
Allicdata Part #: | 495-48-13JB4X8-ND |
Manufacturer Part#: |
495-48-13JB4X8 |
Price: | $ 0.00 |
Product Category: | Crystals, Oscillators, Resonators |
Manufacturer: | IDT, Integrated Device Technology Inc |
Short Description: | CRYSTAL |
More Detail: | Crystal |
DataSheet: | ![]() |
Quantity: | 1000 |
1 +: | 0.00000 |
Specifications
Series: | -- |
Part Status: | Obsolete |
Description
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Crystals are one of the most significance components in modern technology. The 495-48-13JB4X8 application field and working principle make it one of the most important pieces of technology in today\'s world.Crystals are known to have a wide range of applications in various electronics devices, from mobile phones to computers. 495-48-13JB4X8 is a type of crystal oscillator. It is used to produce frequencies and timing signals which are required for the operation of numerous electronic components.Crystals are used extensively in the radio frequency (RF) domain. For instance, crystals are often used in radio transmitters for the modulation and demodulation of radio signals. Apart from radio frequency applications, these crystals are also used to maintain timekeeping in electronic systems as well as for controlling the frequency of electronic oscillators.One of the major advantages of the 495-48-13JB4X8 is its compatibility with a wide array of components. This makes it a very popular and versatile component amongst RF engineers and manufacturers. It has come to be extensively used in applications such as clock recovery, frequency control, and timing control.The 495-48-13JB4X8 crystal oscillator works on the principle of piezoelectricity. This is the ability of certain materials to generate an electric charge when subjected to an external mechanical stress. Common crystals that exhibit this phenomena are made of lead zirconate titanate (PZT) or quartz.In the 495-48-13JB4X8 crystal oscillator, the crystal is placed in between two parallel plates that are charged with the same voltage. The crystal then oscillates at its angular resonance frequency due to the alternate polarization of the plates.The alternate polarizations cause the crystal to stretch and compress periodically, thus generating a voltage. This voltage is then processed and amplified to generate the required frequency signal.This type of crystal oscillator is also known as an AT-cut crystal oscillator due to its sturdiness and high temperature stability. This type of oscillator is also very popular in telecommunications applications. The 495-48-13JB4X8 is extremely reliable, accurate and stable, which makes it ideal for frequency control applications. Some of these applications include voltage-controlled oscillator (VCO) circuits, phase-locked loop (PLL) circuits, and direct digital synthesizer (DDS) circuits.Crystals are also used in the construction of filters and amplifiers which are used to control the flow of current and signals in electronic systems. 495-48-13JB4X8 is considered to be one of the most accurate crystals for this purpose.Crystals are also used for the transmission and reception of radio signals. As crystals are capable of working in the extremely low wattage range of RF signals, they are an essential part of most Radio Frequency Identification (RFID) projects and Wireless Local Area Networks (WLANs).495-48-13JB4X8 application field and working principle has made it one of the most important components in modern technology. Due to its versatile and reliable nature, the crystal is used in a variety of applications. From mobile phones to communications systems, the 495-48-13JB4X8 is sure to continue to be a mainstay in the world of technology for many years to come.The specific data is subject to PDF, and the above content is for reference
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