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AN2353 Datasheet(PDF) 5 Page - STMicroelectronics |
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AN2353 Datasheet(HTML) 5 Page - STMicroelectronics |
5 / 18 page AN2353 Oscillator 5/18 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 start-up time. The oscillation stability mainly depends on external parameters so only the transconductance (gm) can be guaranteed and the start-up time value is defined by measurement at the application level. 1.2 Start-up time Ceramic resonators have a much shorter start-up 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 start-up time and frequency accuracy. From an ST10 perspective, the worst case condition / environment for the oscillator start-up 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 0.7 2.5 6 32 kHz Start-up 20 31 50 µ A/V Normal run 8 17 30 gm min Rs C 2 ×ω 2 × Rs C 2 × 2 π × f × () 2 × == |
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