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DP8464B Datasheet(PDF) 12 Page - National Semiconductor (TI) |
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DP8464B Datasheet(HTML) 12 Page - National Semiconductor (TI) |
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12 / 26 page ![]() Application Information (Continued) This time can be decreased by placing an external resistor across the CAGC For instance if a 100k resistor is placed in parallel with CAGC then the discharge current is 40 mA The time required to increase the amplifier gain is now 40 times faster or 275 ms If this external resistor is made even small- er say 10k then the discharge time will go to 275 ms Now however there is another problem introduced The re- sponse time of the AGC is so fast that it distorts the signal at the output of the Gain Controlled Amplifier Distortion of the signal at the Amplifier Output can affect the time posi- tion of the peaks of this signal Be sure to check this distor- tion over the range of input levels you expect to encounter when choosing the external R and C values for the AGC If the value of the bleed resistor across the CAGC is de- creased (in order to equalize the AGC attack and decay times) the value of CAGC must be increased in order to maintain an AGC response that does not distort the signal There is a second order effect on the amplitude that results from this attack and decay time equalization Referring to Figure 2 notice that the AGC is driven from a full wave rectified version of the Gate Channel Input signal When the AGC is operated normally (ie fast attack and slow decay) the voltage that appears across CAGC is the peak detected value of this full wave rectified waveform However if you equalize the AGC attack and decay times the voltage across CAGC is the RMS voltage (0707 times the peak) of the full wave rectified waveform Thus the voltage across CAGC is less and the amplitude out of the Gain Controlled Amplifier will consequently be 14 times larger It is possible to externally drive the CAGC pin to control the gain of the amplifier It must be noted that the gain of the amplifier is not always exactly 200 when the voltage on CAGC is 34V The transfer curve between the gain of the amplifier and the voltage on CAGC is only approximate This transfer curve will vary between parts and with temperature Care should be taken to prevent the voltage on the CAGC pin from going below ground or above 55V Figure 7 shows a typical curve of the Gain Controlled Amplifier Gain vs the voltage across CAGC (Vpin 16) TLF5283 – 12 FIGURE 7 Gain Controlled Amplifier Gain vs Vpin 16 It is possible to change the time constant of the AGC circuit by switching in different external components at the desired times For instance as shown in Figure 8 an external open collector TTL gate and resistor can be added in parallel with CAGC to decrease the AGC response time Similarly an ex- ternal capacitor could be switched in to increase the re- sponse time Since in the absence of an external resistor the discharge time of CAGC is much longer than the attack time there may be some applications where it is desirable to switch in a parallel resistor to quickly discharge CAGC then switch it out to force a quick attack Because of the quick attack time the AGC obtains the proper level quicker than it would had CAGC simply been allowed to discharge to the new level There are some applications where it is desirable to hold the AGC level for a period of time This can be done by raising the READ WRITE pin This will shut off the input circuitry and it will take time (about 25 ms) for the circuit to recover when going back into the read mode Figure 9 shows a method to hold the AGC level while remaining in the read mode (which could be used in embedded servo applica- tions) If the voltage on VREF is raised to 3V then the ampli- fier output voltage cannot get large enough to turn on the circuitry to charge up CAGC For this to work properly there can not be a large discharge current path (resistor in parallel with CAGC) across CAGC The AGC block can be bypassed altogether by connecting VREF to 3V In this way the user can use his own AGC circuit to drive the CAGC pin directly TLF5283 – 13 FIGURE 8 Circuit to Decrease AGC Response Time TLF5283 – 14 FIGURE 9 Circuit for AGC Hold READ WRITE In the normal read mode the signal from the readwrite head amplifier is in the range of 20 mVpp to 660 mVpp However when data is being written to the disk the signal coming into the analog input of the pulse detector will be on the order of 600 mV Such a large signal will disturb the AGC level and would probably saturate the amplifier In ad- dition if a different readwrite amplifier is selected there will be a transient introduced because the offset of the pream- plifiers are not matched A READ WRITE input pin has been provided to minimize these effects to the pulse detec- tor This is a standard TTL input When the READ WRITE pin is low the pulse detector is in the read mode When the READ WRITE pin is taken high three things happen First the 1k resistors across the AMP IN pins are shunted by 300X resistors as described previ- ously in the Gain Controlled Amplifier section Next the am- plifier is squelched so there is no signal on the Amp Output 12 |
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