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
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
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
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