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order of the filter design, or number of poles, is also a filter parameter. High-order filters,<br />

in general, have more freedom in filter design, giving better magnitude characteristics at<br />

the expense of design difficulty (Skolnick & Levine, 1997) and larger time lag; the slope<br />

of a filter’s transfer function phase is the time lag.<br />

If an 8-pole, elliptic-type AA filter along with 16-bit ADC is employed as in many<br />

applications in civil engineering, the attenuation, A s is about -96 dB ( = ),<br />

and f sb<br />

is 1.28 times f c<br />

. Therefore, the sampling frequency is set about 2.56 times the<br />

highest frequency signal of interest. The combination of another type of AA filter and<br />

ADC with different resolution gives different values for the attenuation and the stopband<br />

cutoff frequency.<br />

A 4-pole, Butterworth low-pass filter with a cutoff frequency of 50 Hz was selected<br />

as the AA filter for the Berkeley Mote platform. The filter order and cutoff frequency were<br />

set in order to investigate concurrently the ‘Tadeo’ acceleration sensor board developed<br />

by Ruiz-Sandoval (2004) and the strain sensor board characteristics over a wide frequency<br />

range (i.e., 0-50 Hz), and to limit the associated time lag. A small time lag is important for<br />

applications with real-time response requirements, such as structural control and<br />

triggering smart sensor tasks based on the measurement; high filter order and a low cutoff<br />

frequency result in large deterministic time lags. From the AA perspective, this 4-pole<br />

filter cannot completely eliminate aliasing for Mica2’s 10-bit ADC when sampled at 100<br />

or 250 Hz. f sb<br />

for a 10-bit ADC is around 230 Hz. The noise is, however, unlikely to have<br />

an amplitude as large as the ADC’s input range. Small noise components below f sb<br />

and all<br />

of the components above are completely eliminated by this filter.<br />

f sb<br />

There are three major designs to implement the AA filter as an electrical circuit: (a)<br />

passive filter, (b) active filter, and (c) switched capacitor filter designs (National<br />

Semiconductor, 1991). A passive filter is made up of passive components without<br />

amplifiers, i.e., resistors, capacitors, and inductors. Though having a small noise level,<br />

being free from power supply, and having the capability to deal with a large voltage and<br />

current are advantages of this filter design, inflexibility in the design of the filter is<br />

detrimental. Active filter designs employ operational amplifiers, eliminating the need for<br />

the hard-to-handle inductors, and have more flexibility in design. The noise level is higher<br />

than that of the passive design, but it is still moderate. Switched-capacitor filters are<br />

clocked, sampled-data systems widely available in monolithic form. The cutoff frequency<br />

is typically set by an external clock frequency. This filter has design flexibility, a variable<br />

cutoff frequency, and insensitivity to temperature change. Poor DC precision and high<br />

noise level, however, need to be addressed by additional external circuits, according to<br />

application requirements. Frequency components higher than half the clock frequency<br />

cannot be eliminated by this filter; they need to be eliminated with passive or active filters.<br />

In this research, an active design was employed because of its design flexibility, moderate<br />

noise level, and good DC precision.<br />

A 4-pole Butterworth filter was realized by the Sallen-Key active filter design (Sallen<br />

& Key, 1955), as shown in Figure 4.5. Rail-to-rail input/output amplifiers, MAX4132<br />

(Maxim Integrated Products, Inc., 2007), give the filter a rail-to-rail input/output property,<br />

which results in the efficient use of the input/output voltage range. The cutoff frequency<br />

45

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