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Electricity 1

Electrostatics
and
Current Electricity
Aim of the lesson
 Static charge
  3.6.26 recall that insulating materials can be
   charged by friction and explain this in terms of
   transfer of charge.
  3.6.27 identify that positively charged objects
   have a deficiency of electrons and negatively
   charged objects have a surplus of electrons.
  3.6.28 describe the dangers and use of
   electrostatic charge generated in everyday
   contexts.
Text Book Reference

  Physics CCEA pg 109-113
  Electrostatics is the study of charges at
   rest
Sir Ben Frank

  Fly that kite…
Electrostatics

        The organisation of the parts of an atom
         has electrons orbiting a large central
         nucleus of nucleons (neutrons and
         protons)




          neutral atom          positive ion   negative ion
These models are NOT to scale
 If there is an unbalanced number of
     protons (positive carriers) compared to
     electrons (negative carriers) then the ion is
     called a charged particle


           -                        -                         -
          ++                       ++                        ++
   -       +
                  -                 +      -           -      +      -
                                                        -
3 electrons, 3 protons-   2 electrons, 3 protons-   4 electrons, 3 protons-
       no charge              positive charge           negative charge
                               (deficiency of       (surplus of electrons)
                                 electrons)
Charging by friction

In this diagram:


The wool and polythene
are each ‘uncharged’.
What does this mean?
Charging by friction

The wool is ‘uncharged’,                +
because…                     + −        −
                              +
…it has equal amounts       + −         +
                            −+−
of positive and negative     −          −
charge.                     + +         −
                             −−
Equal numbers of           +            +
+ and −
On the wool          On the polythene
Charging by friction

Equal numbers of +                 +
and − on the wool:         +   −   −
                             +
(Count them!)              + −     +
                           −+−
7+ 7−                        −     −
                           + +     −
Equal numbers of +          −−
and − on the polythene:   +        +
(Count them!)
3+ 3−
Charging by friction

If you rub the wool on                   +−
the polythene, some            +    −    −
electrons (−) move from            +
                              +   +−
the wool to the polythene.   −+
                                −  −
There are now more +          + + −−
than − on the wool:            −
                             +     +
(Count them!)
So now the wool is charged positively,
with a surplus of 3 +
Charging by friction

What has happened to the            +−
polythene?                 +    −   −
                               +
                            +   +−
There are now more −       −+
than + on the polythene:      −  −
(Count them!)
                            + + −−
                             −
                           +     +
So now the polythene is
charged negatively,
with a surplus of 3 −
Charging by friction
This is summed up
in the diagram-


Both objects are
equally charged,
with opposite charges
because electrons −
(only) have moved
from the wool to the
polythene.
 The overall effect of these charged particles
  produces a force
 If the electrical charge is ‘held’ on the
  surface of a material it is referred to as
  static electricity.
 This type of charge cannot move through
  out the material (an insulator)
 Charged objects exert an electrical force-
  similar charges repel each other and
  opposite charges attract.
 The electrical static charge can be produced
  in two ways- by friction and by induction.
 The attractive forces which keep the
  electrons (negative) close to the nucleus
  (positive) can be easily overcome.
 The electrons have relatively low mass
  compared to the nucleons and therefore it is
  only ever the electrons which can be
  transferred throughout a material or from
  one material to another.
Everyday examples of
electrostatic Page 111 and 112
Lightning- the bottom of a cloud can be
charged by friction of other air particles to
produce a large negative
                                    + + + +
electrostatic charge.
This can be discharged
on the positively charged       - - - - - -     -
upper surface of another
cloud or the positively
                               +   + + + +
charged ground.
 Electrically conductive truck tyres-
  These tyres drain any charge built up by
  passing air particles. This safety feature
  stops any sparks occurring which might
  prove explosive for any trucks carrying
  large amounts of fuel.
Air Purification- Industries release a huge
amount of air pollutants into the atmosphere.
Some of the fine
dust can be                  +
                                   Positives fixed

eliminated by                +
passing the                  +               +
exhaust through              +
                                           + +
charged                       + Electrons
electrostatic plates              repelled

which attract the                               Dust
                                              particle
charged smoke             25000 V                      0V


particles
Aims of the lesson

 Charge flow
  3.6.29 understand that an electric current is a
   flow of electrons and that it is in the opposite
   direction to that of a conventional current.
  3.6.30 recall that charge is measured in
   coulombs.
  3.6.31 recall and use the quantitative
   relationship between current, charge and
   time.
Factoids

  The charge on one Electron is
               1.60 x 10-19 C
 0.000 000 000 000 000 000 160 Coulombs

  There are roughly 1 x 1021 electrons in a
   1 m length of metal wire
 ~1 000 000 000 000 000 000 000 electrons
Current flow within a
circuit
 The flow of electricity in a circuit is due to the
  charge, Q, moving within the material (copper
  wires).

      The speed of the flow is known as the
              current (symbol I)

This is similar to the flow of water in a river being
  called a current- when it flows fast there is a
  strong current.
Current Definition
                                  How fast or the
                                  time it takes…

        Electrical Current is the rate of flow of
         charge past a given point in a circuit
 The number of
charged particles

              Current = Charge / Time
Symbol
Equation             I    =Q /    t
Units
Equation            Amps = Coulombs / Seconds
Electrical Current

  Reference Page 114
Circuit Diagrams

  Page 115
  3.6.34 describe and record
   diagrammatically simple electric circuits.
 - Draw a circuit diagram of the circuit
   which is set up by Mr McClelland
 - A simpler way of representing a circuit
   visually is using the set of electrical
   circuit symbols to represent each
   component. (make sure you know them!)
Draw the circuit


           Voltmeter in    Switch
           parallel over
           a bulb




          Two Bulbs
          in parallel
V


    A
Conventional Flow v Electron Flow
 Page 114- Electrical
  current is
  conventionally known
  as flowing from the
  positive terminal to
  the negative terminal.
 However, we refer to
  the electrons as
  flowing from the
  negative to the
  positive due to the
  attraction that the
  negative charge has
  to the positive
  terminal.
The Movement of
Electrons
  Conductors- The electrons are free to
   move within these materials, very little
   energy is required to free the electrons
   from their atoms. (Metals, carbon)
  Insulators- Charge cannot move through
   these materials as they have very few
   free electrons. (Plastics, ceramics,
   rubber)
Experiment- Electrical
Current
   Set up the following circuits and find the
    electrical current flowing at each point
    indicated.               Parallel
Series     +
Results

  Table   Point on the circuit   Current (A)

                                    0.25

                                    0.25
                                     0.5
                                     0.25

                                     0.25
Conclusion

  The ammeter measures the current
   flowing in the circuit as the electrons
   pass through it.
  For a series circuit the electrical current
   will be the same at every point
  For a parallel circuit the current entering
   the parallel section will be equal to the
   sum of the current of the branches of the
   parallel section (current splits)
Extra Syllabus Reference-

  3.6.36 recall that in a series circuit the
   current is the same everywhere.

  3.6.38 recall that in a parallel circuit the
   sum of the currents in the branches is
   equal to the current entering the parallel
   section.
So eh, what’s the current?
Series-              Parallel-
          +




 Current the same
  everywhere!!      Current into the junction is
                     equal to the current out
Examples of current in a
 circuit
 What is the reading on each of the
  following ammeters-


                                       A3
            3A
                            A1




                           A2
Bad Parents…

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Electrostatics and Current Electricity

  • 2. Aim of the lesson Static charge  3.6.26 recall that insulating materials can be charged by friction and explain this in terms of transfer of charge.  3.6.27 identify that positively charged objects have a deficiency of electrons and negatively charged objects have a surplus of electrons.  3.6.28 describe the dangers and use of electrostatic charge generated in everyday contexts.
  • 3. Text Book Reference  Physics CCEA pg 109-113  Electrostatics is the study of charges at rest
  • 4.
  • 5. Sir Ben Frank  Fly that kite…
  • 6. Electrostatics  The organisation of the parts of an atom has electrons orbiting a large central nucleus of nucleons (neutrons and protons) neutral atom positive ion negative ion These models are NOT to scale
  • 7.  If there is an unbalanced number of protons (positive carriers) compared to electrons (negative carriers) then the ion is called a charged particle - - - ++ ++ ++ - + - + - - + - - 3 electrons, 3 protons- 2 electrons, 3 protons- 4 electrons, 3 protons- no charge positive charge negative charge (deficiency of (surplus of electrons) electrons)
  • 8.
  • 9. Charging by friction In this diagram: The wool and polythene are each ‘uncharged’. What does this mean?
  • 10. Charging by friction The wool is ‘uncharged’, + because… + − − + …it has equal amounts + − + −+− of positive and negative − − charge. + + − −− Equal numbers of + + + and − On the wool On the polythene
  • 11. Charging by friction Equal numbers of + + and − on the wool: + − − + (Count them!) + − + −+− 7+ 7− − − + + − Equal numbers of + −− and − on the polythene: + + (Count them!) 3+ 3−
  • 12. Charging by friction If you rub the wool on +− the polythene, some + − − electrons (−) move from + + +− the wool to the polythene. −+ − − There are now more + + + −− than − on the wool: − + + (Count them!) So now the wool is charged positively, with a surplus of 3 +
  • 13. Charging by friction What has happened to the +− polythene? + − − + + +− There are now more − −+ than + on the polythene: − − (Count them!) + + −− − + + So now the polythene is charged negatively, with a surplus of 3 −
  • 14. Charging by friction This is summed up in the diagram- Both objects are equally charged, with opposite charges because electrons − (only) have moved from the wool to the polythene.
  • 15.  The overall effect of these charged particles produces a force  If the electrical charge is ‘held’ on the surface of a material it is referred to as static electricity.  This type of charge cannot move through out the material (an insulator)  Charged objects exert an electrical force- similar charges repel each other and opposite charges attract.
  • 16.  The electrical static charge can be produced in two ways- by friction and by induction.  The attractive forces which keep the electrons (negative) close to the nucleus (positive) can be easily overcome.  The electrons have relatively low mass compared to the nucleons and therefore it is only ever the electrons which can be transferred throughout a material or from one material to another.
  • 17. Everyday examples of electrostatic Page 111 and 112 Lightning- the bottom of a cloud can be charged by friction of other air particles to produce a large negative + + + + electrostatic charge. This can be discharged on the positively charged - - - - - - - upper surface of another cloud or the positively + + + + + charged ground.
  • 18.  Electrically conductive truck tyres- These tyres drain any charge built up by passing air particles. This safety feature stops any sparks occurring which might prove explosive for any trucks carrying large amounts of fuel.
  • 19. Air Purification- Industries release a huge amount of air pollutants into the atmosphere. Some of the fine dust can be + Positives fixed eliminated by + passing the + + exhaust through + + + charged + Electrons electrostatic plates repelled which attract the Dust particle charged smoke 25000 V 0V particles
  • 20. Aims of the lesson Charge flow  3.6.29 understand that an electric current is a flow of electrons and that it is in the opposite direction to that of a conventional current.  3.6.30 recall that charge is measured in coulombs.  3.6.31 recall and use the quantitative relationship between current, charge and time.
  • 21. Factoids  The charge on one Electron is 1.60 x 10-19 C 0.000 000 000 000 000 000 160 Coulombs  There are roughly 1 x 1021 electrons in a 1 m length of metal wire ~1 000 000 000 000 000 000 000 electrons
  • 22. Current flow within a circuit  The flow of electricity in a circuit is due to the charge, Q, moving within the material (copper wires). The speed of the flow is known as the current (symbol I) This is similar to the flow of water in a river being called a current- when it flows fast there is a strong current.
  • 23. Current Definition How fast or the time it takes…  Electrical Current is the rate of flow of charge past a given point in a circuit The number of charged particles Current = Charge / Time Symbol Equation I =Q / t Units Equation Amps = Coulombs / Seconds
  • 24. Electrical Current  Reference Page 114
  • 25. Circuit Diagrams  Page 115  3.6.34 describe and record diagrammatically simple electric circuits. - Draw a circuit diagram of the circuit which is set up by Mr McClelland - A simpler way of representing a circuit visually is using the set of electrical circuit symbols to represent each component. (make sure you know them!)
  • 26. Draw the circuit Voltmeter in Switch parallel over a bulb Two Bulbs in parallel
  • 27. V A
  • 28. Conventional Flow v Electron Flow  Page 114- Electrical current is conventionally known as flowing from the positive terminal to the negative terminal.  However, we refer to the electrons as flowing from the negative to the positive due to the attraction that the negative charge has to the positive terminal.
  • 29. The Movement of Electrons  Conductors- The electrons are free to move within these materials, very little energy is required to free the electrons from their atoms. (Metals, carbon)  Insulators- Charge cannot move through these materials as they have very few free electrons. (Plastics, ceramics, rubber)
  • 30. Experiment- Electrical Current  Set up the following circuits and find the electrical current flowing at each point indicated. Parallel Series +
  • 31. Results  Table Point on the circuit Current (A) 0.25 0.25 0.5 0.25 0.25
  • 32. Conclusion  The ammeter measures the current flowing in the circuit as the electrons pass through it.  For a series circuit the electrical current will be the same at every point  For a parallel circuit the current entering the parallel section will be equal to the sum of the current of the branches of the parallel section (current splits)
  • 33. Extra Syllabus Reference-  3.6.36 recall that in a series circuit the current is the same everywhere.  3.6.38 recall that in a parallel circuit the sum of the currents in the branches is equal to the current entering the parallel section.
  • 34.
  • 35. So eh, what’s the current? Series- Parallel- + Current the same everywhere!! Current into the junction is equal to the current out
  • 36. Examples of current in a circuit  What is the reading on each of the following ammeters- A3 3A A1 A2