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LOG101 数据表(PDF) 9 Page - Texas Instruments |
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LOG101 数据表(HTML) 9 Page - Texas Instruments |
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9 / 16 page ![]() www.ti.com LOG101 9 SBOS242B TOTAL ERROR The total error is the deviation (expressed in mV) of the actual output from the ideal output of VOUT = 1V • log (I1/I2). Thus, VOUT(ACTUAL) = VOUT(IDEAL) ± Total Error. It represents the sum of all the individual components of error normally associated with the log amp when operated in the current input mode. The worst-case error for any given ratio of I1/I2 is the largest of the two errors when I1 and I2 are considered separately. Temperature can affect total error. ERRORS RTO AND RTI As with any transfer function, errors generated by the func- tion itself may be Referred-to-Output (RTO) or Referred-to- Input (RTI). In this respect, log amps have a unique property: Given some error voltage at the log amp’s output, that error corresponds to a constant percent of the input regardless of the actual input level. USING A LARGER REFERENCE VOLTAGE REDUCES OFFSET ERRORS Using a larger reference voltage to create the reference current minimizes errors due to the LOG101’s input offset voltage. Maintaining an increasing output voltage as a func- tion of increasing photodiode current is also important in many optical sensing applications. All zeros from the A/D converter output represent zero or low-scale photodiode current. Inputting the reference current into I1, and designing IREF such that it is as large or larger than the expected maximum photodiode current is accomplished using this requirement. The LOG101 configured with the reference current connecting I1 and the photodiode current connecting A 1 A 2 LOG101 Q 1 Q 2 OPA703 R 2 R 3 R 2 6 R 3 C C V OUT V REF I REF I REF = I MIN to IMAX V REF R 1 V OUT = VREF – • (1V)LOG ( ) R 2 R 3 I REF I PHOTO I 1 I 2 8 1 I PHOTO A/D Converter R 1 V MIN to VMAX 3 FIGURE 13. Technique for Using Full-Scale Reference Current Such that VOUT Increases with Increasing Photodiode Current. to I2 is shown in Figure 13. The OPA703 is configured as a level shifter with inverting gain and is used to scale the photodiode current directly into the A/D converter input voltage range. The wide dynamic range of the LOG101 is also useful for measuring avalanche photodiode current (APD) (see Figure 14). LOG CONFORMITY For the LOG101, log conformity is calculated the same as linearity and is plotted I1/I2 on a semi-log scale. In many applications, log conformity is the most important specifica- tion. This is because bias current errors are negligible (5pA compared to input currents of 100pA and above) and the scale factor and offset errors may be trimmed to zero or removed by system calibration. This leaves log conformity as the major source of error. Log conformity is defined as the peak deviation from the best fit straight line of the VOUT versus log (I1/I2) curve. This is expressed as a percent of ideal full-scale output. Thus, the nonlinearity error expressed in volts over m decades is: VOUT(NONLIN) = 1V/dec • 2NmV where N is the log conformity error, in percent. INDIVIDUAL ERROR COMPONENTS The ideal transfer function with current input is: VV I I OUT = ( ) • 1 1 2 log The actual transfer function with the major components of error is: VV K II II Nm V OUT B B OS O = ( ) ± ( ) ±± 11 2 11 22 ∆ log – – (6) (7) (8) (9) |
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