ABM11W-19.4400MHZ-8-J2Z-T3 Allicdata Electronics
Allicdata Part #:

ABM11W-19.4400MHZ-8-J2Z-T3-ND

Manufacturer Part#:

ABM11W-19.4400MHZ-8-J2Z-T3

Price: $ 0.30
Product Category:

Crystals, Oscillators, Resonators

Manufacturer: Abracon LLC
Short Description: CRYSTAL 19.4400MHZ 8PF SMD
More Detail: 19.44MHz ±20ppm Crystal 8pF 120 Ohms 4-SMD, No Lea...
DataSheet: ABM11W-19.4400MHZ-8-J2Z-T3 datasheetABM11W-19.4400MHZ-8-J2Z-T3 Datasheet/PDF
Quantity: 1000
3000 +: $ 0.27405
Stock 1000Can Ship Immediately
$ 0.3
Specifications
Series: ABM11W
Packaging: Tape & Reel (TR) 
Part Status: Active
Type: MHz Crystal
Frequency: 19.44MHz
Frequency Stability: ±50ppm
Frequency Tolerance: ±20ppm
Load Capacitance: 8pF
ESR (Equivalent Series Resistance): 120 Ohms
Operating Mode: Fundamental
Operating Temperature: -40°C ~ 105°C
Ratings: --
Mounting Type: Surface Mount
Package / Case: 4-SMD, No Lead
Size / Dimension: 0.079" L x 0.063" W (2.00mm x 1.60mm)
Height - Seated (Max): 0.020" (0.50mm)
Description

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Crystals are a class of materials with a highly ordered and symmetrical arrangement of atoms. They have the unique property of being able to change shape when exposed to an electric field. This property makes them useful in many applications including timing, radio frequency, optical and acoustical applications. The ABM11W-19.4400MHZ-8-J2Z-T3 is one such crystal, and its application field and working principle are outlined below.

The ABM11W-19.4400MHZ-8-J2Z-T3 crystal is mainly used in oscillator circuits, such as those found in radios and microwave blocks. Oscillators are circuits which generate an alternating current (AC) waveform. The waveform is usually a sinusoidal wave, but can be triangle, sawtooth or square in shape. The output frequency of the waveform depends on the frequency of the applied electric field, and the capacitance and inductance of the circuit elements. The ABM11W-19.4400MHZ-8-J2Z-T3 crystal is designed to operate within a specific frequency range, allowing for precise tuning and control of the output waveform.

The ABM11W-19.4400MHZ-8-J2Z-T3 consists of two halves that are held tightly together in a cut parallel to the surface of the crystal. This design allows it to convert electrical energy, in the form of an alternating current, into a mechanical vibration at its resonant frequency, and vice versa. As the two halves of the crystal vibrate against each other, they cause a change in the electric field, which is monitored to maintain the exact frequency of the waveform. This process is known as ‘frequency control’, and is the primary function of the ABM11W-19.4400MHZ-8-J2Z-T3.

The use of the ABM11W-19.4400MHZ-8-J2Z-T3 crystal is not limited to oscillator circuits. It can also be used in filters, frequency multipliers, phase locked loops and crystal oscillators, to name a few. These applications are all based on the same principle as the oscillator applications – the frequency of the waveform is precisely controlled by monitoring the interference between the two halves of the crystal. As the waveform passes through the crystal, it causes the two halves to vibrate against each other, producing a change in the electric field which is monitored to maintain the waveform’s frequency.

The ABM11W-19.4400MHZ-8-J2Z-T3 crystal is a versatile tool which is used in a wide variety of applications. Its ability to convert electrical energy into a mechanical vibration makes it ideal for use in frequency control systems, enabling precise tuning and control of the waveform. Its use can be seen in oscillators, filters, frequency multipliers, phase locked loops and crystal oscillators, making it an extremely useful tool for a variety of applications.

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

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