Kevin and Kyra Moon EE 670 December 1 2011 Background Motivation Problem Theoretical model for backscatter Simulations Estimators ML MAP Example of estimators Results Conclusion Outline ID: 675572
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Slide1
Prediction of permittivity using received backscatter values on Greenland
Kevin and Kyra Moon
EE 670
December 1, 2011Slide2
BackgroundMotivation
Problem
Theoretical model for backscatterSimulationsEstimatorsMLMAPExample of estimatorsResultsConclusion
OutlineSlide3
To get an “image” of the ground, a radar or satellite sends out an electromagnetic wave and measures the return it receives from the ground
The returned value is called “backscatter”, or
.There are many different factors affecting the brightness of
Roughness of surface
Conductivity of surface
BackgroundSlide4
In the highest
part of Greenland, the snow never melts
Called the dry snow zoneUsed frequently for calibration purposesHowever, some annual variation in the backscatter has been detected which is consistent from year to yearBackgroundSlide5
This variation cannot be caused by melt because it does not drop below a specific threshold
Temperatures are typically between
However, it is possible that increasing temperatures do change the permittivity of the snow, thus changing the backscatter
Annual variationSlide6
We decided to test if received backscatter values could predict changes in permittivityThe answer to this would provide insight into possible causes for the annual variation
If backscatter cannot predict changes in permittivity, then it is likely there are other factors affecting the annual variation
ProblemSlide7
We created a model relating permittivity to backscatter (at least for snow)Because knowing the temperature helps us predict the permittivity more accurately, we found a relationship between temperature and permittivity
This model required an intermediate step relating temperature to snow density and snow density to permittivity
Theoretical Model Slide8
The equations for our model were
(temperature to density)
(this is approximately linear)
(density to permittivity)
really complicated (several lines of equations)
Theoretical ModelSlide9
Theoretical ResultsSlide10
We then ran a simulation to see if backscatter could predict permittivity.We assumed that the underlying temperature data was weighted based on real data
SimulationSlide11
Randomly generated temperatures using the histogramNormalized the histogram
Calculated the
cumulative distribution functionGenerated uniformly distributed random numbers between 0 and 1Assigned each random number the temperature value corresponding to the same index as the closest value of the cdf that was still less than the random number
SimulationSlide12
For a given temperature, the snow density, permittivity, and corresponding backscatter were calculated using the earlier equations
The backscatter was then corrupted with additive white Gaussian noise
This simulated real noise between the ground and the satellite receiver, including atmospheric and instrumental noiseSimulationSlide13
To estimate the actual permittivity using the noisy received backscatter
, we used two decision rules
ML: We assumed each permittivity was equally likely
MAP: We assumed each permittivity was weighted according to the histogram (since permittivity is a function of temperature)
EstimationSlide14
The maximum likelihood rule is
That is, we choose the value of permittivity which makes receiving
most likely.
Since
is a function of permittivity, this is equivalent to
Maximum Likelihood (ML)Slide15
The goal is to choose
, because that will give us the correct permittivity
Note that
, where
is a Gaussian random variable with 0 mean and variance related to SNR (white noise)
Hence,
This is a Gaussian random variable
Maximum LikelihoodSlide16
To maximize this probability, the ML rule tells us to minimize the distance between
and
If the noise didn’t move
too far from
, then this will give us the correct backscatter
The permittivity corresponding to the estimated backscatter is chosen to be
.
Maximum LikelihoodSlide17
The maximum a-posteriori rule is
We no longer assume that every permittivity is equally likely
This makes more sense given the distribution of temperatures
Maximum a-posteriori (MAP)Slide18
The derivation for MAP estimation is similar to that of ML
When we reach
,
rather than just choosing
which minimizes the distance
, we choose
which maximizes that constraint
and
is deemed likely by the histogram.
Maximum a-posterioriSlide19
MAP vs
ML example
(or equivalently, permittivity or backscatter)
True value
Received value
What ML would estimate (minimize distance from received)
What MAP would estimate (this value is a lot more likely, even if the distance from received is further)Slide20
Results at 13 dB of SNRSlide21
MAP has superior performance to ML because there is more information availableHowever, neither estimator is a good predictor of permittivity based on received backscatter values
It is likely that the annual variation noticed in Greenland is caused by more than just changes in permittivity
Conclusions