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This level of noise is too small to be resolved at the scale used in these gures Instead, the lack of smoothness is caused by the gyro handling The gyros are speci ed for input rates of 90 deg ; therefore, the roll gyro s measuring p saturates for t [14827, 14837] This saturation causes error in the compute attitude, which the system is able to estimate and remove The curves in the top graph in Figure 104 show the roll and pitch angles as computed by the AHRS approach presented in this chapter It is natural to consider whether eqns (1014 1015) could be used throughout instead of the presented approach For comparison, the curves in the bottom graph of Figure 104 show the roll and pitch angles computed using eqns (1014 1015) Figure 105 magni es a portion of the time axis to allow a more detailed comparison Notice the following:

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versus IB curve is horizontal A small change in IB, in these portions of the curve, causes little or no change in IC But if the transistor is biased near the middle of the straight-line part of the curve in Fig 22-6, the transistor will work as a current amplifier The same situation holds for the curve in Fig 22-4 At some bias points, a small change in EB does not produce much, if any, change in IC; at other points, a small change in EB produces a dramatic change in IC Whenever we want a transistor to amplify a signal, it s important that it be biased in such a way that a small change in the base current or voltage will result in a large change in the collector current

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100 Ang rate, p, dps 50 0 50 100 100 Ang rate, q, dps 50 0 50 100 100 Ang rate, r, dps 50 0 50 100 0 50 100 Time, t, s 150 200 0 50 100 150 200 0 50 100 150 200

Figure 102: Angular rates while the IMU is being manipulated by hand as described in Section 108 The abbreviation dps indicates degrees per second The estimates attained by integrating the angular rates are signi cantly less noisy than those computed from (t) (t) = atan2 (g2 , g3 ) = atan2 g1 ,

Static Current Amplification Current amplification is often called beta by engineers It can range from a factor of just a few times up to hundreds of times The beta of a transistor can be expressed as the static forward current transfer ratio, abbreviated HFE Mathematically, this is the collector current divided by the base current:

(1068) (1069)

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where [g1 , g2 , g3 ] = xa (t) ya (t) The presented approach works well even near 90 degrees pitch, where eqns (1068 1069) become nearly singular To the extent that the designer is able to limit the Kalman lter measurement updates to times where the acceleration is nearly zero, the estimates obtained by integrating the angular rates are not a ected by vehicle acceleration Figure 106 displays information pertaining to the initialization of the AHRS system Throughout the time period of operation, the system maintains a ag which indicates true (ie, 1) when the vehicle is considered to

HFE = IC /IB For example, if a base current, IB, of 1 mA results in a collector current, IC, of 35 mA, then HFE = 35/1 = 35 If IB = 05 mA and IC = 35 mA, then HFE = 35/05 = 70 The HFE specification for a particular transistor represents the greatest amount of current amplification that can be obtained with it

10 Accel, u, m/s2 5 0 5 10 0 10 Accel, v, m/s2 5 0 5 10 0 10 Accel, w, m/s2 5 0 5 10 0 50 100 Time, t, s 150 50 100 150 50 100 150

Dynamic Current Amplification A more practical way to define current amplification is as the ratio of the difference in IC to the difference in IB that occurs when a small signal is applied to the base of a transistor Abbreviate the words the difference in by d Then, according to this second definition:

Figure 103: Gravity estimate gb = ya be non-accelerating and false (ie, 0) when the vehicle is considered to be accelerating At time t, based on the IMU data, this ag is de ned to be true when the logical condition (t) < and u(t) < g and f (t) < f (1070)

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