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Sensors and Methods for Mobile Robot Positioning

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48 Part I <strong>Sensors</strong> <strong>for</strong> <strong>Mobile</strong> <strong>Robot</strong> <strong>Positioning</strong><br />

steel. In actuality, due to hysteresis, µ depends not only on the current value of H, but also the<br />

history of previous values <strong>and</strong> the sign of dH/dt, as will be seen later. The important thing to note<br />

at this point in the discussion is the B-H curve is not linear, but rather starts off with a fairly steep<br />

slope, <strong>and</strong> then flattens out suddenly as H reaches a certain value. Increasing H beyond this “knee”<br />

of the B-H curve yields little increase in B; the material is effectively saturated, with a near-zero<br />

permeability.<br />

Figure 2.14: The slope of the B-H curve, shown here <strong>for</strong> cast iron <strong>and</strong><br />

sheet steel, describes the permeability of a magnetic material, a<br />

measure of its ability (relative to air) to conduct a magnetic flux.<br />

(Adapted from [Carlson <strong>and</strong> Gisser, 1981].)<br />

When a highly permeable material is introduced into a uni<strong>for</strong>m magnetic field, the lines of <strong>for</strong>ce<br />

are drawn into the lower resistance path presented by the material as shown in Figure 2.15.<br />

However, if the material is <strong>for</strong>ced into saturation by some additional magnetizing <strong>for</strong>ce H, the lines<br />

of flux of the external field will be relatively unaffected by the presence of the saturated material,<br />

as indicated in Figure 2.15b. The fluxgate magnetometer makes use of this saturation phenomenon<br />

in order to directly measure the strength of a surrounding static magnetic field.<br />

Various core materials have been employed in different fluxgate designs over the past 50 years,<br />

with the two most common being permalloy (an alloy of iron <strong>and</strong> nickel) <strong>and</strong> mumetal (iron, nickel,

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