Discussion
The only source of ambiguity in this technique was introduced by the
quantization noise of the received frequency. Sampling the received
frequency addressed this problem, but there was a tradeoff between
accuracy and usefulness of the derivative. Large sample period generated
smoother derivatives but distorted the amplitude information, while short
sample periods could not be used to determine the maximum amplitude. For
these reasons, a sample of period of 50 was found to be a good compromise.
This quantization noise introduced ambiguities in both the location of the peak
of the derivative and in the value of the peak of the derivative. These ambiguities
correspond to ambiguities in the latitude and longitude of the EPIRB respectively.
By taking a range of peak locations and values, our rms (root mean squared)
confidence interval was determined to be 150 km or approximately 1.3 degrees.
The confidence interval was determined by varying the quantization value and
calculating the rms difference for the distances.
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