
Allicdata Part #: | 445A22G12M00000-ND |
Manufacturer Part#: |
445A22G12M00000 |
Price: | $ 0.37 |
Product Category: | Crystals, Oscillators, Resonators |
Manufacturer: | CTS-Frequency Controls |
Short Description: | CRYSTAL 12.0000MHZ 30PF SMD |
More Detail: | 12MHz ±20ppm Crystal 30pF 50 Ohms 2-SMD, No Lead |
DataSheet: | ![]() |
Quantity: | 1000 |
1000 +: | $ 0.34020 |
Series: | 445 |
Packaging: | Tape & Reel (TR) |
Part Status: | Active |
Type: | MHz Crystal |
Frequency: | 12MHz |
Frequency Stability: | ±20ppm |
Frequency Tolerance: | ±20ppm |
Load Capacitance: | 30pF |
ESR (Equivalent Series Resistance): | 50 Ohms |
Operating Mode: | Fundamental |
Operating Temperature: | -10°C ~ 60°C |
Ratings: | -- |
Mounting Type: | Surface Mount |
Package / Case: | 2-SMD, No Lead |
Size / Dimension: | 0.197" L x 0.126" W (5.00mm x 3.20mm) |
Height - Seated (Max): | 0.053" (1.35mm) |
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A crystal is a natural or an artificially created solid material that is composed of atoms in an orderly arrangement. The regular arrangement is atomic as well as molecular, and forms a repeating pattern that extends in three dimensions. Crystal structures are formed by the orderly organization of many ions, molecules, or atoms. Although there is a wide variety of crystal structures, the most common is called the cubic crystal structure.
445A22G12M00000 is one of the most advanced crystals for applications in a variety of fields. It has superb characteristics such as stability, reliable electrical performance, and high temperature operation. It exhibits excellent physical and chemical behavior, making it ideal for use in many different applications.
The 445A22G12M00000 crystal is commonly used in many different types of applications. It is often applied in communications systems, control systems, and embedded systems. It is used in circuits where both excellent frequency stability and very low power consumption is required. It is often used in frequency control and oscillator circuits, as well as voltage controlled oscillator (VCO) circuits.
The most important aspect of the 445A22G12M00000 crystal is its working principle. The crystal is made up of two transverse electrodes, which are separated by a piece of piezoelectric material. When a potential is applied between the two electrodes, the piezoelectric material induces an electric field, which causes the crystal to vibrate. This vibration is caused by the piezoelectric effect, where the crystal is subjected to mechanical stress.
As the crystal vibrates, it generates an electrical signal that is the same frequency as the original potential applied between the transverse electrodes. This frequency can be controlled by adjusting the potential applied to the electrodes, which results in an increase or decrease in the frequency of the electrical signal.
The 445A22G12M00000 crystal can be used in various applications due to its stability and reliability. It is commonly used in frequency control and oscillator circuits, as well as voltage controlled oscillator (VCO) circuits. It is often applied in communications systems, control systems, and embedded systems. It is also used in circuits in which low power consumption and excellent frequency stability are desired.
The working principle of the 445A22G12M00000 crystal is based on the piezoelectric effect. When a potential is applied between the two transverse electrodes, the piezoelectric material induces an electric field, which causes the crystal to vibrate. This vibration is then transformed into an electrical signal with a frequency that is the same as the original potential. The frequency of this electrical signal can be controlled by adjusting the potential applied to the transverse electrodes.
The 445A22G12M00000 crystal is an incredibly important feature in the current technological landscape. It is highly versatile, stable, and reliable, making it perfect for many different types of applications. It is commonly used in communications systems, control systems, and embedded systems, and is also used in oscillator and frequency control circuits. The working principle of the crystal is based on the piezoelectric effect, where mechanical stress causes the crystal to vibrate and generate an electrical signal that is the same frequency as the potential applied between the transverse electrodes.
The specific data is subject to PDF, and the above content is for reference
Part Number | Manufacturer | Price | Quantity | Description |
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445A35F25M00000 | CTS-Frequenc... | 0.27 $ | 1000 | CRYSTAL 25.0000MHZ 24PF S... |
445A22E14M31818 | CTS-Frequenc... | 0.37 $ | 1000 | CRYSTAL 14.31818MHZ 20PF ... |
445A22L20M00000 | CTS-Frequenc... | 0.37 $ | 1000 | CRYSTAL 20.0000MHZ 12PF S... |
445A25C20M00000 | CTS-Frequenc... | 0.37 $ | 1000 | CRYSTAL 20.0000MHZ 16PF S... |
445A25C24M57600 | CTS-Frequenc... | 0.37 $ | 1000 | CRYSTAL 24.5760MHZ 16PF S... |
445A32C24M57600 | CTS-Frequenc... | 0.37 $ | 1000 | CRYSTAL 24.5760MHZ 16PF S... |
445A32E30M00000 | CTS-Frequenc... | 0.37 $ | 1000 | CRYSTAL 30.0000MHZ 20PF S... |
445A22F30M00000 | CTS-Frequenc... | 0.37 $ | 1000 | CRYSTAL 30.0000MHZ 24PF S... |
445A2XC27M00000 | CTS-Frequenc... | 0.41 $ | 1000 | CRYSTAL 27.0000MHZ 16PF S... |
445A3XD24M57600 | CTS-Frequenc... | 0.41 $ | 1000 | CRYSTAL 24.5760MHZ 18PF S... |
445A31C24M00000 | CTS-Frequenc... | 0.43 $ | 1000 | CRYSTAL 24.0000MHZ 16PF S... |
445A23A20M00000 | CTS-Frequenc... | 0.37 $ | 1000 | CRYSTAL 20.0000MHZ 10PF S... |
445A2XA30M00000 | CTS-Frequenc... | 0.41 $ | 1000 | CRYSTAL 30.0000MHZ 10PF S... |
445A2XH20M00000 | CTS-Frequenc... | 0.41 $ | 1000 | CRYSTAL 20.0000MHZ 32PF S... |
445A31C24M57600 | CTS-Frequenc... | 0.43 $ | 1000 | CRYSTAL 24.5760MHZ 16PF S... |
445A31C27M00000 | CTS-Frequenc... | 0.43 $ | 1000 | CRYSTAL 27.0000MHZ 16PF S... |
445A31B25M00000 | CTS-Frequenc... | 0.43 $ | 1000 | CRYSTAL 25.0000MHZ 13PF S... |
445A35A12M00000 | CTS-Frequenc... | 0.27 $ | 1000 | CRYSTAL 12.0000MHZ 10PF S... |
445A22E24M57600 | CTS-Frequenc... | 0.37 $ | 1000 | CRYSTAL 24.5760MHZ 20PF S... |
445A25A24M57600 | CTS-Frequenc... | 0.37 $ | 1000 | CRYSTAL 24.5760MHZ 10PF S... |
445A32A20M00000 | CTS-Frequenc... | 0.37 $ | 1000 | CRYSTAL 20.0000MHZ 10PF S... |
445A32S30M00000 | CTS-Frequenc... | 0.37 $ | 1000 | CRYSTAL 30.0000MHZ SERIES... |
445A2XD30M00000 | CTS-Frequenc... | 0.41 $ | 1000 | CRYSTAL 30.0000MHZ 18PF S... |
445A31F30M00000 | CTS-Frequenc... | 0.43 $ | 1000 | CRYSTAL 30.0000MHZ 24PF S... |
445A33D24M57600 | CTS-Frequenc... | 0.27 $ | 1000 | CRYSTAL 24.5760MHZ 18PF S... |
445A33D30M00000 | CTS-Frequenc... | 0.27 $ | 1000 | CRYSTAL 30.0000MHZ 18PF S... |
445A35C14M31818 | CTS-Frequenc... | 0.27 $ | 1000 | CRYSTAL 14.31818MHZ 16PF ... |
445A35S16M00000 | CTS-Frequenc... | 0.27 $ | 1000 | CRYSTAL 16.0000MHZ SERIES... |
445A33C25M00000 | CTS-Frequenc... | 0.27 $ | 1000 | CRYSTAL 25.0000MHZ 16PF S... |
445A35H24M57600 | CTS-Frequenc... | 0.27 $ | 1000 | CRYSTAL 24.5760MHZ 32PF S... |
445A33F16M00000 | CTS-Frequenc... | 0.27 $ | 1000 | CRYSTAL 16.0000MHZ 24PF S... |
445A25D20M00000 | CTS-Frequenc... | 0.37 $ | 1000 | CRYSTAL 20.0000MHZ 18PF S... |
445A32C16M00000 | CTS-Frequenc... | 0.37 $ | 1000 | CRYSTAL 16.0000MHZ 16PF S... |
445A25J25M00000 | CTS-Frequenc... | 0.37 $ | 1000 | CRYSTAL 25.0000MHZ 9PF SM... |
445A32F24M00000 | CTS-Frequenc... | 0.37 $ | 1000 | CRYSTAL 24.0000MHZ 24PF S... |
445A22S25M00000 | CTS-Frequenc... | 0.37 $ | 1000 | CRYSTAL 25.0000MHZ SERIES... |
445A25L20M00000 | CTS-Frequenc... | 0.37 $ | 1000 | CRYSTAL 20.0000MHZ 12PF S... |
445A22C25M00000 | CTS-Frequenc... | 0.37 $ | 1000 | CRYSTAL 25.0000MHZ 16PF S... |
445A23B27M00000 | CTS-Frequenc... | 0.37 $ | 1000 | CRYSTAL 27.0000MHZ 13PF S... |
445A32G13M00000 | CTS-Frequenc... | 0.37 $ | 1000 | CRYSTAL 13.0000MHZ 30PF S... |
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