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TDA8140 数据表(PDF) 6 Page - STMicroelectronics |
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TDA8140 数据表(HTML) 6 Page - STMicroelectronics |
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6 / 10 page ![]() OFF PHASE CONTROL INPUT t I 0 ON PHASE t Ip0 I 0 t don In0 t S IS0 t S dI0 dt = IS0 Figure 6 During the active deflection phase the collector current of the power transistor is linearly rising and the driving circuitry must be adapted to the required base current in order to ensure the power transistor saturation. According to the limited components number the typical approach of the present TVs provides only a rough approximation of this objective ; in Figure 5 we give a comparison between the typical real base current and the ideal base current waveform and the collector waveform. The marked area represents a useless base cur- rent which gives an additional power dissipation on the power transistor. Furthermore during the turn-ON and turn-OFF tran- sient phase of the chassis the power transistor is extremely stressed when the conventional network cannot guarantee the saturation ; for this reason, generally, the driving circuit must be carefully de- signed and is different for each deflection system. The new approach, using the TDA 8140, over- comes these restrictions by means of a feedback principle. As shown in Figure 5, at each instant of time the ideal base current of the power transistor results from its collector current divided by such current gain which ensure the saturation ; thus the required base current Ib can be easily generated by a feed- back transconductance amplifier gm which senses the deflection current across the resistor Rs at the emitter of the power transistor and delivers : Ib = RS . gm . Ie The transconductance must only fulfill the condi- tion : 1 1 + βmin ⋅ 1 RS < gm < 1 RS Where βmin is the minimum current gain of the transistor. This method always ensures the correct base current and acts time independent on princi- ple. For the turn-OFF, the base of the power transistor must be discharged by a quasi linear time decreas- ing current as given in Figure 6. Conventional driver systems inherently result into a stable condition with a constant peak current magnitude. This is due to the constant base charge in the turn-ON phase independent from the collector cur- rent ; hence a high peak current results into a low storage time of the transistor because the excess base charge is a minimum and vice versa. In the active deflection the required function, high peak current-fast switch-OFF and low peak current-slow switch-OFF, is obtained by a controlled base dis- charge current for the power transistor ; the nega- tive slope of this ramp is proportional to the actual sensed current. As a result, the active driving system even im- proves the sharpness of vertical lines on the screen compared with the traditional solution due to the increased stability factor of the loop represented as the variation of the storage time versus the collector peak current. IC IC t t IBIAS D I t S Base Bias Current Off Phase On Phase Off Phase Real Base Current Ideal Base Current Figure 5 : Waveforms of Collector and Base Current TDA8140 6/10 |
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