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AN2867 Datasheet(PDF) 10 Page - STMicroelectronics |
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AN2867 Datasheet(HTML) 10 Page - STMicroelectronics |
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10 / 41 page ![]() Oscillator theory AN2867 10/41 DocID15287 Rev 9 Figure 4. Block diagram of a typical oscillation loop based on a crystal resonator Following the small signals theory and when the active branch (oscillator part) is correctly biased, the latter should have its transconductance equal to the passive branch conductance in order to maintain a stable oscillation around the oscillator biasing voltage. However, at startup, the oscillator transconductance should be higher than (multiple of) the conductance of the passive part of the oscillation loop to maximize the possibility to build up the oscillation from inherent noise of the oscillation loop. Please note that an excessive oscillator transconductance compared to the oscillation loop passive branch conductance may also saturate the oscillation loop and cause a startup failure. In order to ensure the oscillator ability to startup successfully and maintain stable oscillation, a ratio between the negative resistance of the oscillation loop and the crystal maximal equivalent series resistance (ESR) is specified: for STM32 and STM8 microcontrollers, it is recommended to have a ratio higher than x5 for the HSE oscillators and higher than x3 for the LSE oscillators. |
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