| Allicdata Part #: | 416F32013CDR-ND |
| Manufacturer Part#: |
416F32013CDR |
| Price: | $ 0.33 |
| Product Category: | Crystals, Oscillators, Resonators |
| Manufacturer: | CTS-Frequency Controls |
| Short Description: | CRYSTAL 32.000 MHZ 18PF SMT |
| More Detail: | 32MHz ±10ppm Crystal 18pF 200 Ohms 4-SMD, No Lead |
| DataSheet: | 416F32013CDR Datasheet/PDF |
| Quantity: | 1000 |
| 3000 +: | $ 0.29780 |
| Series: | 416 |
| Packaging: | Tape & Reel (TR) |
| Part Status: | Active |
| Type: | MHz Crystal |
| Frequency: | 32MHz |
| Frequency Stability: | ±30ppm |
| Frequency Tolerance: | ±10ppm |
| Load Capacitance: | 18pF |
| ESR (Equivalent Series Resistance): | 200 Ohms |
| Operating Mode: | Fundamental |
| Operating Temperature: | -20°C ~ 70°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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Crystals
Crystals, like other materials, are not uniform throughout, they consist of different metals, minerals and oxides. The main purpose of using crystals is to convert and store energy, as well as to amplify and filter electric and radio signals and frequencies. Crystals are also used in both precision and industrial applications.
416F32013CDR Application Field and Working Principle
416F32013CDR, also known as ultra thin crystal resonator, are designed for telecommunication, computing and general electronic circuits applications. It is an extremely thin crystal resonator that’s usually used together with an oscillator or resonator.
The working principle of 416F32013CDR is based on the piezoelectric effect; which states that when a crystal is subjected to an electric field, it produces a mechanical stress and when the crystal is put under mechanical stress, it produces an electric field. This effect can be used for the generation, transmission, and reception of sound, radio or power.
Since the 416F32013CDR is an ultra thin crystal resonator, it can be used in applications that require high precision because it has high stability in frequency as low as 10Hz and has low equivalent parallel capacitance between pins. It is also used for many other applications such as rotational speed detectors and acoustic sensors.
The 416F32013CDR is also capable of producing low losses at higher frequencies, it is ultra thin therefore it can fit inside the circuit board with less space, and it is also very compact in size and resilient to external factors such as shock, temperature, vibration and other elements.
Overall, the 416F32013CDR is an ultra thin crystal resonator that’s used in many applications ranging from precision instruments to industrial devices. It is used to convert and store energy, amplify and filter electric and radio signals and frequencies, and other applications such as rotational speed detectors and acoustic sensors. It is also known for its high precision and stability, as well as its low losses at higher frequencies.
The specific data is subject to PDF, and the above content is for reference
| Part Number | Manufacturer | Price | Quantity | Description |
|---|
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| 416F300X3AAR | CTS-Frequenc... | 0.33 $ | 1000 | CRYSTAL 30.000 MHZ 10PF S... |
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| 416F36012CSR | CTS-Frequenc... | 0.33 $ | 1000 | CRYSTAL 36.000 MHZ SERIES... |
| 416F36022ALR | CTS-Frequenc... | 0.33 $ | 1000 | CRYSTAL 36.000 MHZ 12PF S... |
| 416F36035ADR | CTS-Frequenc... | 0.33 $ | 1000 | CRYSTAL 36.000 MHZ 18PF S... |
| 416F360X3CLR | CTS-Frequenc... | 0.33 $ | 1000 | CRYSTAL 36.000 MHZ 12PF S... |
| 416F37022ADR | CTS-Frequenc... | 0.33 $ | 1000 | CRYSTAL 37.000 MHZ 18PF S... |
| 416F37022AKR | CTS-Frequenc... | 0.33 $ | 1000 | CRYSTAL 37.000 MHZ 8PF SM... |
| 416F374XXADR | CTS-Frequenc... | 0.33 $ | 1000 | CRYSTAL 37.400 MHZ 18PF S... |
| 416F38422ALR | CTS-Frequenc... | 0.33 $ | 1000 | CRYSTAL 38.400 MHZ 12PF S... |
| 416F40612CLR | CTS-Frequenc... | 0.33 $ | 1000 | CRYSTAL 40.610 MHZ 12PF S... |
| 416F4061XCLR | CTS-Frequenc... | 0.33 $ | 1000 | CRYSTAL 40.610 MHZ 12PF S... |
| 416F406X3ADR | CTS-Frequenc... | 0.33 $ | 1000 | CRYSTAL 40.610 MHZ 18PF S... |
| 416F520X3CSR | CTS-Frequenc... | 0.33 $ | 1000 | CRYSTAL 52.000 MHZ SERIES... |
| 416F30035ISR | CTS-Frequenc... | 0.34 $ | 1000 | CRYSTAL 30.000 MHZ SERIES... |
| 416F384X3ILR | CTS-Frequenc... | 0.34 $ | 1000 | CRYSTAL 38.400 MHZ 12PF S... |
| 416F40022ISR | CTS-Frequenc... | 0.34 $ | 1000 | CRYSTAL 40.000 MHZ SERIES... |
| 416F2601XALT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 26.000 MHZ 12PF S... |
| 416F26022ATT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 26.000 MHZ 6PF SM... |
| 416F27012ILT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 27.000 MHZ 12PF S... |
| 416F27033AAT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 27.000 MHZ 10PF S... |
| 416F30011CLT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 30.000 MHZ 12PF S... |
| 416F300X2ILT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 30.000 MHZ 12PF S... |
| 416F320X2AST | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 32.000 MHZ SERIES... |
| 416F320XXCAT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 32.000 MHZ 10PF S... |
| 416F36022AST | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 36.000 MHZ SERIES... |
| 416F370X2ADT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 37.000 MHZ 18PF S... |
| 416F3841XAKT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 38.400 MHZ 8PF SM... |
| 416F384X3AKT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 38.400 MHZ 8PF SM... |
| 416F40023IKT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 40.000 MHZ 8PF SM... |
| 416F400X2CST | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 40.000 MHZ SERIES... |
| 416F4401XAKT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 44.000 MHZ 8PF SM... |
| 416F44023ILT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 44.000 MHZ 12PF S... |
| 416F44025AAT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 44.000 MHZ 10PF S... |
| 416F440X2CST | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 44.000 MHZ SERIES... |
| 416F4801XCAT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 48.000 MHZ 10PF S... |
| 416F48023IAT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 48.000 MHZ 10PF S... |
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416F32013CDR Datasheet/PDF