445A31D14M31818 Allicdata Electronics
Allicdata Part #:

445A31D14M31818-ND

Manufacturer Part#:

445A31D14M31818

Price: $ 0.43
Product Category:

Crystals, Oscillators, Resonators

Manufacturer: CTS-Frequency Controls
Short Description: CRYSTAL 14.31818MHZ 18PF SMD
More Detail: 14.31818MHz ±30ppm Crystal 18pF 50 Ohms 2-SMD, No ...
DataSheet: 445A31D14M31818 datasheet445A31D14M31818 Datasheet/PDF
Quantity: 1000
1000 +: $ 0.39336
Stock 1000Can Ship Immediately
$ 0.43
Specifications
Series: 445
Packaging: Tape & Reel (TR) 
Part Status: Active
Type: MHz Crystal
Frequency: 14.31818MHz
Frequency Stability: ±10ppm
Frequency Tolerance: ±30ppm
Load Capacitance: 18pF
ESR (Equivalent Series Resistance): 50 Ohms
Operating Mode: Fundamental
Operating Temperature: -10°C ~ 60°C
Ratings: --
Mounting Type: Surface Mount
Package / Case: 2-SMD, No Lead
Size / Dimension: 0.197" L x 0.126" W (5.00mm x 3.20mm)
Height - Seated (Max): 0.053" (1.35mm)
Description

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Crystals have many applications in the fields of electronics, communications, and seismology, to name a few. One of the most common applications of crystals is in oscillators and receivers, where correct and reliable performance requires precise control of frequency and phase. The 445A31D14M31818 is a type of crystal oscillator that can provide reliable and precise radio frequency (RF) sources.

This crystal oscillator is based on a piezoelectric quartz crystal and uses a Pierce-type circuit to achieve excellent frequency-stability and wide operating frequency range. Quartz crystals are widely used due to their low cost, high temperature performance, and excellent temperature stability.

Operation principle

The quartz crystal consists of two metal electrodes, called plates, that have a thin layer of quartz between them. When a voltage is applied, the quartz material deforms slightly. This movement produces an electric current, which is then amplified by an external circuit and filtered to obtain the required frequency.

The Pierce-type oscillator consists of two transistors, a quartz crystal, and a few other passive components. The two transistors are arranged in a classic ?push-pull? configuration. One transistor is used to apply a voltage to the crystal, and the other is used to detect the current that the crystal produces when it deforms. The output of the circuit is the amplified current from the crystal.

By carefully controlling the applied voltage and the gain of the amplifier, the frequency of the oscillation can be controlled with a high degree of accuracy. Additionally, for applications where precise frequency control is not necessary, the circuit can be tuned to produce a particular frequency simply by changing the values of the components.

Application field

The 445A31D14M31818 crystal oscillator has a wide range of applications due to its excellent frequency-stability and wide operating frequency range. It is used in many different types of oscillators, such as voltage-controlled, phase-locked loop (PLL), and voltage-regulated crystal oscillators (VCXOs). It is also used in receivers, transmitters, and tuners.

Due to its excellent performance, the 445A31D14M31818 crystal oscillator is often used for radar applications, where it provides high frequency stability, accuracy, and wide frequency coverage. It is also used in medical equipment, such as cardiac pacemakers and defibrillators, where its precise frequency control ensures reliable operation.

Conclusion

The 445A31D14M31818 crystal oscillator is a reliable and precise radio frequency (RF) source based on a piezoelectric quartz crystal and a Pierce-type circuit. Its wide range of applications include oscillators, receivers, transmitters, tuners, and radar applications, as well as medical equipment. Due to its excellent frequency-stability and wide operating frequency range, it is widely used in many different types of devices.

The specific data is subject to PDF, and the above content is for reference

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