Allicdata Part #: | LP270F35IET-ND |
Manufacturer Part#: |
LP270F35IET |
Price: | $ 0.21 |
Product Category: | Crystals, Oscillators, Resonators |
Manufacturer: | CTS-Frequency Controls |
Short Description: | CRYSTAL 27.000000MHZ SMD |
More Detail: | 27MHz ±30ppm Crystal 20pF 30 Ohms HC-49/US |
DataSheet: | LP270F35IET Datasheet/PDF |
Quantity: | 1000 |
1000 +: | $ 0.19152 |
Series: | ATSSMLP |
Packaging: | Tape & Reel (TR) |
Part Status: | Active |
Type: | MHz Crystal |
Frequency: | 27MHz |
Frequency Stability: | ±50ppm |
Frequency Tolerance: | ±30ppm |
Load Capacitance: | 20pF |
ESR (Equivalent Series Resistance): | 30 Ohms |
Operating Mode: | Fundamental |
Operating Temperature: | -40°C ~ 85°C |
Ratings: | -- |
Mounting Type: | Surface Mount |
Package / Case: | HC-49/US |
Size / Dimension: | 0.437" L x 0.190" W (11.10mm x 4.83mm) |
Height - Seated (Max): | 0.126" (3.20mm) |
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Crystals have been a crucial component of electronic devices ever since their invention. They are typically used in order to control the frequency of signals and to provide a precise timing source. This article will explore the application field and working principle of one particular type of crystal, the LP270F35IET.
The LP270F35IET is designed to be used in frequency control and communication systems, as well as in personal computers, microcontrollers and digital signal processors. This type of crystal is also suitable for use in audio signal sources such as radio receivers and oscillators. Furthermore, this crystal is commonly used to ensure precise timing in automotive and navigation systems.
The working principle of the LP270F35IET is based on the phenomenon of resonance. The crystal consists of two mechanical plates (referred to as plates for short), which vibrate at different frequencies when excited. The two plates are held together with an adhesive between them, and when a signal is applied, the plates begin to vibrate at the same frequency. This frequency is determined by the size and shape of the plates, and the resonance that it produces is known as the quartz frequency.
The LP270F35IET is also equipped with a low-noise amplifier, which helps to improve the accuracy of the signal. The amplifier amplifies the signal before it is sent to the processor, allowing it to be read more accurately. Additionally, the amplifier helps to reduce any restriction or interference of the signal, resulting in a cleaner overall frequency.
Finally, the LP270F35IET also features a temperature compensation circuit that helps to ensure that the crystal remains stable and performs at its optimum level regardless of outside temperature changes. This circuit is responsible for maintaining the accuracy of the signal and ensuring that the crystal functions properly regardless of its environment.
Overall, the LP270F35IET is an example of a crystal with a specific application field and working principle. This type of crystal is ideal for frequency control and communication systems, as well as in personal computers, microcontrollers and digital signal processors. It is also suitable for use in audio signal sources such as radio receivers and oscillators, and for ensuring precise timing in automotive and navigation systems. Finally, it is equipped with a low-noise amplifier and a temperature compensation circuit, both of which improve the accuracy and reliability of the crystal\'s performance.
The specific data is subject to PDF, and the above content is for reference
Part Number | Manufacturer | Price | Quantity | Description |
---|
LP272M035C1P3 | Cornell Dubi... | 2.5 $ | 1 | CAP ALUM 2700UF 20% 35V S... |
LP271M200A1P3 | Cornell Dubi... | 0.0 $ | 1000 | CAP ALUM 270UF 20% 200V S... |
LP271M200C3P3 | Cornell Dubi... | 0.0 $ | 1000 | CAP ALUM 270UF 20% 200V S... |
LP271M200E1P3 | Cornell Dubi... | 0.0 $ | 1000 | CAP ALUM 270UF 20% 200V S... |
LP271M250C3P3 | Cornell Dubi... | 0.0 $ | 1000 | CAP ALUM 270UF 20% 250V S... |
LP272M025C1P3 | Cornell Dubi... | 0.0 $ | 1000 | CAP ALUM 2700UF 20% 25V S... |
LP272M050C1P3 | Cornell Dubi... | 0.0 $ | 1000 | CAP ALUM 2700UF 20% 50V S... |
LP272M100H7P3 | Cornell Dubi... | 0.0 $ | 1000 | CAP ALUM 2700UF 20% 100V ... |
LP272M100H9P3 | Cornell Dubi... | 0.0 $ | 1000 | CAP ALUM 2700UF 20% 100V ... |
LP273M016H7P3 | Cornell Dubi... | 0.0 $ | 1000 | CAP ALUM 27000UF 20% 16V ... |
LP270F23CDT | CTS-Frequenc... | 0.21 $ | 1000 | CRYSTAL 27.000000MHZ SMD2... |
LP270F23CET | CTS-Frequenc... | 0.21 $ | 1000 | CRYSTAL 27.000000MHZ SMD2... |
LP270F33CDT | CTS-Frequenc... | 0.21 $ | 1000 | CRYSTAL 27.000000MHZ SMD2... |
LP270F33CET | CTS-Frequenc... | 0.21 $ | 1000 | CRYSTAL 27.000000MHZ SMD2... |
LP270F35CDT | CTS-Frequenc... | 0.21 $ | 1000 | CRYSTAL 27.000000MHZ SMD2... |
LP270F35CET | CTS-Frequenc... | 0.21 $ | 1000 | CRYSTAL 27.000000MHZ SMD2... |
LP270F35IDT | CTS-Frequenc... | 0.21 $ | 1000 | CRYSTAL 27.000000MHZ SMD2... |
LP270F35IET | CTS-Frequenc... | 0.21 $ | 1000 | CRYSTAL 27.000000MHZ SMD2... |
LP270F23IDT | CTS-Frequenc... | 0.22 $ | 1000 | CRYSTAL 27.000000MHZ SMD2... |
LP270F23IET | CTS-Frequenc... | 0.22 $ | 1000 | CRYSTAL 27.000000MHZ SMD2... |
LP270F33IDT | CTS-Frequenc... | 0.22 $ | 1000 | CRYSTAL 27.000000MHZ SMD2... |
LP270F33IET | CTS-Frequenc... | 0.22 $ | 1000 | CRYSTAL 27.000000MHZ SMD2... |
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