller current at high voltage flows in the secondary circuit

27 Observations about Electric Generators and Motors
A generator provides electric power A generator requires a mechanical power A motor provides mechanical power A motor requires electric power Alternator

28 Click me

29 Electric Generator Rotating magnet makes changing magnetic field
induces AC current in the loop Converts mechanical power into electrical power

30 Electric Motor Input AC power AC current makes changing magnetic field
causes magnet to turn Converts electrical power into mechanical power A motor is a generator run backwards !

31 End of Presentation


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