
Allicdata Part #: | GL037F35IET-ND |
Manufacturer Part#: |
GL037F35IET |
Price: | $ 0.22 |
Product Category: | Crystals, Oscillators, Resonators |
Manufacturer: | CTS-Frequency Controls |
Short Description: | CRYSTAL 3.686400 MHZ SMD |
More Detail: | 3.6864MHz ±30ppm Crystal 20pF 150 Ohms HC-49/US |
DataSheet: | ![]() |
Quantity: | 1000 |
1000 +: | $ 0.20412 |
Series: | ATSSMGL |
Packaging: | Tape & Reel (TR) |
Part Status: | Active |
Type: | MHz Crystal |
Frequency: | 3.6864MHz |
Frequency Stability: | ±50ppm |
Frequency Tolerance: | ±30ppm |
Load Capacitance: | 20pF |
ESR (Equivalent Series Resistance): | 150 Ohms |
Operating Mode: | Fundamental |
Operating Temperature: | -40°C ~ 85°C |
Ratings: | -- |
Mounting Type: | Surface Mount |
Package / Case: | HC-49/US |
Size / Dimension: | 0.461" L x 0.197" W (11.70mm x 5.00mm) |
Height - Seated (Max): | 0.169" (4.30mm) |
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GL037F35IET Application Field and Working Principle
The GL037F35IET crystal is a very wideband, high performance multiplier circuit with wide range of versatility for mixing, demodulating and other signal processing applications. It is a versatile, high-performance IC for crystal clocks, clock-driven logic applications, and other timing and control circuits. This crystal has a high sensitivity of 1.6KHz per volt, allowing it to be used in applications involving high-frequency signals. It is designed to handle both low-voltage, high-impedance, broadband signals, such as those used in receivers and transceivers, as well as higher-voltage, low impedance signals, such as those used in oscillators, pulse generators, regulators, and other signal processing. Because of its high-frequency accuracy, it is also suitable for use in data security and authentication systems.
The GL037F35IET crystal is highly sensitive and accurate, and provides an excellent signal-to-noise ratio. Its wideband characteristics make it suitable for signal conversion and other signal processing applications. It has an extended frequency range from 50 Hz to 1MHZ, making it very suitable for applications involving high frequency, as well as low frequency, signals. Its bandwidth of 1KHz also makes it suitable for applications involving very low frequency signals.
The working principle of the GL037F35IET crystal is based on the piezoelectric effect. When the crystal is excited by an alternating current, the piezo electric effect makes the crystal vibrate at its resonance frequency. This vibration produces an alternating voltage across the crystal, which produces the output signal. The output voltage of the crystal is proportional to the frequency of the input signal and the amplitude of the output signal increases with frequency. Therefore, this crystal can be used in applications where a high frequency signal needs to be amplified or converted.
The GL037F35IET crystal can be used for analog-to-digital conversion, frequency modulation, frequency compensation and crystal oscillation, among other applications. It can be used to generate clock signals for digital circuits, frequency synthesis and to produce a wide range of frequencies. In addition, it can be used to generate phase-locked loops, which synchronize signals of different phases, and to generate phase difference signals. It can also be used to generate and measure frequency modulation signals, and to generate overtones and time-based effects.
In conclusion, the GL037F35IET crystal is an ideal choice for a wide range of applications, including analog-to-digital conversion, frequency modulation, frequency compensation and oscillation, frequency synthesis, and crystal oscillation. Thanks to its wideband characteristics and high sensitivity, it is suitable for use in a variety of signal processing applications. It is also suitable for use in data security and authentication systems. It is highly sensitive and accurate, and provides an excellent signal-to-noise ratio, making it an excellent choice for use in any signal processing application.
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Part Number | Manufacturer | Price | Quantity | Description |
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GL036F35IET | CTS-Frequenc... | 0.22 $ | 1000 | CRYSTAL 3.579545 MHZ SMD3... |
GL037F33CET | CTS-Frequenc... | 0.22 $ | 1000 | CRYSTAL 3.686400 MHZ SMD3... |
GL037F23CDT | CTS-Frequenc... | 0.22 $ | 1000 | CRYSTAL 3.686400 MHZ SMD3... |
GL036F23IET | CTS-Frequenc... | 0.22 $ | 1000 | CRYSTAL 3.579545 MHZ SMD3... |
GL036F35CDT | CTS-Frequenc... | 0.22 $ | 1000 | CRYSTAL 3.579545 MHZ SMD3... |
GL037F23IET | CTS-Frequenc... | 0.22 $ | 1000 | CRYSTAL 3.686400 MHZ SMD3... |
GL037F23CET | CTS-Frequenc... | 0.22 $ | 1000 | CRYSTAL 3.686400 MHZ SMD3... |
GL036F33IDT | CTS-Frequenc... | 0.22 $ | 1000 | CRYSTAL 3.579545 MHZ SMD3... |
GL037F33IDT | CTS-Frequenc... | 0.22 $ | 1000 | CRYSTAL 3.686400 MHZ SMD3... |
GL037F35CET | CTS-Frequenc... | 0.22 $ | 1000 | CRYSTAL 3.686400 MHZ SMD3... |
GL037F33IET | CTS-Frequenc... | 0.22 $ | 1000 | CRYSTAL 3.686400 MHZ SMD3... |
GL036F35IDT | CTS-Frequenc... | 0.22 $ | 1000 | CRYSTAL 3.579545 MHZ SMD3... |
GL036F23CET | CTS-Frequenc... | 0.22 $ | 1000 | CRYSTAL 3.579545 MHZ SMD3... |
GL036F35CET | CTS-Frequenc... | 0.22 $ | 1000 | CRYSTAL 3.579545 MHZ SMD3... |
GL036F33IET | CTS-Frequenc... | 0.22 $ | 1000 | CRYSTAL 3.579545 MHZ SMD3... |
GL036F33CET | CTS-Frequenc... | 0.22 $ | 1000 | CRYSTAL 3.579545 MHZ SMD3... |
GL037F35IET | CTS-Frequenc... | 0.22 $ | 1000 | CRYSTAL 3.686400 MHZ SMD3... |
GL037F35CDT | CTS-Frequenc... | 0.22 $ | 1000 | CRYSTAL 3.686400 MHZ SMD3... |
GL036F23IDT | CTS-Frequenc... | 0.22 $ | 1000 | CRYSTAL 3.579545 MHZ SMD3... |
GL036F23CDT | CTS-Frequenc... | 0.22 $ | 1000 | CRYSTAL 3.579545 MHZ SMD3... |
GL037F33CDT | CTS-Frequenc... | 0.22 $ | 1000 | CRYSTAL 3.686400 MHZ SMD3... |
GL037F35IDT | CTS-Frequenc... | 0.22 $ | 1000 | CRYSTAL 3.686400 MHZ SMD3... |
GL036F33CDT | CTS-Frequenc... | 0.22 $ | 1000 | CRYSTAL 3.579545 MHZ SMD3... |
GL037F23IDT | CTS-Frequenc... | 0.22 $ | 1000 | CRYSTAL 3.686400 MHZ SMD3... |
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