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TMCS1101 Datasheet(PDF) 11 Page - Texas Instruments |
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TMCS1101 Datasheet(HTML) 11 Page - Texas Instruments |
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11 / 31 page ![]() EXT EXT B B I G OUT EXT Hall V IN Hall V OUT,0A V B * S * A I * G * S * A V Hall V S G * S * A NL NL FS V e 100% * V 11 TMCS1101 www.ti.com SBOS825 – SEPTEMBER 2019 Product Folder Links: TMCS1101 Submit Documentation Feedback Copyright © 2019, Texas Instruments Incorporated Accuracy Parameters (continued) (8) 8.1.4 External Magnetic Field Errors The TMCS1101 does not have stray field-rejection capabilities, so external magnetic fields from adjacent high- current traces or nearby magnets can impact the output measurement. The total sensitivity (S) of the device is comprised of the initial transformation of input current to magnetic field quantified as the magnetic coupling factor (G), as well as the sensitivity of the Hall element and the analog circuitry that is factory calibrated to provide a final sensitivity. The output voltage is proportional to the input current by the device sensitivity, as defined in Equation 9. where • S is the TMCS1101 sensitivity in mV/A. • G is the magnetic coupling factor in mT/A. • SHall is the senitivity of the Hall plate in mV/mT. • AV is the analog circuitry gain in V/V. (9) An external field, BEXT, is measured by the Hall sensor and signal chain, in addition to the field generated by the leadframe current, and is added as an extra input term in the total output voltage function: (10) Observable from Equation 10 is that the impact of an external field is an additional equivalent input current signal, IBEXT, shown in Equation 11. This effective additional input current has no dependence on Hall or analog circuitry sensitivity, so all gain variants have equivalent input-referred current error due to external magnetic fields. (11) |
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