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更多>>福克斯要挑战开发枕头形状的石英晶体FX425B-16.000
福克斯要挑战开发枕头形状的石英晶体FX425B-16.000,然而,这些电极的附着被证明是一个巨大的挑战,这取决于振荡的类型。理想情况下,电极应该附着在石英上的一个点上,在这个点上,即使在有电压的情况下,石英晶振的变形也是最小的。使用厚度剪切振子比使用开头提到的弯曲或纵向振子要容易得多。
然而,石英的进一步加工步骤也是必要的。在一台特殊的研磨机中,坯料被研磨成垫子的形状——中间稍厚,向外逐渐变细。石英支架连接到锥形端。以这种方式固定,薄金属电极最终被蒸发到坯件的较厚的中间部分上。
因此,AT切割在石英贴片晶振生产中具有双重功能。首先,它确保在-40到85摄氏度的温度范围内的高频率稳定性,其次,它将坯料的形状定义为厚度剪切振荡器。
原厂编码 | 厂家 | 型号 | 系列 | 频率 | 频率稳定度 |
FQ3225BR-12.000 | FOX晶振 | FQ3225B | MHz Crystal | 12MHz | ±50ppm |
FQ1045AR-6.000 | FOX晶振 | FQ1045A | MHz Crystal | 6MHz | ±30ppm |
FQ1045AR-4.000 | FOX晶振 | FQ1045A | MHz Crystal | 4MHz | ±30ppm |
FQ1045AR-3.6864 | FOX晶振 | FQ1045A | MHz Crystal | 3.6864MHz | ±30ppm |
FOXSLF/0368S | FOX晶振 | HC49SLF | MHz Crystal | 3.6864MHz | ±50ppm |
FOXLF120 | FOX晶振 | HC49ULF | MHz Crystal | 12MHz | ±50ppm |
FOXSDLF/128-20 | FOX晶振 | HC49SDLF | MHz Crystal | 12.288MHz | ±50ppm |
FOXSDLF/081-20 | FOX晶振 | HC49SDLF | MHz Crystal | 8.192MHz | ±50ppm |
FOXSDLF/098-20 | FOX晶振 | HC49SDLF | MHz Crystal | 9.8304MHz | ±50ppm |
FOXSDLF/196-20 | FOX晶振 | HC49SDLF | MHz Crystal | 19.6608MHz | ±50ppm |
FOXSLF/115 | FOX晶振 | HC49SLF | MHz Crystal | 11.0592MHz | ±50ppm |
FOXSLF/200 | FOX晶振 | HC49SLF | MHz Crystal | 20MHz | ±50ppm |
FOXSDLF/0368R-20/TR | FOX晶振 | HC49SDLF | MHz Crystal | 3.6864MHz | ±50ppm |
FOXSDLF/040R/TR | FOX晶振 | HC49SDLF | MHz Crystal | 4MHz | ±50ppm |
FOXSDLF/060R-20/TR | FOX晶振 | HC49SDLF | MHz Crystal | 6MHz | ±50ppm |
FOXSDLF/073R-20/TR | FOX晶振 | HC49SDLF | MHz Crystal | 7.3728MHz | ±50ppm |
FOXSDLF/100R-20/TR | FOX晶振 | HC49SDLF | MHz Crystal | 10MHz | ±50ppm |
FOXSDLF/115R-20/TR | FOX晶振 | HC49SDLF | MHz Crystal | 11.0592MHz | ±50ppm |
FOXSDLF/143R-20/TR | FOX晶振 | HC49SDLF | MHz Crystal | 14.31818MHz | ±50ppm |
FOXSDLF/240FR-20/TR | FOX晶振 | HC49SDLF | MHz Crystal | 24MHz | ±50ppm |
FOXSDLF250F-20 | FOX晶振 | HC49SDLF | MHz Crystal | 25MHz | ±50ppm |
FX252BS-20.000 | FOX晶振 | FX252B | MHz Crystal | 20MHz | ±50ppm |
FQ5032BR-10.000 | FOX晶振 | C5BQ | MHz Crystal | 10MHz | ±30ppm |
FQ5032BR-16.000 | FOX晶振 | C5BQ | MHz Crystal | 16MHz | ±50ppm |
FX532B-10.000 | FOX晶振 | FX532B | MHz Crystal | 10MHz | ±50ppm |
FQ7050B-11.0592 | FOX晶振 | C7BQ | MHz Crystal | 11.0592MHz | ±30ppm |
FX425B-16.000 | FOX晶振 | FX425B | MHz Crystal | 16MHz | ±50ppm |
FQ5032B-19.6608 | FOX晶振 | C5BQ | MHz Crystal | 19.6608MHz | ±30ppm |
FQ5032B-14.7456 | FOX晶振 | C5BQ | MHz Crystal | 14.7456MHz | ±30ppm |
FQ5032B-10.000 | FOX晶振 | C5BQ | MHz Crystal | 10MHz | ±30ppm |
FQ3225B-20.000 | FOX晶振 | FQ3225B | MHz Crystal | 20MHz | ±50ppm |
FQ3225BR-16.000 | FOX晶振 | FQ3225B | MHz Crystal | 16MHz | ±50ppm |
FQ3225BR-20.000 | FOX晶振 | FQ3225B | MHz Crystal | 20MHz | ±50ppm |
FQ1045A-4.9152 | FOX晶振 | FQ1045A | MHz Crystal | 4.9152MHz | ±30ppm |
603-12-67 | Fox晶振 | FX325BS | MHz Crystal | 12MHz | ±50ppm |
617-24.572675-1 | FOX晶振 | FX216B | MHz Crystal | 24.572675MHZ | ±50ppm |
FX532B-11.0592 | FOX晶振 | FX532B | MHz Crystal | 11.0592MHz | ±50ppm |
FX532B-12.000 | FOX晶振 | FX532B | MHz Crystal | 12MHz | ±50ppm |
FX532B-16.000 | FOX晶振 | FX532B | MHz Crystal | 16MHz | ±50ppm |
FX532B-20.000 | FOX晶振 | FX532B | MHz Crystal | 20MHz | ±50ppm |
FX532B-24.000 | FOX晶振 | FX532B | MHz Crystal | 24MHz | ±50ppm |
FX532B-24.576 | FOX晶振 | FX532B | MHz Crystal | 24.576MHz | ±50ppm |
FX425B-20.000 | FOX晶振 | FX425B | MHz Crystal | 20MHz | ±50ppm |
FX425B-24.000 | FOX晶振 | FX425B | MHz Crystal | 24MHz | ±50ppm |
FX425B-24.576 | FOX晶振 | FX425B | MHz Crystal | 24.576MHz | ±50ppm |
217-3.579545-12 | FOX晶振 | FC | MHz Crystal | 3.579545MHz | ±50ppm |
The attachment of these electrodes, however, proves to be a great challenge, depending on the type of oscillation. Ideally, the electrodes should be attached to a point on the quartz where it deforms only minimally, even under voltage. This is much easier with a thickness shear oscillator than with the bending or longitudinal oscillators mentioned at the beginning.
Nevertheless, a further processing step of the quartz is also necessary. In a special lapping machine, the blanks are ground until they assume the shape of a cushion – slightly thicker in the middle and tapering outwards. The quartz holder is attached to the tapered ends. Secured in this way, thin metal electrodes are finally evaporated onto the thicker middle section of the blank.
The AT cut thus fulfils a double function in quartz production. First, it ensures high frequency stability in the temperature range from -40 to 85 degrees Celsius and second, it defines the shape of the blank as a thickness shear oscillator.
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