Remember:
the animations do not work in .pdf
KIT OF PARTS Talking Electronics supplies a kit of parts that can be used to build the majority of the circuits in this eBook. The kit costs $15.00 plus postage.
Learn electronics from the beginning . . .
Milli -
milli means
1/1,000th (one thousandth) - such as one milliamp or one
millivolt.
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Here are all the colours and values for the resistors you will using in this course. Just match-up the colours on your resistor with the resistors above and you will find the value. |
Resistor values are always
OHM values. One ohm is a small value. It might be the
resistance of a length of wire 3 metres long. When a switch is open the resistance is infinite - millions and millions of ohms. The resistance of your body from one hand to the other will be about 70,000 ohms. The resistance between two wires dipped in water will be about 1,000 to 100,000 ohms (depending on the dissolved-salts in the water - pure water has a very high resistance) The resistance of the filament of a 3v globe will be about 30 ohms. The resistance of the winding of a 3v motor will be about 3 ohms. Resistors are made with values from less than one ohm to more than 10 million ohms by adding carbon to the mixture inside the resistor (and cutting a track around the outside of the resistor) then connecting a lead to each end. Adding more carbon reduces the value of resistance. Carbon has a low resistance. Resistance-values are measured with the RESISTANCE settings on a MULTIMETER. This is called the "Ohms Range." Sometimes with the symbol: W A Multimeter will have 2, 3 4 or more scales to cover the range one ohm to 10 million ohms. Low value resistors (from 1 ohm to 999 ohms) are written as 1R, 220R, 470R, 999R. with the letter "R" indicating Resistance (ohms). You can also use the symbol "omega" (W) For values above 1,000 ohms to 99,999 ohms, they are written as: 1k, 2k2, 4k7, 10k, 100k, 220k, 470k, with the letter "k" indicating "kilo" (thousand). 1M = 1,000,000 - one million ohms 1M2, 2M2, 4M7, 10M. The letters "R, k and M" are placed so they take the place of the decimal point. This prevents any mistake, as a decimal point can be missing in a poor photocopy. |
![]() MULTIMETERS There are two types of MULTIMETER. The top two are called DIGITAL MULTIMETERS (DMM) and show numbers on a display. The lower two meters are called ANALOGUE MULTIMETERS and have a pointer and scale. All meters come with a set of red and black leads. The red lead is always connected to the positive of the battery or the positive on a project and the black lead is connected to the negative or earth or chassis. When making a resistance measurement, the leads can be around either way. Resistance measurements are always made with the power removed from a circuit. Any voltage on a circuit will upset the resistance reading. |
![]() Fig 22. Resistance Measurement with Analogue Multimeter | The resistance of a
resistor is measured by placing the leads of the multimeter on the ends of a
resistor and turning the dial on the analogue multimeter to the
resistance scale to make the pointer move to about the centre
of the scale. The resistance scale is marked with a high value on the left and 0 ohm on the right. This is opposite to all the other scales. You must get the pointer to move to the middle of the scale as it is not accurate at left-end. Analogue multimeters are only suitable for reading values from 1 ohm to 100,000 ohms. The scale is too hard to read above 100k. To find the value of a resistor, you can compare the colours with the table above. |
![]() Fig 23. Resistance Measurement with a DMM | A digital
multimeter produces a
more-accurate reading of resistance. It is accurate from 1 ohm to 10M ohms. Select the scale that provides a reading. |
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Fig 24.
Connecting LEDs in series |
![]() Fig 25. Connecting LEDs in series |
Different-colour LEDs
can be connected in series. Add up the total Characteristic
Voltage for the 5 LEDs and see if it is less than 12v. The 220R resistor will have to be reduced to 47R to make the LEDs bright. |
![]() Fig 26. Connecting LEDs in parallel |
LEDs can be
connected in parallel if they are the same colour. In the diagram a red LED drops a CHARACTERISTIC VOLTAGE of 1.7v and if they are from the same manufacturer or the same batch, they will work ok. Although we say the characteristic voltage for a red LED is 1.7v, this can change slightly from different manufacturers and one LED may glow brightly while the other is dull. You have to build the circuit and see the result. |
![]() Fig 27. Connecting LEDs in parallel |
Different colour
LEDs cannot be connected in parallel. The voltage across a red
LED is 1.7v. This becomes the "Supply Voltage" for the green LED and it is too low. The green LED needs a supply of 2.1v to 2.3v. Only the red LED will illuminate. |
![]() Fig 28. Connecting Resistors in Series |
Suppose you
don't have a 220 ohm resistor. You can make a 220 ohm resistor with two resistors in series. The total resistance will be 200 ohms, but resistors are not accurate and the result will be very close to 220R. Electronic circuits are not very critical. You will not be able to see the difference in brightness between 200 ohms and 220 ohms. When resistors are connected in series, the total resistance is found by adding the resistance of each resistor. ![]() |
![]() Fig 29. Connecting Resistors in Parallel |
You can
create a 220 ohm resistor by connecting two resistors in
Parallel. When two equal-value resistors are connected in Parallel, the total resistance across the combination is HALF. 470R in parallel with 470R produces 235R. This is very close to 220R. We are not going into the formula as it is very complex. Three equal-value resistors in parallel produce a total of one-third. Simply get two resistors and connect them in parallel and measure them with a multimeter. |
![]() Fig 29a. Two tricky resistor questions |
Figure
A shows three resistors. It
looks hard to solve so the middle resistor is turned so it
connects directly to the top and bottom rail. Now you can see
the circuit is three resistors in parallel. The result is
one-third of an ohm. Figure C shows twelve 6 ohm resistors. Replace each group with a 2 ohm resistor, because three 6 ohm resistors in parallel is equal to 2 ohms. ![]() The result of two 4 ohm resistors in parallel is 2 ohms. The resistance of the circuit does not change if the switch is open or closed. |
![]() Fig 30. Flashing LED |
There are some
special LEDs that can be connected to 3v to 9v and they flash or
produce a range of colours. These LEDs have a chip and resistor inside the body of the LED to produce the effect and allow the LED to operate on a voltage without the need for a current limiting resistor. |
![]() Fig 31. These diagrams show the resistor needed to produce 1mA to 25mA current through a single LED on 3v, 5v, 9v and 12v supply. |
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THE VOLTAGE DIVIDER In the circuits above, the resistor and LED are forming a VOLTAGE DIVIDER. A red LED is dropping 1.7v across it and the resistor is dropping the remaining voltage. Whenever two (or more) components are placed across a battery, they form a VOLTAGE DIVIDER. Sometimes we want a 6v supply and only have 12v. We can produce the 6v supply by putting two equal-value resistors across the 12v as shown in the circuit opposite. We are not going into the mathematics because the selection of the correct value is very complex and the circuit is very wasteful. |
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THE CURRENT DIVIDER The CURRENT DIVIDER CIRCUIT is actually a LOAD SHARING CIRCUIT. Suppose you are testing a Power Supply and need a 10 watt LOAD. But you only have 5 watt resistors. Placing two 5watt resistors in parallel across the output of the power supply will allow half the current to flow though each resistor. This is called CURRENT SHARING or LOAD SHARING and the current is divided (or passed) through each resistor according to the value of resistance. |
![]() Fig 32. The DIODE |
THE DIODE The next simple electronic component is the DIODE. It only works when connected correctly. A DIODE allows current to flow through it when it is connected as shown in the diagram. A Diode is similar to a one-way water valve. When the diode is "facing down," the motor spins. When it is "facing up" the motor does not spin. |
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The diagram shows
the "current path" around the circuit. The current is measured
in AMPS and we discuss current as CONVENTIONAL CURRENT. This is the way current was thought to flow when electricity was born and they said it flows out the POSITIVE TERMINAL of the battery, around the circuit and into the NEGATIVE TERMINAL. The arrow on the diode shows the current will flow through the diode and allow the motor to spin. The diode is said to be FORWARD BIASED. |
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There is no flow of
current because the diode prevents any current-flow when
connected as shown. The motor DOES NOT WORK. The diode is said to be REVERSE BIASED. |
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Fig 33. A
Signal diode and a Power |
There are hundreds
of different types of diodes. Power diodes, signal diodes, low voltage diodes, high voltage diodes, high-speed diodes and many other types. They all do one thing. They pass current in one direction and if turned around, they do not pass any current.
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![]() Fig 34. A Protection diode |
Diodes perform many function in
electrical and electronic circuits. Here is an application as a
PROTECTION DIODE. It protects the amplifier. If the 12v battery is connected around the wrong way, no current will flow. |
![]() Fig 35. Diode "Voltage Drop" |
When a
diode is placed in a circuit (and
current is flowing), a small voltage develops across the diode.
This voltage is called the FORWARD VOLTAGE DROP.
This voltage is approximately 0.6v. This is due to a junction inside the diode where two different materials are joined. Normally, this voltage is not important because it is only small, but sometimes you need to take it into account. For the circuit above, the amplifier only gets 11.4v |
![]() Fig 36. Measuring Voltage with a Digital Multimeter |
Voltage is measured with a VOLTMETER. Multimeters have 2 or 3 voltage ranges so you can measure low voltage (0v to 20v), medium voltages (0v to 200v and high voltages (0v to 500v). A voltmeter is placed across the component being tested, as shown in the diagram. The Digital Multimeter is detecting 11.4v across the amplifier. |
![]() Fig 37. Measuring Voltage with a Digital Multimeter |
If you place the
probes of a digital multimeter around the wrong way on a
component, the display will show a "-"
The meter will not be damaged. |
![]() Fig 38. Measuring Voltage with an Analogue Multimeter |
An analogue
Multimeter must be connected around the correct way to make the
pointer move "up scale." Select the range that will allow the pointer to show somewhere in the middle of the scale. |
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Fig 39. Measuring Current with an Analogue |
Current is
measured by "breaking
into the circuit" and inserting the leads so the positive probe
is closest to the positive of the battery. If you connect the leads around the other way, the needle will not move but it will hit the "end stop" and you may have to "bump" the meter to get the pointer to move from its jammed position. |
![]() Fig 39a. The Solar Panel and the Blocking Diode |
A DIODE is also used with a
solar panel to prevent the battery discharging into the solar
panel when the sun is not shining. When the solar panel is not receiving any light it becomes a resistor with a large value and a small current can flow through it from the battery. The diode prevents this current-flow. The diode is called a BLOCKING DIODE. |
![]() Fig 39b. The Solar Panel with diodes called BLOCKING DIODES and BYPASS DIODES. |
Diodes are given different
names, according to their function. They all perform the same
job by passing current in one direction and prevent current-flow
in the opposite direction. When the top solar panel is shaded by a cloud, it generates less current and this will reduce the current into the battery. By placing a diode across the panel, the diode will pass the current produced by the lower panel to the battery. These diodes are called BYPASS DIODES. |
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The next component we cover is the
CAPACITOR. There are thousands of different types of capacitor. Each value of capacitor can have a low voltage rating, medium voltage or high voltage. Capacitors can be very small in size and shape or very stable with temperature-rise or simply very cheap to make. A capacitor consists of two thin sheets of metal such as aluminium with a thin sheet of plastic between. The sheets may be rolled up in a cylinder or laid on top of each other. The fact is this: the top sheet of metal does not touch the bottom sheet. This is shown in the symbol. The resistance between the two terminals is INFINITE. The 6th capacitor in the top row is called a MONOBLOCK. |
![]() Fig 41. Electrolytic Capacitor |
A capacitor gets bigger
as its value increases. It also gets bigger when the voltage-rating increases. The basic unit of capacitance is the FARAD. A one-farad capacitor would be the size of a house. To make the capacitor smaller the sheets are etched to increase the surface-area and different insulating materials are used between the sheets. The result is a capacitor called an ELECTROLYTIC. It is a bit like a rechargeable battery. It stores a lot of energy in a small space. The negative lead is shorter and has a black stripe on the side of the electrolytic. |
One FARAD is too big to handle. We
use smaller values. The middle of the range is one microfarad. This is written as 1u. (sometimes you see uF) This is one-millionth of a FARAD. The smallest value of capacitance is one picofarad. This is one millionth of a microfarad. It is written as 1p. Capacitors are broadly separated into two groups. 1p to 1u and 1u to 100,000u Capacitors 1p to 1u are ceramic, polyester, air, styroseal, monoblock and other names. Capacitors 1u to 100,000u are electrolytic or tantalum. A tantalum is the same as an electrolytic - for testing purposes - it is a more-compact electrolytic. 1 microfarad is one millionth of 1 farad. 1 microfarad is divided into smaller parts called nanofarad. 1,000 nanofarad = 1 microfarad Nanofarad is divided into small parts called picofarad 1,000 picofarad = 1 nanofarad. Recapping: 1p = 1 picofarad. 1,000p = 1n ( 1 nanofarad) 1,000,000p = 1u 1,000n = 1u (1 microfarad) 1,000u = 1millifarad 1,000,000u = 1 FARAD. Examples: All ceramic capacitors are marked in "p" (puff") A ceramic with 22 is 22p = 22 picofarad A ceramic with 47 is 47p = 47 picofarad A ceramic with 470 is 470p = 470 picofarad A ceramic with 471 is 470p = 470 picofarad A ceramic with 101 is 100p (it can also be 100) A ceramic with 102 is 1,000p = 1n A ceramic with 223 is 22,000p = 22n A ceramic with 104 is 100,000p = 100n = 0.1u A common 100n is called a MONOBLOCK. A ceramic with 105 is 1u TYPES OF CAPACITOR For testing purposes, there are two types of capacitor. Capacitors from 1p to 100n are non-polar and can be inserted into a circuit around either way. Capacitors from 1u to 100,000u are electrolytics (or tantalum) and are polarised. They must be fitted so the positive lead goes to the supply voltage and the negative lead goes to ground (or earth). |
![]() Fig 42. Charging a Capacitor |
Here is an
experiment to show how much (little) energy is stored in a 100u
electrolytic. When the slide-switch is in position "B", the 100u is charged by the 6v battery. When the slide switch is moved to position "A" the electrolytic supplies energy to illuminate the red LED via the 220R resistor. It will illuminate for a short period of time. By moving the switch back and forth, you can keep the LED illuminated. |
![]() Fig 43. Capacitors in Series |
Capacitors
can be connected in Series or Parallel to obtain a value
of capacitance you may not have available. They are also connected in series to increase the effective VOLTAGE RATING. However when two equal-value capacitors are connected in series, the final value is HALF, and thus you need two with double the final-value to get a value with an increased voltage-rating. When two equal-value capacitors are connected in series, the result is HALF. (This is the opposite to connecting resistors) |
Fig 43a. Non-polar Capacitor |
If you connect the
electrolytic around the wrong way, this layer "breaks-down" and
the resistance of the electrolytic becomes very small and a high
current flows. This heats up the electrolytic and the current
increases. Very soon the capacitor produces gasses and explodes.
One big mistake in many text books shows how to make a non-polar electrolytic by connecting two "back-to-back." They claim 2 x 100u connected back-to-back is equal to 47u. This appears to be case when testing on a meter but the meter simply charges them for a short period of time to get a reading. If you allow them to charge fully you will find the reverse electrolytic has a very small voltage across it. Secondly, when you are charging them, you are putting a high current through the reverse electrolytic and damaging the layer. To prevent this, you need to add two diodes as shown in the diagram. In addition, 2 x 100u "back-to-back" is very near 100u. |
![]() Fig 44. Capacitors in Parallel |
Capacitors can be
connected in Parallel to obtain a value of capacitance
you may not have available. (This does not change the VOLTAGE RATING.) When two equal-value capacitors are connected in parallel, the result is DOUBLE. (This is the opposite to connecting resistors). If one electrolytic is 25v and the other 63v, the answer is the LOWER VOLTAGE = 25v. |
![]() Fig 45. Variable Capacitors and Resistors |
The value of a
capacitor or resistor may need to be increased or decreased in a
circuit to tune in radio stations or increase and decrease the
volume of a speaker. The symbol for these components have an arrow to show they can be adjusted. The resistance of a potentiometer can be from 1 ohm to 5M They come in many different shapes and sizes to suit the PC board or front-panel layout. The "T" represents a trimmer capacitor and this can be from 1p to about 120p. A variable capacitor will be from about 10p to 415p. |
![]() Fig 46. Simple Circuits |
Simple CIRCUITS We have covered enough symbols and components to create a number of simple circuits. These circuits will show how to connect a motor, a LED, (how to make it bright or dull) and how to connect 4 cells to make a battery. Note: The flashing LED does not need a resistor because a resistor and chip are inside the LED, to make it flash and control the current. Connect all the components around the correct way and then connect them around the wrong way to see what happens. Connect the flashing LED in series with a red LED and see what happens.
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QUESTIONS 1. Explain why the Flashing LED circuit has no external resistor. 2. How many 1.5v cells are needed to produce a 6v battery 3. Explain what happens when you reverse the leads to a motor. 4. Identify the positive terminal: ![]() 5. Can 3 green LEDs be connected in series to a 6v supply? 6. A variable resistor is also called: ___________________ 7. The combined resistance of two 1k resistors in series is: _____________ 8. The combined resistance of two 1k resistors in parallel is: _____________ 9. Name the short lead on a LED 10. Name the type of multimeter with a pointer and scale: ___________________ 11. The total capacitance of two 100u electrolytics in series is: ____________ 12. The total capacitance of two 100u electrolytics in parallel is: ____________ 13. Write these values in words: 22R _________ 4k7 _________ 1n ___________ 100u ___________ 14. How many 1.5v cells in a 9v battery? 15. The red probe is: _______________ (positive/negative) 16. Conventional current flows from: _________ (positive to negative / negative to positive) 17. Make a 470u electrolytic with two electrolytics: 18. What is the voltage drop across a diode? 19. Name the component that only allows current to flow in one direction: ____________ 20. Name this symbol: ![]() 21. When resistors are connected in series, the resistance of the combination: _________ (increases / decreases) 22. When two capacitors are connected in parallel, the voltage-rating of the combination: _______________ (increases / equal to the capacitor with the lowest voltage-rating) 23. Draw two 2k2 resistors in parallel. 24. Which is larger: 470R or 22k 25. What is the value of this combination: ![]() 26. What is the name of the resistor in series with a LED: ____________________ 27. What is the voltage across the amplifier: _________ ![]() 28. Identify the fault with these circuits: ![]()
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![]() Fig 47. Passive Components |
Passive Components All the components shown on the left are called PASSIVE COMPONENTS. This means they do not amplify. Write the name beside each symbol. |
![]() Fig 47a. The Potentiometer in action |
The
Potentiometer is a variable resistor. It consists of a curved carbon track with a wiper that touches the track and can be turned via a screwdriver or knob. The wiper is the middle wire on the circuit symbol and it moves up and down as shown in the animation. When the three leads are connected the symbol is called a potentiometer. When two leads are connected it is a variable resistor. When the resistance increases, less current flows through the pot. |
![]() Fig 47b. The Variable Resistor and Potentiometer |
There is a difference in
operation between a Variable Resistor and a
Potentiometer. Both will increase or decrease the sound level as a volume control or the speed of a motor or the brightness of a globe, but a Potentiometer will guarantee zero volume or zero brightness when the pot is turned fully anticlockwise (as shown in the animation). This is because the output will be zero volts, but the variable resistor may still deliver some "energy" (voltage and current) to the circuit when turned fully anticlockwise. |
Potentiometers come in values from 100 ohms to 5 Meg ohms
(500R, 1k, 2k, 5k, 10k, 50k, 100k, 200k, 250k, 500k, 1M are most
popular). They come as linear, or logarithmic where the resistance of the track (per mm) is higher at one end. Because our hearing is not linear, these pots can be used as volume controls to produce a gradual (very nearly linear) increase in volume. Selecting the correct value of resistance for a circuit is VERY complex. If the value is not correct, the volume will not be loud or it will drop to zero before the pot is turned fully anticlockwise. Or the motor will drop to zero at mid-turn of the pot or it will not reduce in RPM to the desired amount. The simple answer is to copy a circuit. Or you can try the whole range of pots and you will find one value is the best. A Potentiometer can be used in hundreds of different circuits to produce hundreds of different effects, but the actual "thing" that flows between the input and output is a percentage of the voltage. At the same time the current will also be passed to the output at a reduced value. A pot actually delivers BOTH reduced values at the same time and the receiving circuit will be designed to "look for" the change in voltage or current. If the supply voltage is not rising or falling, the "values" are called DC values. The voltage can also be in the form of a signal (volume). This is called an AC signal. |
![]() Fig 48. The TRANSISTOR (these diagrams show that NPN and PNP transistors look the same and can have the same collector, base and emitter leads but the transistor must be connected in different ways for it to amplify because NPN is a "mirror" of a PNP transistor) |
The TRANSISTOR A TRANSISTOR is an ACTIVE device. It AMPLIFIES. There are many types of transistor (over 20,000 different types) from hundreds of manufacturers and they have many different names. We are going to study the simplest. It has the technical name BIPOLAR JUNCTION TRANSISTOR (BJT) but we are going to call it a TRANSISTOR. There are two types in this group: PNP and NPN. The type we will study is also called a SMALL-SIGNAL TRANSISTOR. You cannot tell an NPN transistor from PNP by looking at it. You must test it in a circuit. In Fig 65 you will make a Transistor Tester project, but first some basic facts: |
![]() Fig 49. The NPN TRANSISTOR in a Circuit |
The first type of
transistor we are going to study is the NPN. A transistor has three leads: BASE, COLLECTOR and EMITTER Basically, a small current enters the base and a large current flows through the collector-emitter leads as shown in the diagram. The resistor in the collector lead is called the LOAD Resistor. Sometimes the load is a speaker. |
![]() Fig 50. The Water TRANSISTOR |
The transistor is similar
to the diagram opposite. A small drop of water entering the base
is amplified to produce a loud DRIP from the speaker.
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In this experiment we will construct a ONE TRANSISTOR circuit similar to the WATER TRANSISTOR above and observe the results. Make sure the two leads DO NOT TOUCH. If they touch, the transistor will be DESTROYED. The transistor is amplifying the current through your finger via the two leads and it will be very dim. ANIMATION The lower diagram shows the transistor turning ON when a finger is pressed against the two wires. The finger produces a resistance that turns the transistor ON and this turns the transistor into a smaller and smaller resistor. That's how more and more current flows through the LED and it gets brighter and brighter. |
![]() ![]() Fig 52. Two Transistor Circuit |
By adding
another transistor we amplify the current through the finger
about 200 times and now the LED will glow bright. Make sure the bare wires do not touch each other as this will destroy BOTH transistors.
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![]() ![]() Fig 53. Three Transistors |
This circuit
has enormous gain. Each transistor has a gain or more than 200 and the final gain will be more than: 200 x 200 x 200 = 8,000,000 8 MILLION! The circuit is very sensitive to static voltages in the air or electrical waves such as the waveform produced by the electrical wiring in a house. Move the project around a room and detect all the electrical signals. |
You can see the effect of one
transistor. It does not do much. The two transistor circuit allows the resistance of your finger to deliver current into the base of the first transistor and this transistor delivers more current into the base of the second transistor. The result is more collector-emitter current and the LED illuminates. The three transistor circuit produce an ENORMOUS effect. It will pick up STATIC ELECTRICITY and all forms of electro-magnetic energy (radiation) and illuminate the LED. |
![]() Fig 54. Adding a PIEZO |
By adding a piezo
diaphragm to the
output you will be able to hear the hum of the mains. This is the frequency of the supply into your house. It will be either 50 cycles per second or 60 cycles per second. The term: "cycles per second" is given the name HERTZ after Heinrich Rudolf Hertz, who was the first to prove the existence of electromagnetic waves. |
![]() Fig 55. The Piezo |
The Piezo diaphragm
is held around the outer edge inside a plastic case and when a
voltage is applied to the two leads, the thin plate curves very
slightly. When the voltage is removed, the plate returns to its flat shape. If the voltage is reversed, the plate curves in the opposite direction. The curving is due to a thin layer of ceramic material under the plate and then a film of metal is deposited onto the ceramic so a lead can be soldered. There is infinite resistance between the two leads as the ceramic material is an INSULATOR. The capacitance between the two leads is approx 22n. The Piezo is a passive device. It needs a pulse or frequency for it to produce an output.
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![]() Fig 56. Plant Needs Water |
The ONE
TRANSISTOR CIRCUIT above can be turned into a detector to show when a plant
needs water. Place the two probes into the soil and water the plant. The LED will turn off. As the water evaporates the LED will turn ON to let you know the plant needs watering. |
![]() Fig 57. Tap the Piezo |
This experiment
produces a pulse from the piezo when it is tapped and the LED
illuminates briefly. The LED can be connected either way around. This proves the diaphragm flexes when a voltage is applied and also in the reverse situation. A voltage is produces when the diaphragm is tapped. |
![]() Fig 58. Flashing LED and White LED |
A flashing LED is
not very bright. It can be connected to a transistor and the transistor will drive a very bright white LED. The transistor is an amplifier. It is amplifying the current flowing through the flashing LED and supplying a higher current for the white LED. We cannot discuss any further
details of the circuit at the moment because the actual
operation of the circuit is quite complex. |
![]() Fig 59. Soldering Iron We now come to the point of HELPING YOU WITH CONSTRUCTION. We have already shown you 6 different circuits and there are many ways to build them. You can: 1. Solder them. 2. Build them on an Experimenter Board 3. Connect the components with clips or twist the leads together. It does not matter how you build the circuits. The fact is this: YOU MUST START BUILDING. The best soldering iron for a beginner is a CONSTANT TEMPERATURE soldering iron. It has a dial that can be turned to set the desired temperature. An ordinary soldering iron GETS TOO HOT. It is not suitable for soldering electronic circuits. This is something that no-one has mentioned before. An ordinary soldering iron will melt the solder TOO QUICKLY and burn the resin inside the solder and make soldering very difficult for a beginner. Soldering must be done slowly so the resin in the middle of the solder gets hot and cleans the leads of the components so the solder will "stick." That's why you must apply the solder to the leads you are soldering and allow the resin to "attack" the leads and clean them. The cheapest TEMPERATURE CONTROLLED soldering Iron is available on eBay for les than $10.00 (post FREE). You will also need a small roll of solder (0.9mm) and a soldering Iron stand. Email Colin Mitchell for links to eBay. (talking@tpg.com.au) A whole book could be written on the ART OF SOLDERING. Look on the web for articles and videos on SOLDERING. |
SOLDERING 1. Soldering is very easy and very simple. You just need a Temperature Controlled Soldering Iron, Fine solder and clean components. 2. Remember this: It is NOT the solder you need for a joint, but the FLUX. And the flux lasts for only 2 seconds. When the flux is HOT it attacks and cleans the joint so that the solder will stick. 3. Turn ON the Temperature Controlled Soldering Iron to a low temperature. Put solder on the tip. It will not melt. Turn up the temperature slightly. Try more solder. As soon as the solder starts to melt, this is your starting point. Turn up the temperature slightly MORE and this is the correct temperature for small, delicate, fine soldering. 4. Place a component through a hole and bend the lead slightly so the component does not move. Turn the board over and touch the iron on the component and bring the solder FROM THE OTHER SIDE so the solder melts and flows towards the iron. From start-to-finish, count one-two-three and remove the solder. Count four-five and remove the iron. You will have a perfect joint. If you are soldering thick leads or large pads on a circuit board, you will need to turn the temperature UP slightly. You must add enough solder to make the joint "bulge" slightly. Fine solder (1mm or 0.9mm or 0.8mm) makes the best joint because it is easier to use. Use a wet sponge to clean the tip or a ball of "Steel Wool." Steel wool is the best. Here is the steel wool, bending the leads and some examples of poor joints due to insufficient solder:
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![]() ![]() Photo shows a number of components fitted to the breadboard. ![]() Fig 60. BREADBOARD and Components |
BREADBOARD The term BREADBOARD refers to any piece of wood or plastic containing pins or pegs or clips or holes where you can build a circuit. The components can be soldered, twisted clipped or fitted into holes. Breadboard also means the circuit can be easily pulled apart. Some breadboards do not have two rows for the positive and negative rails. Connections under the board for the positive rail is shown with a black line in the photo. Connections on the main section of the board are shown with blue lines. Your breadboard MUST look exactly like the photo opposite. Other breadboards are quite useless. The breadboard in the photo can be purchased on eBay for less than $5.00 (post FREE). |
![]() Fig 61. Jumpers |
The components on
the BREADBOARD are fitted down
the holes and metal strips under the board join each column of 5
holes. If you want to join one hole with another, you can use
0.5mm tinned copper wire or JUMPERS. See photo opposite.
Jumpers can be purchased on eBay for less than $3.00 posted.
Email Colin Mitchell for links to eBay. (talking@tpg.com.au) |
![]() Fig 62. Breadboard with Nails If you don't have a soldering iron or experimental breadboard, you can make your own board with nails. See the photo above. It is a multivibrator circuit and we will be presenting this circuit in a moment. The components can be twisted around the nails and bare wire used to join some of the nails to complete the circuit. Another method of connecting the components is called BIRD-NESTING. This involves soldering the components "in the air" as shown in the 27MHz transmitter circuit below: ![]() Another way to connect the component( if you don't have a soldering iron), is to wind 6 turns of bare wire around each connection and leaving all the components "in the air." The bare wire can be obtained from hook-up flex. This is plastic coated "wire" containing up to 15 fine strands of wire. Use a single strand for the connections. None of the components will touch each other BY MISTAKE and the circuit will work perfectly. Bird-nesting is a good way to build a quick circuit and test its performance. It might look messy but you can easily change any component. |
![]() Fig 63. Wiring the 3-Transistor Circuit using BC547 Transistors The diagram shows how to connect 3 x BC 547 transistors. The leads of a transistor can be collector-base-emitter OR emitter-base-collector and that's why we have provided 2 different wiring diagrams. |
![]() Fig 64. Wiring the 3-Transistor Circuit using 2N2222 Transistors The diagram shows how to connect 3 x 2N2222 transistors. |
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Fig 65. Transistor Tester |
![]() ![]()
Fig 66.
ROBOT MAN |
ROBOT MAN This multivibrator circuit will flash the Robot Man's eyes as shown in the photo. The kit of components is available from Talking Electronics for $8.50 plus postage. Send an email to find out the cost of postage: talking@tpg.com.au The photo shows the LEDs flashing. The circuit is called an ASTABLE MULTIVIBRATOR and this means it is not stable but keeps switching from one transistor to the other. It is also called a FLIP FLOP circuit. |
![]() Fig 67. The TIME DELAY |
The
TIME DELAY circuit consists of a Resistor
R and Capacitor C
in SERIES. When the switch is closed, the electrolytic (called the CAPACITOR) charges slowly because the resistor only allows a small amount of current to flow. It's just like charging your mobile phone. The battery takes time to charge because there is a resistor in the circuit to limit the current. If we remove the resistor in the mobile phone, the battery will get too hot when it is being charged but in the TIME DELAY circuit, we want the capacitor to charge slowly, because we want a TIME DELAY. . |
![]() Fig 68. The charging of a capacitor is the same as building a brick wall. |
CHARGING A CAPACITOR The capacitor in Fig 67 charges via the resistor R. But the voltage on the capacitor does not rise at a constant rate. It starts off charging very quickly and as the voltage across it get higher, the voltage increases at a slower and slower rate. In the photo I am building a brick wall. I am working at a constant rate. When I started building the brick wall, I laid 5 rows of bricks (5 courses) in the first hour. As the wall increased in height, I had to climb the ladder and I could only lay 3 courses an hour and finally the wall was so high I could only lay 1 course per hour. This is exactly the same as a capacitor charging. When the capacitor is uncharged, the supply voltage allows a high current to pass through the resistor R and the energy quickly fills the capacitor. This results in a rapidly increasing voltage on the capacitor. But as the voltage on the capacitor increases, the difference in voltage between that on the capacitor and the supply is very small and only a small current will pass through the resistor. This means the voltage on the capacitor increases at a slower rate. |
![]() Fig 69. Time Units |
It really does not matter how
fast or slow or uneven a capacitor charges because most circuits
detect a voltage on a capacitor and the time taken to reach this
voltage is called the TIME DELAY. But to prevent you thinking the capacitor charges "smoothly" we have to explain what actually happens. The graph on the left shows the capacitor charging. You can see it charges quickly at the beginning and then charges slowly and then very slowly. You can see the first part of the graph is fairly "straight" (constant charging) - NOT "straight up and down" but a straight line - and this applies to a voltage of about 63%. The time taken to reach this voltage is called ONE TIME UNIT - also called ONE TIME CONSTANT. The graph continues for another 4 "time units" (time-constants) and the final voltage is very nearly 100%. (It never reaches 100%.) |
![]() Fig 70. Time Delay Circuit |
A
TIME DELAY
circuit needs three things: 1. A Resistor (R) 2. A Capacitor (C) 3. A "Detection Point." When the switch is pressed, capacitor (C) takes time to charge via resistor (R) and after a short period of time the voltage at the DETECTION POINT is 0.6v and the transistor is TURNED ON. The LED illuminates. Build the circuit with 100u and 100k and see how long it takes before the LED illuminates. |
![]() Fig 71. The "TIME DELAY" in the ROBOT MAN Project |
In the ROBOT MAN
project you can see the "TIME DELAY" circuit made up of the
100u, 10k resistor and the base of the transistor. This is one of the most important BUILDING BLOCKS in electronics. It is the basis of all oscillators and will be discussed below, after we explain a few more details. |
![]() Fig 72. Turning A Transistor ON |
We will use the
TIME DELAY circuit to turn the transistor ON.
Make sure the 100u is uncharged by touching both leads (both ends of the capacitor) at the same time with a JUMPER - this is a piece of wire shown in Fig 61. Push the switch and noting happens. After a short period of time the LED starts to glow and then comes on fully. This shows two things: 1. The transistor is not turned ON when the base voltage is zero. 2. The base voltage must be 0.6v for the transistor to start to turn ON and when the voltage is 0.65v the transistor is turned ON FULLY. |
![]() Fig 73. How the LED turns ON |
Here is an explanation of how the LED turns
ON. When the circuit is first assembled and the switch is not pressed, the transistor is not turned on and it is just like the diagram opposite. The LED is not connected to the transistor. |
![]() Fig 74. The LED turned ON |
When the switch is pushed, the transistor turns ON (after a few seconds) and it pulls the lower lead of the LED down towards the 0v rail and this action turns the LED ON. |
![]() Fig 75. The LED fully turned ON |
When the LED is fully turned ON, the lower lead of the LED is almost directly connected to the 0v rail. In other words: When the transistor is FULLY TURNED ON, the lower lead of the LED is almost directly connected to the 0v rail. The voltage between the lead of the LED and 0v rail is 0.2v. This is the characteristic voltage across the collector-emitter terminals of a transistor when it is TURNED ON. |
In the
three diagrams above you can see the
LED is changed from an OFF condition to an ON
condition by the action of the transistor. The transistor is acting LIKE A SWITCH. This action is one of the most important actions in electronics. It is called: "The Transistor as a SWITCH" It is the basis to ALL Digital Circuits. It is the basis because of these two facts: 1. When the transistor is OFF, the circuit is taking no current and no power is being lost or wasted. 2. When the transistor is ON, the LED is almost at 0v and no resistor is in the lower lead to waste any power. Thus we can turn things ON and OFF without wasting and power. This is the basis to DIGITAL ELECTRONICS. |
DIGITAL ELECTRONICS
revolves around circuits that are either FULLY
ON or FULLY OFF. This means they take almost no power
and we can combines lots of circuits and still take almost no
power. This means they do not get hot and it also means they will last a long time. You may not think turning a transistor ON and OFF will achieve any worthwhile outcome but a circuit can be designed to use two transistors (similar to the ROBOT MAN above). The circuit does not Flip-Flop but requires a switch and when the switch is pressed, the circuit changes state. The two transistors are connected together and it takes two presses of the switch to make the output of the second transistor change state ONCE. The circuit is a divider. It is called a: divide-by-two and is the basis of all counting in a computer. By adding more "divide-by-two" circuits we can get "divide by 4, divide by 8" etc. Two transistors don't do much but when you combine millions of transistors we have a COMPUTER. |
![]() Fig 76. The "MEMORY CELL" When Switch A is pressed, the voltage on the base is removed and transistor A turns OFF. Transistor B turns ON via resistors R1 and R2 and the LED is turned ON. When the switch is released, the voltage on the collector of transistor B is less than 0.6v and the two transistors remain in this state. Pressing switch B turns the LED OFF. (transistor A turns ON via R3, R4 and the LED - very little current flows through the LED and you can hardly see it glowing). The voltage on the collector of transistor A is less than 0.6v and the two transistors remain in this state. |
Two transistors can
do one more thing. They can "REMEMBER." Here is a manual circuit. Pressing Switch A turns the LED ON and pressing switch B turns the LED OFF. The circuit "remembers" or remains in each state called a stable state. The technical name for this circuit is: BISTABLE MULTIVIBRATOR or BISTABLE SWITCH or BISTABLE LATCH. This is the basis to all the memory in a computer. |
In electronics, we talk
about the DIGITAL TRANSISTOR and ANALOGUE TRANSISTOR.
This is just an ordinary transistor (called a Bipolar Junction Transistor) in a DIGITAL CIRCUIT or ANALOGUE CIRCUIT. We are now discussing the DIGITAL CIRCUIT - The Multivibrator - Astable Multivibrator and Bistable Multivibrator (Memory Circuit). The DIGITAL CIRCUIT has 2 STATES. The ON STATE and the OFF STATE. It is conducting in the ON STATE and the LED is illuminated. In the OFF STATE, the LED is not illuminated. In the ON STATE the transistor is said to be CONDUCTING or BOTTOMED. In the OFF STATE the transistor is said to be "CUT OFF or "OFF." These two states are reliable and guaranteed. They are not "half on" or "quarter on" or "75% off." These states are easy to transmit "down a wire." The ON STATE is transmitted as "1" (voltage present) and the OFF STATE is transmitted as "0" (voltage not present). These are the two DIGITAL STATES. ![]() The ROBOT MAN is a DIGITAL CIRCUIT. Each LED is ON or OFF. The waveform on the output of each transistor is called a DIGITAL SIGNAL. The waveform is said to be DIGITAL or SQUARE WAVE. The top line of the graph represents the LED OFF. The bottom line of the graph represents the LED ON. The LED is ON when the collector voltage is LOW because we are pulling the lead of the LED to the 0v rail as shown above. The circuit changes from one state to the other very quickly and this is called the RISE TIME. |
![]() Fig 77. The two Digital States |
Going over the two
DIGITAL STATES for a transistor. In the first diagram the switch is not pressed and the base does not see a voltage to turn the transistor on. The transistor is "OFF" (not conducting) and it is not "grabbing" the LED. The LED is not illuminated. In the second diagram the base of the transistor sees a voltage via the switch and it is TURNED on. The LED is illuminated. |
![]() Fig 78. ROBOT MAN Animation This animation shows how a transistor grabs a LED and pulls it towards the 0v rail to turn it ON. |
![]() Fig 79. TIME DELAY Animation The animation in Fig 78 shows the two transistors turning the LEDs ON and OFF in a FLIP FLOP circuit. We know the 10k and 100u components form a TIME DELAY to create the time for each LED to be illuminated. The timing for one LED plus the other LED creates a CYCLE and this is the FREQUENCY OF OPERATION for the circuit. It is measured in cycles per second - Hertz - Hz. We will now go into more detail of how the TIMING COMPONENTS create the TIME DELAY for each LED. The circuit is more-complex than you think. The 100u is already charged from a previous cycle and we show how it gets discharged via the 10k and charged in the opposite direction by the 10k to create a TIME DELAY. |
THE CAPACITOR![]() In this circuit the capacitors on the input and output prevent DC on the volume control creating "scratchy sounds" when the volume is altered. This is called "DC blocking." The AC (the signal) passes through the capacitors but the DC voltage on the input is blocked. |
CHARGING A
CAPACITOR
Part II It is easy to see how a capacitor charges via a resistor in the TIMING CIRCUIT (Delay Circuit) above but many capacitors are not connected to the 0v rail. They are connected as show in the animation below and their "job" is to pass a waveform. When they pass the waveform they CHARGE and DISCHARGE. The waveform is called an AC SIGNAL and the output is smaller than the input. The circuit is taken from the circuit above, but the same effect applies to all capacitors that "pass a signal." Here's why: ![]() The capacitor charges slightly during the rise of the signal and the right-plate of the capacitor does not rise as high as the left-plate. That's why the output signal is not as large as the input signal. If the capacitor did not charge, the output would be as large as the input. If you use a capacitor with a large value, it will not charge and thus the output will be as large as the input. That's why you use a large capacitor !!!! |
CHARGING A
CAPACITOR
Part III Here is another CAPACITOR in action. ![]()
This animation shows three features: |
NEGATIVE VOLTAGE You will be surprised to learn that many circuits produce a negative voltage or negative spike at some point (when doing circuit-analysis, each location or point or join of components is called a NODE) on the circuit. In other words the voltage will be LESS than the 0v rail of the circuit. This is due to the presence of a capacitor and the animation shows how a capacitor can produce a negative voltage:
When a charged capacitor is "lowered from one position
in a circuit" the positive lead may be lowered by say 3v. This means the
other lead will be lowered by 3v. We are assuming the capacitor can be
lowered and is not directly connected to the 0v rail.
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The Electret Microphone The most common type of microphone is the ELECTRET MICROPHONE. It is incorrectly termed the "Capacitor Microphone" or Condenser Microphone." "Capacitor Microphone" descriptions make no mention of a FET as the amplifying device and a polarized diaphragm to detect the audio, so they are something different. The electret microphone consists of a FET (transistor) inside an aluminium case with a very thin Mylar film at the front. This is charged and when it moves (due to the audio it receives via a small hole in the front of the case), it vibrates and sends a very small voltage to the GATE lead of the Field Effect Transistor. This transistor amplifies the signal and produces a waveform of about 2mV to 20mV at the output. The electret microphone requires about 0.5mA and will operate from 1.5v supply with 4k7 LOAD RESISTOR. For 3v supply, the Load Resistor can be 22k to 47k. For higher supply voltages the resistor will be 68k or higher. Electret microphones are extremely sensitive and will detect a pin-drop at 3 metres. ![]() Most electret microphones have two leads. One lead is connected to the case and this lead goes to the 0v rail. The other lead goes to a LOAD RESISTOR (4k7 to 68k - depending on the voltage of the project). Reducing the value of the load resistor will increase the sensitivity until the background noise is very noticeable. They are used in Hearing Aids and are more-sensitive than the human ear. They are very small, low-cost and very sensitive. |
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The Speaker The most common speaker is about 30mm to 60mm diameter and 8 ohm impedance. This means the voice coil is about 8 ohms resistance. The two leads can be connected either way to a circuit. The speaker shown is 32mm diameter and has a realistic wattage of 100mW (NOT 1watt). These speakers have a Mylar cone and the magnet is a "super magnet" and very small. That's why it is so flat. ![]() A speaker can be used as a microphone (called a Dynamic Microphone) and a circuit to connect the speaker (mic) to an amplifier can be found on Talking Electronics website. It is not as sensitive as an electret microphone and does not Speaker Symbol produce the same output amplitude, but it is an emergency microphone. |
![]() LDR and Light Alarm Circuit |
Light Dependent Resistor (LDR) Also called PHOTOCELL or PHOTO RESISTOR A Light Dependent Resistor is a 2-leaded component containing a layer of semiconductor material. The top contains two interleaving combs of conducting wires with a path of semiconductor material between. When light falls on the component, the resistance of the semiconductor material decreases. In darkness the LDR will be about 300k. In very bright light the resistance will be about 200 ohms. But if the light changes only a very small amount, the resistance CHANGE is VERY SMALL. For a large change, see Photo Transistor. The Light Alarm circuit will produce a squeal when light falls on the LDR. |
![]() The FPT-100 Darlington Photo Transistor is available from Talking Electronics for $1.00 each plus postage. |
Photo Transistor The Photo Transistor is very sensitive to changes in illumination. It is about 100 times more sensitive than the LDR. The Photo Transistor is also available as a DARLINGTON. The Darlington Photo-transistor is 100 x 100 times (10,000) more sensitive than the LDR. The Photo Transistor and Photo Darlington Transistor are connected just like a normal transistor but the base lead is not connected. If the value of the LOAD RESISTOR is large, the transistor will not be very sensitive. ![]() |
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The Inductor Also called "coil," or "Choke." An Inductor consists of one to many turns of wire wrapped around a former (tube of cardboard). The wire can be jumble-wound or wound in layers. The result is the same. This is called an air-cored coil or air-cored inductor. The centre can be filled with a metal such as iron or laminations (thin sheets of metal) or a ferrite material. Different cores operate at higher frequencies. The core can be circular (doughnut) or rectangular and it is called a MAGNETIC CIRCUIT (when it is a closed loop). Additional turns or increasing the diameter of the turns will increase the inductance. A coil with a magnetic core can be used to pick up nails and metal items. It is called an electromagnet. It can be operated on AC or DC. When the metal core is loose and gets pulled into the coil it is called a SOLENOID or ACTUATOR or LINEAR ACTUATOR. It can be operated on AC or DC. The way an inductor works is very complex but we can say it resists any rise or fall in voltage by turning the rise or fall into magnetic flux. If the applied voltage is suddenly turned off, the inductor produces a very high voltage of opposite polarity (these are the two most important things for you to remember). |
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The Antenna The first time you will need an antenna is when making an FM transmitter. The antenna is usually a length of wire equal to half the wavelength of the transmitter. The frequency is about 100MHz and the wavelength is 3 metres. A half-wave antenna is 1.5metres. The length is important but the height is more important. The wire should be as high as possible and "up-and-down" if the antenna on the radio is vertical, to get the maximum range. This is called an end-fed half-wave antenna or half-wave Monopole. The transmitting circuit should have a good ground-plane such as connection to large batteries so the signal can be pushed and pulled into and out of the antenna. This signal is then radiated as electromagnetic radiation to the surroundings. |
![]() A single contact consists of 2 pins -called SPST (single-pole single-throw). Or a single pair of contacts can consist of 3 pins - called change-over or SPDT (single-pole double-throw). A double set of contacts consists of 6 pins, called DPDT (double-pole, double-throw). This is also called a CHANGE-OVER RELAY or REVERSING RELAY (when connected to a motor). |
The
RELAY The word Relay comes from the days of Morse Code where a coil of wire (an electromagnet) closed a switch to allow the Morse code to travel further down the telegraph line. It would "relay" or "pass-on" the information. A relay allows a "weak circuit" (one with low current) to operate a LOAD that needs a large current. It also separates the two circuits electrically and prevents a voltage such as 240v connecting to a 12v circuit. The coil is separated from the contacts and this gives the two circuits isolation. A double-pole double-throw relay can be used to reverse a motor as shown here: ![]() |
![]() The armature is drawn towards the coil when a current flows through the coil. |
Driving A
Relay (Powering A Relay) The first thing you must decide is the voltage of the relay. This will depend on the voltage(s) available. The relay will be driven (activated) by a transistor and the base of the transistor only needs a signal (less than about 1v). This means the project can be operated on a voltage from 3v to 12v and the relay can be connected to a 5v to 12v supply. Next you need to know the current-rating of the contacts. This will depend on the current taken by the LOAD. The rating of most relays is: 1 amp, 5 amp or 10 amp. Finally you need to know how many contacts are required. For a single circuit you will need 2 pins and for two circuits you will need 4 pins (but relays only come with 6 pins). You can get relays that need a very small current for activation. These are called CMOS relays. But most relays need about 100mA. To protect the driving-transistor from spikes when the relay is turned off, you will need a diode across the coil. The top animation shows a "single set of change-over contacts." The lower animation shows the ARMATURE being drawn to the electromagnet. The electromagnet is the coil with a core of magnetic material that becomes a magnet (an electromagnet) when a current flows through the coil. |
![]() ![]() When the circuit is turned ON, the voltage across the 2,200u electrolytic is zero and it gradually charges. When the voltage is about 8v, the coil has enough voltage across it to pull the armature and open the contacts. The electrolytic supplies voltage to the coil for about 1 second and then the electromagnet does not have sufficient magnetism to hold the armature and it returns to close the contacts. |
GATES
Animations of GATES and more details of their operation is covered in DIGITAL ELECTRONICS chapter. |
![]() Fig 80. The "AND" GATE and "OR" GATE with switches |
The next BUILDING BLOCK
we will cover is called the GATE. In its simplest form it is an electrical circuit consisting of switches. Its just two or more switches connected in series or parallel. We give each circuit a name so we can talk about it and explain its action with a single word. Later we will cover the electronic version and show how diodes and a transistor are needed to perform a GATING FUNCTION. The type of GATE we are talking about is a LOGIC GATE. The circuit performs an operation called a LOGICAL OPERATION on an input or a number of inputs and creates a single output - called a LOGICAL OUTPUT. LOGICAL means "understandable" or "correct" and in this case it means DIGITAL - the signal will rise to full rail voltage or fall to zero voltage. The output will not be half rail or quarter-rail voltage. The diagram show an "AND" GATE and "OR" GATE with switches. For the AND GATE close switch A AND switch B for the lamp to illuminate. For the OR GATE close switch A OR switch B for the lamp to illuminate. |
![]() Fig 81. The "NAND" GATE and "NOR" GATE with switches and a transistor |
INVERSION Inversion produces the opposite effect to the results above. Suppose we want to turn OFF a lamp when one or two switches are pressed. We need a transistor. The technical word for Inversion is NOT. It is simplified to the letter "N." For the NAND GATE close switch A PLUS switch B for the lamp to turn OFF. For the NOR GATE close switch A OR switch B for the lamp to turn OFF. These gates are only demonstration-gates to show how one or two switches will turn a lamp OFF. |
![]() Fig 82. The "NOT" GATE |
NOT GATE A single switch and transistor produces a NOT GATE. This is simply an INVERSION. The resistor turns the transistor ON and the lamp illuminates. The switch removes the voltage on the base and the transistor turns OFF. This is only a demonstration circuit to show how a switch can turn a lamp OFF. |
The 5 gates above form the basis to turning a circuit ON and OFF. We will discuss these gates later in the digital section. |
![]() Fig 83. "AND and "OR" gate with diodes |
The next building
block is the GATING DIODE. We have shown a diode allows current to flow when the diode is correctly placed in a circuit and blocks current when it is reversed. The 5 gates above are electrical circuits but an electronic circuit works in a slightly different way. The electronic circuit will be covered later in the DIGITAL section. For the moment we will explain how a diode can be used to create a GATE. In other words it creates a ONE-WAY PATH to allows signals to pass from one stage to another and prevents signals passing in the opposite direction. In the AND GATE circuit, both inputs are LOW and current flows through the resistor (it will get HOT). When one input is taken HIGH, current still flows through the other diode and the lamp does not illuminate. When BOTH inputs are HIGH, current flows through the resistor to illuminate the lamp. No current flows through the diodes. In the OR GATE, when one input is taken HIGH, current flows through the diode to illuminate the lamp. This can be done with EITHER input. |
![]() Fig 84. "NAND" and "NOR" gate with diodes and a transistor. |
A NAND and NOR gate
can be made with diodes and a transistor. This time we the output is either HIGH or LOW. We are gradually producing circuits that are electronic, rather than electrical circuits. In the NAND GATE circuit, taking one of the inputs HIGH will still allow the other input to prevent the transistor turning ON. When BOTH inputs are HIGH, the transistor turns on via resistor R and the output is LOW. In the NOR GATE circuit, taking one of the inputs HIGH will turn the transistor ON and the output will be LOW. |
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Drawing A Circuit
A circuit must be drawn according to simple rules so it can be instantly recognised. An electronics engineer can "see a circuit working" when it is drawn correctly and can see if it is drawn correctly; if the parts-values are correct and can use the circuit to assist in diagnosing a problem with a faulty circuit. The top circuit on is very difficult to visualise because it is not drawn in the normal way. All the components have to be "turned around in your mind," to see what the circuit is doing. |
QUICK QUIZ - to see
how much you know
Answer the following 50 questions .
. . JavaScript is required!
Light Emitting Display
Collector Bias Omitter
A high resistance circuit
4. What is the approximate characteristic voltage that develops
Higher
6. Which is not a "common" value of resistance:
2k7
7. Which value of resistance, placed across a 9v battery
22k
8. If the voltage on the base of a transistor increases, does it:
Turn on
help
47k
11. A resistor with colour bands: red-red-red-gold, has the value:
22k 5%
12. The lead marked with the arrow is:
13. A 10k resistor in parallel with 10k produces:
10k
14. The symbol is:
15. Two 3v batteries are connected as shown.
16. 4 resistors in ascending order are:
22R 270k 2k2 1M
17. The closest value for this combination is:
18. Which LED will illuminate: 19. The four symbols are:
20. The closest value of the combination is:
21. Which motor will work:
Pulse Circuit
5k5
24. Name the 4 components:
25. To obtain a higher value of resistance, resistors are 26. Which LED will
illuminate:
A
27. Name the component that detects light:
28. What is 1,000p?
0.01n
29. The current in a circuit is 45mA. This is:
0.045Amp
30. A 100n capacitor can be expressed as:
0.1u u = microfarad
31. 1mA is equal to:
0.001A
32. 1,200mV is equal to:
12v
33. The approximate current for a toy 3v motor is:
10mA
34. What is the resistance of this resistor:
47k 35. Identify the correctly connected LED:
A
36. Identify the correct statement:
37. The current requirement of a LED is:
1.7mA
38. The multimeter is measuring . . .
41. A DC voltage . . .
rises and falls
42. Arrange these in ascending order: k, R, M
R, k, M
43. A battery produces AC current:
5%, 10%
45. 223 on a capacitor represents:
0.022u u = microfarad
46. Arrange these in ascending order: n, p, u
p, u, n,
0.1u
49. What is the multimeter detecting:
Voltage
50. For the LEDs, what is the characteristic voltage for the red and white
LEDs:
3.6v, 1.7v
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