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AN2595 数据表(PDF) 7 Page - STMicroelectronics |
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AN2595 数据表(HTML) 7 Page - STMicroelectronics |
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7 / 20 page ![]() AN2595 - Application note Oscillator 7/20 The load capacitors C1 and C2 transform the gain of the amplifier (gm) into a negative series resistance RL to compensate for the losses of the crystal. The best frequency stability is obtained when C1 = C2. The oscillation occurs when the sum of RL and Rs (the series resistance of the crystal) is negative. By choosing C1 = C2 = C, the minimal gain of the amplifier (gm) is expressed as follows: The minimal gain of the amplifier also implicitly sets the on-chip oscillator startup time. The oscillation stability mainly depends on external parameters so only the transconductance (gm) can be guaranteed and the startup time value is defined by measurement at the application level. 1.2 Startup time Ceramic resonators have a much shorter startup time than crystals (about 100 times faster) but have a lower accuracy on the frequency (initial tolerance, temperature variations and drift). Depending on applications requirements and possibilities, users can choose between short oscillator startup time and frequency accuracy. From an ST10 perspective, the worst case condition / environment for the oscillator startup time is high temperature and low voltage. Table 1. gm values for different types of oscillators Symbol Parameter Version Conditions Value Unit Min Typ Max gm Oscillator transconductance Wide-swing 8 17 35 mA/V Low-power 1.4 2.6 4.2 32 kHz Startup 203150 µA/V Normal run 8 17 30 gm min Rs C 2 ×ω 2 × Rs C 2 × 2 π × f × () 2 × == |
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