| Allicdata Part #: | 416F48023IDT-ND |
| Manufacturer Part#: |
416F48023IDT |
| Price: | $ 0.00 |
| Product Category: | Crystals, Oscillators, Resonators |
| Manufacturer: | CTS-Frequency Controls |
| Short Description: | CRYSTAL 48.000 MHZ 18PF SMT |
| More Detail: | 48MHz ±20ppm Crystal 18pF 100 Ohms 4-SMD, No Lead |
| DataSheet: | 416F48023IDT Datasheet/PDF |
| Quantity: | 1000 |
| 0 +: | $ 0.00000 |
| Series: | 416 |
| Packaging: | Tape & Reel (TR) |
| Part Status: | Discontinued at Digi-Key |
| Type: | MHz Crystal |
| Frequency: | 48MHz |
| Frequency Stability: | ±30ppm |
| Frequency Tolerance: | ±20ppm |
| Load Capacitance: | 18pF |
| 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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In the field of crystals, 416F48023IDT is recognized as a technologically advanced initiator with the capability to produce larger and more powerful crystals than the predecessor. Its innovation relies on the principle of nucleation, which is based on the decision of the crystal\'s orientation. In order to make a crystal grow, it has to be perfectly oriented. This is because the crystalline structure of the crystal is its basis system. With so many configurations, scientists were able to design the crystal\'s orientation and dictate the properties.
The 416F48023IDT is a generator which produces high-voltage alternating fields to stimulate the nucleation of crystals. This technology allows the crystal nucleation act in a rapid manner rather than the spread. The alternating field causes the ions of the crystal lattice to become similarly arranged, known as crystallization. This happens due to the theory that atoms in lattices tend to mimic each other, which then allows the bonding points between them to become well ordered. This process results in a larger crystal than the previous one as crystals grow quickly when they have sufficient space to grow and few obstacles in the face of them.
The 416F48023IDT also works on the basis of electrostatic attraction. This works when an already existing particle and the particles which are produced by the 416F48023IDT come into contact. The existing particle has an existing electrical boundary and when the other particles are brought within the boundary of the existing particle, the electrostatic attraction takes place. As the particles drawn within the boundary become attached, the size of the crystal multiplies. The multiple particles act as if they are connected in a lattice, enabling the crystal to grow quickly and steadily.
The 416F48023IDT also works on a thermodynamic basis. As the crystals are subjected to the alternating fields, their temperature can be regulated. While the temperature increases, the ions in the crystal lattice can disperse, resulting in the accumulation of heat. This can help the crystals to create much faster and in large sizes than the ones which are generated without thermodynamic regulation. For crystals to grow to large sizes, the temperature needs to be just right, as wrong temperatures can cause the crystals to deteriorate.
To summarize, the working principle of the 416F48023IDT is based on the principle of nucleation, electrostatic attraction and thermodynamic regulation. This technology is used to produce larger and more powerful crystals than periodic lattices and has found applications in numerous industries, such as electronics, communication and aerospace. The 416F48023IDT can be used to produce scale sized crystals and large custom-shaped crystals. In addition, the 416F48023IDT has a high voltage breakdown and can reach temperatures higher than any other initiator in the market.
The specific data is subject to PDF, and the above content is for reference
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| 416F36035ASR | CTS-Frequenc... | 0.33 $ | 1000 | CRYSTAL 36.000 MHZ SERIES... |
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| 416F480X3CKR | CTS-Frequenc... | 0.33 $ | 1000 | CRYSTAL 48.000 MHZ 8PF SM... |
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| 416F50033CTR | CTS-Frequenc... | 0.33 $ | 1000 | CRYSTAL 50.000 MHZ 6PF SM... |
| 416F500XXCLR | CTS-Frequenc... | 0.33 $ | 1000 | CRYSTAL 50.000 MHZ 12PF S... |
| 416F52022ALR | CTS-Frequenc... | 0.33 $ | 1000 | CRYSTAL 52.000 MHZ 12PF S... |
| 416F27023IDR | CTS-Frequenc... | 0.34 $ | 1000 | CRYSTAL 27.000 MHZ 18PF S... |
| 416F270X3ITR | CTS-Frequenc... | 0.34 $ | 1000 | CRYSTAL 27.000 MHZ 6PF SM... |
| 416F271X3ISR | CTS-Frequenc... | 0.34 $ | 1000 | CRYSTAL 27.120 MHZ SERIES... |
| 416F30035ILR | CTS-Frequenc... | 0.34 $ | 1000 | CRYSTAL 30.000 MHZ 12PF S... |
| 416F300X3ITR | CTS-Frequenc... | 0.34 $ | 1000 | CRYSTAL 30.000 MHZ 6PF SM... |
| 416F36012ILR | CTS-Frequenc... | 0.34 $ | 1000 | CRYSTAL 36.000 MHZ 12PF S... |
| 416F36025ILR | CTS-Frequenc... | 0.34 $ | 1000 | CRYSTAL 36.000 MHZ 12PF S... |
| 416F37013IDR | CTS-Frequenc... | 0.34 $ | 1000 | CRYSTAL 37.000 MHZ 18PF S... |
| 416F370X2ISR | CTS-Frequenc... | 0.34 $ | 1000 | CRYSTAL 37.000 MHZ SERIES... |
| 416F50012IAR | CTS-Frequenc... | 0.34 $ | 1000 | CRYSTAL 50.000 MHZ 10PF S... |
| 416F50012IDR | CTS-Frequenc... | 0.34 $ | 1000 | CRYSTAL 50.000 MHZ 18PF S... |
| 416F2401XAAT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 24.000 MHZ 10PF S... |
| 416F270X2AAT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 27.000 MHZ 10PF S... |
| 416F30023IKT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 30.000 MHZ 8PF SM... |
| 416F30033CLT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 30.000 MHZ 12PF S... |
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416F48023IDT Datasheet/PDF