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12 A foam-like material, having a resistance that varies depending on how much it is compressed, is known as (a) an elastomer (b) a fluxgate magnetometer (c) a piezoelectric substance (d) none of the above 13 A stepper motor (a) has torque that increases as its speed increases (b) resists applied torque when stopped with current going through its coils (c) has turning power that does not depend on the speed (d) is easily fooled by body capacitance 14 A permanent magnet is a key component of (a) an elastomer pressure sensor (b) a capacitive pressure sensor (c) a dynamic microphone (d) a piezoelectric microphone 15 An electric motor is an example of (a) an electromechanical transducer (b) a pressure sensor (c) a proximity sensor (d) a texture sensor 16 A capacitive proximity sensor should not be expected to detect the presence of (a) a wooden chair (b) a metal desk (c) a large dog (d) a steel post 17 A well-designed photoelectric proximity sensor (a) is easily fooled by loud noises (b) cannot detect the presence of objects that reflect light (c) is sensitive to magnetic fields (d) is not easily fooled by stray sources of light 18 An acoustic transducer can translate an ac electrical signal into (a) visible light (b) sound or ultrasound (c) a dc electrical signal (d) mechanical torque

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Therefore, because the above derivation can be repeated over any interval of duration T for which the assumption of a constant angular rate is valid, we have the general equation b(tk ) = cos ( w ) I + sin ( w ) W b(tk 1 ) w (D36)

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where w, w and W involve the integral of the angular rates over the k-th sampling interval t (tk 1 , tk ] Note that no approximations were made in this derivation, so the solution is in closed form given the assumption that Q(t) is constant over the interval of length T The solution is easily veri ed to be norm preserving by showing that the norm of the right side of eqn (D36) is equal to b(tk 1 ) The algorithm is not an exact solution to the di erential equation over any interval where the angular rates are not constant In [73] the algorithm of eqn (D36) is shown to be second order and a third order algorithm is also presented The algorithm being second order means the algorithm error contains terms proportional to T 3 and higher powers Because T is small, higher order algorithms have smaller errors; however, the tradeo is that they require additional computation

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19 Body capacitance can be a problem with (a) electrostatic transducers (b) elastomer pressure sensors (c) capacitive pressure sensors (d) all of the above 20 Which of the following devices can be used to limit the torque or force applied by an electromechanical device such as a robot (a) A back-pressure sensor (b) A capacitive proximity sensor (c) A dynamic transducer (d) An optical shaft encoder

The following example clari es the singularity that occurs with the Euler angle representation of attitude as 2 Example D1 Consider the tangent to body direction cosine matrix corresponding to = : 2 0 0 1 c c + s s 0 Rb = s c + c s t s s + c c c s + s c 0 which is well de ned for any and However, there are multiple values of , ( , ] that yield the same orientation Consider two sequences of rotations For each, assume that the tangent and body frames are initially aligned The rst rotation sequence is de ned by a rotation of rads about the navigation frame y-axis to give ( , , ) = 2 (0, , 0) The second rotation sequence is de ned by a rotation about the 2 navigation frame z-axis by rads, rotation about the body frame y-axis 2 by rads, and then rotation about the vehicle x-axis by rads to yield 2 2 ( , , ) = ( , , ) Both of these rotation sequences result in the same 2 2 2 vehicle orientation For each of these rotation sequences the angular rate vectors in body frame are well de ned In the rst case, eg, (p, q, r) = (0, 90, 0)deg/s for 10s In the second case, eg: (p, q, r) = (p, q, r) = (p, q, r) = 0, 0, 0, rad/s for t [0, 1)s 2

other considerations In these applications, low distortion and sound esthetics are more important than amplifier efficiency or gain In this chapter, we ll look at basic acoustics principles, and outline some high-fidelity (hi-fi) components and design concepts

In both cases, the matrix E involved in the computation of the Euler angle derivatives of eqn (274) on page 57 becomes singular For the 2 matrix 1 is large (potentially in nite) which can greatly magnify sensor E errors in the computation of the Euler angle derivatives The following example considers the motion similar to that of the previous example in the sense that the vehicle is maneuvering near = rad, 2 but using a quaternion implementation Example D2 For the initial condition ( , , ) = (0, 0, 0), the initial quaternion is b(0) = [1, 0, 0, 0] Figure D1 shows the body frame angular rates [p, q, r] The quaternion that results from the integration of either eqn (D28) or (D30) is plotted

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