Here are the circuit diagrams drawn as requested:
1.
+ -
2.
+ -
3.
A
V
+ -
Now let's assemble the circuits using the appropriate components.
Thursday, 16 September 2010
CIRCUITS: diagrams & assembly
Draw the following circuit diagrams in the spaces
provided AND when you have finished, assemble them:
1. Two cells in series
+ -
2. Three lamps in parallel
+ -
3. A switch and a lamp in series
S
L
+ -
Now let's assemble the circuits using the appropriate components.
1. ELECTROMAGNETISM
1. Define the following terms & phrases (charge, static electricity, charging by friction/contact/induction,
conductor, insulator, uniform/non-uniform charge distribution, earthing and electrical discharge)
2. Describe the behaviour of like and unlike charges.
3. Name and give symbols for the following: DC power supply, cell, battery, switch, lamp,
resistor, variable resistor, wires joined, wires crossing, ammeter, voltmeter & fuse
4. State the symbol and metric unit for: charge, current, voltage, resistance & power
5. Define the following terms and phrases: Ohm’s law, DC electricity, series, parallel, current
rules and voltage rules.
6. Describe the differences and similarities in the way ammeters and voltmeters are used.
7. Draw and interpret DC circuit diagrams
8. Solve problems using V = IR, P = VI, P = E and Rtotal = R1 + R2
t
9. Describe the magnetic field patterns around permanent magnets, the earth, currents and
coils.
10. State the symbol and unit for magnetic field.
11. Use the right hand grip rule to determine relative field (B) and current (I) directions.
12. Describe how the magnetic field due to a current in a straight wire varies with the size of
current and the distance from the wire.
13. Solve problems using B = µ0I
2 πd
Thursday, 16 September 2010
4. THE LANGUAGE OF ELECTRICITY
Term Definition Word list
Charge an electrical quantity based on an excess or deficiency of electrons
static
a form of electricity where charge does not flow continuously
electricity
Thursday, 16 September 2010
7. CHARGING OBJECTS
Based on atomic structure
Electron (-ve charge)
Neutron
Proton (+ve charge)
The process Empty space
1. Charge transfer - When two objects are in contact with each other, one object can
transfer electrons to the other object. Protons are not transferred because they are
“locked” into the nucleus.
2. Charge imbalance - When the two objects are moved away from each other the
process of charge transfer is unable to be reversed.
• Positively charged objects have had electrons removed
• Negatively charged objects have gained electrons
Oppositely charged objects attract each other. Those with like charges repel.
Thursday, 16 September 2010
8. CHARGE INTERACTION
Oppositely charged objects Objects with the same
attract each other charge repel each other
+ - + + - -
+ - + + - -
Demo: The Van der Graaf Generator
Thursday, 16 September 2010
9. EXAMPLES
Read p52 and 53 (Y10 Pathfinder) and then offer some examples to the class
discussion:
Static electricity
around us
The History of Electricity Generation
Thursday, 16 September 2010
10. LIGHTNING Warm air currents ascend. Ice
crystals descend removing electrons
from cloud particles in this zone.
A zone of positively charged cloud
particles results
At ground level the air becomes
ionized (by losing electrons) and
these positively charged particles
are attracted to the negatively
charged base of the cloud to give
rise to a lightning bolt (an upstrike)
Thursday, 16 September 2010
14. CHARGING OBJECTS
Methods of charging
Induction - the object being charged is not in contact with the object doing the
charging (usually a rod or a ruler). It involves charge transfer to or from the earth to
generate the charge imbalance in the object being charged. A charge imbalance is a
non-uniform charge distribution
Eg.
-- ++++
----
The problem with moisture in the air:
Moisture prevents objects from holding a
+ + charge because it transfers charge to or
+ + from the object resulting in a neutral
This symbol object.
represents
a
connection
to the earth
Contact - the object being charged is contacted by the other object and charge is
transferred directly from one object to another.
Friction - the object is rubbed by a material that has a greater or lesser affinity for
electrons and a transfer takes place. It is more the contact than the friction that is
necessary for the charging to take place.
Thursday, 16 September 2010
15. The importance of the material
Conductors - are materials that allow charges to flow through them. They do not
hold a static charge because any charge imbalance is easily conducted away.
Insulators - are materials that doe not allow charges to flow through them. They will
hold a static charge because the charge imbalance is not easily conducted away.
Example -
ESA: Ex 15A Q.1 ESA: Ex 15B Q.1, 2 & 3
Thursday, 16 September 2010
19. THE ELECTRICAL CIRCUIT -
introducing the idea of the
electron pump
Thursday, 16 September 2010
20. 1. What is an electric current?
2. What are the two requirements necessary for an electric
current to exist?
Power Supply
+ -
A conducting path
Thursday, 16 September 2010
21. THE GRAVITY MODEL
http://regentsprep.org/Regents/physics/phys03/bsimplcir/default.htm
A
B
1.Which part of the model represents the power supply?
2. Which part of the model represents the component?
3. What type of current is being modelled?
Thursday, 16 September 2010
22. THE WATER MODEL
1.Which part of the model represents the power supply?
2. Which part of the model represents the conducting path?
3. Which part of the model represents charge?
Thursday, 16 September 2010
23. THE BIKE MODEL
C
A
B
1.Which part of the model represents the power supply?
2. Which part of the model represents the conducting path?
3. Which part of the model represents charge?
Thursday, 16 September 2010
24. THE BIKE MODEL
one link
THINK OF A LINK AS REPRESENTING A COULOMB OF
CHARGE
1. In terms of this model, what do you think is meant by the
term “current” ??
Thursday, 16 September 2010
25. ELECTRIC CIRCUITS
Requirements: Power Supply
a power supply
conducting path around which charge
(electrons or ions) can flow.
+ -
components (and sometimes meters)
A component
Current A conducting path
is a flow of electrons through a circuit
Two types:
AC - Alternating current (electrons vibrate back and forth in wires)
DC - Direct current (electrons flow in wires in one direction only)
Conventional current - the direction in which positive charges would flow in wires
if they could.
Conventional current is from positive to negative in a circuit (see diagram above)
http://regentsprep.org/Regents/
physics/phys03/bsimplcir/default.htm
Thursday, 16 September 2010
26. ELECTRIC CURRENT
Current - is the rate of flow of electrical charge
- it is the number of coulombs of electrical charge that passes a point in
one second. A coulomb is 6.25 x 1018 charges
- I = electric current (measured in amps, A) by an ammeter:
Red V Black
Connecting an ammeter + -
I
I
A
Red Black
For charge to flow around an electrical circuit there is a need for a voltage source and
a conducting path that is continuous and connects the positive to the negative
terminal of the power supply. - +
Example
charge flows through the
circuit as indicated by the
arrows
Thursday, 16 September 2010
27. VOLTAGE
Voltage
• Voltage (V) is a measure of the energy lost or gained between two points in a
circuit.
• It is measured in the units volts , (V)
where V = potential difference or voltage (Volts, V)
V = ∆Ep
q ∆Ep = change in potential energy that a charge
experiences when it moves from one side to the
other side of a component (Joule, J)
q = the unit of charge (Coulomb, C)
Unit of Voltage: Joule per Coulomb or Volt
(JC-1) or (V)
Example
V
Consider the voltage across a lamp: -
+
A B
1A
If V = 6V then a coulomb of charge has 6J more electrical potential energy at
point A than it does at point B
Thursday, 16 September 2010
28. Notes CIRCUIT SYMBOLS
demo of circuit components ->
+ - V
A •
Two wires joined Two wires crossing
Cell Lamp
Battery (two cells in
Switch
series)
Battery (several
Diode
cells)
Voltmeter Ammeter
Resistor Power supply
variable resistor
fuse
(rheostat)
Thursday, 16 September 2010
29. RE
SI
& ST
OH A N
LA M’ CE
W S
Thursday, 16 September 2010
30. IN
TR
O DU
CT
IO
N
Thursday, 16 September 2010
34. FACTORS THAT AFFECT RESISTANCE
Also, some materials conduct electricity better than others Eg. Copper is better than iron
Thursday, 16 September 2010
35. CONDUCTORS & INSULATORS
In a conductor, electrons In an insulator,
are free to flow electrons are fixed
_______________
Label the materials that the _______________
arrows are pointing to
Thursday, 16 September 2010
36. THE VOLTAGE-CURRENT RATIO
1. Consider a lamp in an electrical circuit:
12V
2A
12V represents the energy difference across the lamp. This drives electrons
through the lamp at the rate (or “speed”) of 2A. The voltage:current ratio is
_____
2. Consider a different lamp in an electrical circuit:
12V
1A
This lamp has higher resistance because 12V across this lamp can only drive
electrons through the lamp at a rate of 1A. The voltage:current ratio is _____
This example shows that the greater the voltage:current ratio then the greater the
resistance is. Resistance is the voltage:current ratio
Thursday, 16 September 2010
37. RESISTANCE
Definitions
1. Resistance, R is a measure of the “electrical friction” in a conductor. (the
opposition to the flow of current)
2. It is the ratio of the voltage across a conductor to the current through it.
Resistance = Voltage
Current R=V Unit of resistance
I is the ohm, Ω
V
I R
Resistance is given by the slope or
gradient of a voltage - current graph
Example
In an experiment, the voltage across a lamp is measured and recorded as the current
is increased 1 A at a time. Calculate the resistance of the lamp.
V (V)
24
20
16
12
8
4
0 1 2 3 4 5 6
I (A)
Thursday, 16 September 2010
38. WHATS HAPPENING TO THE RESISTANCE AS THE CURRENT INCREASES?
24 A conductor that retains a constant
1 V (V) 20 temperature as the current is increased:
16
12
8
4
0 1 2 3 4 5 6 I (A)
A conductor that is allowed to heat
24
2 V (V) up as the current is increased
20
16
12
8
4
I (A)
0 1 2 3 4 5 6
A conductor that is cooled progressively
3 V (V) 24
20 as the current is increased
16
12
8
4
I (A)
0 1 2 3 4 5 6
Thursday, 16 September 2010
41. LIMITATIONS OF OHM’S LAW
24
V (V) 20
When a temperature of a lamp increases its
16 resistance increases
12
8
4
I (A)
0 1 2 3 4 5 6
For most conductors, as the temperature increases the increased vibration of particles
impedes the flow of electrons. Resistance in the conductor will therefore increase. The
graph slopes upwards.
V (V) 24
The resistance of a thermistor decreases as its
20
16
temperature decreases
12
8
4
I (A)
0 1 2 3 4 5 6
Thursday, 16 September 2010
42. BASIC RESISTANCE PROBLEMS
1. What is the resistance of a bulb it a 240 V supply causes a current of 2 A to flow
through it?
2. What current flows through a heating element of 40Ω resistance when the element
is plugged into a 240 V supply?
3. If a current of 3 A is flowing in a resistor across which there is a voltage of 6 V,
what is the resistance?
4. What current must be flowing through a lamp of 0.5Ω resistance if there is a voltage
of 6V across it?
5. A current of 2 A flows through a 6Ω resistor. What is the voltage across it?
6. What voltage is needed it a current of 5A is to flow through a resistance of 3Ω?
Thursday, 16 September 2010
43. RESISTANCE CALCULATIONS
Resistors which are connected end to end are in series with one
another
R1 R2
The total resistance of the series combination, Rs is the sum of the
resistances R1 and R2.
For two or more resistors in series: Rs = R1 + R2 + ...........
Resistors which are connected side by side are in parallel with each other.
R1
R2
The total resistance of the parallel combination, Rp is less than any individual
resistor in the combination.
For two or more resistors in parallel 1 1 1 + ....
the total resistance,Rp is given by: RP = R1 + R2
Thursday, 16 September 2010
46. CIRCUITS: diagrams & assembly
Draw the following circuit diagrams in the spaces
provided AND when you have finished, assemble them:
1.
+ -
2.
+ -
3.
A
V
+ -
Voltmeters are connected _________ components,
ammeters are connected _____ a circuit
Thursday, 16 September 2010
47. CHARACTERISTICS OF SERIES & PARALLEL CIRCUITS
Series Parallel
+ -
+ -
+ -
+ -
components connected each component has its own
1._ 1._ connection with the power
one other the other.
supply
2._ Single pathway 2._ more than one pathway
3._ No junctions 3._ One or more junctions
Thursday, 16 September 2010
48. http://phet.colorado.edu/simulations/ CIRCUIT CONSTRUCTION
sims.php?
sim=Circuit_Construction_Kit_DC_Only
1. Enter the URL (above) into the address bar of your internet browser.
2. Use the simulation tools to construct each of the following 3 circuits (ensure that you use
identical lamps and an the same power supply for each circuit).
3. Record the current in each circuit and explain your observation.
4. Repeat this exercise for the second set of 3 circuits.
1 2 3
+ - + - + -
A A A
3
+ -
2
A
1 + -
+ - A
A
Thursday, 16 September 2010
51. VOLTAGE & CURRENT IN SERIES CIRCUITS
+ -
VT
A1 A3
I1 I3
I2
A2
V1 V2
Current in series is constant I1 = I2 = I3
Voltage in series is shared VT = V1 + V2
Note
Voltage is shared in proportion to the size of the resistance
Thursday, 16 September 2010
52. PARALLEL CIRCUITS
+ -
Current in parallel is shared
IT VT IT
R1
IT = I1 + I2
I1 in other words “charge splits
up as it enters a junction in
a circuit”
V1
R2
I2 Voltage in parallel is constant
V2 VT = V1 = V2
Note
Current is shared in an inverse proportion to the size of the resistance.
For example:
If R1 = 5 and R2 = 10
and IT = 3
“Double the resistance then halve the current”
then I1 = 2 and I2 = 1
Thursday, 16 September 2010
53. SIMPLE CIRCUIT CALCULATIONS
Example 1
+ 8V -
A3 = ________
3A A1 V1 V1 = ________
2A
A2 R1 V2 = ________
A3 R2
Rules used V2
____________________________________________________________________
____________________________________________________________________
Example 2
+ 8V -
3V
V1 V2 V1 = ________
R1
Rule used ___________________________________________________________
Thursday, 16 September 2010
55. ADVANCED CIRCUIT CALCULATIONS
Examples
+ 9V -
1
A1 V1 A3
5Ω 10Ω
A2
V2 V3
For the circuit represented by the circuit diagram above, what is the reading on:
(a) V1
(b) A2
(c) V2
(d) V3
Thursday, 16 September 2010
56. 2 + 15V -
V1
5Ω A3
V2 A1
V3
R 10Ω
A2
For the circuit represented by the circuit diagram above, what is the reading on:
(a) V3 if V2 = 10 V
(b) A1
(c) A2
(d) A3
(e) What is the value of resistor R?
Thursday, 16 September 2010
57. 3 + 12V -
V1
1A 2Ω 4.8Ω V3
A1
V2
3Ω
A2
For the circuit represented by the circuit diagram above, what is the reading on:
(a) V1
(b) V2
(c) V3
(d) A2
Thursday, 16 September 2010
58. RESISTORS IN SERIES
+ -
R1
RT = R1 + R2
R2
Examples
1 2
25 Ω 30 Ω 50 Ω
100 Ω 100 Ω 100 Ω
• •
Total resistance = Total resistance =
As we add resistors in series the resistance increases and therefore the current
drawn decreases
As we add resistors in parallel the resistance decreases and therefore the current
drawn increases
Thursday, 16 September 2010
65. + 9V -
One of these meters has
IT a very high resistance
The other meter has a
A low resistance.
Which is which?
V Explain your answer
Thursday, 16 September 2010
66. METERS
Ammeter
+ 9V -
1. connected in series with IT
other components
A
2. has low resistance so
that it doesn’t slow the
current that it is supposed
to be measuring
Voltmeter
1. connected in parallel with other V
components
2. has high resistance so that it
doesn’t allow much current to flow
through it. This would reduce the
current and voltage through the
component. It is supposed to be
measuring the voltage
Thursday, 16 September 2010
68. POWER
• Power is the rate at which electrical energy is transferred into other forms of
energy.
• It is the amount of work done per second
E E = the amount of energy converted or work done (J)
P = E
t P t t = the time taken (s)
• It can be shown that the electrical power supplied to a device is given by:
P P = power (watts, W) (1W = 1 Js-1)
P = VI V I V = Voltage (volts, V)
I = Current (amps, A)
P = Power (Watts, W)
Thursday, 16 September 2010
69. POWER & ENERGY
Total energy used by a component/appliance
can be calculated from the equation:
E = P.t
When the power value of the component/appliance is known and this value does not
change over time.
If power changes over time then this change can be graphed.
P (W)
14 E = Area under the graph
12
10
8
E = 0.5 (9 + 13) = 4.4 J
6 10
4
2
0 2 4 6 8 10 t (s)
Thursday, 16 September 2010
70. TOTAL POWER USAGE in a parallel circuit
Example
The power usage of the 4 lamps in parallel shown in the circuit below can be
calculated in two ways:
(i) Use the total voltage (supply voltage) and the total current (current drawn from
the supply) to calculate power.
(ii) Add the power usage of each of the components in parallel.
(i) lamps 1 & 2: I = P
12 V V
= 6/12
= 0.5 A
12 V
P1 6W Lamps 3 & 4: I = P
V
12 V = 12/12
P2 6W
=1A
12 V IT = I1 + I2 + I3 + I4 = 0.5 + 0.5 + 1 + 1 = 3A
P3 12 W P = VTIT = 12 x 3 = 36 A
12 V
P4 12 W (ii) PT = P1 + P2 + P3 + P4
= 12 + 12 + 6 + 6
= 36 W
Thursday, 16 September 2010
71. LAMP BRIGHTNESS IN CIRCUITS
Three main points
(i) The brightness of a lamp depends on its power output since for a lamp, power is
the rate at which electrical energy is converted into light (and heat)
(ii) In a circuit which has values of voltage and current, it is both the voltage and
current that determine brightness.
(iii) The lamp’s resistance will determine that voltage:current ratio that it possesses
Example:
The series circuit (below), shows 2 identical lamps. A third identical lamp is
added to the circuit. Explain how the brightness of the lamps in the circuit
changes
12 V
+ -
Thursday, 16 September 2010
73. POWERING THROUGH THE QUESTIONS
TV Stereo Jug Heater Stove torch downlight
Voltage (V) 240 240 240 6
Current (A) 0.3 0.02 8 0.05
Resistance (Ω) 250 450
Power (W) 1000 1200 1800 0.3 140
Running time
20 min 20 min 10 min 3h
(s)
Energy (J) 1000 125000 300000
Thursday, 16 September 2010
74. “PARALLEL WITHIN SERIES”
0.5 A
+ 9V -
A 9 V battery is connected in the
circuit shown. 10Ω
A current of 0.5 A is found to 0.1 A
pass through the 10Ω resistor. 40Ω
X
(a) Calculate the voltage across the 10Ω resistor.
(b) Show that the voltage across the parallel combination of resistors is 4.0 V.
(c) If 0.1 A passes through the 40Ω resistor, determine the current through resistor X.
(d) Show that the resistance of resistor X is 10Ω.
(e) Determine the heat energy generated per second in the whole circuit.
Thursday, 16 September 2010
75. PARALLEL CIRCUIT IN ACTION
A car has two tail lights and two brake lights connected as shown in the diagram:
(a) Calculate the resistance of:
(i) a tail light
(ii) a brake light
(b) Calculate the current supplied by the battery when both S1 and S2 are closed.
(c) When the driver takes her foot off the brake S2 is opened state what
happens to the size of the current from the battery and give a reason
for your answer.
Thursday, 16 September 2010
78. answers “PARALLEL WITHIN SERIES”
(a) 5V
(b) V in series is shared. The combination of the 40Ω resistor and X are in series
with the 10Ω. Therefore V of the combination is 9 - 5 = 4
(c) Current through X = 0.5 - 0.1 = 0.4A because current in parallel is shared. The
total current flowing from the power supply is shared out between the 40Ω
resistor and X.
(d) I through X = 0.4A and V across X = 4V (since voltage in parallel is constant).
R = V/I = 4/0.4 = 10Ω
(e) “Heat energy per second” is the definition of power. For the whole
circuit, I = 0.5A and V = 9V. P = VI = 9 x 0.5 = 4.5W
PARALLEL CIRCUIT IN ACTION
(a) The current through a tail light needs to be calculated first:
P = VI => I = P/V = 6/12 = 0.5A For a tail light, R = V/I = 12/0.5 = 24 Ω
For a brake light, P = VI => I = P/V = 12/12 = 1A R = V/I = 12/1 = 12 Ω
(b) I total = 2 x 0.5 + 2 x 1 = 3 A
(c) Less current flows through the battery because there is now more resistance in
the circuit because of the reduction in the number of pathways available for
charge to flow.
Thursday, 16 September 2010
80. THE MAGNETIC FIELD AROUND A BAR MAGNET AND
THE EARTH’S MAGNETIC FIELD
Thursday, 16 September 2010
81. ---> Demo c bar magnet & major magnet
WHAT IS MAGNETISM?
• Magnetism is caused by moving electrons. (The smallest magnetic field is
produced by the motion of 1 electron)
• When electrons move in a common direction, a magnetic field is produced
(sometimes called a magnetic force field)
• A force will be exerted on an iron object placed in a magnetic field.
• A magnetic field is a region in space where a magnetic force can be detected.
The magnetic field around a bar magnet
Charm compass
S
Magnetic field lines The compass needle is
itself a tiny magnet (the
N North pole of this magnet
points towards the South
end of the magnet)
Strong magnetic field (high density of lines)
Thursday, 16 September 2010
82. THE EARTH’S MAGNETIC FIELD
θ (angle of declination) = 11o
Geographic
North Magnetic
South
compass
S
N
Earth’s axis
• θ changes with time
• Angle of Dip - is the angle that the field lines make with the ground. At the
equator, the angle of dip is zero. Near the poles the angle of dip is close to 90
degrees.
Thursday, 16 September 2010
83. THE EARTH’S MAGNETIC FIELD IS ESSENTIAL FOR
LIFE ON THE PLANET.
Home to millions of species including humans, Earth is currently the only place in the
universe where life is known to exist. The planet formed 4.54 billion years ago, and life
appeared on its surface within a billion years. Since then, Earth's biosphere has
significantly altered the atmosphere and other abiotic conditions on the planet,
enabling the proliferation of aerobic organisms as well as the formation of the ozone
layer which, together with Earth's magnetic field, blocks harmful solar
radiation, permitting life on land.
The physical properties of the Earth, as
well as its geological history and orbit,
have allowed life to persist during this
period. The planet is expected to continue
supporting life for at least another 500
million years.
Thursday, 16 September 2010
86. MAGNETIC THEORY
Ferromagnetic materials (Iron, Cobalt and Nickel) can be permanently magnetised.
Electrons spinning in atoms have magnetic fields around them. They set up tiny North
and South poles. Such an arrangement for an electron is called a dipole moment.
[Illustrate a mag. dipole and mention Exchange Coupling]
N
N
e
S S
For most elements:
magnetic fields cancel.
Iron, Cobalt and Nickel:
Electron structure is such that there is a resultant magnetic field produced by each
atom. These atoms are sometimes called atomic magnets.)
Thursday, 16 September 2010
87. DOMAINS
Regions in a metal where the orientation of the magnetic dipoles is the same are
called domains.
A domain
Unmagnetised Iron Here, a large number
of iron atoms
=> Domains are (magnetic dipoles)
scrambled are aligned.
Partially
magnetised
S N
Fully magnetised
=> the orientation of
the domains is the S N
same
Thursday, 16 September 2010
89. MAGNETISING AND DEMAGNETISING [Solenoid Demo]
“Lining up” the domains - Magnetising
• Stroke the object end to end with a permanent magnet , in the same
direction, using the same pole of the magnet.
• Hold the object inside an D.C or A.C solenoid (Domains line up in the
direction of the magnetic field)
“Scrambling” the domains - Demagnetising
Heat or hammer the magnet (This disturbs the alignment of the domains)
[CAN ALSO BE DEMONSTRATED WITH THE SOLENOID]
“Domains are induced into alignment”
- Picking up iron objects
Thursday, 16 September 2010
95. WIRES
A circular magnetic field is formed around a straight current - carrying conductor:
3D View
I View from above
The direction of the magnetic
field lines is given by the
Right-hand Thumb Rule
•
( “•” represents current directed out of the page)
The right hand thumb rule:
Thumb = direction of the electric current
Curled fingers = direction of the circular magnetic field
Thursday, 16 September 2010
97. B = Magnetic field strength (in Tesla,T)
I = Electric current in the wire (in Amps,A)
B = µ0I
2 d π µo= the permittivity of free space (the ability of a
material to support a magnetic field (TmA-1)
d = Distance from the wire (in metres, m)
Note
1. Reversing the direction of the current reverses the
direction of the magnetic field.
2. Magnetic field strength (symbol, B) is measured in
NA-1m-1 or Tesla,T.
3. As the current in the wire, I increases the strength of the magnetic field
increases
BαI i.e. B is proportional to I
4. As the distance,d from the wire increases the strength of the magnetic field
decreases.
B α 1/d i.e. B is inversely proportional to d
Thursday, 16 September 2010
98. Example
A special meter able to measure the magnetic field strength at any given point in the
vicinity of a wire is shown below (taking a reading). It measures the magnetic field
strength as 8 x 10-4 T at a distance of 0.01m from the centre of the wire. The current
through the wire is 5 A.
Calculate the value of the constant µo.
Exercises
B I d µo
5 x 10-5 T 2A 20 mm 3.14 x 10-6
6 x 10-5 T 3A 0.159 m 2 x 10-5 TmA-1
7.2 x 10-5 T 3.11 A 2.2 cm 3.2 x 10-6 TmA-1
1.05 x 10-3 3A 20 mm 4.4 x 10-5 TmA-1
Thursday, 16 September 2010
101. THE SOLENOID
The magnetic field of a solenoid is
similar in shape to that of a bar
magnet:
Draw the field lines
If the current is known, the poles of the solenoid can be determined using the right
hand thumb rule applied earlier to the straight wire:
Complete this:
Field lines are parallel in the core of the solenoid which --> the magnetic field in the
core is uniform.
The density of magnetic field lines is greatest in the core --> the magnetic field
strength is greatest in the core.
Thursday, 16 September 2010
102. STRENGTH RULZ
Factors affecting the strength of the magnetic field:
1. Increasing the current increases the magnetic field strength.
2. Increasing the number of turns of wire per given length of the
electromagnet increases the magnetic field strength
Predicting North and South poles:
Thumb points to North
pole of the solenoid
from inside the coil
Curled fingers indicate
the direction of the
current
Thursday, 16 September 2010
103. ELECTROMAGNETS
A solenoid which contains an iron core is called an electromagnet.
Adding an iron core increases the strength of the magnetic field because
the iron core itself becomes magnetised and adds to the magnetic field of
the solenoid.
Uses of electromagnets
1. Electromagnets in relays are able to open and close electrical circuits (eg. starter
motor circuit in a car).
2. Used in scrap yards to lift car bodies.
3. Create the ringing sound in electric bells.
4. Electromagnets in the recording heads of tape recorders are used to magnetise
the audio tape during recording.
Thursday, 16 September 2010
104. THE COIL GUN
Induced magnetism
An unmagnetised object will have have its
domains aligned and therefore develop a north
and south pole. The object can be picked up
by the magnet because opposite poles attract.
Cross-section of coil
Attraction to
x x x x x x x x
North of coil
Attraction to South of coil
N S N
- - - - - - - -
North end of coil South end
The dipoles in the object change along the rod as the rod is drawn into the coil and it
is this dipole change which pulls the rod into the coil
Thursday, 16 September 2010
110. PLAYING AROUND WITH STATIC ELECTRICITY
1 plastic rod (charged by rubbing with a cloth)
small pieces
of torn paper
Observation:
Explanation:
2 Balloon rubbed against hair
Removed from head and then brought back to hair
Observation:
Explanation:
Thursday, 16 September 2010
111. 3
Balloon rubbed against jersey
Release
Observation:
Explanation:
cotton
(a) Each balloon charged separately by rubbing against
4
the sleeve of a jersey
(b) Holding the balloons by the cotton, release them,
allowing them to come close to each other.
Observation:
Explanation:
Thursday, 16 September 2010
112. 5
(a) Straw, charged at both
(b) Straw, also charged using a
ends (using a woollen
woollen cloth held horizontally
cloth)
and brought close
(c) Repeat (b) using a silk cloth.
Observation:
Explanation:
Charged plastic rod is held near a thin stream of water
6 Observation:
Explanation:
http://phet.colorado.edu/new/simulations/sims.php?
sim=Balloons_and_Static_Electricity
Thursday, 16 September 2010
113. Equipment
CHARGING OBJECTS dry cloth/jersey
Cap
perspex rod
Insulating material
ebonite rod
electroscope
Body of electroscope
Leaf
Base
Aim
to charge an electroscope by both induction and by contact and to draw charge distribution
diagrams
Method
1. Follow the instructions below
2. Write observations as you perform each step
3. Complete the diagrams only after recording the observations (you may need some help with
these)
Part 1 - Charging by induction
1. Charge the rod by rubbing it with a dry cloth/jersey and hold the rod
near the cap of the electroscope ++++
----
Observation:
+ +
+ +
If the rod was positively charged the charge distribution diagram would look like this:
Thursday, 16 September 2010
114. Complete the diagram to show how charges would distribute on the electroscope should the rod
be negatively charged.
----
2. With the rod in this position, earth the cap with your finger.
Observation: ++++
----
+ +
+ +
This symbol
Complete the diagram to show how charge moves represents
a
when the cap of the electroscope is earthed connection
to the earth
Thursday, 16 September 2010
115. Draw the charge distribution diagram (by adding to ++++
the existing diagram on the right) showing the ----
situation once this charge movement has finished.
+ +
+ +
3. Unearth the cap of the electroscope without removing the
charged rod
Observation:
Draw the resultant charge distribution and the new
position of the leaf on the diagram (right).
4. Remove the charged rod
Observation:
Finally, complete the diagram (right).
Thursday, 16 September 2010
116. Part 2 - Charging by contact
Method
1. Follow the instructions below
2. Write observations as you perform each step
3. Complete the diagrams only after recording the observations (you may need some help with
these)
1. A positively charged rod is held near the cap of the electroscope. ++++
2. The rod makes contact with the cap.
3. The rod is removed.
Thursday, 16 September 2010
117. Lab 12 ALL CHARGED UP Equipment
dry cloth/jersey
Cap perspex rod
Insulating material ebonite rod
electroscope
Body of electroscope
Leaf
Base
Aim
to charge an electroscope by both induction and by contact and to draw charge distribution
diagrams
Method
1. Follow the instructions below
2. Write observations as you perform each step
3. Complete the diagrams only after recording the observations (you may need some help with
these)
Part 1 - Charging by induction
1. Charge the rod by rubbing it with a dry cloth/jersey and hold the rod
near the cap of the electroscope ++++
----
Observation:
The leaf of the electroscope springs up.
+ +
+ +
If the rod was positively charged the charge distribution diagram would look like this:
Thursday, 16 September 2010
118. Complete the diagram to show how charges would distribute on the electroscope should the rod
be negatively charged.
Electrons at the cap are
repelled by the negatively ----
++++
charged rod.
- -
- -
Electrons at the cap are held in
position by the positively
charged rod. The earth supplies
electrons to the positively
charged leaf and lower stem.
2. With the rod in this position, earth the cap with your finger.
Observation: -- ++++
----
Leaf of the electroscope drops
+ +
+ +
This symbol
Complete the diagram to show how charge moves represents
a
when the cap of the electroscope is earthed connection
to the earth
Thursday, 16 September 2010
119. Draw the charge distribution diagram (by adding to ++++
the existing diagram on the right) showing the - - - -
situation once this charge movement has finished.
-
The cap and leaf now have +
- +-
+ +
no overall charge. -
Electrons on the cap are
still held in position.
3. Unearth the cap of the electroscope without removing the ++++
charged rod - - - -
Observation:
Leaf of the electroscope remains in the “dropped”
position. The charge distribution has not changed -
+ +
- -
+
- +
Draw the resultant charge distribution and the new
position of the leaf on the diagram (right).
Negative charge redistributes itself
4. Remove the charged rod around the metal parts of the
electroscope leaving the stem and - -
Observation: leaf with an overall negative charge
The leaf of the electroscope springs up. - -+
+
- -
+ + -
-
Finally, complete the diagram (right).
Thursday, 16 September 2010
120. Part 2 - Charging by contact
Method
1. Follow the instructions below
2. Write observations as you perform each step
3. Complete the diagrams only after recording the observations (you may need some help with
these)
1. A positively charged rod is held near the cap of the electroscope. ++++
- - - -
Charge separation occurs. Positive
repels positive at the stem/leaf
+ +
+ +
2. The rod makes contact with the cap. -
Electrons migrate up
+ + into the rod
+ +
3. The rod is removed. + + +
The electroscope is now left with
+ + an overall positive charge.
+ +
Thursday, 16 September 2010
121. SPARKS
12 Physics > resources > electricity > DC
electricity > videos
Thursday, 16 September 2010
122. THE VAN DER GRAAF
Label the picture of the Van der Graaf (left) using the labels in
the box below
______________
Lower roller
______________
Belt - A piece of surgical tubing
______________
Output terminal - an aluminium or steel sphere
Upper roller - A piece of nylon
______________
Motor
______________
Upper brush - A piece of fine metal wire
______________ Lower Brush
______________
• When the generator is turned on, the electric motor begins turning the belt.
• The belt is made of rubber and the lower roller is covered in silicon tape. Silicon has
a greater affinity for electrons than rubber and so it captures electrons from the
belt. The belt in turn must capture electrons from the dome, leaving the dome
positively charged.
Reference: http://science.howstuffworks.com/vdg3.htm
Thursday, 16 September 2010
123. THE VAN DER GRAAF - OBSERVATIONS & EXPLANATIONS
1. Small dome held close to generator dome
Drawn observation Explanation
2. Hair stands on end when contact is made with the generator
dome
Drawn observation Explanation
3. Aluminium foil plates flying of the top of the generator dome
Drawn observation Explanation
Thursday, 16 September 2010
126. ADDING BULBS IN PARALLEL
1. Set up each of the following circuits, one after the other (making a mental note of
the brightness of the lamps in the circuit.
2. For each circuit read the ammeter and record the current in the space provided.
1 2 3
8V 8V 8V
+ - + - + -
A A A
Current = ______ A
Current = ______ A
Current = ______ A
Observation
Explanation
Thursday, 16 September 2010
127. ADDING BULBS IN SERIES
1. Set up each of the following circuits, one after the other (making a mental note of
the brightness of the lamps in the circuit.
2. For each circuit read the ammeter and record the current in the space provided.
1 2 3
+ - + - + -
A A A
Current = ______ A Current = ______ A Current = ______ A
Observation
Explanation
Thursday, 16 September 2010
128. CURRENT IN THE SERIES CIRCUIT IS CONSTANT
Aim
to look for a pattern in the current through bulbs and resistors in a series circuit.
1. Use ONE ammeter in the three different places shown in the circuit diagram.
2. Without changing the setting on the power pack or the variable resistor write the
current readings in the spaces provided (below):
A1 + 8V -
A1 = ______ A
A3 A2 = ______ A
A3 = ______ A
A2
Equation
Thursday, 16 September 2010
129. CURRENT IN THE PARALLEL CIRCUIT IS SHARED
Aim
to look for a pattern in the current through bulbs and resistors in a parallel circuit.
1. Use ONE ammeter in the each of the four places shown in the circuit diagram.
2. Without changing the setting on the power pack record your results below:
+ 8V -
Results
A1 A4 A1 = ____ A
A2 = ____ A
A2
A3 = ____ A
A4 = ____ A
A3
Conclusion
Current in a parallel circuit is ____________ .
Equation relating the currents
Thursday, 16 September 2010
130. VOLTAGE IN THE SERIES CIRCUIT IS SHARED
Aim
to look for a pattern in the voltages across bulbs and resistors in a series circuit.
1. Set up the circuit (below)
2. Use ONE voltmeter in the three different places shown in the circuit diagram.
3. Without changing the setting on the power pack record your results below:
+ 8V -
Results
V1 V1 (power supply) = __ V
V2 V4 A V2 (variable resistor) = __ V
V3 V3 (bulb) = __ V
V3 (ammeter) = __ V
Conclusion
The power supply voltage is _____________ between the components in the circuit
Equation relating the voltages
Thursday, 16 September 2010
131. VOLTAGE IN THE PARALLEL CIRCUIT IS CONSTANT
Aim
to look for a pattern in the voltages across bulbs and resistors in a series circuit.
1. Set up the circuit (below)
2. Use ONE voltmeter in the three different places shown in the circuit diagram.
3. Without changing the setting on the power pack record your results below:
+ 8V -
V1 Results
V1 = ___ V
V2
V2 = ___ V
V3 = ___ V
V3
Conclusion
The voltage across components connected in parallel is __________
Equation relating the voltages
Thursday, 16 September 2010
132. VOLTAGES AND CURRENTS IN SERIES AND PARALLEL
Aim
to investigate voltage and current in a series circuit that has a parallel portion in it.
1. Set up the circuit (below)
2. Use ONE voltmeter in the four different places shown in the circuit diagram
and ONE ammeter in the four different places shown.
3. Without changing the setting on the power pack record your results below:
Results
A1 + 8V -
A1 = __A
V1 A2 = __A
V2 A4 V4
A3 = __A
V3
A4 = __A
A2
V1 = __V
A3 V2 = __V
V3 = __V
V4
V4 = __V
Thursday, 16 September 2010
134. Lab 14 OHM’S LAW
Method
1. Set up the following circuit using
iced water to cool the immersion + -
coil.
2. Increase the voltage in regular
increments through an A V
appropriate range (widest
possible range)
ice
immersion coil beaker
water
Results
Voltage setting of Power pack
2 4 6 8 10 12
(V)
Voltage, V (V)
Current, I (A)
Thursday, 16 September 2010
135. Draw a graph
of Voltage
against Current
on the grid
provided
Conclusion
Notes
• The iced water was used to keep the temperature of the coil constant .
• If the iced water was forgotten and the coil was allowed to heat up then the graph would curve up.
Repeat the experiment but this time replace the coil with a lamp (that will
increase in temperature as the current through it increases)
Thursday, 16 September 2010
137. RESISTANCE AND POWER in series and parallel
Measurements Resistance
Resistance calculated Calculated
specified Voltage Current
from Power output
measurements
R1
R2
R3
across drawn from
Resistance calculated For any circuit, set power
combination the power
(formula provided for parallel resistors)
of resistors supply supply voltage to 8V
R1 & R2 in series
R 1 & R2 & R3 in series
R1 & R2 in parallel
R 1 & R2 & R3 in parallel
Thursday, 16 September 2010
141. HANGING MAGNETS I
1. Cut out the net
2. Suspend the
and fold it at the
magnet in the
dotted lines to
cradle
create a cradle
S N
+
3. Use a short
length of cotton S N
to suspend the
4. Repeat using a magnet from a
second magnet. retort stand
Thursday, 16 September 2010
142. 1. Position your two magnets in the
HANGING MAGNETS II orientations shown
2. For each orientation, record your
observations
N
A B
S N
S N N S
S
Observation Observation
C D
S
S N S N S N
N
Observation Observation
Thursday, 16 September 2010
143. STROKING MAGNETS
A. Try magnetising
an iron nail using
a magnet
S N
B. Once you have
finished, check for a
magnetic field using a
charm compass.
Thursday, 16 September 2010
144. PLOTTING MAGNETIC FIELDS
Follow the instructions (below) and draw your observations
A. Place one or more B. Use a pencil to mark the
compasses around a bar North pole of each
magnet magnet using a dot
Charm compasses (moved around in a
variety of positions around the magnet
C. Connect the dots using a
smooth curve
D. Plot several field lines
and mark the North and
South poles of the magnet.
E. Wrap your magnet in glad
wrap and spring iron filings
over it.
Thursday, 16 September 2010