SIT1602BC-11-28N-31.250000G

Oscillators are electrical circuits that generate periodic signals. An oscillator either produces a periodic waveform directly or by transforming an input signal into a periodic waveform. The oscillator SIT1602BC-11-28N-31.250000G belongs to the family of crystal oscillators, and can be used in a variety of applications.

Application field of SIT1602BC-11-28N-31.250000G

The SIT1602BC-11-28N-31.250000G crystal oscillator is a HC49U standard crystal used for precision digital timing signals for a variety of applications. It can be used in a wide variety of applications, including clock generators, RF synthesizers, and frequency converters. It can also be used in medical and industrial instrumentation, laboratory test and measurement, aerospace and navigation, and automotive and consumer electronic applications.

Working Principle of SIT1602BC-11-28N-31.250000G

The SIT1602BC-11-28N-31.250000G crystal oscillator consists of a quartz crystal, a quartz holder, an inductor, and a capacitor connected to the crystal. The quartz crystal is a piezoelectric material and is connected to two electrodes, called the plates. When a voltage is applied to the electrodes, a small mechanical stress is put on the crystal, causing it to oscillate at its resonant frequency. The inductor and capacitor connected to the crystal form a parallel resonance circuit which further amplifies the oscillations produced by the quartz crystal. The frequency of the oscillations created by the SIT1602BC-11-28N-31.250000G oscillator is determined by the resonance frequency of the quartz crystal. The frequency can be changed by adjusting the capacitor or the inductor.

Conclusion

The SIT1602BC-11-28N-31.250000G crystal oscillator is an useful and versatile oscillator which can be used in a variety of applications such as clock generators, RF synthesizers, and frequency converters. It consists of a quartz crystal, a quartz holder, an inductor, and a capacitor connected to the crystal, which create the oscillations. The frequency of the oscillations can be changed by adjusting the capacitor or the inductor connected to the crystal.