637E14856C3T Allicdata Electronics
Allicdata Part #:

637E14856C3T-ND

Manufacturer Part#:

637E14856C3T

Price: $ 2.34
Product Category:

Crystals, Oscillators, Resonators

Manufacturer: CTS-Frequency Controls
Short Description: OSC XO 84.7739MHZ LVPECL SMD
More Detail: 84.7739MHz XO (Standard) LVPECL Oscillator 3.3V En...
DataSheet: 637E14856C3T datasheet637E14856C3T Datasheet/PDF
Quantity: 1000
1000 +: $ 2.10564
Stock 1000Can Ship Immediately
$ 2.34
Specifications
Frequency Stability: ±20ppm
Current - Supply (Disable) (Max): --
Height - Seated (Max): 0.079" (2.00mm)
Size / Dimension: 0.276" L x 0.197" W (7.00mm x 5.00mm)
Package / Case: 6-SMD, No Lead
Mounting Type: Surface Mount
Ratings: --
Current - Supply (Max): 88mA
Operating Temperature: -20°C ~ 70°C
Series: 637
Voltage - Supply: 3.3V
Output: LVPECL
Function: Enable/Disable
Frequency: 84.7739MHz
Type: XO (Standard)
Base Resonator: Crystal
Part Status: Active
Packaging: Tape & Reel (TR) 
Description

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Oscillators are key elements of modern electronic devices used in generating a continuous output waveform signal. 637E14856C3T oscillators represent one of the most popular types of oscillator.

637E14856C3T oscillators are used in a variety of applications, such as communication systems, test and measurement, industrial control, audio frequency applications, radio frequency applications, and phase locked loop applications. They can be used to generate stable, precise waveforms, provide signal sources for logic, and create reference frequencies for control systems.

At the heart of 637E14856C3T oscillators is a type of self-excited oscillator circuit known as the Hartley oscillator. This oscillator utilizes two capacitors, two inductors and one resistor in order to produce an output signal. It can be used to produce signals with frequencies ranging from kilohertz to megahertz.

The two inductors are connected in series between the AC power source and ground. The analog signal output is then taken from the point between the two inductors, which is known as the output node. The two capacitors are connected in parallel, one between the output node and the ground, and the other between the output node and the AC power source. The resistor is connected between the AC power source and the output node.

The Hartley oscillator will function when an alternating voltage is applied. This voltage is typically AC. When the applied voltage reaches the point at which it’s large enough to cause an avalanche breakdown of the capacitance, the oscillator begins to oscillate. From this point on the oscillator will continue to oscillate at a frequency determined by the capacitance and inductance values.

The circuit has a positive feedback mechanism that causes the output voltage to increase, which in turn increases the current through the inductors, further increasing the output voltage. This loop carries on until the current and voltage move back into balance, and the oscillator will remain at this frequency until the applied voltage changes. This allows the oscillator to maintain a steady and consistent frequency.

637E14856C3T oscillators have the advantage of being very stable and they can operate over a wide range of frequencies. Their small size makes them especially suitable for applications where space is at a premium. Additionally, they often come in ‘plug and play’ packages, making them easy to install and use.

637E14856C3T oscillators are reliable and offer a wide range of applications due to their ability to generate a steady and consistent output. They are commonly used in communication systems, test and measurement, industrial control, audio frequency applications, radio frequency applications, and phase locked loop applications.

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

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