Q 30,0-JXS21-10-10/15-T1-FU-WA-LF Allicdata Electronics
Allicdata Part #:

Q30,0-JXS21-10-10/15-T1-FU-WA-LF-ND

Manufacturer Part#:

Q 30,0-JXS21-10-10/15-T1-FU-WA-LF

Price: $ 0.29
Product Category:

Crystals, Oscillators, Resonators

Manufacturer: Jauch Quartz
Short Description: CRYSTAL 30MHZ 10PF SMD
More Detail: 30MHz ±10ppm Crystal 10pF 60 Ohms 4-SMD, No Lead
DataSheet: Q 30,0-JXS21-10-10/15-T1-FU-WA-LF datasheetQ 30,0-JXS21-10-10/15-T1-FU-WA-LF Datasheet/PDF
Quantity: 1000
1000 +: $ 0.26460
Stock 1000Can Ship Immediately
$ 0.29
Specifications
Series: JXS21-WA
Packaging: Tape & Reel (TR) 
Part Status: Active
Type: MHz Crystal
Frequency: 30MHz
Frequency Stability: ±15ppm
Frequency Tolerance: ±10ppm
Load Capacitance: 10pF
ESR (Equivalent Series Resistance): 60 Ohms
Operating Mode: Fundamental
Operating Temperature: -40°C ~ 85°C
Ratings: --
Mounting Type: Surface Mount
Package / Case: 4-SMD, No Lead
Size / Dimension: 0.079" L x 0.063" W (2.00mm x 1.60mm)
Height - Seated (Max): 0.022" (0.55mm)
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

Q 30,0-JXS21-10-10/15-T1-FU-WA-LF Application Field and Working Principle

Q 30,0-JXS21-10-10/15-T1-FU-WA-LF, or quartz crystal resonators, are widely used in crystal oscillators due to their high frequency stability. Quartz crystal resonators have several advantages over other types of oscillators. In addition to providing a high frequency stability, their temperature characteristics are much better than most other materials. As such, quartz crystal resonators are well suited for use in precision electronic applications.

A quartz crystal resonator consists of three parts: the piezoelectric crystal, the electrodes, and a housing. The piezoelectric crystal is composed mainly of quartz and has a naturally occurring piezoelectric effect. This effect causes the crystal to vibrate when a voltage is applied across its two electrodes. The electrodes capture the mechanical vibrations, amplify them, and convert them back into an electrical signal that can be used by the oscillator circuit.

The mechanical properties of the quartz crystal are used to determine the frequency of operation of the crystal oscillator. The small size and low power requirements of quartz crystals make them ideal for use in many different types of applications. Quartz crystal resonators are widely used in consumer electronics such as clocks, watches, computers, and mobile phones. In addition, they are used extensively in industrial and military applications, as well as in satellite communications systems.

The frequency stability of quartz crystal resonators is much better than that of most other oscillators. This is due to the very low temperature coefficient and the fact that the frequency is determined by the mechanical properties of the crystal. The frequency of a quartz crystal oscillator is determined by a combination of the quartz crystal resonance and the frequency of the radio oscillator. The greater the frequency of the radio oscillator, the more precise the frequency of the quartz crystal oscillator. The low temperature coefficient of quartz crystal oscillators makes them well suited for applications that require precise frequency stability over a wide range of temperature.

Quartz crystal resonators are available in a variety of shapes and sizes, depending on their intended use. For example, some crystals are designed for use in high-frequency microwave applications, while others are designed for use in medical and industrial applications. The frequency stability of a quartz crystal resonator is also determined by the type of electrodes and the type of crystal used in its construction.

Quartz crystal resonators are a vital part of modern electronics, and their importance in many applications cannot be overlooked. The precise frequency stability and the low temperature coefficient make them an ideal choice for many electronic and industrial applications. Whether used in a clock, a computer, or a satellite communications system, quartz crystal resonators are a reliable and precise choice.

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

Related Products
Search Part number : "Q 30" Included word is 40
Part Number Manufacturer Price Quantity Description
EWA-Q30C15A14 Panasonic El... 0.0 $ 1000 POT SLIDE 10K OHM .06W 60...
EWA-Q30C15D14 Panasonic El... 0.0 $ 1000 POT SLIDE 10K OHM .06W 60...
Q30N-12 XP Power 137.21 $ 4 SINGLE O/P, DC-HV DC PCB ...
Q30-12 XP Power 137.21 $ 3 SINGLE O/P, DC-HV DC PCB ...
Q3062 QT Brightek ... 0.6 $ 1000 OPTOISOLATOR 5KV TRIAC 6D...
Q3063 QT Brightek ... 0.6 $ 1000 OPTOISOLATOR 5KV TRIAC 6D...
Q3082 QT Brightek ... 0.6 $ 1000 OPTOISOLATOR 5KV TRIAC 6D...
Q3083 QT Brightek ... 0.6 $ 1000 OPTOISOLATOR 5KV TRIAC 6D...
Q3052 QT Brightek ... 0.46 $ 1000 OPTOISOLATOR 5KV TRIAC 6D...
Q3053 QT Brightek ... 0.46 $ 1000 OPTOISOLATOR 5KV TRIAC 6D...
Q3022 QT Brightek ... 0.48 $ 1000 OPTOISOLATOR 5KV TRIAC 6D...
Q3023 QT Brightek ... 0.48 $ 1000 OPTOISOLATOR 5KV TRIAC 6D...
BC6-Q308-02 TE Connectiv... 2.23 $ 1132 CONN BARRIER STRIP 2CIRC ...
JC6-Q308-07 TE Connectiv... 4.6 $ 238 CONN BARRIER STRIP 7CIRC ...
JC6-Q307-04 TE Connectiv... 4.82 $ 943 CONN BARRIER STRIP 4CIRC ...
JC6-Q308-05 TE Connectiv... 5.38 $ 303 CONN BARRIER STRIP 5CIRC ...
JC6-Q307-10 TE Connectiv... 7.46 $ 1000 CONN BARRIER STRP 10CIRC ...
BC6-Q308-13 TE Connectiv... 7.68 $ 1000 CONN BARRIER STRP 13CIRC ...
Q302013PCI Hoffman Encl... 73.64 $ 1 BOX PLASTIC GRAY 11.81"LX...
Q302013PCICC Hoffman Encl... 73.64 $ 1 BOX PLASTIC GRY/CLR 11.8"...
Q3020PI Hoffman Encl... 10.47 $ 11 PANEL FITS 300X200MMPanel...
BC6-Q308-03 TE Connectiv... 1.74 $ 1000 CONN BARRIER STRIP 3CIRC ...
JC6-Q307-03 TE Connectiv... 1.67 $ 1000 CONN BARRIER STRIP 3CIRC ...
JC6-Q308-02 TE Connectiv... 2.17 $ 1000 CONN BARRIER STRIP 2CIRC ...
JC6-Q307-02 TE Connectiv... 0.95 $ 1000 CONN BARRIER STRIP 2CIRC ...
JC6-Q307-12 TE Connectiv... 4.31 $ 1000 CONN BARRIER STRP 12CIRC ...
JC6-Q307-16 TE Connectiv... 5.57 $ 1000 CONN BARRIER STRP 16CIRC ...
JC6-Q307-08 TE Connectiv... 5.66 $ 1000 CONN BARRIER STRIP 8CIRC ...
BC6-Q308-06 TE Connectiv... 4.81 $ 1000 CONN BARRIER STRIP 6CIRC ...
JC6-Q307-07 TE Connectiv... 4.98 $ 1000 CONN BARRIER STRIP 7CIRC ...
JC6-Q305-12 TE Connectiv... 5.14 $ 1000 CONN BARRIER STRP 12CIRC ...
JC6-Q307-15 TE Connectiv... 5.49 $ 1000 CONN BARRIER STRP 15CIRC ...
JC6-Q307-06 TE Connectiv... 3.24 $ 1000 CONN BARRIER STRIP 6CIRC ...
JC6-Q307-09 TE Connectiv... 3.37 $ 1000 CONN BARRIER STRIP 9CIRC ...
JC6-Q307-18 TE Connectiv... 6.45 $ 1000 CONN BARRIER STRP 18CIRC ...
JC6-Q308-06 TE Connectiv... 6.55 $ 1000 CONN BARRIER STRIP 6CIRC ...
JC6-Q307-05 TE Connectiv... 2.7 $ 1000 CONN BARRIER STRIP 5CIRC ...
Q30-5 XP Power 150.93 $ 1 DC DC CONVERTER 3000V 500...
JC6-Q308-03 TE Connectiv... 1.79 $ 1000 CONN BARRIER STRIP 3CIRC ...
Q3067543 STMicroelect... 21.46 $ 1000 KIT DIODES 18VALUES 5 EAC...
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