Gunn Oscillatoron 24/2/2012 & Updated on 4/9/2018
DC BiasIn the case of Gunn diode, as the applied DC bias increases, the current begins to increase at the initial stage, which continues till the threshold voltage. After this, the current continues to fall as the voltage increases until the breakdown voltage is reached. This region which spans from the peak to the valley point, is called the negative resistance region (Figure 1).
This property of the Gunn diode along with its timing properties cause it to behave as an oscillator provided an optimum value of current flows through it. This is because, the negative resistance property of the device nullifies the effect of any real resistance existing in the circuit. This results in the generation of sustained oscillations till the DC bias is present while preventing the growth of oscillations. Further, the amplitude of the resultant oscillations will be limited by the limits of the negative resistance region as evident from Figure 1.
Tuning CircuitIn the case of Gunn oscillators, the oscillation frequency primarily depends on the middle active layer of the gunn diode. However the resonant frequency can be tuned externally either by mechanical or by electrical means. In the case of electronic tuning circuit, the control can be brought about by using a waveguide or microwave cavity or varactor diode or YIG sphere. Here the diode is mounted inside the cavity in such a way that it cancels the loss resistance of the resonator, producing oscillations. On the other hand, in the case of mechanical tuning, the size of the cavity or the magnetic field (for YIG spheres) is varied mechanically by the means of, say, an adjusting screw, inorder to tune the resonant frequency.
These types of oscillators are used to generate microwave frequencies ranging from 10 GHz to few THz, as decided by the dimensions of the resonant cavity. Usually the coaxial and microstrip/planar based oscillator designs have low power factor and are less stable in terms of temperature. On the other hand, the waveguide and the dielectric resonator stabilized circuit designs have greater power factor and can be made thermally stable, quite easily.
Figure 2 shows a coaxial resonator based Gunn oscillator which is used to generate the frequencies ranging from 5 to 65 GHz. Here as the applied voltage Vb is varied, the Gunn diode induced fluctuations travel along the cavity to get reflected from its other end and reach back their starting point after time t given by Where, l is the length of the cavity and c is the speed of light. From this, the equation for the resonant frequency of the Gunn oscillator can be deduced as where, n is the number of half-waves which can fit into the cavity for a given frequency. This n ranges from 1 to l/ctd where td is the time taken by the gunn diode to respond to the changes in the applied voltage.
Here the oscillations are initiated when the loading of the resonator is slightly higher than the maximum negative resistance of the device. Next, these oscillations grow interms of amplitude until the average negative resistance of the gunn diode becomes equal to the resistance of the resonator after which one can get sustained oscillations. Further, these kind of relaxation oscillators have a large capacitor connected across the gunn diode so as to avoid burning-out of the device due to the large amplitude signals. Lastly, it is to be noted that the Gunn diode oscillators are extensively used as radio transmitters and receivers, velocity-detecting sensors, parametric amplifiers, radar sources, traffic monitoring sensors, motion detectors, remote vibration detectors, rotational speed tachometers, moisture content monitors, microwave transceivers (Gunnplexers) and in the case of automatic door openers, burglar alarms, police radars, wireless LANs, collision avoidance systems, anti-lock brakes, pedestrian safety systems, etc.
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