Allicdata Part #: | 631-1214-ND |
Manufacturer Part#: |
FC4STCBMF12.288-BAG200 |
Price: | $ 0.25 |
Product Category: | Crystals, Oscillators, Resonators |
Manufacturer: | Fox Electronics |
Short Description: | CRYSTAL 12.2880MHZ 20PF T/H |
More Detail: | 12.288MHz ±30ppm Crystal 20pF 60 Ohms HC-49/US |
DataSheet: | FC4STCBMF12.288-BAG200 Datasheet/PDF |
Quantity: | 527 |
1 +: | $ 0.22050 |
10 +: | $ 0.18207 |
50 +: | $ 0.16367 |
100 +: | $ 0.14553 |
500 +: | $ 0.13826 |
1000 +: | $ 0.11642 |
2500 +: | $ 0.10915 |
5000 +: | $ 0.10551 |
10000 +: | $ 0.10187 |
Series: | HC49SLF |
Packaging: | Bulk |
Part Status: | Active |
Type: | MHz Crystal |
Frequency: | 12.288MHz |
Frequency Stability: | ±50ppm |
Frequency Tolerance: | ±30ppm |
Load Capacitance: | 20pF |
ESR (Equivalent Series Resistance): | 60 Ohms |
Operating Mode: | Fundamental |
Operating Temperature: | -20°C ~ 70°C |
Ratings: | -- |
Mounting Type: | Through Hole |
Package / Case: | HC-49/US |
Size / Dimension: | 0.447" L x 0.183" W (11.35mm x 4.65mm) |
Height - Seated (Max): | 0.142" (3.60mm) |
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Crystals play an important role in a wide range of applications, from precision clock oscillators to radio communication systems, from medical imaging systems to aerospace guidance systems. The FC4STCBMF12.288-BAG200 is one such crystal and it has a wide range of applications with its unique working principle. In this article, we will discuss the applications and working principles of the FC4STCBMF12.288-BAG200.
The FC4STCBMF12.288-BAG200 is a crystal oscillator that is made using a high-Q (Quality) quartz crystal. It is designed to offer excellent frequency stability, low temperature drift and long-term reliability. It is a hermetically sealed crystal oscillator that operates with a frequency of 12.288MHz and operates within a reliable temperature range of -40°C to +85°C. It is available in various frequencies such as 10MHz, 12.288MHz, 13MHz, 19.5MHz, 22.7MHz, 25.5MHz and 30MHz.
The FC4STCBMF12.288-BAG200 is used in several applications such as in radio communication systems, GPS navigation systems, cellular phones, monitoring systems, automotive electronics and other consumer electronics. The quartz crystal in the FC4STCBMF12.288-BAG200 is used to provide accurate timing pulses to precision radio transmission systems. It is also used in sonar systems, processors, and other applications where highly precise signals are required.
Another application in which the FC4STCBMF12.288-BAG200 can be found is in data transmission systems. For example, the quartz crystal in the FC4STCBMF12.288-BAG200 is used to create a high-precision signal which is received by a transceiver and is then passed through a data line to the desired destination. This is an efficient method of data transmission as it helps reduce data errors and ensures fast and reliable data transmission.
The working principle of the FC4STCBMF12.288-BAG200 is based on the vibration of a quartz crystal that is caused by electrical energy applied to it. A quartz crystal is a type of piezoelectric material, which means that it is capable of converting electrical energy into mechanical vibration, and vice versa. This vibration is then passed on to the output pins, providing a precise square wave signal with a very high frequency (12.288MHz). This is the basic operating principle of the FC4STCBMF12.288-BAG200.
The high-Q (Quality) quartz crystal in the FC4STCBMF12.288-BAG200 ensures that the frequency and phase stability of the oscillator are maintained over a wide temperature range. The frequency is also very consistent and the phase noise is very low. This makes the FC4STCBMF12.288-BAG200 a reliable and robust crystal oscillator which is suitable for many applications.
In conclusion, the FC4STCBMF12.288-BAG200 is a high-Q quartz crystal oscillator which is designed to offer excellent frequency stability, low temperature drift and long-term reliability. Its range of applications includes radio communication systems, GPS navigation systems, cellular phones, monitoring systems, automotive electronics and other consumer electronics. It operates using a basic principle of energy applied to the quartz crystal causing it to vibrate and creating a square wave output. The high-Q quartz crystal ensures that the frequency and phase stability of the oscillator are maintained over a wide temperature range. The FC4STCBMF12.288-BAG200 is a reliable and robust crystal oscillator which is suitable for many applications.
The specific data is subject to PDF, and the above content is for reference
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FC4SDCBMF11.0592-T1 | Fox Electron... | 0.11 $ | 39000 | CRYSTAL 11.0592MHZ 20PF S... |
FC4SDCBMF24.0-T1 | Fox Electron... | 0.11 $ | 26000 | CRYSTAL 24.0000MHZ 20PF S... |
FC4SDCBMF16.0-T1 | Fox Electron... | 0.11 $ | 14000 | CRYSTAL 16.0000MHZ 20PF S... |
FC4SDCBMF4.0-T1 | Fox Electron... | 0.11 $ | 13000 | CRYSTAL 4.0000MHZ 20PF SM... |
FC4SDCBMF10.0-T1 | Fox Electron... | 0.11 $ | 11000 | CRYSTAL 10.0000MHZ 20PF S... |
FC4SDCBMF14.7456-T1 | Fox Electron... | 0.11 $ | 8000 | CRYSTAL 14.7456MHZ 20PF S... |
FC4SDCBMF20.0-T1 | Fox Electron... | 0.11 $ | 8000 | CRYSTAL 20.0000MHZ 20PF S... |
FC4SDCBMF6.0-T1 | Fox Electron... | 0.11 $ | 6000 | CRYSTAL 6.0000MHZ 20PF SM... |
FC4SDCBLF3.579545-T1 | Fox Electron... | 0.11 $ | 5000 | CRYSTAL 3.579545MHZ 18PF ... |
FC4SDCBMF18.432-T1 | Fox Electron... | 0.11 $ | 5000 | CRYSTAL 18.4320MHZ 20PF S... |
FC4SDCBMM8.0-T1 | Fox Electron... | 0.14 $ | 4000 | CRYSTAL 8.0000MHZ 20PF SM... |
FC4STCBMF25.0-BAG200 | Fox Electron... | 0.22 $ | 3816 | CRYSTAL 25.0000MHZ 20PF T... |
FC4STCBMF8.0-BAG200 | Fox Electron... | 0.25 $ | 15571 | CRYSTAL 8.0000MHZ 20PF T/... |
FC4STCBMF12.0-BAG200 | Fox Electron... | 0.25 $ | 15047 | CRYSTAL 12.0000MHZ 20PF T... |
FC4STCBMF20.0-BAG200 | Fox Electron... | 0.25 $ | 11771 | CRYSTAL 20.0000MHZ 20PF T... |
FC4STCBMF4.0-BAG200 | Fox Electron... | 0.25 $ | 4613 | CRYSTAL 4.0000MHZ 20PF T/... |
FC4STCBMF11.0592-BAG200 | Fox Electron... | 0.25 $ | 3484 | CRYSTAL 11.0592MHZ 20PF T... |
FC4STCBLF3.579545-BAG200 | Fox Electron... | 0.25 $ | 3274 | CRYSTAL 3.579545MHZ 18PF ... |
FC4STCBMF16.0-BAG200 | Fox Electron... | 0.25 $ | 2459 | CRYSTAL 16.0000MHZ 20PF T... |
FC4STCBMF14.7456-BAG200 | Fox Electron... | 0.25 $ | 1906 | CRYSTAL 14.7456MHZ 20PF T... |
FC4STCBMF10.0-BAG200 | Fox Electron... | 0.25 $ | 1565 | CRYSTAL 10.0000MHZ 20PF T... |
FC4STCBMF7.3728-BAG200 | Fox Electron... | 0.25 $ | 1255 | CRYSTAL 7.3728MHZ 20PF T/... |
FC4STCBMF18.432-BAG200 | Fox Electron... | 0.25 $ | 1108 | CRYSTAL 18.4320MHZ 20PF T... |
FC4SDCBMM16.0-T1 | Fox Electron... | 0.14 $ | 1000 | CRYSTAL 16.0000MHZ 20PF S... |
FC4STCBAF16.0-BAG200 | Fox Electron... | 0.25 $ | 1000 | CRYSTAL 16.0000MHZ SERIES... |
FC4STCBMF24.576-BAG200 | Fox Electron... | 0.25 $ | 1000 | CRYSTAL 24.5760MHZ 20PF T... |
FC4SDCBMF8.192-T1 | Fox Electron... | 0.13 $ | 1000 | CRYSTAL 8.1920MHZ 20PF SM... |
FC4SDCBMF9.8304-T1 | Fox Electron... | 0.13 $ | 1000 | CRYSTAL 9.8304MHZ 20PF SM... |
FC4SDCBMF19.6608-T1 | Fox Electron... | 0.13 $ | 1000 | CRYSTAL 19.6608MHZ 20PF S... |
FC4STCBAF11.0592-BAG200 | Fox Electron... | 0.16 $ | 1000 | CRYSTAL 11.0592MHZ SERIES... |
FC4STCBAF20.0-BAG200 | Fox Electron... | 0.16 $ | 1000 | CRYSTAL 20.0000MHZ SERIES... |
FC4SDCBMM3.6864-T1 | Fox Electron... | 0.18 $ | 1000 | CRYSTAL 3.6864MHZ 20PF SM... |
FC4SDCBMM4.0-T1 | Fox Electron... | 0.18 $ | 1000 | CRYSTAL 4.0000MHZ 20PF SM... |
FC4SDCBMM6.0-T1 | Fox Electron... | 0.18 $ | 1000 | CRYSTAL 6.0000MHZ 20PF SM... |
FC4SDCBMM7.3728-T1 | Fox Electron... | 0.18 $ | 1000 | CRYSTAL 7.3728MHZ 20PF SM... |
FC4SDCBMM10.0-T1 | Fox Electron... | 0.18 $ | 1000 | CRYSTAL 10.0000MHZ 20PF S... |
FC4SDCBMM11.0592-T1 | Fox Electron... | 0.18 $ | 1000 | CRYSTAL 11.0592MHZ 20PF S... |
FC4SDCBMM14.31818-T1 | Fox Electron... | 0.18 $ | 1000 | CRYSTAL 14.31818MHZ 20PF ... |
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