Model Dimensions (Nominal) | Frequency Range | Reference Data Sheets | CX1 L = 8.00 mm W = 3.56 mm H = 1.65 mm | 10 kHz to 600 kHz
| 10121 (For use in Pierce Oscillator Circuits) 10122 (For use in Series Oscillator Circuits) 10183 (High Temperature Crystal) | 530 kHz to 2.1 MHz
| 10129 10185 (High Temperature Crystal) | 6 MHz to 250 MHz
| 10107 10108 (High Shock Crystal) 10184 (High Temperature Crystal) | CX3 L = 6.68 mm W = 2.46 mm H = 1.35 mm | 18 kHz to 600 kHz
| 10104 (For use in Pierce Oscillator Circuits) 10146 (For use in Series Oscillator Circuits)
| 800 kHz to 1.35 MHz
| 10123
| 9.6 MHz to 250 MHz | 10120 10182 (High Shock Crystal) | CX4 L = 5.00 mm W = 1.83 mm H = 1.14 mm | 30 kHz to 250 kHz | 10103 10183 (High Temperature Crystal) | 600 kHz to 1.4 MHz (Fundamental) | 10161 | 1.8432 MHz to 2.5 MHz (Overtone) | 10185 (High Temperature Crystal) | 14 MHz to 50 MHz | 10165 (High Shock Crystal) | 14 MHz to 250 MHz | 10150 10184 (High Temperature Crystal) | CX9 L = 4.10 mm W = 1.50 mm H = 0.87 mm | 32 kHz to 250 kHz | 10157 10183 (High Temperature Crystal) | 13.5 MHz to 250 MHz | 10158 10184 (High Temperature Crystal) | CX11 / CX11L L = 3.20 mm W = 1.50 mm H = 0.74 mm H = 0.51 mm (CX11L) | 32 kHz to 180 kHz | 10174 | 16 MHz to 250 MHz | 10179 10188 (Telemetry Crystal) | 16 MHz - 50 MHz | 10193 (High Shock Crystal) | CX16 L = 2.00 mm W = 1.20 mm H = 0.43 mm | 24 MHz to 50 MHz | 10200 (Telemetry Crystal) | CX17 L = .4.80 mm W = 3.00 mm H = 0.90 mm | 12 MHz to 200 MHz | 10206 | CX18 L = 1.55 mm W = 0.95 mm H = 0.35 mm | 30 MHz to 50 MHz | 10207
| CX20 L = 2.50 mm W = 1.20 mm H = 0.53 mm | 16 MHz to 50 MHz | 10219 (Telemetry Crystal) | SWCX1 L = 8.00 mm W = 3.56 mm H =1.78 mm | 6 MHz to 250 MHz | 10199 | SX1 (TO-39 Gold Plated) W = 9.66 mm H = 4.79 mm | 30 kHz to 250 MHz | 10194 | Tape and Reel 7" Reels or 13" Reels | The center hole (hub hole) diameter is per EIA-481-2A standard 13 mm size | 10109 |
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笔记:
有关操作和储存温度和温度稳定性,请参阅个别数据表。
“V”表示Pierce操作的晶体,“H”表示串联操作的晶体。 “V”和“H”型号仅适用于频率从10 kHz到600 kHz的调音叉设计。
可提供MIL-C-3098测试。
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