![416F38022IAR Allicdata Electronics](https://files.allicdata.com/upload/common/default.jpg)
Allicdata Part #: | 416F38022IAR-ND |
Manufacturer Part#: |
416F38022IAR |
Price: | $ 0.34 |
Product Category: | Crystals, Oscillators, Resonators |
Manufacturer: | CTS-Frequency Controls |
Short Description: | CRYSTAL 38.000 MHZ 10PF SMT |
More Detail: | 38MHz ±20ppm Crystal 10pF 200 Ohms 4-SMD, No Lead |
DataSheet: | ![]() |
Quantity: | 1000 |
3000 +: | $ 0.30511 |
Series: | 416 |
Packaging: | Tape & Reel (TR) |
Part Status: | Active |
Type: | MHz Crystal |
Frequency: | 38MHz |
Frequency Stability: | ±20ppm |
Frequency Tolerance: | ±20ppm |
Load Capacitance: | 10pF |
ESR (Equivalent Series Resistance): | 200 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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Crystallography is a branch of physical chemistry that studies the structure and symmetry of crystals, enabling us to understand the atomic form of substances. The 416F38022IAR is an application of crystallography which is used in the study of a wide range of materials including glasses, ceramics, semiconductors and nanomaterials. This application can determine the optical, mechanical, electrical and thermal properties of these materials.
The 416F38022IAR is based on an x-ray diffraction technique. X-rays are a type of electromagnetic radiation which, when passed through a material, can detect the presence of regular arrangement of atoms which create patterns from the reflected radiation. The 416F38022IAR uses a rotating crystal as the window onto the atomic structure of the material. A goniometer rotates the crystal, changing the diffraction angle at which the reflected x-rays interact with the material. This angular movement of the crystal surface is measured by a detector, and the resulting data is used to form an image of the crystal lattice. This image then provides a detailed analysis of the material’s structure.
This method requires two components in order to work effectively: the goniometer and the detector. The goniometer is a device that is used to rotate the crystal sample. This rotation of the crystal causes the diffraction angle to change, which in turn affects the reflected x-rays. The detector is then used to measure the angular movement of the crystal and record the resulting data. The data is then used to form an image of the crystal lattice, providing a detailed analysis of the material’s structure.
The 416F38022IAR is a powerful tool for studying the structures and properties of a wide range of materials, from glasses and ceramics to semiconductors and nanomaterials. It is a valuable tool for materials scientists and engineers, enabling them to analyse the atomic structure of materials and gain a better understanding of the properties of these materials.
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Part Number | Manufacturer | Price | Quantity | Description |
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416F52022CKR | CTS-Frequenc... | 0.33 $ | 3000 | CRYSTAL 52.000 MHZ 8PF SM... |
416F26022IKR | CTS-Frequenc... | 0.34 $ | 12000 | CRYSTAL 26.000 MHZ 8PF SM... |
416F48022IKR | CTS-Frequenc... | 0.34 $ | 3000 | CRYSTAL 48.000 MHZ 8PF SM... |
416F52022IKR | CTS-Frequenc... | 0.34 $ | 3000 | CRYSTAL 52.000 MHZ 8PF SM... |
416F48022CKR | CTS-Frequenc... | 0.33 $ | 1000 | CRYSTAL 48.000 MHZ 8PF SM... |
416F32022IKR | CTS-Frequenc... | 0.34 $ | 1000 | CRYSTAL 32.000 MHZ 8PF SM... |
416F27022CKR | CTS-Frequenc... | 0.33 $ | 1000 | CRYSTAL 27.000 MHZ 8PF SM... |
416F30022CKR | CTS-Frequenc... | 0.33 $ | 1000 | CRYSTAL 30.000 MHZ 8PF SM... |
416F36022CKR | CTS-Frequenc... | 0.33 $ | 1000 | CRYSTAL 36.000 MHZ 8PF SM... |
416F40022CKR | CTS-Frequenc... | 0.33 $ | 1000 | CRYSTAL 40.000 MHZ 8PF SM... |
416F44022CKR | CTS-Frequenc... | 0.33 $ | 1000 | CRYSTAL 44.000 MHZ 8PF SM... |
416F36022IKR | CTS-Frequenc... | 0.34 $ | 1000 | CRYSTAL 36.000 MHZ 8PF SM... |
416F40022IKR | CTS-Frequenc... | 0.34 $ | 1000 | CRYSTAL 40.000 MHZ 8PF SM... |
416F24022IKR | CTS-Frequenc... | 0.34 $ | 1000 | CRYSTAL 24.000 MHZ 8PF SM... |
416F24011AAT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 24.000 MHZ 10PF S... |
416F24011ADT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 24.000 MHZ 18PF S... |
416F24011AKT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 24.000 MHZ 8PF SM... |
416F24011ALT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 24.000 MHZ 12PF S... |
416F24011AST | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 24.000 MHZ SERIES... |
416F24011ATT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 24.000 MHZ 6PF SM... |
416F24011CAT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 24.000 MHZ 10PF S... |
416F24011CDT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 24.000 MHZ 18PF S... |
416F24011CKT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 24.000 MHZ 8PF SM... |
416F24011CLT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 24.000 MHZ 12PF S... |
416F24011CST | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 24.000 MHZ SERIES... |
416F24011CTT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 24.000 MHZ 6PF SM... |
416F24012AAT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 24.000 MHZ 10PF S... |
416F24012ADT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 24.000 MHZ 18PF S... |
416F24012AKT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 24.000 MHZ 8PF SM... |
416F24012ALT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 24.000 MHZ 12PF S... |
416F24012AST | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 24.000 MHZ SERIES... |
416F24012ATT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 24.000 MHZ 6PF SM... |
416F24012CAT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 24.000 MHZ 10PF S... |
416F24012CDT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 24.000 MHZ 18PF S... |
416F24012CKT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 24.000 MHZ 8PF SM... |
416F24012CLT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 24.000 MHZ 12PF S... |
416F24012CST | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 24.000 MHZ SERIES... |
416F24012CTT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 24.000 MHZ 6PF SM... |
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