| Allicdata Part #: | ATS126-E-ND |
| Manufacturer Part#: |
ATS126-E |
| Price: | $ 0.13 |
| Product Category: | Crystals, Oscillators, Resonators |
| Manufacturer: | CTS-Frequency Controls |
| Short Description: | CRYSTAL 12.3520MHZ SERIES T/H |
| More Detail: | 12.352MHz ±30ppm Crystal Series 40 Ohms HC-49/US |
| DataSheet: |  ATS126-E Datasheet/PDF |
| Quantity: | 1000 |
| 1000 +: | $ 0.12096 |
Specifications
| Series: | ATS |
| Packaging: | Bulk |
| Part Status: | Active |
| Type: | MHz Crystal |
| Frequency: | 12.352MHz |
| Frequency Stability: | ±50ppm |
| Frequency Tolerance: | ±30ppm |
| Load Capacitance: | Series |
| ESR (Equivalent Series Resistance): | 40 Ohms |
| Operating Mode: | Fundamental |
| Operating Temperature: | -40°C ~ 85°C |
| Ratings: | -- |
| Mounting Type: | Through Hole |
| Package / Case: | HC-49/US |
| Size / Dimension: | 0.427" L x 0.177" W (10.85mm x 4.50mm) |
| Height - Seated (Max): | 0.145" (3.68mm) |
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 areimportant components in a wide range of electronic and other applications. In a wide variety of communication and industrial automation systems, a common form of crystal is used in the form of a crystal oscillator. They form the basis of circuits thatgenerate precise, low frequency signals and are used to define and regulate the frequency of manycommunication and control systems. This article focuses on one type of crystal oscillator, theATS126-E, and outlines its application field and working principle.
A crystal oscillator is a simple electrical circuit that uses the properties of a crystal tocombine and convert electrical energy into a precise frequency output. Typically, the crystalsused in these circuits are small pieces of quartz, usually cut in the shape of a thin rectangularbar or in the form of a disk. Quartz is an excellent material for use in this application dueto its stability over a wide temperature range, which ensures a consistent frequency output.Within a quartz crystal, when an electrical field is applied, due to the piezoelectric effect, animportant phenomenon is produced in which the crystal vibrates at a specific and precisefrequency.
The ATS126-E is an integrated, surface-mount crystal oscillator with a wide operatingrange, from 8MHz to 16MHz. It has a frequency range of 1MHz to 30MHz, a temperature rangeof -15 °C to 70 °C, a power consumption of 1.5 mA, and a maximum supply voltage of 3.3V.The ATS126-E also has very low jitter, ensuring a stable and accurate output. It features bothamplitude and phase modulation sides, enabling it to operate in a wide range of applications andenvironments. The oscillator is also compact, occupying only a small form factor, making itideal for applications where space is limited.
The ATS126-E works by converting electrical energy into a specific frequency output. It isbased on a two-stage, differential input amplifier connected to a quartz crystal via an inductiveimpedance similarity. The crystal is connected in parallel with the input of the amplifiers and asthe electrical input is increased, the frequency output of the signal is increased. The twostages of the amplifier prevent the signal from overdriving the crystal, and thus enabling a stableoperation over the entire operating range. As the signal is applied to the quartz crystal, it vibratesat its resonance frequency, producing a precise output frequency.
The ATS126-E is suitable for a wide range of applications. It can be found in manyautomotive and industrial systems, such as power supplies, electronic control units, and drivesystems. It is also commonly used in wireless communications, where its precision and stabilityare very advantageous. The ATS126-E is also a popular choice for medical and farm equipment,communication systems, and test and measurement systems.
In conclusion, the ATS126-E crystal oscillator is a highly accurate, reliable and low poweredevice that can be used in a wide range of applications. Its small form factor also makes it anattractive choice for systems where space is limited. The ATS126-E is a great option whenselecting a crystal oscillator for any application that requires accurate, low frequency signals.
The specific data is subject to PDF, and the above content is for reference
Related Products
Search Part number : "ATS1" Included word is 39
| Part Number | Manufacturer | Price | Quantity | Description |
|---|
| ATS15A-INS | CTS-Frequenc... | 0.54 $ | 1000 | CRYSTAL 15.36MHZ 20PF THR... |
| ATS100B | CTS-Frequenc... | 0.25 $ | 1000 | CRYSTAL 10.0000MHZ 18PF T... |
| ATS122B-E | CTS-Frequenc... | 0.16 $ | 1000 | CRYSTAL 12.2880MHZ 18PF T... |
| ATS140BSM-1 | CTS-Frequenc... | 0.16 $ | 1000 | CRYSTAL 14MHZ 18PF SMD14M... |
| ATS120B-E | CTS-Frequenc... | 0.25 $ | 1495 | CRYSTAL 12.0000MHZ 18PF T... |
| ATS126SM-1 | CTS-Frequenc... | 0.14 $ | 1000 | CRYSTAL 12.3520MHZ 20PF S... |
| ATS19ASM-1 | CTS-Frequenc... | 0.14 $ | 1000 | CRYSTAL 19.6608MHZ 20PF S... |
| ATS147SM-1E | CTS-Frequenc... | 0.14 $ | 1000 | CRYSTAL 14.7456MHZ SERIES... |
| ATS196B-E | CTS-Frequenc... | 0.16 $ | 1000 | CRYSTAL 19.6608MHZ 18PF T... |
| ATS120-E | CTS-Frequenc... | 0.16 $ | 1000 | CRYSTAL 12.0000MHZ SERIES... |
| ATS111C | CTS-Frequenc... | 0.25 $ | 67 | CRYSTAL 11.0592MHZ 32PF T... |
| ATS150SM-1E | CTS-Frequenc... | 0.14 $ | 1000 | CRYSTAL 15.0000MHZ SERIES... |
| ATS111ASM-1E | CTS-Frequenc... | 0.16 $ | 1000 | CRYSTAL 11.0592MHZ SERIES... |
| ATS137-PG-A-A | Diodes Incor... | 0.0 $ | 1000 | MAGNETIC SWITCH UNIPOLAR ... |
| ATS137-PL-A-A | Diodes Incor... | 0.0 $ | 1000 | MAGNETIC SWITCH UNIPOLAR ... |
| ATS137-PL-B-A | Diodes Incor... | -- | 1000 | MAGNETIC SWITCH UNIPOLAR ... |
| ATS177-PG-B-A | Diodes Incor... | 0.0 $ | 1000 | IC HALL EFFECT LATCH 3SIP... |
| ATS120C | CTS-Frequenc... | 0.16 $ | 1000 | CRYSTAL 12.0000MHZ 32PF T... |
| ATS160-1 | CTS-Frequenc... | 0.16 $ | 1000 | CRYSTAL 16MHZ SERIES THRU... |
| ATS130SM-1 | CTS-Frequenc... | 0.16 $ | 1000 | CRYSTAL 13MHZ 18PF SMD13M... |
| ATS19510LSNBTN-RSWBLUJ | Allegro Micr... | 1.73 $ | 1000 | 2-WIRE, DIFF. SPD AND DIR... |
| ATS120CSM-1 | CTS-Frequenc... | 0.14 $ | 1000 | CRYSTAL 12.0000MHZ 32PF S... |
| ATS147-E | CTS-Frequenc... | 0.33 $ | 632 | CRYSTAL 14.7456MHZ SERIES... |
| ATS100BSM-1 | CTS-Frequenc... | 0.14 $ | 1000 | CRYSTAL 10.0000MHZ 18PF S... |
| ATS12A-E | CTS-Frequenc... | 0.25 $ | 795 | CRYSTAL 12.0000MHZ 20PF T... |
| ATS184BSM-1E | CTS-Frequenc... | 0.14 $ | 1000 | CRYSTAL 18.4320MHZ 18PF S... |
| ATS14ASM-1E | CTS-Frequenc... | 0.14 $ | 1000 | CRYSTAL 14.31818MHZ 20PF ... |
| ATS135BSM-1 | CTS-Frequenc... | 0.16 $ | 1000 | CRYSTAL 13.5MHZ 20PF THRU... |
| ATS177-WLA-A | Diodes Incor... | -- | 1000 | IC HALL EFFECT LATCHDigit... |
| ATS10A-E | CTS-Frequenc... | 0.25 $ | 1079 | CRYSTAL 10.0000MHZ 20PF T... |
| ATS122B | CTS-Frequenc... | 0.25 $ | 409 | CRYSTAL 12.2880MHZ 18PF T... |
| ATS120CSM-1E | CTS-Frequenc... | 0.28 $ | 1568 | CRYSTAL 12.0000MHZ 32PF S... |
| ATS19A-E | CTS-Frequenc... | 0.25 $ | 986 | CRYSTAL 19.6608MHZ 20PF T... |
| ATS160 | CTS-Frequenc... | 0.25 $ | 1040 | CRYSTAL 16.0000MHZ SERIES... |
| ATS122BSM-1 | CTS-Frequenc... | -- | 1000 | CRYSTAL 12.2880MHZ 18PF S... |
| ATS147BSM-1 | CTS-Frequenc... | 0.14 $ | 1000 | CRYSTAL 14.7456MHZ 18PF S... |
| ATS147SM-E | CTS-Frequenc... | 0.16 $ | 1000 | CRYSTAL 14.7456MHZ SERIES... |
| ATS147B | CTS-Frequenc... | 0.25 $ | 1580 | CRYSTAL 14.7456MHZ 18PF T... |
| ATS15A-E | CTS-Frequenc... | 0.13 $ | 1000 | CRYSTAL 15.3600MHZ 20PF T... |
Latest Products
CSTCE8M59G55A-R0
Crystal 8.59MHz 39pF 3-Pin CSMD T/R - Ta...
416F520X3CLT
CRYSTAL 52.000 MHZ 12PF SMT52MHz 15ppm C...
416F500X3AKT
CRYSTAL 50.000 MHZ 8PF SMT50MHz 15ppm Cr...
416F48022CKT
CRYSTAL 48.000 MHZ 8PF SMT48MHz 20ppm Cr...
416F44023ITT
CRYSTAL 44.000 MHZ 6PF SMT44MHz 20ppm Cr...
416F406X2AST
CRYSTAL 40.610 MHZ SERIES SMT40.61MHz 15...