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The ADXL202 is a true accelerometer, easily capable of shock/vibration sensing with virtually no external signal conditioning circuitry Since the ADXL202 is also sensitive to static (gravitational) acceleration, tilt sensing is also possible Tilt sensing requires a very low noise oor which usually necessitates restricting the bandwidth of the accelerometer, while shock/vibration sensing requires wide bandwidth These con icting requirements may be met using clever design techniques Principle of Operation The ADXL202 is set up to acquire acceleration from 0 to 200 Hz (the maximum frequency of interest) Figure 1564 shows a block diagram of the system The accelerometer s output is fed into two lters; a low pass lter with a corner frequency at 125 Hz used to lower the noise oor suf ciently for accurate tilt sensing, and a band pass lter to minimize the noise in the shock/vibration pass band of interest The low pass ltered (tilt) output then goes to a differentiator (described in the Tilt Sensing section) where the determination is made as to whether the accelerometer actually sensed tilt or some other event such as noise or temperature drift Then an auto-zero block performs further signal processing to reject temperature drift The band pass ltered output goes to an integrator (described in the Shock Sensing section) that measures vibrational energy over a small period of time (40 ms) A decision as to whether or not to set off the alarm may then be made by the microcontroller Most of these tasks are most easily implemented in the digital domain and require very little computational power

Since the two measurements (shock/vibration and tilt) are basically exclusive and only share a common sensor, their respective signal processing tasks will be described separately Tilt Sensing Fundamentals The alarm system must detect a change in tilt slow enough to be the result of the vehicle being towed or jacked up, but must be immune to temperature changes and movement due to passing vehicles or wind Note that the ADXL202 is most sensitive to tilt when its sensitive axes are perpendicular

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FiSMA From the FiSMA 11 Functional Size Measurement Method document the major steps are summarized as follows:

+ ~ 1556 cos (377t)

71 Show that the equalities in equation 79 hold when phasor notation is used 72 Consider the circuit shown in Figure 710 Find the load impedance of the circuit,

SETTING A REFERENCE TO THE VB .NET NAMESPACE FROM C#

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and compute the average power dissipated by the load 73 Use the expression Pav = I 2 |Z| cos to compute the average power dissipated by the load of Example 72

74 Compute the power dissipated by the internal source resistance in Example 72 75 Compute the power factor for an inductive load with L = 100 mH and R = 04

The expression for the instantaneous power given in equation 73 may be further expanded to provide further insight into AC power Using trigonometric identities, we obtain the following expressions: p(t) = V2 [cos + cos cos(2 t) + sin sin(2 t)] |Z| (722)

= I 2 |Z|[cos + cos cos(2 t) + sin sin(2 t)] = I 2 |Z| cos (1 + cos(2 t)) + I 2 |Z| sin sin(2 t)

1 Gather documentation and software development artifacts to describe the functional user requirements for the software (to be or already) developed 2 Determine the scope of the functional size measurement 3 Determine which are the functional user requirements to be measured 4 Identify the base functional components within the functional user requirements in two main parts: (a) measuring the enduser interface services, and (b) measuring indirect services 5 Classify the base functional components into the appropriate base functional component type services 6 Assign the appropriate numeric value to each base functional component 7 Calculate the functional size 8 Document the instance of the FiSMA 11 count details

Recalling the geometric interpretation of the impedance Z of Figure 74, you may recognize that |Z| cos = R and |Z| sin = X are the resistive and reactive components of the load impedance, respectively On the basis of this fact, it becomes possible to write the instantaneous power as: p(t) = I 2 R(1 + cos(2 t)) + I 2 X sin(2 t) = I 2 R + I 2 R cos(2 t) + I 2 X sin(2 t) (724) (723)

In order to access VB routines from C# code (such as the Shell() method mentioned in this chapter), execute the following steps from within a C# application: 1. Select Project Add Reference. The Add Reference dialog will display, as shown in Figure 5-7.

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