595BG491M520DG

Frequency Stability:	±50ppm
Current - Supply (Disable) (Max):	75mA
Height - Seated (Max):	0.071" (1.80mm)
Size / Dimension:	0.276" L x 0.197" W (7.00mm x 5.00mm)
Package / Case:	6-SMD, No Lead
Mounting Type:	Surface Mount
Ratings:	--
Current - Supply (Max):	110mA
Operating Temperature:	-40°C ~ 85°C
Absolute Pull Range (APR):	±35ppm
Series:	Si595
Voltage - Supply:	3.3V
Output:	LVDS
Function:	Enable/Disable
Frequency:	491.52MHz
Type:	VCXO
Base Resonator:	Crystal
Part Status:	Active
Packaging:	Strip

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Oscillators Oscillators are regularly used in electronic systems to generate periodic electronic signals. These signals can either be used directly for communication, like a clock signal, or used to modulate signals for transmission. One such type of oscillator is the 595BG491M520DG oscillator, which is a very versatile oscillator with a wide array of application fields. The 595BG491M520DG oscillator is based on a bipolar quantum tunneling transistor. This transistor is able to take an input voltage within a certain range and generate a square wave output that is much higher in frequency. This output can then be further processed and adjusted by changing the capacitance, resistance, or mass of the transistor. The main application field of the 595BG491M520DG oscillator is communication, particularly for short range and long-range radio signals. It is an extremely efficient system due to the low power consumption and the high fidelity of its output. The 595BG491M520DG oscillator can also be used in pulsed laser systems, radar systems, and optical systems, due to its wide range of adjustable features. The working principle behind a 595BG491M520DG oscillator is based on the fact that it is a bipolar quantum tunneling transistor. As the transistor is biased, two quantum wells are created in each of its terminals. When a voltage is applied to the quantum wells, the trapped electric charges jump across them and generate electrical current. This current then goes through the collector and the emitter. The frequency of the output signal then corresponds with the voltage applied to the quantum wells. The frequency of the 595BG491M520DG oscillator can be further adjusted by changing the capacitance, resistance, or mass of the transistor. By changing these values, the operating frequency of the transistor is shifted, which in turn changes the frequency of the output signal. These are just a few of the many applications and principles behind the 595BG491M520DG oscillator. With its wide range of features, it is an excellent choice for many types of communication, and its low power consumption makes it ideal for long-range radio signals. Additionally, the adjustable features of the 595BG491M520DG allow it to be used in pulsed laser systems, radar systems, and optical systems.

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