LP270F33IDT Allicdata Electronics
Allicdata Part #:

LP270F33IDT-ND

Manufacturer Part#:

LP270F33IDT

Price: $ 0.22
Product Category:

Crystals, Oscillators, Resonators

Manufacturer: CTS-Frequency Controls
Short Description: CRYSTAL 27.000000MHZ SMD
More Detail: 27MHz ±30ppm Crystal 18pF 30 Ohms HC-49/US
DataSheet: LP270F33IDT datasheetLP270F33IDT Datasheet/PDF
Quantity: 1000
1000 +: $ 0.19908
Stock 1000Can Ship Immediately
$ 0.22
Specifications
Series: ATSSMLP
Packaging: Tape & Reel (TR) 
Part Status: Active
Type: MHz Crystal
Frequency: 27MHz
Frequency Stability: ±30ppm
Frequency Tolerance: ±30ppm
Load Capacitance: 18pF
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)
Description

Due to market price fluctuations, if you need to purchase or consult the price. You can contact us or emial to us:   sales@allicdata.com

Crystals can be used for a variety of applications, from electronics to medical equipment. One of the most popular crystals on the market today is the LP270F33IDT crystal. It is a versatile, easy-to-use, efficient, and cost-effective crystal ideal for electronic applications, including clock oscillators and other electronic circuits. In this article, we will explore the application field and working principle of the LP270F33IDT crystal.

This type of crystal is generally used in electronic clock and frequency circuits, such as oscillators, frequency dividers, phase detectors, etc. It is the perfect choice for designs that require high precision and stable frequency control, such as in PCs and other digital products. Additionally, this type of crystal is ideal for extremely high frequency (up to 200 MHz) applications, making it the go-to choice for numerous digital applications.

In terms of its working principle, the LP270F33IDT crystal works by passing an alternating current through two electrodes. This alternating current creates an electromagnetic field inside the crystal. If the two electrodes are cut in a precise way, and the same alternating current is passed through them, the crystal will vibrate at a frequency determined by its size, shape, and parameters of the alternating current.

Furthermore, due to its frequency stability, the LP270F33IDT crystal is perfect for applications where long-term accuracy is needed. For example, it is the perfect choice for use in quartz clocks and watches, as it ensures the accurate timekeeping of the timepiece. Thus, it is a reliable and efficient choice for time-sensitive applications.

In addition to frequency stability, the LP270F33IDT crystal also has low noise generation and low power consumption, making it ideal for use in low power consumption applications. Due to these features, it is especially useful for data transmission and other high-performance applications. Additionally, because this crystal is designed to be mounted in a convenient through-hole package, it is easy to integrate into electronics projects.

As can be seen, the LP270F33IDT crystal offers a variety of benefits and is a great choice whenever precise frequency control is desired. Its stable frequency, low power consumption, and low noise generation make it the perfect choice for a wide range of applications, including clocks, electronic devices, and data transmission systems. This versatile and efficient crystal is truly the perfect choice for numerous digital applications.

The specific data is subject to PDF, and the above content is for reference

Related Products
Search Part number : "LP27" Included word is 22
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...
Latest Products
CSTCE8M59G55A-R0

Crystal 8.59MHz 39pF 3-Pin CSMD T/R - Ta...

CSTCE8M59G55A-R0 Allicdata Electronics
416F520X3CLT

CRYSTAL 52.000 MHZ 12PF SMT52MHz 15ppm C...

416F520X3CLT Allicdata Electronics
416F500X3AKT

CRYSTAL 50.000 MHZ 8PF SMT50MHz 15ppm Cr...

416F500X3AKT Allicdata Electronics
416F48022CKT

CRYSTAL 48.000 MHZ 8PF SMT48MHz 20ppm Cr...

416F48022CKT Allicdata Electronics
416F44023ITT

CRYSTAL 44.000 MHZ 6PF SMT44MHz 20ppm Cr...

416F44023ITT Allicdata Electronics
416F406X2AST

CRYSTAL 40.610 MHZ SERIES SMT40.61MHz 15...

416F406X2AST Allicdata Electronics