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L4916 Scheda tecnica(PDF) 4 Page - STMicroelectronics |
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L4916 Scheda tecnica(HTML) 4 Page - STMicroelectronics |
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4 / 8 page ![]() Figure 2 : P.C. Board and Component Layout of Fig. 1 (1 : 1 scale). PRINCIPLE OF OPERATION During normal operation (input voltage upper than VI MIN =VOUT NOM + ∆VI/O). The device works as a normal voltage regulator built aroundthe OP1 of the block diagram. The series pass element use a PNP-NPN connec- tion to reduce the dropout. The reference voltage of the OP1 is derived from a REF through the OP2and Q3, acting as an active zener diode of value VREF. In this condition the device works in the range (1) of the characteristic of the non linear drop control unit (see fig.3). The output voltage is fixed to its nominal value: R1 VOUT NOM =VREF (1 + ) = R2 R1 VCFT (1 + ) R2 R1 = INTERNALLY FIXED RATIO = 2.4 R2 The ripple rejection is quite high (70 dB) and inde- pendent from CFT value. On the usual voltage regulators, when the input vol- tage goes below the nominal value, the regulation transistors (series element) saturate bringing the system out of regulation making it very sensible to every variation of the input voltage. On the contrary, a control loop on the L4916 consents to avoid the saturation of the series element by regulating the value of the reference voltage (pin 2). In fact, when- ever the input voltage decreases below VI MIN the supervisor loop, utilizing a non linear OTA, forces the reference voltage at pin 2 to decrease by dis- charging CFT. So, during the static mode, when the input voltage goes below VMIN the drop out is kept fixed to about 1.6V. In this condition the device works as a low pass filter in the range (2) of the OTA characteristic. The ripple rejection is externally ad- justable acting on CFT as follows : VI (jw) SVR (jw) = = Vout (jw) 10 -6 1+ gm R1 (1 + ) jwCFT R2 Where: gm = 2 . 10 -5 Ω-1 =OTA’S typical transconductance value on linear region R1 = fixed ratio R2 CFT = value of capacitor in µF The reaction time of the supervisor loop is given by the transconductanceof the OTA and by CFT. When the value of the ripple voltage is so high and its ne- gative peak is fast enough to determine an istanta- neous decrease of the dropout till 1.2 V, the OTA works in a higher transconductance condition [range (3) of the characteristic] and discharge the capacitor rapidously. If the ripple frequency is high enough the capacitor won’t charge itself completely, and the output volt- age reaches a small value allowinga betterripple re- jection ; the device’s again working as a filter (fast transient range). With CFT =10 µF; f= 100Hz a SVRof35is obtained. L4916 4/8 |
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