416F52022IKR Crystals, Oscillators, Resonators |
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Allicdata Part #: | CTX1422TR-ND |
Manufacturer Part#: |
416F52022IKR |
Price: | $ 0.34 |
Product Category: | Crystals, Oscillators, Resonators |
Manufacturer: | CTS-Frequency Controls |
Short Description: | CRYSTAL 52.000 MHZ 8PF SMT |
More Detail: | 52MHz ±20ppm Crystal 8pF 100 Ohms 4-SMD, No Lead |
DataSheet: | 416F52022IKR Datasheet/PDF |
Quantity: | 3000 |
3000 +: | $ 0.30511 |
6000 +: | $ 0.29459 |
15000 +: | $ 0.28407 |
Series: | 416 |
Packaging: | Tape & Reel (TR) |
Part Status: | Active |
Type: | MHz Crystal |
Frequency: | 52MHz |
Frequency Stability: | ±20ppm |
Frequency Tolerance: | ±20ppm |
Load Capacitance: | 8pF |
ESR (Equivalent Series Resistance): | 100 Ohms |
Operating Mode: | Fundamental |
Operating Temperature: | -40°C ~ 85°C |
Ratings: | -- |
Mounting Type: | Surface Mount |
Package / Case: | 4-SMD, No Lead |
Size / Dimension: | 0.063" L x 0.047" W (1.60mm x 1.20mm) |
Height - Seated (Max): | 0.018" (0.45mm) |
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Introduction
Crystals are used to generate accurate frequencies in the range of tens of cycles to hundreds of million cycles per second. They are used to generate clock signals for many electronic applications, from high tech communications systems to digital watches. The 416F52022IKR is a crystal oscillator designed to generate a frequency of 28.675 MHz. This article will explain the application fields and working principles of the 416F52022IKR crystal.
Application Fields
The 416F52022IKR crystal can be used in a variety of applications. It is used primarily in communications systems, such as satellite ground stations and microwave transmitters, where it can generate a specific frequency for the purpose of modulating data. The crystal can also be used in digital watches, where its accuracy is used to keep time. It can also be used in audio systems, where it can be used to generate accurate frequencies for low distortion audio.
Working Principle
The 416F52022IKR crystal oscillator works by harnessing the piezoelectric effect, in which a crystal will generate an electrical potential when subjected to mechanical stresses. Applying a voltage to the crystal will cause it to vibrate at a specific frequency determined by its size, shape, and internal structure. This vibration is then converted into an electrical signal at the same frequency by an associated circuit, producing a stable signal at exact, predetermined frequency.
Conclusion
The 416F52022IKR crystal is an important component for many modern communication systems and devices. It relies on the piezoelectric effect to generate a stable signal at a predetermined frequency, making it ideal for use in a variety of applications. From communications systems to digital watches, the 416F52022IKR crystal oscillator is an important part of modern technology.
The specific data is subject to PDF, and the above content is for reference
Part Number | Manufacturer | Price | Quantity | Description |
---|
416F32022CKR | CTS-Frequenc... | 0.33 $ | 24000 | CRYSTAL 32.000 MHZ 8PF SM... |
416F26022CKR | CTS-Frequenc... | 0.33 $ | 3000 | CRYSTAL 26.000 MHZ 8PF SM... |
416F52022CKR | CTS-Frequenc... | 0.33 $ | 3000 | CRYSTAL 52.000 MHZ 8PF SM... |
416F26022IKR | CTS-Frequenc... | 0.34 $ | 12000 | CRYSTAL 26.000 MHZ 8PF SM... |
416F48022IKR | CTS-Frequenc... | 0.34 $ | 3000 | CRYSTAL 48.000 MHZ 8PF SM... |
416F52022IKR | CTS-Frequenc... | 0.34 $ | 3000 | CRYSTAL 52.000 MHZ 8PF SM... |
416F48022CKR | CTS-Frequenc... | 0.33 $ | 1000 | CRYSTAL 48.000 MHZ 8PF SM... |
416F32022IKR | CTS-Frequenc... | 0.34 $ | 1000 | CRYSTAL 32.000 MHZ 8PF SM... |
416F27022CKR | CTS-Frequenc... | 0.33 $ | 1000 | CRYSTAL 27.000 MHZ 8PF SM... |
416F30022CKR | CTS-Frequenc... | 0.33 $ | 1000 | CRYSTAL 30.000 MHZ 8PF SM... |
416F36022CKR | CTS-Frequenc... | 0.33 $ | 1000 | CRYSTAL 36.000 MHZ 8PF SM... |
416F40022CKR | CTS-Frequenc... | 0.33 $ | 1000 | CRYSTAL 40.000 MHZ 8PF SM... |
416F44022CKR | CTS-Frequenc... | 0.33 $ | 1000 | CRYSTAL 44.000 MHZ 8PF SM... |
416F36022IKR | CTS-Frequenc... | 0.34 $ | 1000 | CRYSTAL 36.000 MHZ 8PF SM... |
416F40022IKR | CTS-Frequenc... | 0.34 $ | 1000 | CRYSTAL 40.000 MHZ 8PF SM... |
416F24022IKR | CTS-Frequenc... | 0.34 $ | 1000 | CRYSTAL 24.000 MHZ 8PF SM... |
416F24011AAT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 24.000 MHZ 10PF S... |
416F24011ADT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 24.000 MHZ 18PF S... |
416F24011AKT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 24.000 MHZ 8PF SM... |
416F24011ALT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 24.000 MHZ 12PF S... |
416F24011AST | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 24.000 MHZ SERIES... |
416F24011ATT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 24.000 MHZ 6PF SM... |
416F24011CAT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 24.000 MHZ 10PF S... |
416F24011CDT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 24.000 MHZ 18PF S... |
416F24011CKT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 24.000 MHZ 8PF SM... |
416F24011CLT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 24.000 MHZ 12PF S... |
416F24011CST | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 24.000 MHZ SERIES... |
416F24011CTT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 24.000 MHZ 6PF SM... |
416F24012AAT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 24.000 MHZ 10PF S... |
416F24012ADT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 24.000 MHZ 18PF S... |
416F24012AKT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 24.000 MHZ 8PF SM... |
416F24012ALT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 24.000 MHZ 12PF S... |
416F24012AST | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 24.000 MHZ SERIES... |
416F24012ATT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 24.000 MHZ 6PF SM... |
416F24012CAT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 24.000 MHZ 10PF S... |
416F24012CDT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 24.000 MHZ 18PF S... |
416F24012CKT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 24.000 MHZ 8PF SM... |
416F24012CLT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 24.000 MHZ 12PF S... |
416F24012CST | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 24.000 MHZ SERIES... |
416F24012CTT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 24.000 MHZ 6PF SM... |
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