Allicdata Part #: | 490-6008-3-ND |
Manufacturer Part#: |
CSTLS8M00G56-A0 |
Price: | $ 0.08 |
Product Category: | Crystals, Oscillators, Resonators |
Manufacturer: | Murata Electronics North America |
Short Description: | CER RES 8.0000MHZ 47PF T/H |
More Detail: | 8MHz Ceramic Resonator Built in Capacitor 47pF -0.... |
DataSheet: | CSTLS8M00G56-A0 Datasheet/PDF |
Quantity: | 2000 |
2000 +: | $ 0.07318 |
4000 +: | $ 0.06861 |
6000 +: | $ 0.06632 |
10000 +: | $ 0.06403 |
Series: | CERALOCK® CSTLS |
Packaging: | Tape & Box (TB) |
Part Status: | Active |
Type: | Ceramic |
Frequency: | 8MHz |
Frequency Stability: | -0.4, +0.2% |
Frequency Tolerance: | ±0.5% |
Features: | Built in Capacitor |
Capacitance: | 47pF |
Impedance: | 25 Ohms |
Operating Temperature: | -20°C ~ 80°C |
Mounting Type: | Through Hole |
Package / Case: | Radial - 3 Lead, 2.50mm Pitch |
Size / Dimension: | 0.315" L x 0.118" W (8.00mm x 3.00mm) |
Height: | 0.236" (6.00mm) |
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Resonators are essential components in many systems, and a variety of resonators that use different physical processes can be used, depending on the system’s requirements. Among these resonators, the CSTLS8M00G56-A0 is a type of quartz crystal resonator with a miniature size, low power consumption and excellent electrical performance. This article will discuss the application field and working principle of CSTLS8M00G56-A0.
The CSTLS8M00G56-A0 is generally used in low-power communication systems, such as wireless remote control systems, radio frequency data receivers, TV signals reception systems, etc. It has good frequency stability and temperature compensation characteristics, and is suitable for the harsh environment of high-temperature and low-temperature. Moreover, its wide frequency range of 1-12MHz allows it to be used in various applications.
The CSTLS8M00G56-A0 comprises of two metal plates made of silicon and two metal plates made of steel. The two metal plates can move by applying an electrical field to the quartz crystal. The two metal plates are positioned on opposite sides of the quartz crystal plate, creating a “sandwich” of metal plates. When a voltage is applied, the electrical field will cause the metal plates to move relative to each other. This movement creates a frequency-dependent change in the physical properties of the crystal and this frequency is called the resonant frequency of the resonator.
The frequency of the resonator is determined by the physical characteristics of the quartz crystal, such as its size, shape and composition. The size, shape and composition of the quartz crystal affect the electrical field applied to it and this determines the resonant frequency. As the frequency of the resonator changes, the capacitance of the metal plates changes and this is what determines the frequency of the output signal.
The working principle of the CSTLS8M00G56-A0 is further explained by its electrical equivalent circuit, which is shown in the diagram. The quartz crystal is represented by a series capacitor and inductor. When an AC voltage is applied across the terminals, the two metal plates will start to move, resulting in a change of the series capacitor and inductor values. This variation in the electrical properties produces a frequency dependent change in the output frequency and this is how the resonator produces its output signal.
In conclusion, the CSTLS8M00G56-A0 quartz crystal resonator has a wide frequency range and excellent electrical performance, making it suitable for low-power communication systems. Its working principle is based on the fluctuation of the electrical properties of the quartz crystal when an AC voltage is applied across the terminals. All these factors make the CSTLS8M00G56-A0 an ideal resonator for many applications.
The specific data is subject to PDF, and the above content is for reference
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CSTLS8M00G53-B0 | Murata Elect... | -- | 8246 | CER RES 8.0000MHZ 15PF T/... |
CSTLS6M00G53-B0 | Murata Elect... | 0.15 $ | 2816 | CER RES 6.0000MHZ 15PF T/... |
CSTLS10M0G53-B0 | Murata Elect... | -- | 5483 | CER RES 10.0000MHZ 15PF T... |
CSTLS20M0X53-A0 | Murata Elect... | 0.17 $ | 2000 | CER RES 20.0000MHZ 15PF T... |
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CSTLS16M0X53-B0 | Murata Elect... | -- | 1701 | CER RES 16.0000MHZ 15PF T... |
CSTLS20M0X53-B0 | Murata Elect... | 0.32 $ | 3240 | CER RES 20.0000MHZ 15PF T... |
CSTLS8M00G56-A0 | Murata Elect... | 0.08 $ | 2000 | CER RES 8.0000MHZ 47PF T/... |
CSTLS4M91G53-A0 | Murata Elect... | 0.08 $ | 2000 | CER RES 4.9150MHZ 15PF T/... |
CSTLS7M16G53-A0 | Murata Elect... | 0.09 $ | 2000 | CER RES 7.16000MHZ 15PF T... |
CSTLS7M20G53-A0 | Murata Elect... | 0.09 $ | 2000 | CER RES 7.2000MHZ 15PF T/... |
CSTLS4M00G56-B0 | Murata Elect... | 0.15 $ | 2649 | CER RES 4.0000MHZ 47PF T/... |
CSTLS16M0X55-A0 | Murata Elect... | 0.15 $ | 2000 | CER RES 16.0000MHZ 30PF T... |
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CSTLS10M0G56-A0 | Murata Elect... | 0.08 $ | 1000 | CER RES 10.0000MHZ 47PF T... |
CSTLS4M00G56Z-A0 | Murata Elect... | 0.09 $ | 2000 | CER RES 4.0000MHZ 47PF T/... |
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CSTLS8M00G53Z-A0 | Murata Elect... | 0.09 $ | 1000 | CER RES 8.0000MHZ 15PF T/... |
CSTLS16M0X51-A0 | Murata Elect... | -- | 1000 | CER RES 16.0000MHZ 5PF T/... |
CSTLS8M00G56-B0 | Murata Elect... | -- | 650 | CER RES 8.0000MHZ 47PF T/... |
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