Allicdata Part #: | 633L15366A2T-ND |
Manufacturer Part#: |
633L15366A2T |
Price: | $ 2.36 |
Product Category: | Crystals, Oscillators, Resonators |
Manufacturer: | CTS-Frequency Controls |
Short Description: | OSC XO 153.6000MHZ LVDS SMD |
More Detail: | 153.6MHz XO (Standard) LVDS Oscillator 2.5V Enable... |
DataSheet: | 633L15366A2T Datasheet/PDF |
Quantity: | 1000 |
1000 +: | $ 2.12324 |
Frequency Stability: | ±20ppm |
Current - Supply (Disable) (Max): | -- |
Height - Seated (Max): | 0.039" (1.00mm) |
Size / Dimension: | 0.126" L x 0.098" W (3.20mm x 2.50mm) |
Package / Case: | 6-SMD, No Lead |
Mounting Type: | Surface Mount |
Ratings: | -- |
Current - Supply (Max): | 66mA |
Operating Temperature: | -10°C ~ 60°C |
Series: | 633 |
Voltage - Supply: | 2.5V |
Output: | LVDS |
Function: | Enable/Disable |
Frequency: | 153.6MHz |
Type: | XO (Standard) |
Base Resonator: | Crystal |
Part Status: | Active |
Packaging: | Tape & Reel (TR) |
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Oscillators have a wide variety of applications and 633L15366A2T is no exception. It is an oscillator that is known primarily for its low operating voltage, wide temperature range, low noise output, and low consumer current. This makes it attractive for applications in a variety of industries where low-power, high-performance oscillators are important, such as automotive and consumer electronics. In this article, we will discuss the application fields and working principle of 633L15366A2T oscillator.
One of the primary applications of the 633L15366A2T oscillator is in precision clock sources. It is typically used for timing signals in a wide range of applications including consumer electronics, automotive systems, medical devices, and aerospace components. As its core feature, the 633L15366A2T oscillator has a very low-power consumption which allows it to work with devices that require a high level of precision without draining too much power. With its low consumer current, it can deliver accurate timing signals to precision instruments for measurements and calibration.
In addition to its use as a precision clock source, 633L15366A2T can be used in other applications such as data communications, signal processing, and RF/wireless systems. With its wide frequency range and high frequency accuracy, it is ideal for these types of applications as it can accurately process data and signals without too much deviation or interference from external sources. It can also be used for high-speed data transmission and bidirectional communication. Its wide temperature range also makes it a great choice for applications where changes in temperature and environmental conditions may affect performance.
The working principle of the 633L15366A2T oscillator can be broadly described as a type of electro-mechanical oscillator. This type of timestep oscillator uses a combination of a piezoelectric crystal and an electrostatically charged magnetic field to create a pulse at a set frequency. This pulse is then fed into a counter which is used to measure the time period of the pulse. The counter is then used to determine the frequency of the pulse and in turn the timing of the oscillator.
At the heart of the 633L15366A2T oscillator is a quartz crystal which creates a vibration when an electric field is applied to it. This oscillation is then coupled to the counter which can accurately measure the frequency of the pulse. The usefulness of 633L15366A2T oscillator in precision clock sources is determined by the accuracy of the pulse and the counter. This accuracy is around 1 microsecond in the case of the 633L15366A2T oscillator, making it a dependable and precise source for timing applications.
In summary, the 633L15366A2T oscillator is an important component in a wide range of industries where low-power, high-performance oscillators are important. It is used mainly in precision clock sources and for other applications such as data communications, signal processing, and RF/wireless systems. Its working principle, as a type of electro-mechanical oscillator, involves a combination of a piezoelectric crystal and an electrostatically charged magnetic field to create a pulse at a set frequency. This pulse is then sent to a counter to measure the frequency of the pulse and in turn the timing of the oscillator.
The specific data is subject to PDF, and the above content is for reference
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