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TMCS1101 Datasheet(PDF) 19 Page - Texas Instruments |
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TMCS1101 Datasheet(HTML) 19 Page - Texas Instruments |
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19 / 31 page ![]() OS EXT 2 2 2 2 RSS I PSRR CMRR B S NL e (%) e e e e e e OS, T EXT worst, T I PSRR CMRR B S, T NL e (%) e e e e e e ' ' ' OS EXT worst I PSRR CMRR B S NL e (%) e e e e e e T S S S,drift S,FT e (%) min e e * 1000 * T;e ' ª º ' ¬ ¼ OS, T OS,RT OS,drift OS,FT I IN min I I * T;I e (%) I ' ª º ' ¬ ¼ EXT EXT B IN B G e (%) I S PSRR IN PSRR * (V 5) e (%) I CM CMRR IN CMRR * V e (%) I OS OS I IN I e (%) I 19 TMCS1101 www.ti.com SBOS825 – SEPTEMBER 2019 Product Folder Links: TMCS1101 Submit Documentation Feedback Copyright © 2019, Texas Instruments Incorporated Application Information (continued) 10.1.1 Total Error Calculation Examples Total error can be calculated for any arbitrary device condition and current level. Error sources considered should include input-referred offset current, power-supply rejection, input common-mode rejection, sensitivity error, nonlinearity, and the error caused by any external fields. Compare each of these error sources in percentage terms, as some are significant drivers of error and some have inconsequential impact to current error. Offset (Equation 18), CMRR (Equation 19), PSRR (Equation 20), and external field error (Equation 21) are all referred to the input, and so, are divided by the actual input current IIN to arrive percentage errors. For calculations of sensitivity error and nonlinearity error, the percentage limits explicitly specified in the Electrical Characteristics table can be used. (18) (19) (20) (21) When calculating error contributions across temperature, only the input offset current and sensitivity error contributions vary significantly. In both cases, specifications for both the maximum device temperature range and the parameter drift across temperature are provided. For determining actual performance limits across a narrower temperature range than the specified –40°C to +125°C, use Equation 22 and Equation 23 for offset error and sensitivity error, respectively. In both of these calculations, the maximum specified drift for the parameter can be multiplied by the desired temperature deviation from room temperature (ΔT). Use the smaller value of this drift calculation and the specified range over the full temperature range. The sensitivity drift (eS,drift) is specified in ppm/°C, and must be converted to percentage error. (22) (23) In order to accurately calculate the total expected error of the device, the contributions from each of the individual components above must be understood in reference to operating conditions. There are two separate ways to calculate total error for any particular system. In a worst case scenario, each error term would be at its absolute maximum with the same polarity. In such a case, the total system error would be a mathematical summation of each individual error source, as shown in Equation 24 for room temperature. For across temperature worst case error, the input referred offset and sensitivity error for the relevant range should be substituted in place of the room temperature values, as in Equation 25. (24) (25) Because the statistical probability of any device actually existing in this worst case corner is insignificant, a better methodology is to use a root sum squared (RSS) calculation for uncorrelated error sources. This method takes into account the statistically uncorrelated nature of the individual error terms to provide a more realistic total error based on the distributions of each error component. For the TMCS1101, only the input referred offset current (IOS), CMRR, and PSRR are statistically correlated. These error terms are lumped in an RSS calculation in order to reflect this nature, as shown in Equation 26 for room temperature and Equation 27 for across a given temperature range. (26) |
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