
Allicdata Part #: | 416F25012CSR-ND |
Manufacturer Part#: |
416F25012CSR |
Price: | $ 0.33 |
Product Category: | Crystals, Oscillators, Resonators |
Manufacturer: | CTS-Frequency Controls |
Short Description: | CRYSTAL 25.000 MHZ SERIES SMT |
More Detail: | 25MHz ±10ppm Crystal Series 200 Ohms 4-SMD, No Lea... |
DataSheet: | ![]() |
Quantity: | 1000 |
3000 +: | $ 0.29780 |
Series: | 416 |
Packaging: | Tape & Reel (TR) |
Part Status: | Active |
Type: | MHz Crystal |
Frequency: | 25MHz |
Frequency Stability: | ±20ppm |
Frequency Tolerance: | ±10ppm |
Load Capacitance: | Series |
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 comprise the cornerstone of many electronic circuits, used in everything from wristwatches to cell phones and communications technology. The 416F25012CSR Crystal is one such component, and its wide range of applications and inner workings have made it indispensable to the modern world.In this article, we’ll take a look at the field of application and inner workings of the 416F25012CSR crystal.
The 416F25012CSR is a high-frequency crystal oscillator, making it ideal for general-purpose timing, frequency control and signal flow. One of the essential aspects of the 416F25012CSR is its resonator. This component give the crystal its unique characteristics, including its high frequency and outwardly smooth performance. It is composed of quartz and its main properties include temperature tolerance, precision and high frequency stability, making it suitable for a number of tasks.
The 416F25012CSR is most useful for applications that require consistent, high-precision timing. Its range of frequency spreads from 20 MHz up to 50 MHz, with exceptional stability and accuracy. Its range includes applications from 1080p and beyond, making it a versatile solution for digital products.
The working principle of the 416F25012CSR crystal is relatively straightforward. The oscillation frequency of this component is established through the physical characteristics of the quartz. This resonator is connected in parallel to a capacitor, with an external load on the other side. When a current is supplied, it causes the quartz to generate an electrical signal, which is then reflected in phase with the signal upon reaching the other end. Over time, this reflected signal aligns with the initial signal and the resonance is sustained, generating an oscillation frequency which is determined by the resonator’s physical characteristics.
The 416F25012CSR crystal is an indispensible component to any project that requires accurate timing. Its combination of a high-precision resonator and low-frequency capability makes it a go-to-solution for a wide range of tasks. A few of these tasks include radio and audio applications, phase-locked loops, microcontrollers and timing circuits.
The 416F25012CSR crystal is an especially attractive option for designers working in the audio/video and data communication fields, where the low profile and exceptional frequency stability of this component make it invaluable. Its wide range of frequency makes it suitable for almost any application, from digital to analog.
In conclusion, the 416F25012CSR is a crystal oscillator specifically designed for precision tasks, combining a range of high frequency stable operation and low frequency tolerance. The resonance created by the quartz resonator is the essential aspect of its working principle, making for a smooth and consistent frequency distribution. Its array of uses, from audio and video applications to microcontroller-based products and timing circuits, make it a highly desirable component for a variety of projects.
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416F40612CST | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 40.610 MHZ SERIES... |
416F44012ILT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 44.000 MHZ 12PF S... |
416F44012ITT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 44.000 MHZ 6PF SM... |
416F44025CST | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 44.000 MHZ SERIES... |
416F4801XALT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 48.000 MHZ 12PF S... |
416F48033AST | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 48.000 MHZ SERIES... |
416F480X3ALT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 48.000 MHZ 12PF S... |
416F52012IST | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 52.000 MHZ SERIES... |
416F52025CTT | CTS-Frequenc... | 0.0 $ | 1000 | CRYSTAL 52.000 MHZ 6PF SM... |
416F2501XCDR | CTS-Frequenc... | 0.33 $ | 1000 | CRYSTAL 25.000 MHZ 18PF S... |
416F25025AAR | CTS-Frequenc... | 0.33 $ | 1000 | CRYSTAL 25.000 MHZ 10PF S... |
416F250X3ASR | CTS-Frequenc... | 0.33 $ | 1000 | CRYSTAL 25.000 MHZ SERIES... |
416F26012CTR | CTS-Frequenc... | 0.33 $ | 1000 | CRYSTAL 26.000 MHZ 6PF SM... |
416F260XXCKR | CTS-Frequenc... | 0.33 $ | 1000 | CRYSTAL 26.000 MHZ 8PF SM... |
416F300X2ALR | CTS-Frequenc... | 0.33 $ | 1000 | CRYSTAL 30.000 MHZ 12PF S... |
416F36011CSR | CTS-Frequenc... | 0.33 $ | 1000 | CRYSTAL 36.000 MHZ SERIES... |
416F37012CTR | CTS-Frequenc... | 0.33 $ | 1000 | CRYSTAL 37.000 MHZ 6PF SM... |
416F37433CAR | CTS-Frequenc... | 0.33 $ | 1000 | CRYSTAL 37.400 MHZ 10PF S... |
416F374X3ALR | CTS-Frequenc... | 0.33 $ | 1000 | CRYSTAL 37.400 MHZ 12PF S... |
416F4001XCKR | CTS-Frequenc... | 0.33 $ | 1000 | CRYSTAL 40.000 MHZ 8PF SM... |
416F44012AAR | CTS-Frequenc... | 0.33 $ | 1000 | CRYSTAL 44.000 MHZ 10PF S... |
416F50033CAR | CTS-Frequenc... | 0.33 $ | 1000 | CRYSTAL 50.000 MHZ 10PF S... |
416F260X3IKR | CTS-Frequenc... | 0.34 $ | 1000 | CRYSTAL 26.000 MHZ 8PF SM... |
416F27013IKR | CTS-Frequenc... | 0.34 $ | 1000 | CRYSTAL 27.000 MHZ 8PF SM... |
416F27035IDR | CTS-Frequenc... | 0.34 $ | 1000 | CRYSTAL 27.000 MHZ 18PF S... |
416F27133ISR | CTS-Frequenc... | 0.34 $ | 1000 | CRYSTAL 27.120 MHZ SERIES... |
416F27133ITR | CTS-Frequenc... | 0.34 $ | 1000 | CRYSTAL 27.120 MHZ 6PF SM... |
416F37022IAR | CTS-Frequenc... | 0.34 $ | 1000 | CRYSTAL 37.000 MHZ 10PF S... |
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