| Allicdata Part #: | 402F37433CAT-ND |
| Manufacturer Part#: |
402F37433CAT |
| Price: | $ 0.00 |
| Product Category: | Crystals, Oscillators, Resonators |
| Manufacturer: | CTS-Frequency Controls |
| Short Description: | CRYSTAL 37.4000MHZ 10PF SMD |
| More Detail: | 37.4MHz ±30ppm Crystal 10pF 60 Ohms 4-SMD, No Lead |
| DataSheet: | 402F37433CAT Datasheet/PDF |
| Quantity: | 1000 |
| 0 +: | $ 0.00000 |
| Series: | 402 |
| Packaging: | Tape & Reel (TR) |
| Part Status: | Discontinued at Digi-Key |
| Type: | MHz Crystal |
| Frequency: | 37.4MHz |
| Frequency Stability: | ±30ppm |
| Frequency Tolerance: | ±30ppm |
| 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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.402F37433CAT application field and working principle
402F37433CAT is a type of crystal structure that is widely used by a variety of industries due to its unique properties and applications. This type of crystal, also known as a Bimonte double-ended tuning fork, has a special field of application, which includes the generation of various frequency signals, synchronization and oscillation control, tilt sensing and vibration sensing. Additionally, the crystal structure can also be used in medical and telecommunications applications.
Crystal Structure
The 402F37433CAT crystal is typically composed of a two-terminal quartz crystal enclosed in a metal case. This double-ended tuning fork consists of four slender forks connected at their ends, forming a rectangular base. Each fork is composed of two identically cut quartz slabs, with the flat surfaces laid parallel to each other and the pointed ends directed outward. The flat surface is usually held at a constant negative charge and forms a diaphragm across the entire crystal.
When a voltage is applied, the diaphragm causes a voltage gradient between the two ends. The electric field across the entire crystal surface is thus strongly influenced by the applied voltage. As a result, the crystal structure vibrates at a certain frequency that is proportional to the applied voltage.
Applications and Working Principles
The 402F37433CAT crystal can be used in a variety of applications, mainly owing to its unique frequency-generating capabilities. In putative applications, it is used to generate electrical oscillations, which can be used to control the frequency of radio receivers and other electronic equipment. Additionally, it is also used as an oscillator in radio receiver circuits, or as a frequency source in telemetry applications. In medical applications, the crystal is used for timing and synchronization purposes, such as determining the heart rate and other vital functions.
The main working principle for the 402F37433CAT crystal centers around its ability to generate a voltage gradient. As the applied voltage increases, the frequency of oscillations generated by the crystal also increases. This is because the field between the two ends of the crystal increases in strength, thereby causing more resonance and higher frequencies. Additionally, due to the symmetrical geometry of the crystal, it has excellent thermal stability and can maintain a constant frequency without oscillation drift.
Advantages
The 402F37433CAT crystal offers several advantages over other crystal structures. Firstly, it has an enhanced drive performance, allowing it to be used with high input voltages of up to 18 VDC. This makes the crystal structure ideal for applications that need to produce larger-scale frequencies, such as radios and telemetry. Additionally, the crystal has excellent thermal characteristics, resulting in improved reliability and a longer operating life. Furthermore, it offers superior frequency control, allowing it to accurately generate specific frequency ranges.
Disadvantages
Although the 402F37433CAT crystal is excellent for a variety of applications, it does have some drawbacks. The primary disadvantage is its size, which makes it difficult to integrate into smaller-sized devices. Additionally, this type of crystal can be expensive to manufacture due to its intricate geometric structure.
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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402F37433CAT Datasheet/PDF