Cover Image
close this bookRadio and Electronics (DED Philippinen, 66 p.)
View the document(introduction...)
close this folder1. INTRODUCTION
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View the document1.1. A TRIAL TO STATE A DEFINITION OF ELECTRONICS
View the document1.2. A SHORT HISTORY OF ELECTRONICS
View the document1.3. CLASSIFICATION OF ELECTRONIC DEVICES
close this folder2. PRINCIPLES OF RADIO COMMUNICATION UNICATION
View the document2.1. BASICAL IDEAS ABOUT COMMUNICATION
View the document2.2. DEVELOPMENT OF LONG DISTANCE COMMUNICATION
View the document2.3. FIDELITY AND DISTORTION
close this folder3. TRANSDUCERS
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View the document3.1. MICROPHONES
View the document3.2. LOUDSPEAKERS
View the document3.3. THE TELEPHON SYSTEM
View the document3.4. PROBLEM OF FREQUENCY RANGES
View the document3.5. BANDWIDTH
close this folder4. RADIOWAVES
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View the document4.1. ORIGIN OF RADIOWAVES
View the document4.2. PARAMETERS OF ELECTROMAGNETIC WAVES
View the document4.3. PROPAGATION OF RADIOWAVES
View the document4.4. SPECTRUM OF RADIOWAVES AND BANDS OF RADIOWAVES
close this folder5. MODULATION OF RADIOWAVES
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View the document5.1. THE AMPLITUDE MODULATION (AM)
View the document5.2. FREQUENCY MODULATION (FM)
View the document5.3. SIDEBANDS
View the document5.4. TRANSMISSION OF RADIOSIGNALS
close this folder6. RECEPTION OF RADIOSIGNALS (AM - TYPE)
View the document6.1. AERIAL
View the document6.2. THE TUNED CIRCUIT
View the document6.3. INCIDENTAL REMARK ON BLOCK DIAGRAMS
View the document6.4. DETECTOR OR DEMODULATOR
View the document6.5. POWER SUPPLY
View the document6.6. AMPLIFIER
View the document6.7. SUPERHET RECEIVER (the SUPER)
View the document6.8 INCIDENTAL REMARK ON MIXING FREQUENCIES
View the document6.9. CONSTRUCTION OF A SUPERHETRADIO
close this folder7. COMPONENTS OF MODERN RADIO RECEIVERS
View the document7.1.1. HANDLING OF ELECTRONIC COMPONENTS
View the document7.1.2. HANDLING OF PRINTED CIRCUITS
View the document7.1.3. DIFFERENTIATION OF COMPONENTS
close this folder8. PASSIVE COMPONENTS
View the document8.1. RESISTORS ELECTRICAL CHARACTERISTICS
View the document8.2. CAPACITORS
View the document8.3. INDUCTORS
close this folder8.4. COMBINATION OF PASSIVE COMPONENTS
View the document8.4.1. SERIES CONNECTION OF R AND C, OR R AND L
View the document8.4.2. COMBINATION OF L AND C, RESONANT (TUNED) CIRCUITS
close this folder8.4.3. TUNED CIRCUIT CONNECTED TO AN AC-VOLTAGE
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View the document8.4.4.1. QUALITY OF TUNED CIRCUITS
View the document8.4.4.2. BANDWIDTH
close this folder9. ACTIVE COMPONENTS -1- DIODES
View the document9.1. CHARACTERISTICS OF SEMICONDUCTORS
close this folder9.2. THE PN-JUNCTION OR DIODE
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View the document9.2.1. PN-JUNCTION CONNECTED TO VOLTAGE
View the document9.2.2. CHARACTERISTICS OF A PN-JUNCTION OR DIODE
View the document9.2.3. ZENERDIODE
close this folder10. BLOCKS OF RADIOS / -1- / POWER SUPPLIES
View the document10.1. GENERAL CONSIDERATIONS
View the document10.2. TRANSFORMER
View the document10.3. THE RECTIFIERS.
close this folder10.4. SMOOTHING AND FILTER CIRCUITS
View the document10.4.1. THE RESERVOIR CAPACITOR
View the document10.4.2. FILTER CIRCUITS
close this folder10.5. STABILIZATION
close this folder10.5.1. GENERAL REMARKS
View the document10.5.1.1. LOAD VARIATIONS
View the document10.5.1.2. INTERNAL RESISTANCE OF VOLTAGESOURCES
View the document10.5.1.3. PROBLEMS CAUSED BY THE SMOOTHING CIRCUIT
close this folder10.5.5. METHODS OF STABILIZATION
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View the document10.5.5.1. PARALLEL-STABILIZATION
View the document10.5.2.2. SERIES STABILIZATION
close this folder11. ACTIVE COMPONENTS -2- / TRANSISTORS
View the document11.1. CONSTRUCTION OF A TRANSISTOR
close this folder11.2. CHARACTERISTICS OF TRANSISTORS
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close this folder11.2.1 HANDLING OF CHARACTERISTICS OF TRANSISTORS
View the document11.2.1.1. CONSTRUCTION OF THE STATIC-MUTUAL-CHARACTERISTICS
View the document11.2.1.2. CONSTRUCTION OF THE DYNAMIC MUTUAL CHARACTERISTICS
View the document11.2.1.3. CONSTRUCTION OF THE MAXIMUM-POWER-LINE
close this folder12. AMPLIFIERS
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View the document12.1. STRUCTURE OF A CLASS A AMPLIFIER
View the document12.2. FUNCTION OF A SIMPLE CLASS A AMPLIFIER
View the document12.3. ADVANCED CLASS A AMPLIFIER
View the document12.4. STABILIZATION OF THE QUIESCENT VOLTAGE
close this folder13. CLASS B AMPLIFIERS
View the document13.1. LIMITS OF CLASS A AMPLIFIERS
View the document13.2. CLASS B AMPLIFIERS WITH TRANSFORMERS
View the document13.3. CLASS B AMPLIFIERS WITHOUT TRANSFORMERS
View the document13.4. POWER AMPLIFIER WITH COMPLIMENTARY TRANSISTORS.
View the document14. DETECTOR OR DEMODULATOR
View the document15. AGC-AUTOMATIC GAIN CONTROL
View the document16. IF-AMPLIFIERS
View the document17. FEEDBACK
View the document18. OSCILLATORS
View the document19. FREQUENCY CHANGERS MIXERSTAGE
View the document20. DECOUPLING CIRCUITS
View the document21. MATCHING OF AMPLIFIERSTAGES
View the document22. COUPLING OF AMPLIFIERSTAGES
close this folder23. RADIO SERVICING
View the document23.1. IMPORTANCE AND SUBJECT OF FAULT FINDING
View the document23.2. FAULTS AND FAULT FINDING
View the document23.3. FAULT FINDING METHODS
View the document24. THE USE OF THE OSCILLOSCOPE

8.3. INDUCTORS

ELECTRICAL CHARACTERISTICS OF INDUCTORS

A) Inductors at dc

If we connect an inductor to a dc-voltage-source we will find: it takes some time till the current has reachted its full value. The amount of current flowing at last will be depending only on the voltage connected and the ohmic resistance (the resistance of the wire).


fig. 63

B) Inductor at ac

If we connect the same inductor to an ac-voltage of the same magnitude than the dc was, we find a much smaller current flowing.

We know, that the resistance of the copperwire will not have changed. But we know too, that in every circuit the current is governed by Ohm's Law.

So the decreased current is only possible if the ac-voltage has somehow decreased in the circuit.

We know too that in a coil in case of change of current is produced a so called BACK-EMF.

Applying this knowledge we can assume the shape of the back emf. It will be slightly smaller but exactly inverse to the original voltage. The rest of the voltage left over is necessary for the resistance of the copperwire. We know too that the amount of back emf is depending on the change of current in the coil. Applying this we can state: the current must have its fastest changes when the back emf has its maximum. So the back emf has an opposite direction the current must change positively to produce a negative back emf and vice versa. Also we can state: the current must not change anyhow while the back emf is “0”. We have got now four conditions for the shape of the current flowing in the circuit of an inductor connected to an ac-voltage. We can easily foresee, that the current will flow in the shape of a sinewave.


fig. 64

We can also predict some facts about the phase relation between voltage and current.


fig. 67

PHASE RELATION

As we concluded above at an inductor the current must be LAGGING BEHIND THE VOLTAGE. The biggest phaseshift possible is 90 degrees. But this value cannot be reached in practice.

FREQUENCY RESPONSE

As we found the back emf depends on the change of the current. If the frequency of the sinewave is higher we will find a faster change of current, and therefore there will be produced a bigger back emf.

So we can derive: as higher the frequency as lower will be the current - this means as higher the frequency as higher the impedance of the inductor.

The impedance of the inductor is to be calculated by the formula:

And the inductive reactance of the inductor can be calculated by the formula:

MAIN FUNCTIONS OF INDUCTORS

Inductors can be divided into two main groups:

A) LOW- (or audio-) FREQUENCY INDUCTORS. They are used for smoothing the dc of the supply or for letting through only audio frequency and to cut off high frequencies.


fig. 68

B) HIGH- (or radio-) FREQUENCY INDUCTORS They are used in tuned circuits and for aerial coils onferrite rods. They are small compared with those of group A and often they do not even have an ironcore.


figure

If the frequency is very high the wires are mode out of a lot of extremly thin strands in order to avoid the so called “skin effect”.

SPECIALITIES:

A) Sometimes we find in superhet receivers for cars instead of variable capacitors so called variable inductors used for the tuned circuits.

B) To cut off very high frequencies in wires entering a special part of a radio or another electronic equipment, there are used simple pearls of ferrite which are just put on the wire.

CHECKING AND HANDLING OF INDUCTORS

The possibilities to check an inductor by simple means are very limitted.

With a normal AVO-meter we can just measure the ohmic resistance across the two terminals. But we will hardly read more than 10 Ohms. Mostly we will measure values near “0” Ohms and if we find that, we can be sure that the wire is at least not broken, but we do not know

- if there is short circuited winding, or
- if there is anything wrong with the ironcore.

These kinds of faults can cause very considerable changes of the inductivity of the inductor.

If we suspect a fault like that we can only replace the inductor by one of the same type, or we have to measure the impedance of it at the frequencies it is meant for.

PLEASE KEEP IN MIND: There are always found inductors with an iron core which resembles a screw. They are meant for adjustment but....

NEVER TRY TO ADJUST THESE INDUCTORS ONLY FOR FUN AND WITHOUT MEASURING THE SIGNALS PRODUCED! YOU WILL MISALIGN THE RADIO!!

NEVER TOUCH THE IRON CORES WITH A NORMAL SCREWDRIVER. YOU MIGHT MAGNETIZE IT, AND THAN IT WILL NOT WORK PROPERLY ANYMORE.

CHECK YOURSELF

1. What are passive components

2. Compare the behaviour of a) resistors, b) capacitors, d) inductors at ac voltages with different frequencies.

3. Explain the term phaseshift and state which kind of phaseshift we find at a) resistors, b) capacitors and c) inductors.