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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

8.4.2. COMBINATION OF L AND C, RESONANT (TUNED) CIRCUITS

Combinations of inductors and capacitors have always a special characteristic referring to their RESPONSE to different frequencies. If we want to understand their behaviour we have two main possibilities:

FREE OSCILLATING CIRCUIT

Let us suppose a capacitor is charged with a certain voltage. As soon as this capacitor is connected across an inductor there starts to flow a current. The amount of current is slowly increasing because of the self-induced voltage across the coil.


figure


figure


figure

On the one hand this current is discharging the capacitor which lets drop the voltage of the capacitor. On the other hand the increasing current is building up a magnetic field around the coil. The current will reach its maximum just when the capacitor is discharged totally. At that very instant the voltage at the capacitor is Cero while the current is at its maximum, and therefore the magnetic field has its maximum too.


figure

There is no charge left at the capacitor, therefore the capacitor cannot deliver any current anymore. Combinations of inductors and capacitors have always a special characteristic referring to their RESPONSE to different frequencies. If we want to explain their behaviour we have two main possibilities:

FREE OSCILLATING CIRCUIT

Let us suppose a capacitor is charged with a certain voltage.

As soon as this capacitor is connected across an inductor there starts to flow a current. The amount of current is slowly increasing, because of the selfinduced voltage across the coil.

On the one hand this current is discharging the capacitor which lets drop the voltage of the capacitor. On the other hand the increasing current is building up a magnetic field around the coil.

The current will reach its maximum just when the capacitor is discharged totallyted across an inductor.

At that very instant the voltage at the capacitor is Cero while the current is at its maximum, and therefore the magnetic field has its maximum too.

There is no charge left at the capacitor, therefore the capacitor cannot deliver any current anymore. The current will have to vanish, but it will not stop to flow immediately. As soon as the current will be Cero the magnetic field must have vanished too. But before this can be the case, the magnetic field has to collapse first. The collapsing field will induce a voltage across the coil which will have a direction opposite to the voltage connected to it when the current started to flow.

This selfinduced voltage will cause a current to flow. This current will have the same direction as before, and it will charge the capacitor again but now in opposite direction.

As soon as the magnetic field has vanished totally the capacitor will be charged again to a voltage of the same amount as it was in the beginning, but in opposite direction.

Now the same process will start again, and cause a second halfwave of a sinusoidal ac-current and voltage. Summarizing: If we inject some electric energy to a parallel connection of a capacitor and an inductor there will appear an ac-voltage across the circuit with a frequency depending on the inductance and on the capacity.

But in reality these oscillations will fade out very soon, because the current flowing in this circuit to and for has to pass some obstacles. So for example the resistance of the wires forming the coil, or the resistance of the interconnecting wires. There will vanish also some of the charges stored in the capacitor by moving through the insulating dieelectricum.

All in all, after a short time we will find no more oscillations.

We can explain this effect also from another point of view:

ENERGY CONSIDERATIONS

If we look at the process explained in the last chapter from the point of view of energy, we will find that this LC combination is behaving very similar like a pendulum.


fig. 77


fig. 78

A pendulum starts with a lifted mass which means there is POTENTIAL MECHANICAL ENERGY

When released, the mass gains more and more velocity during its movement downward to the lowest point. In terms of energy: the potential energy is turned into CINETIC ENERGY.

This cinetic energy will cause the mass moving on upwards after passing the lowest point and - by moving upward again - turning the cinetic energy back into POTENTIAL MECHANICAL ENERGY.

TUNED CIRCUIT

Starts with seperated charges on the plates of the capacitor which means ELECTRIC ENERGY.

Once connected to the inductor, the capacitor starts to discharge and push current through the inductor. The current will cause a magnetic field in the inductor and - as soon as the capacitor is totally discharged - the former electric energy is turned into MAGNETIC ENERGY.

So the capacitor is free of charges now, it cannot supply any current anymore, and therefore the magnetic field starts to collapse now.

The collapsing magnetic field induces a voltage and causes the current to go on flowing as before.

This will charge the capacitor no in opposite direction as before. This effect goes on till the capacitor is charged again and the magnetic field has been turned into ELECTRIC ENERGY again.

CHECK YOURSELF:

1. Describe the construction of a tuned circuit.
2. Describe what happens in such a circuit after some energy into it.
3. Explain the similarities between pendulum and resonant circuit.
4. What is the reason for the fast vanishing of oscillations in such a circuit?