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Prediction of permittivity using received backscatter values on Greenland Kevin and Kyra Moon EE 670 December 1, 2011

Kevin and Kyra Moon EE 670 December 1, 2011. Background ◦ Motivation ◦ Problem Theoretical model for backscatter Simulations Estimators ◦ ML ◦

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Prediction of permittivity using received backscatter

values on GreenlandKevin and Kyra Moon

EE 670December 1, 2011

Background◦ Motivation◦ Problem

Theoretical model for backscatter Simulations Estimators

◦ ML◦ MAP

Example of estimators Results Conclusion

Outline

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

Background

In the highest part of Greenland, the snow never melts◦ Called the dry snow zone◦ Used frequently for calibration purposes

However, some annual variation in the backscatter has been detected which is consistent from year to year

Background

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 variation

We decided to test if received backscatter values could predict changes in permittivity

The 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

Problem

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

The equations for our model were (temperature to density)

(this is approximately linear)

(density to permittivity)

really complicated (several lines of equations)

Theoretical Model

Theoretical Results

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

Simulation

Randomly generated temperatures using the histogram◦ Normalized the histogram◦ Calculated the cumulative distribution function◦ Generated uniformly distributed random numbers

between 0 and 1◦ Assigned 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

Simulation

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 noise

Simulation

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)

Estimation

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)

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 Likelihood

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 Likelihood

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)

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-posteriori

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)

Results at 13 dB of SNR

MAP has superior performance to ML because there is more information available

However, 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