| Allicdata Part #: | 402F54011CAT-ND |
| Manufacturer Part#: |
402F54011CAT |
| Price: | $ 0.00 |
| Product Category: | Crystals, Oscillators, Resonators |
| Manufacturer: | CTS-Frequency Controls |
| Short Description: | CRYSTAL 54.0000MHZ 10PF SMD |
| More Detail: | 54MHz ±10ppm Crystal 10pF 60 Ohms 4-SMD, No Lead |
| DataSheet: | 402F54011CAT Datasheet/PDF |
| Quantity: | 1000 |
| 0 +: | $ 0.00000 |
| Series: | 402 |
| Packaging: | Tape & Reel (TR) |
| Part Status: | Discontinued at Digi-Key |
| Type: | MHz Crystal |
| Frequency: | 54MHz |
| Frequency Stability: | ±10ppm |
| Frequency Tolerance: | ±10ppm |
| Load Capacitance: | 10pF |
| ESR (Equivalent Series Resistance): | 60 Ohms |
| Operating Mode: | Fundamental |
| Operating Temperature: | -20°C ~ 70°C |
| Ratings: | -- |
| Mounting Type: | Surface Mount |
| Package / Case: | 4-SMD, No Lead |
| Size / Dimension: | 0.079" L x 0.063" W (2.00mm x 1.60mm) |
| Height - Seated (Max): | 0.022" (0.55mm) |
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402F54011CAT application field and working principle
A 402F54011CAT crystal is a type of oscillator that produces electrical signals at very precise intervals. It is a quartz oscillator with a control layer known as an AT cut. This crystal has a high frequency stability and an extremely low aging behavior. It also features a wide operating temperature range and is suitable for high-voltage operation.
AT cut crystals are widely used in a broad range of applications, spanning communications, industrial automation, medical, automotive, and consumer electronics. These crystals can be used in standalone operation or incorporated in embedded systems, where they are frequently found in low-power radio frequency modules, LCD modules, avionics, and other applications.
Working Principle
The working principle of a 402F54011CAT crystal is based on the piezoelectric effect: the mechanical strain induced in a crystal when an electric field is applied. This piezoelectric effect helps the oscillator generate a precise frequency as its output.
In this specific oscillator, the AT cut crystal acts as the resonator, providing the crystal\'s high stability and wide temperature range. The characteristic frequency is generated by the field effect transistor (FET) circuit, which is connected to the crystal. Every time the voltage is applied, the crystal will oscillate at its resonant frequency, producing an electrical output.
Components
A 402F54011CAT crystal system consists of several components, including a quartz crystal, a voltage-controlled oscillator, a frequency detector, and a counter. All of these components are connected together in order to generate the desired frequency.
The quartz crystal serves as the resonator for the oscillations. It is powered by the voltage-controlled oscillator, which is responsible for the desired frequency of the output. The frequency detector is then used to measure the signal and detect any variations in frequency. After that, the counter is used to register the signal output and process it accordingly.
Advantages
The 402F54011CAT crystal has several advantages compared to other types of oscillators. First, it offers excellent frequency accuracy and stability, making it suitable for highly precise applications. It also has a lower noise level than other crystals, meaning that it produces less interference with sensitive circuitry. In addition, it has a wide operating temperature range and is resistant to vibration and shock, making it suitable for use in harsh environments.
Applications
A 402F54011CAT crystal can be found in a variety of different applications. It is used in industrial automation equipment, avionics equipment, medical monitor systems, automotive systems, and consumer electronics. In addition, this crystal can be used in mobile communications systems, such as WCDMA, WiMAX, and LTE systems.
Due to its performance and reliability, this crystal is also used in high-precision timing systems, such as GPS and satellite navigation systems, as well as in scientific instruments, including atomic clocks and laboratory systems.
Conclusion
The 402F54011CAT crystal offers excellent performance and reliability, making it a popular choice in a variety of different applications. Its wide operating temperature range and high frequency stability make it suitable for use in precision timing, communications, and automotive systems. With its easy installation and reliable performance, this crystal is sure to meet the demands of any system.
The specific data is subject to PDF, and the above content is for reference
| Part Number | Manufacturer | Price | Quantity | Description |
|---|
| 402F1921XIAR | CTS-Frequenc... | 0.29 $ | 1000 | CRYSTAL 19.2000MHZ 10PF S... |
| 402F37422IDR | CTS-Frequenc... | 0.29 $ | 1000 | CRYSTAL 37.4000MHZ 18PF S... |
| 402F37411CJT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 37.4000MHZ 9PF SM... |
| 402F480XXCAT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 48.0000MHZ 10PF S... |
| 402F160XXCDT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 16.0000MHZ 18PF S... |
| 402F38433CLT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 38.4000MHZ 12PF S... |
| 402F20022IKT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 20.0000MHZ 8PF SM... |
| 402F3601XIJR | CTS-Frequenc... | 0.29 $ | 1000 | CRYSTAL 36.0000MHZ 9PF SM... |
| 402F32011CLT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 32.0000MHZ 12PF S... |
| 402F27011CDT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 27.0000MHZ 18PF S... |
| 402F240XXCKT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 24.0000MHZ 8PF SM... |
| 402F160XXCJT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 16.0000MHZ 9PF SM... |
| 402F240XXCLT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 24.0000MHZ 12PF S... |
| 402F32012IKT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 32.0000MHZ 8PF SM... |
| 402F19222IJT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 19.2000MHZ 9PF SM... |
| 402F384XXCLR | CTS-Frequenc... | 0.29 $ | 1000 | CRYSTAL 38.4000MHZ 12PF S... |
| 402F19233CAR | CTS-Frequenc... | 0.29 $ | 1000 | CRYSTAL 19.2000MHZ 10PF S... |
| 402F37412ILR | CTS-Frequenc... | 0.29 $ | 1000 | CRYSTAL 37.4000MHZ 12PF S... |
| 402F54033CJR | CTS-Frequenc... | 0.3 $ | 1000 | CRYSTAL 54.0000MHZ 9PF SM... |
| 402F3001XIJT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 30.0000MHZ 9PF SM... |
| 402F50022IKT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 50.0000MHZ 8PF SM... |
| 402F250XXCKT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 25.0000MHZ 8PF SM... |
| 402F1601XILT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 16.0000MHZ 12PF S... |
| 402F50022ILT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 50.0000MHZ 12PF S... |
| 402F2501XIAR | CTS-Frequenc... | 0.29 $ | 9000 | CRYSTAL 25.0000MHZ 10PF S... |
| 402F4001XIKR | CTS-Frequenc... | 0.29 $ | 1000 | CRYSTAL 40.0000MHZ 8PF SM... |
| 402F27112IKR | CTS-Frequenc... | 0.29 $ | 1000 | CRYSTAL 27.1200MHZ 8PF SM... |
| 402F500XXCDR | CTS-Frequenc... | 0.3 $ | 1000 | CRYSTAL 50.0000MHZ 18PF S... |
| 402F48033CAR | CTS-Frequenc... | 0.3 $ | 1000 | CRYSTAL 48.0000MHZ 10PF S... |
| 402F40011CAT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 40.0000MHZ 10PF S... |
| 402F20411CKT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 20.4800MHZ 8PF SM... |
| 402F50011CLT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 50.0000MHZ 12PF S... |
| 402F3601XIJT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 36.0000MHZ 9PF SM... |
| 402F27022IDT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 27.0000MHZ 18PF S... |
| 402F30022IDT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 30.0000MHZ 18PF S... |
| 402F27111CKR | CTS-Frequenc... | 0.32 $ | 1000 | CRYSTAL 27.1200MHZ 8PF SM... |
| 402F37411CDR | CTS-Frequenc... | 0.32 $ | 1000 | CRYSTAL 37.4000MHZ 18PF S... |
| 402F384XXCLT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 38.4000MHZ 12PF S... |
| 402F50022IJT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 50.0000MHZ 9PF SM... |
| 402F48022IAT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 48.0000MHZ 10PF S... |
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402F54011CAT Datasheet/PDF