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  • 8/10/2019 Tuned CollectorTuned Collector Oscillator

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    Tuned collectorTuned collector oscillator.

    Tuned collector oscillation is a type of transistor LC oscillator where the tuned

    circuit (tank) consists of a transformer and a capacitor is connected in the collector

    circuit of the transistor. Tuned collector oscillator is of course the simplest and the

    basic type of LC oscillators. The tuned circuit connected at the collector circuit

    behaves like a purely resistive load at resonance and determines the oscillator

    frequency.The common applications of tuned collector oscillator are RF oscillator

    circuits, mixers, frequency demodulators, signal generators etc. The circuit diagram

    of a conventional tuned collector oscillator is shown in the figure below.

    Circuit diagram.

    In the circuit diagram resistor R1

    and R2 forms a voltage divider bias for the transistor. Re is the emitter resistor

    which is meant for thermal stability. It also limits the collector current of the

    transistor. Ce is the emitter by-pass capacitor. The job of Ce is to by-pass the

    amplified oscillations. If Ce is not there, the amplified AC oscillations will drop

    across Re and will add on to the base-emitter voltage (Vbe) of the transistor and this

    will alter the DC biasing conditions. Capacitor C1 and primary of the transformer L1forms the tank circuit. C2 is the by-pass capacitor for resistor R2.

    Working of the tuned collector oscillator.

    When the power supply is switched ON, the transistor starts conducting and the

    capacitor C1 starts charging. When the capacitor is fully charged, it starts

    discharging through the primary coil L1. When the capacitor is fully discharged, the

    http://www.circuitstoday.com/wp-content/uploads/2009/10/tuned-collector-oscillator.png
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    energy stored in the capacitor as electrostatic field will be moved to the inductor as

    electromagnetic field. Now there will be no more voltage across the capacitor to keep

    the current through the coil starts to collapse. In order to oppose this the coil L1

    generates a back emf (by electromagnetic induction) and this back emf charges the

    capacitor again. Then capacitor discharges through the coil and the cycle is repeated.

    This charging and discharging sets up a series of oscillations in the tank circuit.

    The oscillations produced in the tank circuit is fed back to the base of transistor Q1

    by the secondary coil by inductive coupling. The amount of feedback can be adjusted

    by varying the turns ratio of the transformer. The winding direction of the secondary

    coil (L2) is in such a way that the voltage across it will be 180 phase opposite to that

    of the voltage across primary (L1). Thus the feedback circuit produces a phase shift

    of 180 and the transistor alone produces a phase shift of another 180. As a result a

    total phase shift of 360 is obtained between input and output and it is a very

    necessary condition for positive feedback and sustained oscillations.

    The collector current of the transistor compensates the energy lost in the tank

    circuit. This is done by taking a small amount of voltage from the tank circuit,

    amplifying it and applying it back to the tank circuit. Capacitor C1 can be made

    variable in variable frequency applications.

    The frequency of oscillations of the tank circuit can be expressed using the following

    equation:

    F = 1/[2(L1C1)]Where Fis the frequency of oscillation. L1is the inductance of the transformer

    primary and C1is the capacitance.

    oscillator.

    Tuned collector oscillation is a type of transistor LC oscillator where the tuned circuit (tank)

    consists of a transformer and a capacitor is connected in the collector circuit of the

    transistor. Tuned collector oscillator is of course the simplest and the basic type of LC

    oscillators. The tuned circuit connected at the collector circuit behaves like a purely resistive

    load at resonance and determines the oscillator frequency.The common applications of

    tuned collector oscillator are RF oscillator circuits, mixers, frequency demodulators, signal

    generators etc. The circuit diagram of a conventional tuned collector oscillator is shown in

    the figure below.

    Circuit diagram.

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    In the circuit diagram resistor R1 andR2 forms a voltage divider bias for the transistor. Re is the emitter resistor which is meant

    for thermal stability. It also limits the collector current of the transistor. Ce is the emitter

    by-pass capacitor. The job of Ce is to by-pass the amplified oscillations. If Ce is not there,

    the amplified AC oscillations will drop across Re and will add on to the base-emitter voltage

    (Vbe) of the transistor and this will alter the DC biasing conditions. Capacitor C1 and

    primary of the transformer L1 forms the tank circuit. C2 is the by-pass capacitor for resistor

    R2.

    Working of the tuned collector oscillator.

    When the power supply is switched ON, the transistor starts conducting and the capacitorC1 starts charging. When the capacitor is fully charged, it starts discharging through the

    primary coil L1. When the capacitor is fully discharged, the energy stored in the capacitor as

    electrostatic field will be moved to the inductor as electromagnetic field. Now there will be

    no more voltage across the capacitor to keep the current through the coil starts to collapse.

    In order to oppose this the coil L1 generates a back emf (by electromagnetic induction) and

    this back emf charges the capacitor again. Then capacitor discharges through the coil and

    the cycle is repeated. This charging and discharging sets up a series of oscillations in the

    tank circuit.

    The oscillations produced in the tank circuit is fed back to the base of transistor Q1 by thesecondary coil by inductive coupling. The amount of feedback can be adjusted by varying

    the turns ratio of the transformer. The winding direction of the secondary coil (L2) is in

    such a way that the voltage across it will be 180 phase opposite to that of the voltage across

    primary (L1). Thus the feedback circuit produces a phase shift of 180 and the transistor

    alone produces a phase shift of another 180. As a result a total phase shift of 360 is

    http://www.circuitstoday.com/wp-content/uploads/2009/10/tuned-collector-oscillator.png
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    obtained between input and output and it is a very necessary condition for positive

    feedback and sustained oscillations.

    The collector current of the transistor compensates the energy lost in the tank circuit. This is

    done by taking a small amount of voltage from the tank circuit, amplifying it and applying it

    back to the tank circuit. Capacitor C1 can be made variable in variable frequencyapplications.

    The frequency of oscillations of the tank circuit can be expressed using the following

    equation:

    F = 1/[2(L1C1)]

    Where F is the frequency of oscillation. L1 is the inductance of the transformer primary

    and C1is the capacitance.