Allicdata Part #: | 445A31E12M00000-ND |
Manufacturer Part#: |
445A31E12M00000 |
Price: | $ 0.43 |
Product Category: | Crystals, Oscillators, Resonators |
Manufacturer: | CTS-Frequency Controls |
Short Description: | CRYSTAL 12.0000MHZ 20PF SMD |
More Detail: | 12MHz ±30ppm Crystal 20pF 50 Ohms 2-SMD, No Lead |
DataSheet: | 445A31E12M00000 Datasheet/PDF |
Quantity: | 1000 |
1000 +: | $ 0.39336 |
Series: | 445 |
Packaging: | Tape & Reel (TR) |
Part Status: | Active |
Type: | MHz Crystal |
Frequency: | 12MHz |
Frequency Stability: | ±10ppm |
Frequency Tolerance: | ±30ppm |
Load Capacitance: | 20pF |
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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Crystals are one of the oldest and most versatile materials that have been used for centuries, ranging from jewelry to watches to advanced electronics. One of the more intriguing crystal structures is the "445A31E12M00000," which is a type of dielectric material commonly used in the electronics industry. This article will examine the application field and working principle of this type of crystal.
The 445A31E12M00000 crystal is a ceramic material primarily composed of titanium dioxide (TiO2). In its raw form, it appears as a white powder. Under proper processing conditions, it can be heat treated and crystallized into hafnium oxide (HfO2) with near-perfect crystallinity. The resulting material has excellent electrical insulation qualities, making it highly suitable for passive electronic components such as capacitors, resistors, and diodes.
The 445A31E12M00000 crystal structure exhibits several properties that make it particularly attractive for use in electronic applications. First, its dielectric constant – the measure of how much an applied electrical field affects its electrical properties – is exceptionally high, giving it excellent insulation properties. Second, its dissipation factor – the measure of how much energy is dissipated in the form of heat when an AC current passes through it – is extremely low, making it ideal for use in circuits that require precise electrical signals to pass through them with minimal distortion. Finally, its dielectric strength – the measure of its ability to withstand electrical breakdown – is extremely high, making it resistant to short circuits and other sources of electrical stress.
One of the primary application fields of the 445A31E12M00000 crystal structure is in capacitors. Because of its high dielectric constant, low dissipation factor, and high dielectric strength, this type of crystal can store energy in electric fields to a very high degree. This makes it highly suitable for use in components such as multi-layer capacitors, which can store and release electric energy as needed for various applications. The 445A31E12M00000 also finds use in high-frequency communication systems, such as mobile phones and radios, because of its superior electrical insulation properties.
The working principle of the 445A31E12M00000 crystal is based on the flow of electrical charge through it. When an electrical potential is applied to the crystal, free electrons begin to move within the crystal along with their associated charge, causing a decrease in the number of electric charges on the surface of the crystal. This movement of electrons is known as the electric field effect. The resulting change in electric potential causes a decrease in the overall dielectric strength of the crystal, allowing electric current to pass through it. This current flow can be used to power electronic devices or convert electrical energy into useful forms.
In summary, the 445A31E12M00000 crystal structure is a type of dielectric ceramic material characterized by its high dielectric constant, low dissipation factor, and high dielectric strength. It is widely used in the electronics industry for passive components such as capacitors, resistors, and diodes, as well as for high-frequency communication systems. Its working principle is based on the electric field effect, which enables it to store and convert electric energy into useful forms.
The specific data is subject to PDF, and the above content is for reference
Part Number | Manufacturer | Price | Quantity | Description |
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445A33G16M00000 | CTS-Frequenc... | 0.27 $ | 1000 | CRYSTAL 16.0000MHZ 30PF S... |
445A33H13M00000 | CTS-Frequenc... | 0.27 $ | 1000 | CRYSTAL 13.0000MHZ 32PF S... |
445A33H16M00000 | CTS-Frequenc... | 0.27 $ | 1000 | CRYSTAL 16.0000MHZ 32PF S... |
445A33J13M00000 | CTS-Frequenc... | 0.27 $ | 1000 | CRYSTAL 13.0000MHZ 9PF SM... |
445A33J16M00000 | CTS-Frequenc... | 0.27 $ | 1000 | CRYSTAL 16.0000MHZ 9PF SM... |
445A35B13M00000 | CTS-Frequenc... | 0.27 $ | 1000 | CRYSTAL 13.0000MHZ 13PF S... |
445A35B16M00000 | CTS-Frequenc... | 0.27 $ | 1000 | CRYSTAL 16.0000MHZ 13PF S... |
445A35F13M00000 | CTS-Frequenc... | 0.27 $ | 1000 | CRYSTAL 13.0000MHZ 24PF S... |
445A35F16M00000 | CTS-Frequenc... | 0.27 $ | 1000 | CRYSTAL 16.0000MHZ 24PF S... |
445A35G13M00000 | CTS-Frequenc... | 0.27 $ | 1000 | CRYSTAL 13.0000MHZ 30PF S... |
445A35G16M00000 | CTS-Frequenc... | 0.27 $ | 1000 | CRYSTAL 16.0000MHZ 30PF S... |
445A35H13M00000 | CTS-Frequenc... | 0.27 $ | 1000 | CRYSTAL 13.0000MHZ 32PF S... |
445A35H16M00000 | CTS-Frequenc... | 0.27 $ | 1000 | CRYSTAL 16.0000MHZ 32PF S... |
445A35J13M00000 | CTS-Frequenc... | 0.27 $ | 1000 | CRYSTAL 13.0000MHZ 9PF SM... |
445A35J16M00000 | CTS-Frequenc... | 0.27 $ | 1000 | CRYSTAL 16.0000MHZ 9PF SM... |
445A33S12M00000 | CTS-Frequenc... | 0.27 $ | 1000 | CRYSTAL 12.0000MHZ SERIES... |
445A33A12M00000 | CTS-Frequenc... | 0.27 $ | 1000 | CRYSTAL 12.0000MHZ 10PF S... |
445A33D12M00000 | CTS-Frequenc... | 0.27 $ | 1000 | CRYSTAL 12.0000MHZ 18PF S... |
445A33E12M00000 | CTS-Frequenc... | 0.27 $ | 1000 | CRYSTAL 12.0000MHZ 20PF S... |
445A33K12M00000 | CTS-Frequenc... | 0.27 $ | 1000 | CRYSTAL 12.0000MHZ 8PF SM... |
445A33L12M00000 | CTS-Frequenc... | 0.27 $ | 1000 | CRYSTAL 12.0000MHZ 12PF S... |
445A33C12M00000 | CTS-Frequenc... | 0.27 $ | 1000 | CRYSTAL 12.0000MHZ 16PF S... |
445A33S13M00000 | CTS-Frequenc... | 0.27 $ | 1000 | CRYSTAL 13.0000MHZ SERIES... |
445A33A13M00000 | CTS-Frequenc... | 0.27 $ | 1000 | CRYSTAL 13.0000MHZ 10PF S... |
445A33D13M00000 | CTS-Frequenc... | 0.27 $ | 1000 | CRYSTAL 13.0000MHZ 18PF S... |
445A33E13M00000 | CTS-Frequenc... | 0.27 $ | 1000 | CRYSTAL 13.0000MHZ 20PF S... |
445A33K13M00000 | CTS-Frequenc... | 0.27 $ | 1000 | CRYSTAL 13.0000MHZ 8PF SM... |
445A33L13M00000 | CTS-Frequenc... | 0.27 $ | 1000 | CRYSTAL 13.0000MHZ 12PF S... |
445A33C13M00000 | CTS-Frequenc... | 0.27 $ | 1000 | CRYSTAL 13.0000MHZ 16PF S... |
445A33S14M31818 | CTS-Frequenc... | 0.27 $ | 1000 | CRYSTAL 14.31818MHZ SERIE... |
445A33A14M31818 | CTS-Frequenc... | 0.27 $ | 1000 | CRYSTAL 14.31818MHZ 10PF ... |
445A33D14M31818 | CTS-Frequenc... | 0.27 $ | 1000 | CRYSTAL 14.31818MHZ 18PF ... |
445A33E14M31818 | CTS-Frequenc... | 0.27 $ | 1000 | CRYSTAL 14.31818MHZ 20PF ... |
445A33K14M31818 | CTS-Frequenc... | 0.27 $ | 1000 | CRYSTAL 14.31818MHZ 8PF S... |
445A33L14M31818 | CTS-Frequenc... | 0.27 $ | 1000 | CRYSTAL 14.31818MHZ 12PF ... |
445A33C14M31818 | CTS-Frequenc... | 0.27 $ | 1000 | CRYSTAL 14.31818MHZ 16PF ... |
445A33S16M00000 | CTS-Frequenc... | 0.27 $ | 1000 | CRYSTAL 16.0000MHZ SERIES... |
445A33A16M00000 | CTS-Frequenc... | 0.27 $ | 1000 | CRYSTAL 16.0000MHZ 10PF S... |
445A33D16M00000 | CTS-Frequenc... | 0.27 $ | 1000 | CRYSTAL 16.0000MHZ 18PF S... |
445A33E16M00000 | CTS-Frequenc... | 0.27 $ | 1000 | CRYSTAL 16.0000MHZ 20PF S... |
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