SIT1602BI-21-18N-74.176000E

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Oscillators are special electronic components that can generate periodic electrical signals. SIT1602BI-21-18N-74.176000E is a type of oscillator, which is widely used in the field of electronic engineering. This article will discuss the application field and working principle of SIT1602BI-21-18N-74.176000E oscillator.

The application field of SIT1602BI-21-18N-74.176000E oscillator mainly includes communication, industrial control, and measuring instrumentation. For communication, it can be applied to communication products such as analog modems and computers. It is an important part of the frequency translation and signal conversion in these devices. In industrial control, it can be used in the frequency generation circuit of the frequency inverter, the frequency comparison and voltage adjustment circuit of the frequency regulator, and the microprocessor external clock. Oscillator SIT1602BI-21-18N-74.176000E can also be used in measuring instruments, such as in pyrometers, thermocouples, and other temperature measurement instruments.

The working principle of SIT1602BI-21-18N-74.176000E oscillator is based on the concept of feedback. The oscillator contains a negative feedback amplifier within which output and input are connected by a feedback network, so that the output voltage and current will be fed back to the input. The feedback loop controls the point on the frequency characteristic curve, so that the signal supplied is continuously regenerated and the oscillation is established. The frequency of the oscillator can be calculated by the following formula: ƒ = 1/2π√(LC), where L is the inductance of the coil and C is the capacitance of the capacitor.

In conclusion, SIT1602BI-21-18N-74.176000E oscillator is a type of oscillator that can be applied in communication, industrial control, and measuring instrumentation fields. Its working principle is based on the concept of feedback, where the output and input of the oscillator are connected through a feedback network. The frequency of the oscillator can be calculated by ƒ = 1/2π√(LC).

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