CX2520DB25000D0FLJC1

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Crystals are fundamental to many technologies, from high-precision time keeping to high-speed communication and data transmission. The CX2520DB25000D0FLJC1 is an example of a quartz crystal oscillator that is used in a wide range of applications. In this article, we will discuss the application fields and working principles of the CX2520DB25000D0FLJC1.

Application Field of CX2520DB25000D0FLJC1

The CX2520DB25000D0FLJC1 is a high-stability electrode-driven quartz crystal oscillator, which is specifically designed to provide reliable high frequency operation in a wide range of applications. It is ideal for use in communications, computer, consumer, and industrial applications where accuracy and stability are of critical importance. The device offers a high stability in both temperature and aging, with a temperature stability of ±1 ppm and an aging rate of ±0.2 ppm/year. In addition, it has a wide operating temperature range from -20 to +85 ℃.

The CX2520DB25000D0FLJC1 can be used in RF applications such as cellular base stations, Wi-Fi networks, and GPS for stabilizing signal timing. It is also commonly used in computers, data systems, and consumer applications such as Blu-ray players, TV tuners, and audio systems for providing the stable frequencies required for their operation. In addition, it is an ideal solution for medical and industrial applications due to its reliable performance and wide temperature range.

Working Principle of CX2520DB25000D0FLJC1

The CX2520DB25000D0FLJC1 utilizes a quartz crystal as its resonator. It works due to the piezoelectric effect, which is the ability of certain materials to generate a voltage when they are deformed by mechanical stress. Quartz crystals are composed of some of the most piezoelectrically active materials and can be made to vibrate at a precise frequency when an electrical voltage is applied across the crystal.

The CX2520DB25000D0FLJC1 operates by applying a small voltage to the electrodes attached to the quartz crystal resonator. The voltage is then converted into mechanical stress which causes the crystal to vibrate at its natural frequency. The cr

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