| Allicdata Part #: | 402F19211CAT-ND |
| Manufacturer Part#: |
402F19211CAT |
| Price: | $ 0.00 |
| Product Category: | Crystals, Oscillators, Resonators |
| Manufacturer: | CTS-Frequency Controls |
| Short Description: | CRYSTAL 19.2000MHZ 10PF SMD |
| More Detail: | 19.2MHz ±10ppm Crystal 10pF 120 Ohms 4-SMD, No Lea... |
| DataSheet: | 402F19211CAT Datasheet/PDF |
| Quantity: | 1000 |
| 0 +: | $ 0.00000 |
| Series: | 402 |
| Packaging: | Tape & Reel (TR) |
| Part Status: | Discontinued at Digi-Key |
| Type: | MHz Crystal |
| Frequency: | 19.2MHz |
| Frequency Stability: | ±10ppm |
| Frequency Tolerance: | ±10ppm |
| Load Capacitance: | 10pF |
| ESR (Equivalent Series Resistance): | 120 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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Crystals
CAT (Crystal Acoustic Transducer) is a kind of piezoelectric crystal acoustic transducer based on the inverse piezoelectric effect, which has a wide range of applications in the acoustic fields such as sound detection and conversion, frequency modulation, and wireless transmission. A crystal transducer is composed of two main components, an active crystal material and a conductor element, which interact with each other to produce electrical signals in response to acoustic stimulation. It can be used in various fields such as medical instruments, mobile phones, digital media players, home theaters, and automotive audio systems.
The working principle of a crystal transducer is based on the phenomenon of inverse piezoelectric effect, whereby an electric field is generated when a pressure wave (such as sound) is applied to certain kinds of crystals or ceramics. When the applied wave reaches the surface of the crystal, it causes it to vibrate, inducing a mechanical strain in the crystalline structure. This strain results in the formation of electrical charges on the surface of the crystal, which can subsequently be detected and converted into an electrical signal. In other words, the wave can be used to produce an electrical signal that corresponds to the wave that initiated it.
In the field of CATs, the working principle is similar but slightly different. This is because the active element used in a CAT is a piezoelectric crystal that itself has a built-in electric field. The idea behind using a CAT is to convert the acoustic energy into electrical energy for use in the electronic circuits. When an acoustic wave is applied to the crystal, it causes the crystal to vibrate, which induces an electric field in the crystal surface. This electric field is then detected and converted into an electrical signal which can then be used to control an electronic circuit. This makes the CAT particularly suitable for digital signal processing and various audio applications.
CATs can be used in a wide range of applications. In medical devices, they can be used to detect changes in sound or pressure inside the body, allowing for the measurement of intracranial pressure or blood pressure. In wireless communication, they can be used to detect, convert and transmit signals that enable communication between electronic devices. CATs can also be used in acoustic sensing for industrial applications. They are particularly suitable for detecting and measuring vibrations in industrial machinery.
CATs offer a number of advantages over other types of acoustic transducers. The crystal material used is typically higher in quality compared to other transducer materials, and its performance is more consistent and reliable. They are also more efficient in terms of electrical power consumption, resulting in less energy waste and lower costs. Another advantage is that they require fewer components than other transducer types, which makes them more lightweight and easier to implement in acoustic systems.
In conclusion, CATs are a versatile and reliable type of acoustic transducer with many applications in the acoustic fields. Their ability to convert acoustic energy into electrical energy efficiently makes them useful in a variety of audio and communication applications, such as medical devices, wireless communication, and acoustic sensing for industrial purposes. They are also more efficient in terms of power consumption and require fewer components, making them lightweight and easy to implement.
The specific data is subject to PDF, and the above content is for reference
| Part Number | Manufacturer | Price | Quantity | Description |
|---|
| 402F2601XIAR | CTS-Frequenc... | 0.29 $ | 1000 | CRYSTAL 26.0000MHZ 10PF S... |
| 402F50011CDT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 50.0000MHZ 18PF S... |
| 402F360XXCLT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 36.0000MHZ 12PF S... |
| 402F26033CAT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 26.0000MHZ 10PF S... |
| 402F2401XIAR | CTS-Frequenc... | 0.29 $ | 1000 | CRYSTAL 24.0000MHZ 10PF S... |
| 402F3741XIAR | CTS-Frequenc... | 0.29 $ | 1000 | CRYSTAL 37.4000MHZ 10PF S... |
| 402F24012IJR | CTS-Frequenc... | 0.29 $ | 1000 | CRYSTAL 24.0000MHZ 9PF SM... |
| 402F48011CJT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 48.0000MHZ 9PF SM... |
| 402F24012ILR | CTS-Frequenc... | 0.29 $ | 1000 | CRYSTAL 24.0000MHZ 12PF S... |
| 402F2001XIDR | CTS-Frequenc... | 0.29 $ | 1000 | CRYSTAL 20.0000MHZ 18PF S... |
| 402F16022IAR | CTS-Frequenc... | 0.29 $ | 1000 | CRYSTAL 16.0000MHZ 10PF S... |
| 402F20022ILR | CTS-Frequenc... | 0.29 $ | 1000 | CRYSTAL 20.0000MHZ 12PF S... |
| 402F30022IDR | CTS-Frequenc... | 0.29 $ | 1000 | CRYSTAL 30.0000MHZ 18PF S... |
| 402F54011CLR | CTS-Frequenc... | 0.33 $ | 1000 | CRYSTAL 54.0000MHZ 12PF S... |
| 402F36011CJT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 36.0000MHZ 9PF SM... |
| 402F19211CDT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 19.2000MHZ 18PF S... |
| 402F26033CDR | CTS-Frequenc... | 0.29 $ | 1000 | CRYSTAL 26.0000MHZ 18PF S... |
| 402F24012IAR | CTS-Frequenc... | 0.29 $ | 1000 | CRYSTAL 24.0000MHZ 10PF S... |
| 402F38422IJR | CTS-Frequenc... | 0.29 $ | 1000 | CRYSTAL 38.4000MHZ 9PF SM... |
| 402F40022IAR | CTS-Frequenc... | 0.29 $ | 1000 | CRYSTAL 40.0000MHZ 10PF S... |
| 402F54033CKR | CTS-Frequenc... | 0.3 $ | 1000 | CRYSTAL 54.0000MHZ 8PF SM... |
| 402F20011CJT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 20.0000MHZ 9PF SM... |
| 402F48011CDT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 48.0000MHZ 18PF S... |
| 402F30033CDT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 30.0000MHZ 18PF S... |
| 402F2501XIKT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 25.0000MHZ 8PF SM... |
| 402F25022ILT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 25.0000MHZ 12PF S... |
| 402F2601XIDR | CTS-Frequenc... | 0.29 $ | 1000 | CRYSTAL 26.0000MHZ 18PF S... |
| 402F204XXCKT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 20.4800MHZ 8PF SM... |
| 402F20033CAT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 20.0000MHZ 10PF S... |
| 402F30722IDT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 30.7200MHZ 18PF S... |
| 402F40022IDT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 40.0000MHZ 18PF S... |
| 402F32033CKR | CTS-Frequenc... | 0.29 $ | 1000 | CRYSTAL 32.0000MHZ 8PF SM... |
| 402F32033CLR | CTS-Frequenc... | 0.29 $ | 1000 | CRYSTAL 32.0000MHZ 12PF S... |
| 402F20033CDR | CTS-Frequenc... | 0.29 $ | 1000 | CRYSTAL 20.0000MHZ 18PF S... |
| 402F37412IAR | CTS-Frequenc... | 0.29 $ | 1000 | CRYSTAL 37.4000MHZ 10PF S... |
| 402F40033CAR | CTS-Frequenc... | 0.29 $ | 1000 | CRYSTAL 40.0000MHZ 10PF S... |
| 402F2701XIDR | CTS-Frequenc... | 0.29 $ | 1000 | CRYSTAL 27.0000MHZ 18PF S... |
| 402F20412IAR | CTS-Frequenc... | 0.29 $ | 1000 | CRYSTAL 20.4800MHZ 10PF S... |
| 402F40012ILR | CTS-Frequenc... | 0.29 $ | 1000 | CRYSTAL 40.0000MHZ 12PF S... |
| 402F3001XIAT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 30.0000MHZ 10PF S... |
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CRYSTAL 50.000 MHZ 8PF SMT50MHz 15ppm Cr...
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402F19211CAT Datasheet/PDF