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ã TPS 1 
2002
2 
Electronics 
Introduction 
Ohm’s Law 
Power Calculations 
Resistors in Series and Parallel 
Capacitors 
Alternating Current 
Waveforms 
The Potential Divider 
Transistor Circuits 
Questions
3 
Introduction 
Basic Concepts 
Simple Circuits 
Questions 
Main Menu
4 
Basic Concepts 
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Electric current is due to the flow of charge. 
In a solid conductor, the charge is carried by electrons. 
In a solid conductor, an electric current is due to the flow 
of electrons.
5 
Basic Concepts 
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Conductors include: 
copper 
gold 
silver 
lead 
All metals 
And water (not distilled) which is why you should not use mains 
appliances in the presence of water.
6 
Basic Concepts 
Return previous slide 
Insulators include: 
Rubber 
Plastic 
Most solid non metals 
Glass 
Glass, unless it is very hot, is one of the best insulators available.
Electric current (I) is measured in ampere (A) - I is the symbol used to 
indicate current. 
The “amp” is a rather large unit for most electronic applications so we 
use the following sub-multiples: 
1 mA = 0.001A that is 1 / 1 000 th of an ampere 
You already know that 1mm is 1/1000th of an metre so there is nothing 
7 
Basic Concepts 
Return previous slide 
new here. 
1 mA = 0.000 001A that is 1 / 1 000 000 th of an ampere
Common sub-multiples of the volt (less than a volt) include: 
8 
Basic Concepts 
Return previous slide 
Voltage is measured in volt (V) 
1 mV = 0.001V that is 1 / 1 000 th of a volt 
1 mV = 0.000 001V that is 1 / 1 000 000 th of a volt 
Common multiples of the volt (greater than a volt) include: 
1 kV = 1 000 V 
1 MV = 1 000 000 V 
The kV and the MV are not common in electronics.
Common sub-multiples of the ohm (less than an ohm) include: 
9 
Basic Concepts 
Return previous slide 
Resistance is measured in ohm (W) 
1 m W = 0.001 W that is 1 / 1 000 th of an ohm 
1 m W = 0.000 001 W that is 1 / 1 000 000 th of an ohm 
This is pronounced micro ohm 
Common multiples of the ohm (greater than an ohm) include: 
1 k W = 1 000 W 
1 M W = 1 000 000 W 
The mW and the m W are not common in electronics.
Common sub-multiples of the farad (less than a farad) include: 
10 
Basic Concepts 
Return previous slide 
Capacitance is measured in farad (F) 
1 m F = 0.001 F that is 1 / 1 000 th of a farad 
1 m F = 0.000 001 F that is 1 / 1 000 000 th of a farad 
1 n F = 0.000 000 001 F that is 1 / 1 000 000 000 th of a farad 
this is written in full as a nano farad 
1 p F = 0.000 000 000 001 F that is 1 / 1 000 000 000 000 th of a farad 
This is written in full as pico farad
Here is a summary of many of the available multiples and sub-multiples 
Symbol Prefix Multiplication factor 
T tera 1012 1 000 000 000 000 
G giga 109 1 000 000 000 
M mega 106 1 000 000 
k kilo 103 1 000 
h hecto 102 100 
da deca 101 10 
d deci 10-1 0.1 
c centi 10-2 0.01 
m milli 10-3 0.001 
m micro 10-6 0.000 001 
n nano 10-9 0.000 000 001 
p pico 10-12 0.000 000 000 001 
f femto 10-15 0.000 000 000 000 001 
a atto 10-18 0.000 000 000 000 000 001 
The most 
frequently used 
are in bold. 
11 
Basic Concepts 
Return previous slide
This gold band indicates that the tolerance 
of the resistor is ±5% (plus or minus 5 percent). 
This means that its resistance is between 3 400 W 
and 3 800 W. We say it is nominally 3 600 W. 
The third band is red. This means that there are 2 
zeros. 
The second band is blue. This means the second digit is 6. 
12 
Return previous slide 
Basic Concepts 
Resistors are marked with a series of coloured rings to give us an idea of 
how big their resistance is. 
The first band is orange. This means the first digit is 
3. 
So the resistor is nominally 3 600 W.or 3k6
The colours used for the first three bands and their meanings are as 
follows: 
Colour Number Number of zeros 
Black 0 none 
Brown 1 0 
Red 2 00 
Orange 3 000 
Yellow 4 0 000 
Green 5 00 000 
Blue 6 000 000 
Violet 7 0 000 000 
Grey 8 00 000 000 
White 9 000 000 000 
13 
Basic Concepts 
Return previous slide
The colours used for the last band and their meanings are as follows: 
Gold ± 5 % 
Silver ± 10 % 
No band ± 20 % 
Resistors are manufactured in “preferred values”. That 
means that you can only buy certain values. 
The preferred values for resistors with a tolerance of 
±20% are: 10,15,22,33,47,68 and 100. These are just 
the first two significant figures. You can buy a 1500W 
but not a 2000 W. 
14 
Basic Concepts 
Return previous slide
15 
Basic Concepts 
Return previous slide 
The preferred values for 10% resistors are: 
10 
12 
15 
18 
22 
27 
33 
39 
47 
56 
58 
82 
100 
&
16 
Basic Concepts 
Return previous slide 
The preferred values for 5% resistors are: 
10 
11 
39 
12 
43 
13 
47 
15 
51 
16 
18 
& 
56 
62 
20 
68 
22 
75 
24 
82 
27 
91 
30 
100 
33 
36
17 
Basic Concepts 
In summary: 
Voltage is measured in 
Current is measured in 
Resistance is measured in 
Capacitance is measured in 
Volt (V) 
Ampere (A) 
ohm (W) 
farad (F) 
3MV = 3 000 000 V 
2kV = 2 000 V 
5mV = 0.005 A 
7mA = 0.000 007 A 
& 1nF = 0.000 000 001 F 
Home 
1pF = 0.000 000 000 001 F 
Return previous slide
This is called a block diagram. 
•The processor is the decision-making part of the system. 
•The input is a sensor that transforms everyday phenomena such as 
temperature and heat to an electric signal that the processor can deal 
with. 
•The output is a device that converts an electric signal from the processor 
into something that we want. 
18 
Simple Circuits 
Simple circuits have three main blocks of components in common that 
perform the same type of job. These are: 
Input Processor Output 
Return to menu slide
19 
Simple Circuits 
Simple circuits have three main blocks of components in common that 
perform the same type of job. These are: 
Input Processor Output 
Return to previous slide 
Examples of input devices include: 
Pressure pads 
LDRs 
Thermistors 
Reed switches
20 
Simple Circuits 
Simple circuits have three main blocks of components in common that 
perform the same type of job. These are: 
Input Processor Output 
Return to previous slide 
Examples of output devices include: 
Lamps 
LEDs 
Motors 
Solenoids
21 
Simple Circuits 
Simple circuits have three main blocks of components in common that 
perform the same type of job. These are: 
Input Processor Output 
Return to previous slide 
Examples of basic processors include: 
Transistors 
Operational amplifiers
22 
Simple Circuits 
Home 
Simple circuits have three main blocks of components in common that 
perform the same type of job. These are: 
Input Processor Output 
What would the block diagram look like for a system that brought on a 
light when it got dark? 
LDR Processor Lamp 
Return to previous slide
Questions - Simple Circuits 
1 Write down the units of voltage, capacitance, resistance and 
current. What is the symbol for current? 
2 Write out 22mA and 420 pF in full. 
3 Give three examples of input devices. 
4 Write out a block circuit diagram for a device that could lift up a 
trap door when a beam of light was broken. 
5 What is the nominal value and tolerance of this resistor? 
6 What would the colours of a 47MW resistor be? 
23 
ANSWER 
ANSWER 
ANSWER 
ANSWER 
ANSWER 
ANSWER 
Return to menu slide
Solutions - Simple Circuits 
1 Write down the units of voltage, capacitance, resistance and 
current. What is the symbol for current? 
24 
Voltage volt (V) 
Capacitance farad (F) 
Resistance ohm (W) 
Current ampere (A) 
The symbol for current is I 
Return
Solutions - Simple Circuits 
25 
2 Write out 22mA and 420 pF in full. 
22mA = 22 x 0.001 A = 0 . 22 A 
420 pF = 420 x 0.000 000 000 001 F = 0 . 000 000 000 42 F 
Return
Solutions - Simple Circuits 
26 Return 
3 Give three examples of input devices. 
Pressure pads 
LDRs 
Thermistors 
Reed switches
Solutions - Simple Circuits 
4 Write out a block circuit diagram for a device that could lift up a 
trap door when a beam of light was broken. 
LDR Processor Motor 
27 
or 
LDR Processor Solenoid 
Note that a bulb is not an input device as it gives out light. 
Return
Solutions - Simple Circuits 
5 What is the nominal value and tolerance of this resistor? 
This gold band indicates that the tolerance 
of the resistor is ±5% (plus or minus 5 percent). 
The third band is red. This means that there are 2 
zeros. 
The second band is black. This means the second digit is 0. 
The first band is brown. This means the first digit is 1. 
28 
So the resistor is nominally 1 200 W. 
Return
Solutions - Simple Circuits 
6 What would the colours of a 47MW resistor be? 
The third band is blue. This means that there are 6 zeros. 
The second band is violet. This means the second digit is 7. 
The first band is yellow. This means the first digit is 4. 
29 
The resistor is nominally 47 000 000 W. 
This gold band indicates that the tolerance 
of the resistor is ±5% (plus or minus 5 percent). 
Return
30 
Ohm’s Law 
Ohm’s Law states that so long as the physical conditions remain 
constant, the current through a conductor is proportional to the voltage 
across it. 
This gives us the formula: 
Voltage = current x resistance 
V = I R 
We can rearrange this equation to give either 
R = V / I 
or 
I = V / R 
Return to menu slide
31 
Ohm’s Law 
What does it mean? 
“Physical conditions remaining constant” - This really means as long 
as the temperature remains constant. Usually it does. 
“The current through a conductor is proportional to the voltage across 
it” - this means that if you double the voltage, you get twice the 
current. Triple the voltage and you triple the current etc. 
Voltage 
Current 
Low resistance 
High resistance 
Return previous slide
32 
Ohm’s Law 
Return previous slide 
Calculations using Ohm’s law fall into three types: 
What is the resistance 
What is the current 
if ? 
if ? 
What is the voltage 
(Use R = V / I) if ? (Use V = I x R) 
E.G. 
What resistance could 
you use with a 10V 
supply to limit the 
current to 15mA? 
R = V / I = 10 / 0.015 
667 W so use 680 W 
(Use I = V / R) 
E.G. 
A 430 W resistor 
protects an LED in a 
5V circuit. What is 
the current through 
the LED? 
I = V / R = 5 / 430 
= 12 mA 
E.G. 
12mA runs through 
a prorctive resistor 
of resistance 820 W. 
What is the voltage 
across the resistor ? 
V = IR = 0.012x820 
= 9.84 V
The voltage across the diode is 0.7 
V and the cell produces 1.5 V. 
What is the current through the 
resistor? 
0.7 V 
820 W Diode 
If you can’t see how to do it straight away, write the values 
given onto the diagram. 
33 
Ohm’s Law 
Return previous slide 
1.5V 
Voltage across the resistor = 1.5V (provided by the cell) 
- 0.7V (lost across the diode) = 0.8V 
Using I = V / R = 0.8 / 820 = 1mA
Home 
1 A power supply drives a current of 500mA through a bulb with a 
working resistance of 3W. What voltage is the power supply? 
2 A power supply provides 12 V to a bulb passing 3 A. What is the 
working resistance of the bulb? 
3 A 47 kW resistor has a pd of 9 V across it. What current passes 
through the resistor? 
4 An 18V power supply is placed across a resistor of resistance 
10kW. What current will flow through the resistor? 
5 The effective resistance of a small motor is 5 W. What current 
passes through it if a cell of voltage 6 V is placed across it? 
Solution 1 Solution 2 Solution 3 Solution 4 Solution 5 
34 
Ohm’s Law - Questions 
Return previous slide
35 
Ohm’s Law - Solutions 
1 A power supply drives a current of 500mA through a bulb with a 
working resistance of 3W. What voltage is the power supply? 
V = I x R 
so V = 0.5 x 3 
=1.5 volt 
Return
2 A power supply provides 12 V to a bulb passing 3 A. What is the 
working resistance of the bulb? 
36 
Ohm’s Law - Solutions 
V = I x R 
So R = V / I 
= 12 / 3 
= 4 A 
Return
37 
Ohm’s Law - Solutions 
3 A 47 kW resistor has a pd of 9 V across it. What current passes 
through the resistor? 
V = I x R 
So I = V / R 
= 9 / 47 000 
= 0.000 191 A 
= 191 mA 
Return
38 
Ohm’s Law - Solutions 
4 An 18V power supply is placed across a resistor of resistance 
10kW. What current will flow through the resistor? 
V = I x R 
so I = V / R 
= 18 / 10 000 
= 0.001 8 A 
= 1.8 mA 
Return
5 The effective resistance of a small motor is 5 W. What current 
passes through it if a cell of voltage 6 V is placed across it? 
39 
Ohm’s Law - Solutions 
V = I x R 
So I = V / R 
= 6 / 5 
= 1.2 A 
Return
40 
Power Calculations 
The detail from the bottom of an 
electrical appliance shown here 
gives a very useful, commonly 
used method of writing the power 
of the appliance. 
20 VA is exactly the same as 20 W (20 watts). 
The more powerful an appliance is, the greater the number will be. 
An electric fire might well be 2 or 3 kW (2 000 or 3 000 W). 
1W is sometimes called 1VA because you can calculate the 
power by multiplying “the volts by the amps”! 
Power = current x voltage or P = I V 
Return main menu
This device runs from a 230V mains supply. What can we learn from 
this information? Well, we know that P = IV; we also know the 
voltage and the power, so we can calculate the current I. 
41 
Power Calculations 
Remember that : 
20VA means a power of 20W 
and that 
P = I x V 
Return previous slide 
I = P / V 
So I = 20 / 230 
= 87 mA
Can you match these typical power ratings with the device that they 
describe? 
42 
Power Calculations 
Light emitting diode 
Halogen desk lamp 
Return previous slide 
Power station 
Electric lamp 
Torch Bulb
43 
Power Calculations 
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Light emitting diode 
Halogen desk lamp 
Power station 
Electric lamp 
Torch Bulb
Power Calculations - the formulae 
44 
Power = current x voltage 
P = IV 
so I = P / V and V = P / I 
But from Ohm’s Law, V = I x R 
So P = I x IR 
P = I2R 
And from Ohm’s Law, I = V / R 
So P = (V/R) x V 
P = V2/R 
Return previous slide
Power Calculations - Questions 
Home 
1 A diode has a voltage of 0.7V across it and a current of 100mA 
flowing through it. What is the power dissipated in the diode? 
2 A wire carries a current of 5 mA and the power dissipated in the 
wire is 2.5 mW. What is the voltage across the wire? 
3 What is the current passing through a coil that dissipates 40mW 
when a voltage of 5V is applied across it? 
4 A current of 10 mA passes through a 10W resistor. What is the 
power dissipated in the resistor? 
5 A voltage of 9 V is applied across a 10 k W resistor. What power 
is dissipated in the resistor? 
45 
Return previous slide
Power Calculations - Solutions 
1 A diode has a voltage of 0.7V across it and a current of 100mA 
flowing through it. What is the power dissipated in the diode? 
46 
P = IV 
so P = 0.1 x 0.7 
= 0.07 
= 70 mW
Power Calculations - Solutions 
2 A wire carries a current of 5 mA and the power dissipated in the 
wire is 2.5 mW. What is the voltage across the wire? 
47 
P = IV 
So V = P / I 
= 0.000 0025 / 0.005 
= 0.000 5 W 
= 0.5 mW 
= 500 mW
Power Calculations - Solutions 
3 What is the current passing through a coil that dissipates 40mW 
when a voltage of 5V is applied across it? 
48 
P = IV 
So I = P / V 
= 0.04 / 5 
= 0.008 W 
= 8mW
Power Calculations - Solutions 
4 A current of 10 mA passes through a 10W resistor. What is the 
power dissipated in the resistor? 
49 
P = I2R 
= 0.012 x 10 
= 0.001 
=1mW
Power Calculations - Solutions 
5 A voltage of 9 V is applied across a 10 k W resistor. What power 
is dissipated in the resistor? 
50 
P =V2/R 
= 92 / 10 000 
0.0081 
= 8.1 mW
Resistors in Series and Parallel 
Resistors are said to be connected in series when the same current has to 
pass through each resistor i.e. the current does not have to split. 
These three resistors are connected in series. 
51 
And so are these 5 resistors 
Return to main menu
Resistors in Series and Parallel 
Resistors are said to be connected in parallel when the current has to 
split to pass through each resistor i.e. the current through each resistor 
might not be the same. 
These three resistors are connected in 
52 
parallel. 
And so are these two. 
Return to previous slide
Resistors in Series and Parallel 
R1 R2 R3 
47 MW 47 MW 47 MW 
These three resistors connected in series, could be replaced by 
one resistor of resistance 141MW. 
53 
That is 47 MW + 47 MW + 47 MW = 141 MW 
(This is not available so we might use a 150 MW) 
As a general formula we could write: 
R total= R1 + R2 + R3 or R = R1 + R2 + R3 
Return to previous slide
Resistors in Series and Parallel 
54 
R1 
R2 
R3 
The resistance of each of the resistors 
in this parallel network is 47 MW. 
The effective resistance of three 
resistors is 15.7 MW (use 16 MW). 
You would expect the resistance to be less than any of the individual 
resistances in the network as there are three possible routes for the 
electricity to take. 
The formula used to add the resistances is: 
1 = 1 + 1 + 
1 
R R R R total 
1 2 3 
or 
R R R 
1 2 3 
RTotal = + + 
R R R R R R 
1 2 2 3 3 1 
Return to previous slide
Resistors in Series and Parallel - Questions 
1 What is the combined resistance of a 39k W and a 47k W resistor 
connected in series? 
2 What is the combined resistance of a 39k W and a 47k W resistor 
connected in parallel? 
3 What is the combined resistance of a 10k W, 20k W and 47k W 
resistor connected in series? 
4 What is the combined resistance of a 10k W, 20k W and 47k W 
resistor connected in parallel? 
5 Suppose you need a 30k W resistor but you only have a 27k W 
and a handful of assorted resistors. What other resistor would you search 
for and how would you connect them together? 
55 
Home 
Return to previous slide
Resistors in Series and Parallel - Answers 
1 What is the combined resistance of a 39k W and a 47k W resistor 
connected in series? 
R total= R1 + R2 + R3 or R = R1 + R2 + R3 
56 
So R = 39 000 + 47 000 = 86 000 
= 86kW 
Return to menu slide
Resistors in Series and Parallel - Answers 
2 What is the combined resistance of a 39k W and a 47k W resistor 
connected in parallel? 
1 1 1 
R R R Total 
1 2 
57 
So 1/R = (1/39 000) +(1/47 000) 
= 0.00002564 + 0.00002128 = 0.00004692 
So R = 1/0.00004692 = 21 314W 
= 21.3kW 
= 22kW 
Return to menu slide 
= +
Resistors in Series and Parallel - Answers 
3 What is the combined resistance of a 10 kW, 20 kW and 47 kW 
resistor connected in series? 
R total= R1 + R2 + R3 or R = R1 + R2 + R3 
58 
So R = 10 000 + 20 000 + 47 000 
= 77 000 W 
= 77 k W 
Return to menu slide
Resistors in Series and Parallel - Answers 
4 What is the combined resistance of a 10kW, 20kW and 47kW 
resistor connected in parallel? 
1 = 1 + 1 + 
1 
R R R R Total 
1 2 3 
The numbers here could get very big so let us omit three zeros and give 
the answer in kW as all the resistances are in kW anyway. 
59 
R = (1/10) +(1/20) +(1/47) 
= 0.1000 + 0.0500 + 0.0213 = 0.1713 
=5.84 kW 
Use 5.8 kW 
Return to menu slide
Resistors in Series and Parallel - Answers 
5 Suppose you need a 30 kW resistor but you only have a 27 kW 
and a handful of assorted resistors. What other resistor would you search 
for and how would you connect them together? 
You are looking to increase the resistance by adding another resistor. 
This can only be done by adding a resistor in series. 
R total= R1 + R2 + R3 or R = R1 + R2 + R3 
60 
We know that Rtotal is 30 kW and R1 is 27 kW 
So 30 = 27 + R2 
R2 = 30 - 27 
= 3 kW 
Return to menu slide
Capacitors 
Capacitors store charge. The greater the 
voltage that you apply to them, the greater the 
charge that they store. In fact the ratio of the 
charge stored to the voltage applied is called 
the capacitance. 
Capacitance = Charge / Voltage 
61 
or C = Q / V 
Capacitance is measured in farad (F) but the farad is a large unit of 
capacitance so you usually see microfarad mF (millionth of a farad 10-6 
or 0. 000 001 F), nanofarad nF (10-9) or picofarad pF (10-12). 
The capacitor in the picture is a 470 mF (0.000 47 F) polar (you must 
connect it the correct way around in the circuit) capacitor rated at 40V 
(the working voltage should not exceed 40V). 
Return to main menu
62 
Capacitors - Symbols 
This is a non-polar capacitor - 
it does not matter which way 
around you place it in the 
circuit. 
This is a polar capacitor. It 
is essential that the 
capacitor is connected into 
the circuit the correct way 
around. 
Return to previous slide
63 
Capacitors 
Capacitor Characteristics 
Time Constant Calculations 
Capacitors in Series 
Capacitors in Parallel 
Questions 
Return to previous slide
64 
Capacitor Characteristics 
Closing the switch allows the capacitor 
to charge. As this happens, the voltage 
across the capacitor will rise in line 
with the fall of current through it as it 
becomes fully charged. 
V 
A 
Voltage 
Current 
Time 
Time 
Return to menu slide
65 
Capacitor Characteristics 
The circuit has now been adapted so 
that closing the switch allows the 
capacitor to discharge through the 
resistor. Note now that the current will 
fall as the voltage falls. 
V 
A 
Voltage 
Current 
Time 
Time 
Return to previous slide
66 
Capacitor Characteristics 
The circuit on the left allows us to 
investigate the charging and discharging 
of a capacitor simply. 
Connecting the flying lead S to point X 
will charge the capacitor from the cell 
through the resistor R. 
Connecting the flying lead S to Y will 
then discharge the capacitor through the 
resistor. 
S 
It has been found that increasing either the capacitance or the 
resistance will increase the time taken for the capacitor to charge. 
Return to previous slide 
A 
V 
X Y 
C 
R
67 
Capacitor Characteristics 
When the flying lead S is connected to X, 
the capacitor will charge up through the 
resistor. 
At first there will be little or no charge in the 
capacitor so the current flows into the 
capacitor (via the resistor), quite rapidly. 
The current through the resistor develops a 
voltage over the resistor. The voltage across 
the capacitor will be proportional to the 
charge in it. Since the charging has only just 
begun, it will be small but growing. 
S 
The capacitor begins to charge: It gets harder for more charge to flow 
into the capacitor so the current decreases. As the charge on the 
capacitor is increasing, the voltage across it increases too. 
Return to previous slide 
A 
V 
X Y 
C 
R
Home 
The capacitor is said to be fully charged.. 
68 
A 
V 
Capacitor Characteristics 
X Y 
C 
S 
R 
Eventually the capacitor will “fill”. This 
really means that it approaches the condition 
such that the voltage across it is equal to the 
supply voltage. 
There will no longer be any current flowing. 
The time taken to achieve this increases with 
increased capacitance and /or resistance. 
Increasing the supply voltage makes no difference to the time taken 
for the voltage across the capacitor to approach the voltage across the 
supply. 
Return to previous slide
Time Constant Calculations 
69 
The time constant is the time taken for: 
the current or voltage to have fallen to 37% of its original value 
or 
the voltage to have risen to 63% of its original value 
We can calculate the time constant for a circuit by multiplying the 
capacitance of the capacitor by the resistance of the resistor: 
T = C x R 
The units of the time constant are seconds if the resistance is in ohms 
and the capacitance in farads. 
Return to menu
Time Constant Calculations 
E.G. One 
A 10M0 resistor is connected in series with a 470 pF capacitor. How 
long will it take to discharge the capacitor to 37V from an initial voltage 
of 100V? 
Note that the voltage is falling to 37% of its initial value, so we are 
looking at one time constant. 
70 
Using T = C R 
T = 0.000 000 000 470 x 10 000 000 
= 0.004 7 s 
Return to previous slide
Time Constant Calculations 
E.G. Two 
A 10M0 resistor is connected in series with a capacitor. If the time 
constant is 0.001s, what is the capacitance of the capacitor? 
71 
Using T = C R 
0.001 = C x 10 000 000 
C = 0.001 / 10 000 000 
= 0.000 000 000 1 F 
= 100 pF 
Home 
Return to previous slide
72 
Capacitors in Series 
C1 C2 C3 
These three capacitors are 
connected in series. Their combined 
capacitance is given by: 
1 = 1 + 1 + 
1 
C C C C total 
1 2 3 
or 
C C C C Total + + 
1 2 3 
C C C 
1 2 3 
= 
Return to menu
Capacitors in Series 
Home 
4 What is the combined capacitance of a 10 mF, 20 mF and 47 mF 
capacitor connected in series? 
C C C C Total + + 
1 2 3 
C C C 
The numbers here could get very small so let us omit 5 zeros and give 
the answer in mF as all the capacitances are in mF anyway. 
73 
C = (10 x 20 x 47) / (10 + 20 + 47) 
= 9400 / 77 
=122 mF 
1 2 3 
= 
C1 C2 C3 
Return to previous slide
74 
Capacitors in Parallel 
C1 
C2 
C3 
These three capacitors are connected in 
parallel with each other. 
Note that because they are in parallel, 
they must have the same voltage 
across each other. 
The combined capacitance of the network 
of capacitances is given by: 
Ctotal = C1 + C2 + C3 
Return to menu
Home 
Suppose that the capacitances are 10 mF, 20 
mF and 47 mF. 
75 
Capacitors in Parallel 
C1 
C2 
C3 
Ctotal = C1 + C2 + C3 
So C = 10 + 20 + 47 
= 77 mF 
Return to previous slide
76 
Capacitors - Questions 
1 What is the combined capacitance of a 10pF and a 20pF capacitor 
connected in series? 
2 What is the combined capacitance of a 10pF and a 20pF capacitor 
connected in parallel? 
3 What is the time constant for a 1000 pF capacitor connected to a 
100kW resistance? 
4 What capacitance would you need to combine with a 200 mF 
capacitor to give the combinations a capacitance of 100 mF? How would 
you connect them together to achieve this? 
5 What resistor could you connect with a 47 mF capacitor to give a 
time constant of 1.83 s ? 
Return to previous slide
C C C C Total + + 
C C C 
77 
Capacitors - Answers 
1 What is the combined capacitance of a 10pF and a 20pF capacitor 
connected in series? 
1 2 3 
The numbers here could get very small so let us omit 11 zeros and give 
the answer in pF as all the capacitances are in pF anyway. 
C = (10 x 20) / (10 + 20) 
= 200 / 30 
=6.7 pF 
1 2 3 
= 
C1 C2 C3 
Return to menu
78 
Capacitors - Answers 
2 What is the combined capacitance of a 10pF and a 20pF capacitor 
connected in parallel? 
C1 
C2 
C3 
Ctotal = C1 + C2 + C3 
So C = 10 + 20 
= 30 pF 
Return to menu
79 
Capacitors - Answers 
3 What is the time constant for a 1000 pF capacitor connected to a 
100kW resistance? 
T = C x R 
= (1000 x 0.000 000 000 001) x 100 000 
= 0.000 1 s 
Return to menu
C C C C Total + + 
C C C 
80 
Capacitors - Answers 
4 What capacitance would you need to combine with a 200 mF 
capacitor to give the combinations a capacitance of 100 mF? How would 
you connect them together to achieve this? 
In order to get a smaller capacitance, you need to connect them in series. 
1 2 3 
1 2 3 
= 
C1 C2 C3 
So 100 = 200 x C2 / (200 + C2) 
100 (200 + C2) = 200C2 
20 000 + 100C2 = 200C2 
20 000 = 200C2 - 100C2 
100 C2 = 20 000 
C2 = 200 mF Return to menu
81 
Capacitors - Answers 
5 What resistor could you connect with a 47 mF capacitor to give a 
time constant of 1.83 s ? 
T = C x R 
1.83 = 0.000 047 x R 
R = 1.83 / 0.000 047 
= 38 936 W 
Use 39 kW 
Return to menu
82 
Alternating Current 
Direct current (DC) is the current that comes from a cell or battery. 
It is unidirectional. That is to say that the net drift of electrons is in one 
direction. This one direction will always be from positive to negative for 
electrons but negative to positive for conventional flow. 
It is easier to convert voltages from one value to another if the direction 
of the current is rapidly changing. 
This is called an alternating current (AC). 
Return to main menu
83 
Alternating Current 
Alternating current has some strange properties: 
•it can appear to pass through a capacitor 
•it produces the discharges that you see in a plasma ball 
•it can be stepped up (to higher voltages and lower current) 
•it can be stepped down (to lower voltages and higher current) 
Mains voltage is always due to an alternating current. It is used because 
it can be stepped up or down easily. 
Return to previous slide
84 
Alternating Current 
Throughout Europe, mains voltage is supplied at a frequency of 50 Hz. 
You will remember that Hz is the abbreviation for hertz - the unit of 
frequency. 
This means that the electricity goes through one complete cycle 50 times 
every second. 
This means that the voltage will: 
•start from zero and build up in one direction until it reaches a 
maximum value (about 325 V). 
•Fall back to zero 
•Change direction and start to build up to a maximum value (about - 
325 V) 
•Fall back to zero 
•50 times per second 
Alternating voltages (and currents) can have extremely high frequencies. 
The current that produces radio waves can be many MHz (millions of 
hertz). Return to previous slide
85 
Alternating Current - Questions 
Home 
1 What is the frequency of the mains voltage in the UK and 
Europe? 
2 What is the frequency of the mains voltage in the USA? 
3 How long is a complete cycle of mains ac at 50 Hz? 
4 How many times does the electricity in 50 Hz ac mains, change 
direction? 
5 Write out 250 MHz in full. 
Return to previous slide
Alternating Current - Answers 
1 What is the frequency of the mains voltage in the UK and 
Europe? 50Hz 
2 What is the frequency of the mains voltage in the USA? 60Hz 
3 How long is a complete cycle of mains ac at 50 Hz? 
86 
1/50th of a second = 0.02s 
Home 
4 How many times does the electricity in 50 Hz ac mains, change 
direction? 
Twice each cycle so 100 times 
5 Write out 250 MHz in full 
250 000 000 hertz 
Return to menu
87 
Waveforms 
As alternating currents and voltages vary with time, it is useful to have a 
graphical representation of them. 
The electronic device that does this for us is called an oscilloscope. 
The essence of an oscilloscope is its ability to plot a graph for us, 
showing the variation of voltage with time. It is particularly useful 
because it works extremely quickly and it barely interferes with the 
circuit from which you are taking the measurements. 
When you first look at an oscilloscope, the number of knobs, levers and 
buttons can be bewildering but you will soon get used to it. In fact, you 
rarely need to use most of them. 
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88 
Waveforms 
Screen showing the trace On / off switch 
x input 
The trace shows a graph with voltage on the y axis (vertical) and time on 
the x axis (horizontal). 
Return to previous slide
89 
Waveforms 
The waveform produced by mains voltage looks like this: 
Voltage 
time 
This shape of waveform is called a sinusoidal wave. 
Return to previous slide
90 
Waveforms 
The waveform produced by mains voltage looks like this: 
Voltage 
time 
The arrows indicate a complete cycle. A cycle is the time that it takes to 
reach the next adjacent identical position on the waveform. 
Return to previous slide
Waveforms 
The waveform produced by mains voltage looks like this: 
91 
Voltage 
time 
This arrow indicates the peak voltage. For mains it is about 325V in the 
UK. The value of 230V that is quoted is the peak divided by the square 
root of 2. (It is the dc equivalent voltage that would produce the same 
heating effect as an ac with a peak voltage of 325V. Dividing by root 2 
only works for sinusoidal waveforms). The peak voltage is the maximum 
voltage. 
Return to previous slide
Waveforms 
The waveform produced by mains voltage looks like this: 
92 
Voltage 
time 
This arrow indicates the peak to peak voltage. Notice that the peak to 
peak voltage is twice the peak voltage. For mains it is about 650V in the 
UK and Europe. 
Return to previous slide
93 
Waveforms 
Another common waveform called the square wave looks like this: 
Voltage 
time 
The arrows indicate a complete cycle. A cycle is the time that it takes to 
reach the next adjacent identical position on the waveform. 
Return to previous slide
94 
Waveforms 
Another common waveform called the square wave looks like this: 
Voltage 
time 
This arrow indicates the peak voltage. 
Return to previous slide
95 
Waveforms 
Another common waveform called the square wave looks like this: 
Voltage 
time 
This arrow indicates the peak to peak voltage. It will be twice the peak 
voltage 
Return to previous slide
96 
Waveforms 
Another common waveform called the saw-tooth wave looks like this: 
Voltage 
time 
The arrows indicate a complete cycle. A cycle is the time that it takes to 
reach the next adjacent identical position on the waveform. 
Return to previous slide
97 
Waveforms 
Another common waveform called the saw-tooth wave looks like this: 
Voltage 
time 
This arrow indicates the peak voltage. 
Return to previous slide
98 
Waveforms 
Another common waveform called the saw-tooth wave looks like this: 
Voltage 
time 
This arrow indicates the peak to peak voltage. 
Return to previous slide
99 
Waveforms - Questions 
Home 
1 What is the name of the 
trace shown on the oscilloscope? 
2 How many complete cycles 
can you see? 
3 If the scale on the y-axis is 2V per division, estimate the peak 
voltage. What is the peak to peak voltage? 
4 If the scale on the x-axis is 2ms per division, estimate the 
length of a cycle. 
5 Using your answer to question 4, calculate the frequency of 
the wave. 
Return to previous slide
100 
Waveforms - Answers 
1 What is the name of the 
trace shown on the oscilloscope? 
Return to menu
101 
Waveforms - Answers 
2 How many complete cycles 
can you see? 
ONE TWO THREE 
Return to menu
3 If the scale on the y-axis is 
2V per division, estimate the peak 
voltage. What is the peak to peak 
voltage? 
102 
Waveforms - Answers 
5 divisions 
so 5 divisions x 2 V per division 
= 10V 
Return to menu
103 
Waveforms - Answers 
4 If the scale on the x-axis is 
2ms per division, estimate the length 
of a cycle. 
Count as many complete cycles as you can to get as accurate an 
answer as possible. 
3 cycles is about 35 divisions 
1 cycle is about 11.7 divisions 
11.7 divisions is 11.7 x 2 ms 
= 23.4 ms 
Return to menu
104 
Waveforms - Answers 
5 Using your answer to question 4, calculate the frequency of the 
wave. 
From question 4 one cycle is about = 23.4 ms 
23.4ms = 23.4 x 0.001s 
= 0.0234s 
How many of these can we get into 1 second? 
= 1 / 0.0234 
= 42.7 Hz 
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105 
The Potential Divider 
Voltage is sometimes referred to as 
potential difference. The potential divider 
simply divides up a potential or voltage. 
In its simplest form it is two resistors 
placed across a power supply. The voltage 
across of each resistor is less than the 
supply voltage. Adding the voltage across 
each resistor will give the supply voltage. 
It is probably easiest to understand if you 
look at the diagram. 
+9V 
0 V 
Here the power supply is 9V. Note that both 
the resistances are the same. 
The voltage from the supply will be split (divided) equally as 4.5V. Of 
course 4.5V + 4.5V = 9V. 
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106 
+9V 
0 V 
The Potential Divider 
In this potential divider circuit, the 
resistances are not the same. 
2 000 W 1 000 W 
The bigger resistance here 
means that there will be a 
bigger voltage here. 
The smaller resistance here 
means that there will be a 
smaller voltage here. 
It is 2/3rds 
of the 
resistance. 
It is 2/3rds 
of the 
resistance. 
It is 1/3rd 
of the 
resistance. 
It is 1/3rd 
of the 
resistance. 
It develops 
2/3rds of 
the 
voltage. 
It develops 
2/3rds of 
the 
voltage. 
It develops 
1/3rd of 
the 
voltage. 
It develops 
1/3rd of 
the 
voltage. 
2/3 x 9V = 6V 
1/3 x 9V = 3V 
If you would like to work through this again, step back through 
the sequence using the left arrow key. 
Return to previous slide
107 
+V 
0 V 
The Potential Divider 
R1 
R2 
V1 
V2 
You can calculate the voltage across each 
resistor using a formula too. 
VV11 VV 11 == VV xx RR11 // ((RR11 ++ RR22)) 
V1 = 9 x 2 000 / (1 000 + 2000) = 9 x 2 / 3 = 6V 
VV 22 == VV xx RR22 // ((RR11 ++ RR22)) 
V1 = 9 x 1 000 / (1 000 + 2000) = 9 x 1 / 3 = 3V 
Return to previous slide
108 
The Potential Divider 
The potential divider does not have to be made up of two fixed resistors. 
One of them could be variable, or even both. 
R1 
R2 
V1 
V2 
As R1 increases so does V1 but V2 
will fall. 
As R1 decreases so does V1 but V2 
will rise. 
It is just as if there is only one cake to 
go around (the voltage). If R1 
increases then V1gets more cake so 
there is less left for V2! 
Return to previous slide
109 
The Potential Divider 
Now the variable resistor has been moved to the lower position in the 
network.. 
R1 
R2 
V1 
V2 
As R2 increases so does V2 but V1 
will fall. 
As R2 decreases so does V2 but V1 
will rise. 
It can be handy to change the position 
of the variable resistor. Later you will 
see that it can change the action of a 
transistor circuit so make sure that 
you follow it. 
Return to previous slide
110 
The Potential Divider 
+V 
0V 
With this potential divider, the “tap” in the 
middle is a “slider”. It probably moves 
along a track of carbon. 
R1 and V1 will be the resistance and 
voltage “above” the slider. 
R1 V1 
R2 and V2 will be the resistance and 
voltage “below” the slider. 
R2 V2 
As R1 increases, R2 decreases. This will 
result in V1 increasing and V2 decreasing. 
As R1 decreases, R2 increases. This will 
result in V1 decreasing and V2 increasing. 
Return to previous slide
Here is a component that could be used as a potential divider. 
The black ring is 
the carbon track. 
You adjust it by 
putting a 
screwdriver in 
here and turning 
the outer metal 
ring. 
111 
The Potential Divider 
Return to previous slide
You adjust it by 
putting a 
screwdriver in 
here and turning 
the outer metal 
ring. 
112 
The Potential Divider 
Return to previous slide 
Here is another:
It is possible to use many different components that vary their resistance 
in a potential divider circuit. Here are a few that you might find and the 
physical conditions that change their resistance. 
Light Dependent Resistor (LDR) - decreases resistance with increased 
illumination. 
Thermistor - decreases its resistance with increased temperature 
(negative temperature coefficient). 
Microphone - changes resistance with sound. 
Strain gauge - changes its resistance when stressed. 
Photodiode - decreases resistance with increased illumination. 
113 
The Potential Divider 
Return to previous slide
The Potential Divider - Questions 
1 A 2k and a 3k resistor are used in potential divider using a 10V 
supply. Sketch a possible set up and label the resistors and the voltages 
across them. 
2 Suggest two possible fixed resistors that could be used to obtain 
3V from a 15V supply. 
3 A 27k and a 62k resistor are used in potential divider using a 
12V supply. Sketch a possible set up and label the resistors and the 
voltages across them. 
4 A 15V supply is attached across a potential divider. If one of the 
resistors is a 390k and there is a voltage of 9V across the other, what is 
the second resistance? 
5 A potential divider is created from a fixed resistor and an LDR. 
Explain how the network produces different voltages. 
114 
Home 
Return to previous slide 
Answer 
Answer 
Answer 
Answer 
Answer
The Potential Divider - Answers 
1 A 2k and a 3k resistor are used in potential divider using a 10V 
supply. Sketch a possible set up and label the resistors and the voltages 
across them. 
115 
+10V 
0 V R 1 = 2 000 W 
V1= 4V 
V2 = 6V 
VV11 VV 11 == VV xx RR11 // ((RR11 ++ RR22)) 
V1 = 10 x 2 000 / (3 000 + 2000) = 10 x 2 / 5 = 4V 
VV 22 == VV xx RR22 // ((RR11 ++ RR22)) 
V1 = 10 x 3 000 / (3 000 + 2000) = 10 x 3 / 5 = 6V 
R 2 = 3 000 W 
Return to menu
The Potential Divider - Answers 
2 Suggest two possible fixed resistors that could be used to obtain 
3V from a 15V supply. 
VV11 VV 11 == VV xx RR11 // ((RR11 ++ RR22)) So 3 = 15 x R1 / (R1 + R2) 
We could use more or less any combination. However, they should be 
quite high so that they do not drain a lot of current. 
116 
Let us choose R1 as being 100k. 
3 = 15 x 100 / (100 +R2) 
3(100 + R2) = 1 500 
300 + 3R2 = 1 500 
3R2 = 1 500 - 300 = 1 200 
R2 = 1 200 / 3 = 400k. 
Return to menu
The Potential Divider - Answers 
3 A 27k and a 62k resistor are used in potential divider using a 
12V supply. Sketch a possible set up and label the resistors and the 
voltages across them. 
VV11 VV 11 == VV xx RR11 // ((RR11 ++ RR22)) 
V1 = 12 x 27 / (27 + 62) = 12 x 27 / 89 = 3.64V 
VV 22 == VV xx RR22 // ((RR11 ++ RR22)) 
117 
+12V 
0 V R 1 = 27kW 
V1= 3.64V 
V2 = 8.36V 
V1 = 12 x 62 / (27 + 62) = 12 x 62 / 89 = 8.36V 
R 2 = 62kW 
Return to menu
The Potential Divider - Answers 
4 A 15V supply is attached across a potential divider. If one of the 
resistors is a 390k and there is a voltage of 9V across the other, what is 
the second resistance? 
118 
So V1 = 15 - 9 = 6V 
VV11 VV 11 == VV xx RR11 // ((RR11 ++ RR22)) 
Now 6 = 15 x R1 / (R1 +390) 
6 (R1 + 390) = 15 R1 
6 R1 + 2 340 = 15 R1 
9R1 = 2 340 
R1 = 2 340 / 9 = 260k so use 270k 
Return to menu
The Potential Divider - Answers 
5 A potential divider is created from a fixed resistor and an LDR. 
Explain how the network produces different voltages. 
In bright illumination the LDR’s resistance falls. The voltage across the 
LDR will consequently fall while the voltage across the fixed resistance 
will rise. 
As it goes dark, the LDR’s resistance will increase, increasing the 
voltage across the LDR. As this happens, the voltage across the resistor 
will fall. 
119 
Return to menu
The transistor is a three connection component that can be used either as 
an amplifier or a switch. 
+V 
0V 
120 
Transistor Circuits 
+0.7V 
base 
collector 
emitter 
Essentially the circuit is set up so as to try to force electrons through the 
emitter and out of the collector. This might be to light a bulb. 
However, under normal circumstances, there is a very high resistance 
between the emitter and the collector so the bulb will not light. 
If we make the base go positive, the collector / emitter junction conducts 
and the bulb will light. Return to menu
121 
Transistor Circuits 
The clever part now is to control the base bias voltage that turns the 
transistor on. 
+V 
0V 
The base bias voltage is the voltage between 
the base and the emitter. If it is anything 
much less that 0.7V, the transistor will be off. 
The transistor switches 
on when it is 0.7V. 
You should never allow the base bias voltage 
to get too high as this will overheat the base 
and burn out the transistor. For this reason 
you will frequently find a resistor connected 
to the base. 
c 
e 
b 
Rb 
Return
Correct selection of the 
two resistors Rand R1 2 
will take the base to 
0.7V and turn the 
transistor on. 
Suppose Rwas much 
2 higher than R. The 
1voltage across Rwould 
2 be high so the transistor 
would switch on. 122 
Return 
Transistor Circuits 
The clever part now is to control the base bias voltage that turns the 
transistor on. 
+V 
0V 
c 
e 
b 
This can be achieved 
using a potential divider. 
Rb 
R1 
R2
123 
Transistor Circuits 
The clever part now is to control the base bias voltage that turns the 
transistor on. 
+V 
0V 
c 
e 
b 
Rb 
R1 
R2 
Now suppose R2 was an 
LDR. 
In the bright light, its 
resistance would be low 
so the voltage across it 
would be low, the 
transistor switched off 
and the lamp off. 
But suppose that it 
now goes dark! 
Return
It has just gone dark! 
The resistance of the 
LDR rises. 
The voltage across the 
LDR rises. 
The base bias voltage 
reaches 0.7V 
The transistor 
switches on. The bulb lights. 124 
Return 
Transistor Circuits 
The clever part now is to control the base bias voltage that turns the 
transistor on. 
+V 
0V 
c 
e 
b 
Rb 
R1 
R2
125 
Transistor Circuits 
The clever part now is to control the base bias voltage that turns the 
transistor on. 
+V 
0V 
c 
e 
b 
Rb 
R1 
R2 
Suppose that we now 
swap the positions of 
the resistor and the 
LDR. 
The bulb will now come 
on in daylight! It might 
be useful as a warning 
light circuit in certain 
circumstances. 
Return
126 
Transistor Circuits 
The clever part now is to control the base bias voltage that turns the 
transistor on. 
+V 
0V 
c 
e 
b 
Rb 
R1 
R2 
Now let us consider: 
•Ib the base current 
that flows into the 
transistor 
•Ie the emitter 
current that flows 
out of the transistor 
Ib 
Ie 
•IC the collector 
current that flows 
into the transistor 
Ie = Ib + Ic 
Ic 
Return
127 
Transistor Circuits 
The clever part now is to control the base bias voltage that turns the 
transistor on. 
+V 
0V 
c 
e 
b 
Rb 
R1 
R2 
Ib 
Ie 
Ie = Ib + Ic 
Ic The base current will 
be very small as it has 
passed through R1 and 
Rb so it is almost true 
that Ie = Ic. 
The ratio of Ic : Ib is 
important. It shows 
that the transistor is 
amplifying. It is often 
around about 100. Return
Ie = Ib + Ic 
That is to say that the Ic 
collector current is a 
always a constant 
amount bigger than 
the base current. 
Feed a small current 
to the base and you 
get a big current in 
the collector. 
128 
Transistor Circuits 
The clever part now is to control the base bias voltage that turns the 
transistor on. 
+V 
0V 
c 
e 
b 
Rb 
R1 
R2 
Ib 
Ie 
Return
129 
Transistor Circuits 
The clever part now is to control the base bias voltage that turns the 
transistor on. 
+V 
0V 
c 
e 
b 
Rb 
R1 
R2 
Ib 
Ie 
Ie = Ib + Ic 
Ic The ratio is called hfe. 
hfe = Ic / Ib 
Return
130 
Click on a 
component to find 
out what it does. 
Transistor Circuits 
+V 
0V 
c 
e 
b 
Rb 
R1 
R2 
C1 
Relay 
CONTINUE 
Return
131 
Transistor Circuits 
Click on a 
component to find 
out what it does. 
Capacitor 
This stores charge. It 
acts as a time delay 
to any switching. If 
the transistor is on 
and tries to go off, it 
will act as a reservoir 
and keep the 
transistor on for a 
while longer. 
+V 
0V 
c 
e 
b 
Rb 
R1 
R2 
C1 
Relay 
CONTINUE 
Return
132 
Click on a 
component to find 
out what it does. 
LDR Light 
Dependent Resistor 
Its resistance 
decreases with 
increased 
illumination. In the 
dark, the resistance 
goes up turning the 
transistor on. 
Transistor Circuits 
+V 
0V 
c 
e 
b 
Rb 
R1 
R2 
C1 
Relay 
CONTINUE 
Return
133 
Click on a 
component to find 
out what it does. 
Base Bias Resistor 
This fixed resistor 
protects the base 
from too much 
current. 
Transistor Circuits 
+V 
0V 
c 
e 
b 
Rb 
R1 
R2 
C1 
Relay 
CONTINUE 
Return
134 
Click on a 
component to find 
out what it does. 
Potential Divider 
The LDR and R2 are 
a potential divider. 
Transistor Circuits 
+V 
0V 
c 
e 
b 
Rb 
R1 
R2 
C1 
Relay 
CONTINUE 
Return
135 
Click on a 
component to find 
out what it does. 
Transistor 
A small voltage at 
the base will allow 
current to flow 
through the emitter 
from the collector. 
Transistor Circuits 
+V 
0V 
c 
e 
b 
Rb 
R1 
R2 
C1 
Relay 
CONTINUE 
Return
136 
Click on a 
component to find 
out what it does. 
Diode - this only 
allows current to 
flow in the direction 
of the arrow head. 
Rapid changes in the 
magnetic field of the 
relay can cause high 
voltage that would 
damage the 
transistor. 
The diode 
diverts the 
currents 
formed by 
this 
process. 
Transistor Circuits 
+V 
0V 
c 
e 
b 
Rb 
R1 
R2 
C1 
Relay 
CONTINUE 
Return
137 
Click on a 
component to find 
out what it does. 
Relay - current 
through the relay 
produces a magnetic 
field that throws a 
switch in another 
external circuit. The 
external circuit can 
be a much higher 
powered circuit. 
Transistor Circuits 
+V 
0V 
c 
e 
b 
Rb 
R1 
R2 
C1 
Relay 
CONTINUE 
Return
Transistor Circuits - Questions 
1 The collector current in a circuit is 120mA when the base current 
is 3mA. What is hfe and the emitter current? 
2 Why do we connect a resistor directly to the base of the 
transistor? 
3 Sketch a circuit that will throw a relay in the dark that in turn will 
turn on a switch. 
4 Why should a diode be connected across a relay in the collector 
circuit of a network? 
5 Explain what happens when the resistance of the base bias 
resistor falls in a transistor circuit controlling a motor. 
138 
Answers: 
1 2 3 4 5 
Return to previous slide
Transistor Circuits - Answers 
1 The collector current in a circuit is 120mA when the base current 
is 3mA. What is hfe and the emitter current? 
139 
hfe = Ic / Ib 
= 120 / 3 
= 40 
Return to menu
Transistor Circuits - Answers 
2 Why do we connect a resistor directly to the base of the 
transistor? 
The resistor limits the current entering the base. This stops the base from 
overheating due to excessive currents which would burn the transistor 
140 
out. 
Return to menu
Transistor Circuits - Answers 
3 Sketch a circuit that will throw a relay in the dark that in turn will 
turn on a switch. 
141 
+V 
0V 
c 
e 
b 
R1 
C1 
Relay 
LDR 
Return to menu
Transistor Circuits - Answers 
4 Why should a diode be connected across a relay in the collector 
circuit of a network? 
The relay can create large voltages due to rapid changes in magnetic 
fields as they switch off. The diode provides a short circuit for the 
current due to this voltage. As diodes only carry current in one direction, 
the diode connected to the relay will have no effect in normal operation 
142 
of the relay. 
Return to menu
Transistor Circuits - Answers 
5 Explain what happens when the resistance of the base bias 
resistor falls in a transistor circuit controlling a motor. 
As the resistance falls, so will the voltage across it. 
The voltage across the base will consequently fall. 
143 
This will turn off the transistor. 
The collector current will fall to zero (or extremely close to zero). 
The motor will switch off. 
Return to menu
144 
Electronics Questions 
1 What is the nominal value and tolerance of this resistor? 
2 A power supply drives a current of 150mA through a bulb with a 
working resistance of 10W. What voltage is the power supply? 
3 What is the current passing through a heater that dissipates 40W 
when a voltage of 10V is applied across it? 
Return to menu
4 What is the combined resistance of a 30k W, 20k W and 47k W 
resistor connected in parallel? 
5 Suppose you need a 50k W resistor but you only have a 47k W 
and a handful of assorted resistors. What other resistor would you search 
for and how would you connect them together? 
6 What is the combined capacitance of a 47pF and a 20pF capacitor 
connected in series? 
7 What is the combined capacitance of a 47pF and a 20pF capacitor 
connected in parallel? 
8 What is the time constant for a 1000 mF capacitor connected to a 
10MW resistance? 
145 
Electronics Questions 
Return to previous slide
9 If the scale on the y-axis is 4mV per division, estimate the 
peak voltage. What is the peak to peak voltage? 
10 If the scale on the x-axis is 50 ms per division, estimate the 
length of a cycle. Using your answer, calculate the frequency of the 
wave. 
146 
Electronics Questions 
Return to previous slide
Retu1r4n7 to previous slide 
Return to main menu
1 What is the nominal value and tolerance of this resistor? 
This gold band indicates that the tolerance 
of the resistor is ±5% (plus or minus 5 percent). 
The third band is black. This means that there are no zeros. 
The second band is green. This means the second digit is 5. 
The first band is violet. This means the first digit is 7. 
148 
So the resistor is nominally 75 W. 
Return to menu 
Electronics Answers
2 A power supply drives a current of 150mA through a bulb with a 
working resistance of 10W. What voltage is the power supply? 
149 
V = I x R 
so V = 0.15 x 10 
=1.5 V 
Return to menu 
Electronics Answers
3 What is the current passing through a coil that dissipates 40W 
when a voltage of 10V is applied across it? 
150 
P = IV 
So I = P / V 
= 40 / 10 
= 4 W 
Return to menu 
Electronics Answers
4 What is the combined resistance of a 30kW, 20kW and 47kW 
resistor connected in parallel? 
R R R R Total + + 
1 2 3 
R R R 
1 2 3 
151 
= 
The numbers here could get very big so let us omit three zeros and give 
the answer in kW as all the resistances are in kW anyway. 
R = (30 x 20 x 47) / (30 + 20 + 47) 
= 28 200 / 97 
=291 kW 
Use 300 kW 
Return to menu 
Electronics Answers
5 Suppose you need a 50 kW resistor but you only have a 47 kW 
and a handful of assorted resistors. What other resistor would you search 
for and how would you connect them together? 
You are looking to increase the resistance by adding another resistor. 
This can only be done by adding a resistor in series. 
R total= R1 + R2 + R3 or R = R1 + R2 + R3 
152 
We know that Rtotal is 50 kW and R1 is 47 kW 
So 50 = 47 + R2 
R2 = 50 - 47 
= 3 kW 
Return to menu 
Electronics Answers
6 What is the combined capacitance of a 47pF and a 20pF capacitor 
connected in series? 
C C C C Total + + 
1 2 3 
C C C 
The numbers here could get very small so let us omit 11 zeros and give 
the answer in pF as all the capacitances are in pF anyway. 
153 
C = (47 x 20) / (47 + 20) 
= 940 / 67 
=14 pF 
1 2 3 
= 
C1 C2 C3 
Return to menu 
Electronics Answers
7 What is the combined capacitance of a 47pF and a 20pF capacitor 
connected in parallel? 
154 
C1 
C2 
C3 
Ctotal = C1 + C2 + C3 
So C = 47 + 20 
= 67 pF 
Return to menu 
Electronics Answers
8 What is the time constant for a 1000 mF capacitor connected to a 
10MW resistance? 
155 
T = C x R 
= (1000 x 0.000 001) x 10 000 000 
= 10 000 s 
Return to menu 
Electronics Answers
9 If the scale on the y-axis is 
4mV per division, estimate the 
peak voltage. What is the peak to 
peak voltage? 
156 
5 divisions 
so 5 divisions x 4mV per division 
= 20mV 
Return to menu 
Electronics Answers
Electronics Answers 
10 If the scale on the x-axis is 50 
ms per division, estimate the length of 
a cycle. 
Count as many complete cycles as you can to get as accurate an answer 
as possible. 
157 
3 cycles is about 35 divisions 
1 cycle is about 11.7 divisions 
11.7 divisions is 11.7 x 2 ms 
= 23.4 ms
10 continued Using your previous answer, calculate the frequency of 
the wave. 
From question 4 one cycle is about = 23.4 ms 
158 
23.4 ms = 23.4 x 0.000 001s 
= 0.000 023 4s 
How many of these can we get into 1 second? 
= 1 / 0.000 023 4s 
= 42.7 kHz 
Return to menu 
Electronics Answers
Home 
Retu1r5n9 to previous slide 
Introduction 
Ohm’s Law 
Power Calculations 
Resistors in Series and Parallel 
Capacitors 
Alternating Current 
Waveforms 
Transistor Circuits 
The Potential Divider 
Components 
Questions

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The Python for beginners. This is an advance computer language.
The Python for beginners. This is an advance computer language.The Python for beginners. This is an advance computer language.
The Python for beginners. This is an advance computer language.
 

Electronics

  • 1. Electronics Use your mouse to move around the software. You can either click anywhere on the screen to get the next animation or click on a button if you can see one on the screen. Always move the mouse before you click it. ã TPS 1 2002
  • 2. 2 Electronics Introduction Ohm’s Law Power Calculations Resistors in Series and Parallel Capacitors Alternating Current Waveforms The Potential Divider Transistor Circuits Questions
  • 3. 3 Introduction Basic Concepts Simple Circuits Questions Main Menu
  • 4. 4 Basic Concepts Return previous slide Electric current is due to the flow of charge. In a solid conductor, the charge is carried by electrons. In a solid conductor, an electric current is due to the flow of electrons.
  • 5. 5 Basic Concepts Return previous slide Conductors include: copper gold silver lead All metals And water (not distilled) which is why you should not use mains appliances in the presence of water.
  • 6. 6 Basic Concepts Return previous slide Insulators include: Rubber Plastic Most solid non metals Glass Glass, unless it is very hot, is one of the best insulators available.
  • 7. Electric current (I) is measured in ampere (A) - I is the symbol used to indicate current. The “amp” is a rather large unit for most electronic applications so we use the following sub-multiples: 1 mA = 0.001A that is 1 / 1 000 th of an ampere You already know that 1mm is 1/1000th of an metre so there is nothing 7 Basic Concepts Return previous slide new here. 1 mA = 0.000 001A that is 1 / 1 000 000 th of an ampere
  • 8. Common sub-multiples of the volt (less than a volt) include: 8 Basic Concepts Return previous slide Voltage is measured in volt (V) 1 mV = 0.001V that is 1 / 1 000 th of a volt 1 mV = 0.000 001V that is 1 / 1 000 000 th of a volt Common multiples of the volt (greater than a volt) include: 1 kV = 1 000 V 1 MV = 1 000 000 V The kV and the MV are not common in electronics.
  • 9. Common sub-multiples of the ohm (less than an ohm) include: 9 Basic Concepts Return previous slide Resistance is measured in ohm (W) 1 m W = 0.001 W that is 1 / 1 000 th of an ohm 1 m W = 0.000 001 W that is 1 / 1 000 000 th of an ohm This is pronounced micro ohm Common multiples of the ohm (greater than an ohm) include: 1 k W = 1 000 W 1 M W = 1 000 000 W The mW and the m W are not common in electronics.
  • 10. Common sub-multiples of the farad (less than a farad) include: 10 Basic Concepts Return previous slide Capacitance is measured in farad (F) 1 m F = 0.001 F that is 1 / 1 000 th of a farad 1 m F = 0.000 001 F that is 1 / 1 000 000 th of a farad 1 n F = 0.000 000 001 F that is 1 / 1 000 000 000 th of a farad this is written in full as a nano farad 1 p F = 0.000 000 000 001 F that is 1 / 1 000 000 000 000 th of a farad This is written in full as pico farad
  • 11. Here is a summary of many of the available multiples and sub-multiples Symbol Prefix Multiplication factor T tera 1012 1 000 000 000 000 G giga 109 1 000 000 000 M mega 106 1 000 000 k kilo 103 1 000 h hecto 102 100 da deca 101 10 d deci 10-1 0.1 c centi 10-2 0.01 m milli 10-3 0.001 m micro 10-6 0.000 001 n nano 10-9 0.000 000 001 p pico 10-12 0.000 000 000 001 f femto 10-15 0.000 000 000 000 001 a atto 10-18 0.000 000 000 000 000 001 The most frequently used are in bold. 11 Basic Concepts Return previous slide
  • 12. This gold band indicates that the tolerance of the resistor is ±5% (plus or minus 5 percent). This means that its resistance is between 3 400 W and 3 800 W. We say it is nominally 3 600 W. The third band is red. This means that there are 2 zeros. The second band is blue. This means the second digit is 6. 12 Return previous slide Basic Concepts Resistors are marked with a series of coloured rings to give us an idea of how big their resistance is. The first band is orange. This means the first digit is 3. So the resistor is nominally 3 600 W.or 3k6
  • 13. The colours used for the first three bands and their meanings are as follows: Colour Number Number of zeros Black 0 none Brown 1 0 Red 2 00 Orange 3 000 Yellow 4 0 000 Green 5 00 000 Blue 6 000 000 Violet 7 0 000 000 Grey 8 00 000 000 White 9 000 000 000 13 Basic Concepts Return previous slide
  • 14. The colours used for the last band and their meanings are as follows: Gold ± 5 % Silver ± 10 % No band ± 20 % Resistors are manufactured in “preferred values”. That means that you can only buy certain values. The preferred values for resistors with a tolerance of ±20% are: 10,15,22,33,47,68 and 100. These are just the first two significant figures. You can buy a 1500W but not a 2000 W. 14 Basic Concepts Return previous slide
  • 15. 15 Basic Concepts Return previous slide The preferred values for 10% resistors are: 10 12 15 18 22 27 33 39 47 56 58 82 100 &
  • 16. 16 Basic Concepts Return previous slide The preferred values for 5% resistors are: 10 11 39 12 43 13 47 15 51 16 18 & 56 62 20 68 22 75 24 82 27 91 30 100 33 36
  • 17. 17 Basic Concepts In summary: Voltage is measured in Current is measured in Resistance is measured in Capacitance is measured in Volt (V) Ampere (A) ohm (W) farad (F) 3MV = 3 000 000 V 2kV = 2 000 V 5mV = 0.005 A 7mA = 0.000 007 A & 1nF = 0.000 000 001 F Home 1pF = 0.000 000 000 001 F Return previous slide
  • 18. This is called a block diagram. •The processor is the decision-making part of the system. •The input is a sensor that transforms everyday phenomena such as temperature and heat to an electric signal that the processor can deal with. •The output is a device that converts an electric signal from the processor into something that we want. 18 Simple Circuits Simple circuits have three main blocks of components in common that perform the same type of job. These are: Input Processor Output Return to menu slide
  • 19. 19 Simple Circuits Simple circuits have three main blocks of components in common that perform the same type of job. These are: Input Processor Output Return to previous slide Examples of input devices include: Pressure pads LDRs Thermistors Reed switches
  • 20. 20 Simple Circuits Simple circuits have three main blocks of components in common that perform the same type of job. These are: Input Processor Output Return to previous slide Examples of output devices include: Lamps LEDs Motors Solenoids
  • 21. 21 Simple Circuits Simple circuits have three main blocks of components in common that perform the same type of job. These are: Input Processor Output Return to previous slide Examples of basic processors include: Transistors Operational amplifiers
  • 22. 22 Simple Circuits Home Simple circuits have three main blocks of components in common that perform the same type of job. These are: Input Processor Output What would the block diagram look like for a system that brought on a light when it got dark? LDR Processor Lamp Return to previous slide
  • 23. Questions - Simple Circuits 1 Write down the units of voltage, capacitance, resistance and current. What is the symbol for current? 2 Write out 22mA and 420 pF in full. 3 Give three examples of input devices. 4 Write out a block circuit diagram for a device that could lift up a trap door when a beam of light was broken. 5 What is the nominal value and tolerance of this resistor? 6 What would the colours of a 47MW resistor be? 23 ANSWER ANSWER ANSWER ANSWER ANSWER ANSWER Return to menu slide
  • 24. Solutions - Simple Circuits 1 Write down the units of voltage, capacitance, resistance and current. What is the symbol for current? 24 Voltage volt (V) Capacitance farad (F) Resistance ohm (W) Current ampere (A) The symbol for current is I Return
  • 25. Solutions - Simple Circuits 25 2 Write out 22mA and 420 pF in full. 22mA = 22 x 0.001 A = 0 . 22 A 420 pF = 420 x 0.000 000 000 001 F = 0 . 000 000 000 42 F Return
  • 26. Solutions - Simple Circuits 26 Return 3 Give three examples of input devices. Pressure pads LDRs Thermistors Reed switches
  • 27. Solutions - Simple Circuits 4 Write out a block circuit diagram for a device that could lift up a trap door when a beam of light was broken. LDR Processor Motor 27 or LDR Processor Solenoid Note that a bulb is not an input device as it gives out light. Return
  • 28. Solutions - Simple Circuits 5 What is the nominal value and tolerance of this resistor? This gold band indicates that the tolerance of the resistor is ±5% (plus or minus 5 percent). The third band is red. This means that there are 2 zeros. The second band is black. This means the second digit is 0. The first band is brown. This means the first digit is 1. 28 So the resistor is nominally 1 200 W. Return
  • 29. Solutions - Simple Circuits 6 What would the colours of a 47MW resistor be? The third band is blue. This means that there are 6 zeros. The second band is violet. This means the second digit is 7. The first band is yellow. This means the first digit is 4. 29 The resistor is nominally 47 000 000 W. This gold band indicates that the tolerance of the resistor is ±5% (plus or minus 5 percent). Return
  • 30. 30 Ohm’s Law Ohm’s Law states that so long as the physical conditions remain constant, the current through a conductor is proportional to the voltage across it. This gives us the formula: Voltage = current x resistance V = I R We can rearrange this equation to give either R = V / I or I = V / R Return to menu slide
  • 31. 31 Ohm’s Law What does it mean? “Physical conditions remaining constant” - This really means as long as the temperature remains constant. Usually it does. “The current through a conductor is proportional to the voltage across it” - this means that if you double the voltage, you get twice the current. Triple the voltage and you triple the current etc. Voltage Current Low resistance High resistance Return previous slide
  • 32. 32 Ohm’s Law Return previous slide Calculations using Ohm’s law fall into three types: What is the resistance What is the current if ? if ? What is the voltage (Use R = V / I) if ? (Use V = I x R) E.G. What resistance could you use with a 10V supply to limit the current to 15mA? R = V / I = 10 / 0.015 667 W so use 680 W (Use I = V / R) E.G. A 430 W resistor protects an LED in a 5V circuit. What is the current through the LED? I = V / R = 5 / 430 = 12 mA E.G. 12mA runs through a prorctive resistor of resistance 820 W. What is the voltage across the resistor ? V = IR = 0.012x820 = 9.84 V
  • 33. The voltage across the diode is 0.7 V and the cell produces 1.5 V. What is the current through the resistor? 0.7 V 820 W Diode If you can’t see how to do it straight away, write the values given onto the diagram. 33 Ohm’s Law Return previous slide 1.5V Voltage across the resistor = 1.5V (provided by the cell) - 0.7V (lost across the diode) = 0.8V Using I = V / R = 0.8 / 820 = 1mA
  • 34. Home 1 A power supply drives a current of 500mA through a bulb with a working resistance of 3W. What voltage is the power supply? 2 A power supply provides 12 V to a bulb passing 3 A. What is the working resistance of the bulb? 3 A 47 kW resistor has a pd of 9 V across it. What current passes through the resistor? 4 An 18V power supply is placed across a resistor of resistance 10kW. What current will flow through the resistor? 5 The effective resistance of a small motor is 5 W. What current passes through it if a cell of voltage 6 V is placed across it? Solution 1 Solution 2 Solution 3 Solution 4 Solution 5 34 Ohm’s Law - Questions Return previous slide
  • 35. 35 Ohm’s Law - Solutions 1 A power supply drives a current of 500mA through a bulb with a working resistance of 3W. What voltage is the power supply? V = I x R so V = 0.5 x 3 =1.5 volt Return
  • 36. 2 A power supply provides 12 V to a bulb passing 3 A. What is the working resistance of the bulb? 36 Ohm’s Law - Solutions V = I x R So R = V / I = 12 / 3 = 4 A Return
  • 37. 37 Ohm’s Law - Solutions 3 A 47 kW resistor has a pd of 9 V across it. What current passes through the resistor? V = I x R So I = V / R = 9 / 47 000 = 0.000 191 A = 191 mA Return
  • 38. 38 Ohm’s Law - Solutions 4 An 18V power supply is placed across a resistor of resistance 10kW. What current will flow through the resistor? V = I x R so I = V / R = 18 / 10 000 = 0.001 8 A = 1.8 mA Return
  • 39. 5 The effective resistance of a small motor is 5 W. What current passes through it if a cell of voltage 6 V is placed across it? 39 Ohm’s Law - Solutions V = I x R So I = V / R = 6 / 5 = 1.2 A Return
  • 40. 40 Power Calculations The detail from the bottom of an electrical appliance shown here gives a very useful, commonly used method of writing the power of the appliance. 20 VA is exactly the same as 20 W (20 watts). The more powerful an appliance is, the greater the number will be. An electric fire might well be 2 or 3 kW (2 000 or 3 000 W). 1W is sometimes called 1VA because you can calculate the power by multiplying “the volts by the amps”! Power = current x voltage or P = I V Return main menu
  • 41. This device runs from a 230V mains supply. What can we learn from this information? Well, we know that P = IV; we also know the voltage and the power, so we can calculate the current I. 41 Power Calculations Remember that : 20VA means a power of 20W and that P = I x V Return previous slide I = P / V So I = 20 / 230 = 87 mA
  • 42. Can you match these typical power ratings with the device that they describe? 42 Power Calculations Light emitting diode Halogen desk lamp Return previous slide Power station Electric lamp Torch Bulb
  • 43. 43 Power Calculations Return previous slide Light emitting diode Halogen desk lamp Power station Electric lamp Torch Bulb
  • 44. Power Calculations - the formulae 44 Power = current x voltage P = IV so I = P / V and V = P / I But from Ohm’s Law, V = I x R So P = I x IR P = I2R And from Ohm’s Law, I = V / R So P = (V/R) x V P = V2/R Return previous slide
  • 45. Power Calculations - Questions Home 1 A diode has a voltage of 0.7V across it and a current of 100mA flowing through it. What is the power dissipated in the diode? 2 A wire carries a current of 5 mA and the power dissipated in the wire is 2.5 mW. What is the voltage across the wire? 3 What is the current passing through a coil that dissipates 40mW when a voltage of 5V is applied across it? 4 A current of 10 mA passes through a 10W resistor. What is the power dissipated in the resistor? 5 A voltage of 9 V is applied across a 10 k W resistor. What power is dissipated in the resistor? 45 Return previous slide
  • 46. Power Calculations - Solutions 1 A diode has a voltage of 0.7V across it and a current of 100mA flowing through it. What is the power dissipated in the diode? 46 P = IV so P = 0.1 x 0.7 = 0.07 = 70 mW
  • 47. Power Calculations - Solutions 2 A wire carries a current of 5 mA and the power dissipated in the wire is 2.5 mW. What is the voltage across the wire? 47 P = IV So V = P / I = 0.000 0025 / 0.005 = 0.000 5 W = 0.5 mW = 500 mW
  • 48. Power Calculations - Solutions 3 What is the current passing through a coil that dissipates 40mW when a voltage of 5V is applied across it? 48 P = IV So I = P / V = 0.04 / 5 = 0.008 W = 8mW
  • 49. Power Calculations - Solutions 4 A current of 10 mA passes through a 10W resistor. What is the power dissipated in the resistor? 49 P = I2R = 0.012 x 10 = 0.001 =1mW
  • 50. Power Calculations - Solutions 5 A voltage of 9 V is applied across a 10 k W resistor. What power is dissipated in the resistor? 50 P =V2/R = 92 / 10 000 0.0081 = 8.1 mW
  • 51. Resistors in Series and Parallel Resistors are said to be connected in series when the same current has to pass through each resistor i.e. the current does not have to split. These three resistors are connected in series. 51 And so are these 5 resistors Return to main menu
  • 52. Resistors in Series and Parallel Resistors are said to be connected in parallel when the current has to split to pass through each resistor i.e. the current through each resistor might not be the same. These three resistors are connected in 52 parallel. And so are these two. Return to previous slide
  • 53. Resistors in Series and Parallel R1 R2 R3 47 MW 47 MW 47 MW These three resistors connected in series, could be replaced by one resistor of resistance 141MW. 53 That is 47 MW + 47 MW + 47 MW = 141 MW (This is not available so we might use a 150 MW) As a general formula we could write: R total= R1 + R2 + R3 or R = R1 + R2 + R3 Return to previous slide
  • 54. Resistors in Series and Parallel 54 R1 R2 R3 The resistance of each of the resistors in this parallel network is 47 MW. The effective resistance of three resistors is 15.7 MW (use 16 MW). You would expect the resistance to be less than any of the individual resistances in the network as there are three possible routes for the electricity to take. The formula used to add the resistances is: 1 = 1 + 1 + 1 R R R R total 1 2 3 or R R R 1 2 3 RTotal = + + R R R R R R 1 2 2 3 3 1 Return to previous slide
  • 55. Resistors in Series and Parallel - Questions 1 What is the combined resistance of a 39k W and a 47k W resistor connected in series? 2 What is the combined resistance of a 39k W and a 47k W resistor connected in parallel? 3 What is the combined resistance of a 10k W, 20k W and 47k W resistor connected in series? 4 What is the combined resistance of a 10k W, 20k W and 47k W resistor connected in parallel? 5 Suppose you need a 30k W resistor but you only have a 27k W and a handful of assorted resistors. What other resistor would you search for and how would you connect them together? 55 Home Return to previous slide
  • 56. Resistors in Series and Parallel - Answers 1 What is the combined resistance of a 39k W and a 47k W resistor connected in series? R total= R1 + R2 + R3 or R = R1 + R2 + R3 56 So R = 39 000 + 47 000 = 86 000 = 86kW Return to menu slide
  • 57. Resistors in Series and Parallel - Answers 2 What is the combined resistance of a 39k W and a 47k W resistor connected in parallel? 1 1 1 R R R Total 1 2 57 So 1/R = (1/39 000) +(1/47 000) = 0.00002564 + 0.00002128 = 0.00004692 So R = 1/0.00004692 = 21 314W = 21.3kW = 22kW Return to menu slide = +
  • 58. Resistors in Series and Parallel - Answers 3 What is the combined resistance of a 10 kW, 20 kW and 47 kW resistor connected in series? R total= R1 + R2 + R3 or R = R1 + R2 + R3 58 So R = 10 000 + 20 000 + 47 000 = 77 000 W = 77 k W Return to menu slide
  • 59. Resistors in Series and Parallel - Answers 4 What is the combined resistance of a 10kW, 20kW and 47kW resistor connected in parallel? 1 = 1 + 1 + 1 R R R R Total 1 2 3 The numbers here could get very big so let us omit three zeros and give the answer in kW as all the resistances are in kW anyway. 59 R = (1/10) +(1/20) +(1/47) = 0.1000 + 0.0500 + 0.0213 = 0.1713 =5.84 kW Use 5.8 kW Return to menu slide
  • 60. Resistors in Series and Parallel - Answers 5 Suppose you need a 30 kW resistor but you only have a 27 kW and a handful of assorted resistors. What other resistor would you search for and how would you connect them together? You are looking to increase the resistance by adding another resistor. This can only be done by adding a resistor in series. R total= R1 + R2 + R3 or R = R1 + R2 + R3 60 We know that Rtotal is 30 kW and R1 is 27 kW So 30 = 27 + R2 R2 = 30 - 27 = 3 kW Return to menu slide
  • 61. Capacitors Capacitors store charge. The greater the voltage that you apply to them, the greater the charge that they store. In fact the ratio of the charge stored to the voltage applied is called the capacitance. Capacitance = Charge / Voltage 61 or C = Q / V Capacitance is measured in farad (F) but the farad is a large unit of capacitance so you usually see microfarad mF (millionth of a farad 10-6 or 0. 000 001 F), nanofarad nF (10-9) or picofarad pF (10-12). The capacitor in the picture is a 470 mF (0.000 47 F) polar (you must connect it the correct way around in the circuit) capacitor rated at 40V (the working voltage should not exceed 40V). Return to main menu
  • 62. 62 Capacitors - Symbols This is a non-polar capacitor - it does not matter which way around you place it in the circuit. This is a polar capacitor. It is essential that the capacitor is connected into the circuit the correct way around. Return to previous slide
  • 63. 63 Capacitors Capacitor Characteristics Time Constant Calculations Capacitors in Series Capacitors in Parallel Questions Return to previous slide
  • 64. 64 Capacitor Characteristics Closing the switch allows the capacitor to charge. As this happens, the voltage across the capacitor will rise in line with the fall of current through it as it becomes fully charged. V A Voltage Current Time Time Return to menu slide
  • 65. 65 Capacitor Characteristics The circuit has now been adapted so that closing the switch allows the capacitor to discharge through the resistor. Note now that the current will fall as the voltage falls. V A Voltage Current Time Time Return to previous slide
  • 66. 66 Capacitor Characteristics The circuit on the left allows us to investigate the charging and discharging of a capacitor simply. Connecting the flying lead S to point X will charge the capacitor from the cell through the resistor R. Connecting the flying lead S to Y will then discharge the capacitor through the resistor. S It has been found that increasing either the capacitance or the resistance will increase the time taken for the capacitor to charge. Return to previous slide A V X Y C R
  • 67. 67 Capacitor Characteristics When the flying lead S is connected to X, the capacitor will charge up through the resistor. At first there will be little or no charge in the capacitor so the current flows into the capacitor (via the resistor), quite rapidly. The current through the resistor develops a voltage over the resistor. The voltage across the capacitor will be proportional to the charge in it. Since the charging has only just begun, it will be small but growing. S The capacitor begins to charge: It gets harder for more charge to flow into the capacitor so the current decreases. As the charge on the capacitor is increasing, the voltage across it increases too. Return to previous slide A V X Y C R
  • 68. Home The capacitor is said to be fully charged.. 68 A V Capacitor Characteristics X Y C S R Eventually the capacitor will “fill”. This really means that it approaches the condition such that the voltage across it is equal to the supply voltage. There will no longer be any current flowing. The time taken to achieve this increases with increased capacitance and /or resistance. Increasing the supply voltage makes no difference to the time taken for the voltage across the capacitor to approach the voltage across the supply. Return to previous slide
  • 69. Time Constant Calculations 69 The time constant is the time taken for: the current or voltage to have fallen to 37% of its original value or the voltage to have risen to 63% of its original value We can calculate the time constant for a circuit by multiplying the capacitance of the capacitor by the resistance of the resistor: T = C x R The units of the time constant are seconds if the resistance is in ohms and the capacitance in farads. Return to menu
  • 70. Time Constant Calculations E.G. One A 10M0 resistor is connected in series with a 470 pF capacitor. How long will it take to discharge the capacitor to 37V from an initial voltage of 100V? Note that the voltage is falling to 37% of its initial value, so we are looking at one time constant. 70 Using T = C R T = 0.000 000 000 470 x 10 000 000 = 0.004 7 s Return to previous slide
  • 71. Time Constant Calculations E.G. Two A 10M0 resistor is connected in series with a capacitor. If the time constant is 0.001s, what is the capacitance of the capacitor? 71 Using T = C R 0.001 = C x 10 000 000 C = 0.001 / 10 000 000 = 0.000 000 000 1 F = 100 pF Home Return to previous slide
  • 72. 72 Capacitors in Series C1 C2 C3 These three capacitors are connected in series. Their combined capacitance is given by: 1 = 1 + 1 + 1 C C C C total 1 2 3 or C C C C Total + + 1 2 3 C C C 1 2 3 = Return to menu
  • 73. Capacitors in Series Home 4 What is the combined capacitance of a 10 mF, 20 mF and 47 mF capacitor connected in series? C C C C Total + + 1 2 3 C C C The numbers here could get very small so let us omit 5 zeros and give the answer in mF as all the capacitances are in mF anyway. 73 C = (10 x 20 x 47) / (10 + 20 + 47) = 9400 / 77 =122 mF 1 2 3 = C1 C2 C3 Return to previous slide
  • 74. 74 Capacitors in Parallel C1 C2 C3 These three capacitors are connected in parallel with each other. Note that because they are in parallel, they must have the same voltage across each other. The combined capacitance of the network of capacitances is given by: Ctotal = C1 + C2 + C3 Return to menu
  • 75. Home Suppose that the capacitances are 10 mF, 20 mF and 47 mF. 75 Capacitors in Parallel C1 C2 C3 Ctotal = C1 + C2 + C3 So C = 10 + 20 + 47 = 77 mF Return to previous slide
  • 76. 76 Capacitors - Questions 1 What is the combined capacitance of a 10pF and a 20pF capacitor connected in series? 2 What is the combined capacitance of a 10pF and a 20pF capacitor connected in parallel? 3 What is the time constant for a 1000 pF capacitor connected to a 100kW resistance? 4 What capacitance would you need to combine with a 200 mF capacitor to give the combinations a capacitance of 100 mF? How would you connect them together to achieve this? 5 What resistor could you connect with a 47 mF capacitor to give a time constant of 1.83 s ? Return to previous slide
  • 77. C C C C Total + + C C C 77 Capacitors - Answers 1 What is the combined capacitance of a 10pF and a 20pF capacitor connected in series? 1 2 3 The numbers here could get very small so let us omit 11 zeros and give the answer in pF as all the capacitances are in pF anyway. C = (10 x 20) / (10 + 20) = 200 / 30 =6.7 pF 1 2 3 = C1 C2 C3 Return to menu
  • 78. 78 Capacitors - Answers 2 What is the combined capacitance of a 10pF and a 20pF capacitor connected in parallel? C1 C2 C3 Ctotal = C1 + C2 + C3 So C = 10 + 20 = 30 pF Return to menu
  • 79. 79 Capacitors - Answers 3 What is the time constant for a 1000 pF capacitor connected to a 100kW resistance? T = C x R = (1000 x 0.000 000 000 001) x 100 000 = 0.000 1 s Return to menu
  • 80. C C C C Total + + C C C 80 Capacitors - Answers 4 What capacitance would you need to combine with a 200 mF capacitor to give the combinations a capacitance of 100 mF? How would you connect them together to achieve this? In order to get a smaller capacitance, you need to connect them in series. 1 2 3 1 2 3 = C1 C2 C3 So 100 = 200 x C2 / (200 + C2) 100 (200 + C2) = 200C2 20 000 + 100C2 = 200C2 20 000 = 200C2 - 100C2 100 C2 = 20 000 C2 = 200 mF Return to menu
  • 81. 81 Capacitors - Answers 5 What resistor could you connect with a 47 mF capacitor to give a time constant of 1.83 s ? T = C x R 1.83 = 0.000 047 x R R = 1.83 / 0.000 047 = 38 936 W Use 39 kW Return to menu
  • 82. 82 Alternating Current Direct current (DC) is the current that comes from a cell or battery. It is unidirectional. That is to say that the net drift of electrons is in one direction. This one direction will always be from positive to negative for electrons but negative to positive for conventional flow. It is easier to convert voltages from one value to another if the direction of the current is rapidly changing. This is called an alternating current (AC). Return to main menu
  • 83. 83 Alternating Current Alternating current has some strange properties: •it can appear to pass through a capacitor •it produces the discharges that you see in a plasma ball •it can be stepped up (to higher voltages and lower current) •it can be stepped down (to lower voltages and higher current) Mains voltage is always due to an alternating current. It is used because it can be stepped up or down easily. Return to previous slide
  • 84. 84 Alternating Current Throughout Europe, mains voltage is supplied at a frequency of 50 Hz. You will remember that Hz is the abbreviation for hertz - the unit of frequency. This means that the electricity goes through one complete cycle 50 times every second. This means that the voltage will: •start from zero and build up in one direction until it reaches a maximum value (about 325 V). •Fall back to zero •Change direction and start to build up to a maximum value (about - 325 V) •Fall back to zero •50 times per second Alternating voltages (and currents) can have extremely high frequencies. The current that produces radio waves can be many MHz (millions of hertz). Return to previous slide
  • 85. 85 Alternating Current - Questions Home 1 What is the frequency of the mains voltage in the UK and Europe? 2 What is the frequency of the mains voltage in the USA? 3 How long is a complete cycle of mains ac at 50 Hz? 4 How many times does the electricity in 50 Hz ac mains, change direction? 5 Write out 250 MHz in full. Return to previous slide
  • 86. Alternating Current - Answers 1 What is the frequency of the mains voltage in the UK and Europe? 50Hz 2 What is the frequency of the mains voltage in the USA? 60Hz 3 How long is a complete cycle of mains ac at 50 Hz? 86 1/50th of a second = 0.02s Home 4 How many times does the electricity in 50 Hz ac mains, change direction? Twice each cycle so 100 times 5 Write out 250 MHz in full 250 000 000 hertz Return to menu
  • 87. 87 Waveforms As alternating currents and voltages vary with time, it is useful to have a graphical representation of them. The electronic device that does this for us is called an oscilloscope. The essence of an oscilloscope is its ability to plot a graph for us, showing the variation of voltage with time. It is particularly useful because it works extremely quickly and it barely interferes with the circuit from which you are taking the measurements. When you first look at an oscilloscope, the number of knobs, levers and buttons can be bewildering but you will soon get used to it. In fact, you rarely need to use most of them. Return to menu
  • 88. 88 Waveforms Screen showing the trace On / off switch x input The trace shows a graph with voltage on the y axis (vertical) and time on the x axis (horizontal). Return to previous slide
  • 89. 89 Waveforms The waveform produced by mains voltage looks like this: Voltage time This shape of waveform is called a sinusoidal wave. Return to previous slide
  • 90. 90 Waveforms The waveform produced by mains voltage looks like this: Voltage time The arrows indicate a complete cycle. A cycle is the time that it takes to reach the next adjacent identical position on the waveform. Return to previous slide
  • 91. Waveforms The waveform produced by mains voltage looks like this: 91 Voltage time This arrow indicates the peak voltage. For mains it is about 325V in the UK. The value of 230V that is quoted is the peak divided by the square root of 2. (It is the dc equivalent voltage that would produce the same heating effect as an ac with a peak voltage of 325V. Dividing by root 2 only works for sinusoidal waveforms). The peak voltage is the maximum voltage. Return to previous slide
  • 92. Waveforms The waveform produced by mains voltage looks like this: 92 Voltage time This arrow indicates the peak to peak voltage. Notice that the peak to peak voltage is twice the peak voltage. For mains it is about 650V in the UK and Europe. Return to previous slide
  • 93. 93 Waveforms Another common waveform called the square wave looks like this: Voltage time The arrows indicate a complete cycle. A cycle is the time that it takes to reach the next adjacent identical position on the waveform. Return to previous slide
  • 94. 94 Waveforms Another common waveform called the square wave looks like this: Voltage time This arrow indicates the peak voltage. Return to previous slide
  • 95. 95 Waveforms Another common waveform called the square wave looks like this: Voltage time This arrow indicates the peak to peak voltage. It will be twice the peak voltage Return to previous slide
  • 96. 96 Waveforms Another common waveform called the saw-tooth wave looks like this: Voltage time The arrows indicate a complete cycle. A cycle is the time that it takes to reach the next adjacent identical position on the waveform. Return to previous slide
  • 97. 97 Waveforms Another common waveform called the saw-tooth wave looks like this: Voltage time This arrow indicates the peak voltage. Return to previous slide
  • 98. 98 Waveforms Another common waveform called the saw-tooth wave looks like this: Voltage time This arrow indicates the peak to peak voltage. Return to previous slide
  • 99. 99 Waveforms - Questions Home 1 What is the name of the trace shown on the oscilloscope? 2 How many complete cycles can you see? 3 If the scale on the y-axis is 2V per division, estimate the peak voltage. What is the peak to peak voltage? 4 If the scale on the x-axis is 2ms per division, estimate the length of a cycle. 5 Using your answer to question 4, calculate the frequency of the wave. Return to previous slide
  • 100. 100 Waveforms - Answers 1 What is the name of the trace shown on the oscilloscope? Return to menu
  • 101. 101 Waveforms - Answers 2 How many complete cycles can you see? ONE TWO THREE Return to menu
  • 102. 3 If the scale on the y-axis is 2V per division, estimate the peak voltage. What is the peak to peak voltage? 102 Waveforms - Answers 5 divisions so 5 divisions x 2 V per division = 10V Return to menu
  • 103. 103 Waveforms - Answers 4 If the scale on the x-axis is 2ms per division, estimate the length of a cycle. Count as many complete cycles as you can to get as accurate an answer as possible. 3 cycles is about 35 divisions 1 cycle is about 11.7 divisions 11.7 divisions is 11.7 x 2 ms = 23.4 ms Return to menu
  • 104. 104 Waveforms - Answers 5 Using your answer to question 4, calculate the frequency of the wave. From question 4 one cycle is about = 23.4 ms 23.4ms = 23.4 x 0.001s = 0.0234s How many of these can we get into 1 second? = 1 / 0.0234 = 42.7 Hz Return to menu
  • 105. 105 The Potential Divider Voltage is sometimes referred to as potential difference. The potential divider simply divides up a potential or voltage. In its simplest form it is two resistors placed across a power supply. The voltage across of each resistor is less than the supply voltage. Adding the voltage across each resistor will give the supply voltage. It is probably easiest to understand if you look at the diagram. +9V 0 V Here the power supply is 9V. Note that both the resistances are the same. The voltage from the supply will be split (divided) equally as 4.5V. Of course 4.5V + 4.5V = 9V. Return to menu
  • 106. 106 +9V 0 V The Potential Divider In this potential divider circuit, the resistances are not the same. 2 000 W 1 000 W The bigger resistance here means that there will be a bigger voltage here. The smaller resistance here means that there will be a smaller voltage here. It is 2/3rds of the resistance. It is 2/3rds of the resistance. It is 1/3rd of the resistance. It is 1/3rd of the resistance. It develops 2/3rds of the voltage. It develops 2/3rds of the voltage. It develops 1/3rd of the voltage. It develops 1/3rd of the voltage. 2/3 x 9V = 6V 1/3 x 9V = 3V If you would like to work through this again, step back through the sequence using the left arrow key. Return to previous slide
  • 107. 107 +V 0 V The Potential Divider R1 R2 V1 V2 You can calculate the voltage across each resistor using a formula too. VV11 VV 11 == VV xx RR11 // ((RR11 ++ RR22)) V1 = 9 x 2 000 / (1 000 + 2000) = 9 x 2 / 3 = 6V VV 22 == VV xx RR22 // ((RR11 ++ RR22)) V1 = 9 x 1 000 / (1 000 + 2000) = 9 x 1 / 3 = 3V Return to previous slide
  • 108. 108 The Potential Divider The potential divider does not have to be made up of two fixed resistors. One of them could be variable, or even both. R1 R2 V1 V2 As R1 increases so does V1 but V2 will fall. As R1 decreases so does V1 but V2 will rise. It is just as if there is only one cake to go around (the voltage). If R1 increases then V1gets more cake so there is less left for V2! Return to previous slide
  • 109. 109 The Potential Divider Now the variable resistor has been moved to the lower position in the network.. R1 R2 V1 V2 As R2 increases so does V2 but V1 will fall. As R2 decreases so does V2 but V1 will rise. It can be handy to change the position of the variable resistor. Later you will see that it can change the action of a transistor circuit so make sure that you follow it. Return to previous slide
  • 110. 110 The Potential Divider +V 0V With this potential divider, the “tap” in the middle is a “slider”. It probably moves along a track of carbon. R1 and V1 will be the resistance and voltage “above” the slider. R1 V1 R2 and V2 will be the resistance and voltage “below” the slider. R2 V2 As R1 increases, R2 decreases. This will result in V1 increasing and V2 decreasing. As R1 decreases, R2 increases. This will result in V1 decreasing and V2 increasing. Return to previous slide
  • 111. Here is a component that could be used as a potential divider. The black ring is the carbon track. You adjust it by putting a screwdriver in here and turning the outer metal ring. 111 The Potential Divider Return to previous slide
  • 112. You adjust it by putting a screwdriver in here and turning the outer metal ring. 112 The Potential Divider Return to previous slide Here is another:
  • 113. It is possible to use many different components that vary their resistance in a potential divider circuit. Here are a few that you might find and the physical conditions that change their resistance. Light Dependent Resistor (LDR) - decreases resistance with increased illumination. Thermistor - decreases its resistance with increased temperature (negative temperature coefficient). Microphone - changes resistance with sound. Strain gauge - changes its resistance when stressed. Photodiode - decreases resistance with increased illumination. 113 The Potential Divider Return to previous slide
  • 114. The Potential Divider - Questions 1 A 2k and a 3k resistor are used in potential divider using a 10V supply. Sketch a possible set up and label the resistors and the voltages across them. 2 Suggest two possible fixed resistors that could be used to obtain 3V from a 15V supply. 3 A 27k and a 62k resistor are used in potential divider using a 12V supply. Sketch a possible set up and label the resistors and the voltages across them. 4 A 15V supply is attached across a potential divider. If one of the resistors is a 390k and there is a voltage of 9V across the other, what is the second resistance? 5 A potential divider is created from a fixed resistor and an LDR. Explain how the network produces different voltages. 114 Home Return to previous slide Answer Answer Answer Answer Answer
  • 115. The Potential Divider - Answers 1 A 2k and a 3k resistor are used in potential divider using a 10V supply. Sketch a possible set up and label the resistors and the voltages across them. 115 +10V 0 V R 1 = 2 000 W V1= 4V V2 = 6V VV11 VV 11 == VV xx RR11 // ((RR11 ++ RR22)) V1 = 10 x 2 000 / (3 000 + 2000) = 10 x 2 / 5 = 4V VV 22 == VV xx RR22 // ((RR11 ++ RR22)) V1 = 10 x 3 000 / (3 000 + 2000) = 10 x 3 / 5 = 6V R 2 = 3 000 W Return to menu
  • 116. The Potential Divider - Answers 2 Suggest two possible fixed resistors that could be used to obtain 3V from a 15V supply. VV11 VV 11 == VV xx RR11 // ((RR11 ++ RR22)) So 3 = 15 x R1 / (R1 + R2) We could use more or less any combination. However, they should be quite high so that they do not drain a lot of current. 116 Let us choose R1 as being 100k. 3 = 15 x 100 / (100 +R2) 3(100 + R2) = 1 500 300 + 3R2 = 1 500 3R2 = 1 500 - 300 = 1 200 R2 = 1 200 / 3 = 400k. Return to menu
  • 117. The Potential Divider - Answers 3 A 27k and a 62k resistor are used in potential divider using a 12V supply. Sketch a possible set up and label the resistors and the voltages across them. VV11 VV 11 == VV xx RR11 // ((RR11 ++ RR22)) V1 = 12 x 27 / (27 + 62) = 12 x 27 / 89 = 3.64V VV 22 == VV xx RR22 // ((RR11 ++ RR22)) 117 +12V 0 V R 1 = 27kW V1= 3.64V V2 = 8.36V V1 = 12 x 62 / (27 + 62) = 12 x 62 / 89 = 8.36V R 2 = 62kW Return to menu
  • 118. The Potential Divider - Answers 4 A 15V supply is attached across a potential divider. If one of the resistors is a 390k and there is a voltage of 9V across the other, what is the second resistance? 118 So V1 = 15 - 9 = 6V VV11 VV 11 == VV xx RR11 // ((RR11 ++ RR22)) Now 6 = 15 x R1 / (R1 +390) 6 (R1 + 390) = 15 R1 6 R1 + 2 340 = 15 R1 9R1 = 2 340 R1 = 2 340 / 9 = 260k so use 270k Return to menu
  • 119. The Potential Divider - Answers 5 A potential divider is created from a fixed resistor and an LDR. Explain how the network produces different voltages. In bright illumination the LDR’s resistance falls. The voltage across the LDR will consequently fall while the voltage across the fixed resistance will rise. As it goes dark, the LDR’s resistance will increase, increasing the voltage across the LDR. As this happens, the voltage across the resistor will fall. 119 Return to menu
  • 120. The transistor is a three connection component that can be used either as an amplifier or a switch. +V 0V 120 Transistor Circuits +0.7V base collector emitter Essentially the circuit is set up so as to try to force electrons through the emitter and out of the collector. This might be to light a bulb. However, under normal circumstances, there is a very high resistance between the emitter and the collector so the bulb will not light. If we make the base go positive, the collector / emitter junction conducts and the bulb will light. Return to menu
  • 121. 121 Transistor Circuits The clever part now is to control the base bias voltage that turns the transistor on. +V 0V The base bias voltage is the voltage between the base and the emitter. If it is anything much less that 0.7V, the transistor will be off. The transistor switches on when it is 0.7V. You should never allow the base bias voltage to get too high as this will overheat the base and burn out the transistor. For this reason you will frequently find a resistor connected to the base. c e b Rb Return
  • 122. Correct selection of the two resistors Rand R1 2 will take the base to 0.7V and turn the transistor on. Suppose Rwas much 2 higher than R. The 1voltage across Rwould 2 be high so the transistor would switch on. 122 Return Transistor Circuits The clever part now is to control the base bias voltage that turns the transistor on. +V 0V c e b This can be achieved using a potential divider. Rb R1 R2
  • 123. 123 Transistor Circuits The clever part now is to control the base bias voltage that turns the transistor on. +V 0V c e b Rb R1 R2 Now suppose R2 was an LDR. In the bright light, its resistance would be low so the voltage across it would be low, the transistor switched off and the lamp off. But suppose that it now goes dark! Return
  • 124. It has just gone dark! The resistance of the LDR rises. The voltage across the LDR rises. The base bias voltage reaches 0.7V The transistor switches on. The bulb lights. 124 Return Transistor Circuits The clever part now is to control the base bias voltage that turns the transistor on. +V 0V c e b Rb R1 R2
  • 125. 125 Transistor Circuits The clever part now is to control the base bias voltage that turns the transistor on. +V 0V c e b Rb R1 R2 Suppose that we now swap the positions of the resistor and the LDR. The bulb will now come on in daylight! It might be useful as a warning light circuit in certain circumstances. Return
  • 126. 126 Transistor Circuits The clever part now is to control the base bias voltage that turns the transistor on. +V 0V c e b Rb R1 R2 Now let us consider: •Ib the base current that flows into the transistor •Ie the emitter current that flows out of the transistor Ib Ie •IC the collector current that flows into the transistor Ie = Ib + Ic Ic Return
  • 127. 127 Transistor Circuits The clever part now is to control the base bias voltage that turns the transistor on. +V 0V c e b Rb R1 R2 Ib Ie Ie = Ib + Ic Ic The base current will be very small as it has passed through R1 and Rb so it is almost true that Ie = Ic. The ratio of Ic : Ib is important. It shows that the transistor is amplifying. It is often around about 100. Return
  • 128. Ie = Ib + Ic That is to say that the Ic collector current is a always a constant amount bigger than the base current. Feed a small current to the base and you get a big current in the collector. 128 Transistor Circuits The clever part now is to control the base bias voltage that turns the transistor on. +V 0V c e b Rb R1 R2 Ib Ie Return
  • 129. 129 Transistor Circuits The clever part now is to control the base bias voltage that turns the transistor on. +V 0V c e b Rb R1 R2 Ib Ie Ie = Ib + Ic Ic The ratio is called hfe. hfe = Ic / Ib Return
  • 130. 130 Click on a component to find out what it does. Transistor Circuits +V 0V c e b Rb R1 R2 C1 Relay CONTINUE Return
  • 131. 131 Transistor Circuits Click on a component to find out what it does. Capacitor This stores charge. It acts as a time delay to any switching. If the transistor is on and tries to go off, it will act as a reservoir and keep the transistor on for a while longer. +V 0V c e b Rb R1 R2 C1 Relay CONTINUE Return
  • 132. 132 Click on a component to find out what it does. LDR Light Dependent Resistor Its resistance decreases with increased illumination. In the dark, the resistance goes up turning the transistor on. Transistor Circuits +V 0V c e b Rb R1 R2 C1 Relay CONTINUE Return
  • 133. 133 Click on a component to find out what it does. Base Bias Resistor This fixed resistor protects the base from too much current. Transistor Circuits +V 0V c e b Rb R1 R2 C1 Relay CONTINUE Return
  • 134. 134 Click on a component to find out what it does. Potential Divider The LDR and R2 are a potential divider. Transistor Circuits +V 0V c e b Rb R1 R2 C1 Relay CONTINUE Return
  • 135. 135 Click on a component to find out what it does. Transistor A small voltage at the base will allow current to flow through the emitter from the collector. Transistor Circuits +V 0V c e b Rb R1 R2 C1 Relay CONTINUE Return
  • 136. 136 Click on a component to find out what it does. Diode - this only allows current to flow in the direction of the arrow head. Rapid changes in the magnetic field of the relay can cause high voltage that would damage the transistor. The diode diverts the currents formed by this process. Transistor Circuits +V 0V c e b Rb R1 R2 C1 Relay CONTINUE Return
  • 137. 137 Click on a component to find out what it does. Relay - current through the relay produces a magnetic field that throws a switch in another external circuit. The external circuit can be a much higher powered circuit. Transistor Circuits +V 0V c e b Rb R1 R2 C1 Relay CONTINUE Return
  • 138. Transistor Circuits - Questions 1 The collector current in a circuit is 120mA when the base current is 3mA. What is hfe and the emitter current? 2 Why do we connect a resistor directly to the base of the transistor? 3 Sketch a circuit that will throw a relay in the dark that in turn will turn on a switch. 4 Why should a diode be connected across a relay in the collector circuit of a network? 5 Explain what happens when the resistance of the base bias resistor falls in a transistor circuit controlling a motor. 138 Answers: 1 2 3 4 5 Return to previous slide
  • 139. Transistor Circuits - Answers 1 The collector current in a circuit is 120mA when the base current is 3mA. What is hfe and the emitter current? 139 hfe = Ic / Ib = 120 / 3 = 40 Return to menu
  • 140. Transistor Circuits - Answers 2 Why do we connect a resistor directly to the base of the transistor? The resistor limits the current entering the base. This stops the base from overheating due to excessive currents which would burn the transistor 140 out. Return to menu
  • 141. Transistor Circuits - Answers 3 Sketch a circuit that will throw a relay in the dark that in turn will turn on a switch. 141 +V 0V c e b R1 C1 Relay LDR Return to menu
  • 142. Transistor Circuits - Answers 4 Why should a diode be connected across a relay in the collector circuit of a network? The relay can create large voltages due to rapid changes in magnetic fields as they switch off. The diode provides a short circuit for the current due to this voltage. As diodes only carry current in one direction, the diode connected to the relay will have no effect in normal operation 142 of the relay. Return to menu
  • 143. Transistor Circuits - Answers 5 Explain what happens when the resistance of the base bias resistor falls in a transistor circuit controlling a motor. As the resistance falls, so will the voltage across it. The voltage across the base will consequently fall. 143 This will turn off the transistor. The collector current will fall to zero (or extremely close to zero). The motor will switch off. Return to menu
  • 144. 144 Electronics Questions 1 What is the nominal value and tolerance of this resistor? 2 A power supply drives a current of 150mA through a bulb with a working resistance of 10W. What voltage is the power supply? 3 What is the current passing through a heater that dissipates 40W when a voltage of 10V is applied across it? Return to menu
  • 145. 4 What is the combined resistance of a 30k W, 20k W and 47k W resistor connected in parallel? 5 Suppose you need a 50k W resistor but you only have a 47k W and a handful of assorted resistors. What other resistor would you search for and how would you connect them together? 6 What is the combined capacitance of a 47pF and a 20pF capacitor connected in series? 7 What is the combined capacitance of a 47pF and a 20pF capacitor connected in parallel? 8 What is the time constant for a 1000 mF capacitor connected to a 10MW resistance? 145 Electronics Questions Return to previous slide
  • 146. 9 If the scale on the y-axis is 4mV per division, estimate the peak voltage. What is the peak to peak voltage? 10 If the scale on the x-axis is 50 ms per division, estimate the length of a cycle. Using your answer, calculate the frequency of the wave. 146 Electronics Questions Return to previous slide
  • 147. Retu1r4n7 to previous slide Return to main menu
  • 148. 1 What is the nominal value and tolerance of this resistor? This gold band indicates that the tolerance of the resistor is ±5% (plus or minus 5 percent). The third band is black. This means that there are no zeros. The second band is green. This means the second digit is 5. The first band is violet. This means the first digit is 7. 148 So the resistor is nominally 75 W. Return to menu Electronics Answers
  • 149. 2 A power supply drives a current of 150mA through a bulb with a working resistance of 10W. What voltage is the power supply? 149 V = I x R so V = 0.15 x 10 =1.5 V Return to menu Electronics Answers
  • 150. 3 What is the current passing through a coil that dissipates 40W when a voltage of 10V is applied across it? 150 P = IV So I = P / V = 40 / 10 = 4 W Return to menu Electronics Answers
  • 151. 4 What is the combined resistance of a 30kW, 20kW and 47kW resistor connected in parallel? R R R R Total + + 1 2 3 R R R 1 2 3 151 = The numbers here could get very big so let us omit three zeros and give the answer in kW as all the resistances are in kW anyway. R = (30 x 20 x 47) / (30 + 20 + 47) = 28 200 / 97 =291 kW Use 300 kW Return to menu Electronics Answers
  • 152. 5 Suppose you need a 50 kW resistor but you only have a 47 kW and a handful of assorted resistors. What other resistor would you search for and how would you connect them together? You are looking to increase the resistance by adding another resistor. This can only be done by adding a resistor in series. R total= R1 + R2 + R3 or R = R1 + R2 + R3 152 We know that Rtotal is 50 kW and R1 is 47 kW So 50 = 47 + R2 R2 = 50 - 47 = 3 kW Return to menu Electronics Answers
  • 153. 6 What is the combined capacitance of a 47pF and a 20pF capacitor connected in series? C C C C Total + + 1 2 3 C C C The numbers here could get very small so let us omit 11 zeros and give the answer in pF as all the capacitances are in pF anyway. 153 C = (47 x 20) / (47 + 20) = 940 / 67 =14 pF 1 2 3 = C1 C2 C3 Return to menu Electronics Answers
  • 154. 7 What is the combined capacitance of a 47pF and a 20pF capacitor connected in parallel? 154 C1 C2 C3 Ctotal = C1 + C2 + C3 So C = 47 + 20 = 67 pF Return to menu Electronics Answers
  • 155. 8 What is the time constant for a 1000 mF capacitor connected to a 10MW resistance? 155 T = C x R = (1000 x 0.000 001) x 10 000 000 = 10 000 s Return to menu Electronics Answers
  • 156. 9 If the scale on the y-axis is 4mV per division, estimate the peak voltage. What is the peak to peak voltage? 156 5 divisions so 5 divisions x 4mV per division = 20mV Return to menu Electronics Answers
  • 157. Electronics Answers 10 If the scale on the x-axis is 50 ms per division, estimate the length of a cycle. Count as many complete cycles as you can to get as accurate an answer as possible. 157 3 cycles is about 35 divisions 1 cycle is about 11.7 divisions 11.7 divisions is 11.7 x 2 ms = 23.4 ms
  • 158. 10 continued Using your previous answer, calculate the frequency of the wave. From question 4 one cycle is about = 23.4 ms 158 23.4 ms = 23.4 x 0.000 001s = 0.000 023 4s How many of these can we get into 1 second? = 1 / 0.000 023 4s = 42.7 kHz Return to menu Electronics Answers
  • 159. Home Retu1r5n9 to previous slide Introduction Ohm’s Law Power Calculations Resistors in Series and Parallel Capacitors Alternating Current Waveforms Transistor Circuits The Potential Divider Components Questions