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A1360 Datasheet(PDF) 23 Page - Allegro MicroSystems |
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A1360 Datasheet(HTML) 23 Page - Allegro MicroSystems |
23 / 25 page ![]() A1360, A1361, and A1362 The flux density measured by the A136x SIP is related to the size of the gap cut into the core. The larger the gap in the core, the smaller the flux density per ampere of applied current (see figure 8). Figure 9 depicts the magnetic flux density through the center of the SIP as a function of SIP to core alignment. Note that a core with a larger cross-sectional area would reduce the attenuation in flux density that results from any SIP misalignment. The flat portion of the curve in figure 9 would span a larger distance in millimeters if the cross-sectional area of the core were increased. Wire +B mm –2 2 0 Ring concentrator Magnetic flux in gap Measurement plane (midplane of gap) Figure 9. Side view of example current-conducting wire and split ring concentrator (left), and magnetic profile (right) through the midplane of the gap in the split ring concentrator. The flux denisty through the center of the gap varies between the inside and the outside of the gap. 7.0 6.5 6.0 5.5 5.0 4.5 4.0 3.5 3.0 –2.0 Radial Displacement from Concentrator Centerline (mm) Interior side of Concentrator Exterior side of Concentrator –1.0 1.0 2.0 0 Figure 8. The flux density per ampere measured by the A136x Hall sen- sor IC is related to the core gap, as shown. This figure assumes that the current sensing application is constructed using the example setup. Flux Density per Ampere vs. Gap for a Feedthrough Sensor 0 2 4 6 8 10 12 14 0.5 1 1.5 2 2.5 3 3.5 Gap (mm) Low-Noise Programmable Linear Hall Effect Sensor ICs with Adjustable Bandwidth (50 kHz Maximum) and Analog Output 23 Allegro MicroSystems, Inc. 115 Northeast Cutoff Worcester, Massachusetts 01615-0036 U.S.A. 1.508.853.5000; www.allegromicro.com |
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