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AN2867 数据表(PDF) 9 Page - STMicroelectronics |
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AN2867 数据表(HTML) 9 Page - STMicroelectronics |
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9 / 41 page ![]() DocID15287 Rev 9 9/41 AN2867 Oscillator theory 40 The part of the I-V curve represented in purple shows a negative transresistance: while the parts of the curve in blue shows a positive transresistance: Figure 3. I-V curve of a dipole showing a negative transresistance area (in purple) 2.2 Transconductance Like the conductance which is defined as the inverse of the resistance, the transconductance is also defined as the inverse of the transresistance. Transconductance can also be defined as the differential conductance which expressed by the formula: 2.3 Negative-resistance oscillator principles An oscillation loop is made of two branches (see Figure 4): • The active branch of the oscillation loop which is composed of the oscillator itself. This branch is responsible for providing enough energy at startup to make the oscillation start and build up until it reaches the stable oscillation phase. When a stable oscillation is reached, the oscillator branch provides enough energy to compensate for the oscillation loop passive branch losses. • The passive branch is mainly composed of the resonator, the two load capacitors and all the parasitic capacitances. ΔV ΔI -------- VD () VC () – ID () IC () – --------------------------------- 0 < = ΔV ΔI -------- VB () VA () – IB () IA () – -------------------------------- 0 > = ΔV ΔI -------- |
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