lrowaccal

This program applies dark, flat-field, radiometric, and temperature corrections for each framelet based on the band's filter number. There is also an optional mask to replace special pixels in the calibrated image. In order to output in I/F units, the cube must have spice data.

Corrections are applied in the following order: Dark, Flat-field, Radiometric, Special pixel mask, and Temperature.

Dark Correction:

If the DarkFile parameter is set, the given file(s) will be used for calibration. If DarkFile is set to "Default" or not set at all, the dark files will be looked up based on the time and temperature in the WAC being calibrated. The parameter,MiddleTemperatureFpa, is used for temperature and StartTime for time. This program, lrowaccal, will attempt to find the 2 dark files with closest time/temperature and interpolate/extrapolate from them. The method for finding dark files is as follows:

• Create filename template based on WAC image offset and type (UV, BW, etc). Example: WAC_UV_Offset68_*C_*T_Dark.????.cub
• Look in $lro/calibration/wac_darks for matching files.
• Sort files on two factors:
  1. abs(dark temp - WAC temp)
  2. abs(dark time - WAC time)
• Example:
  WAC Temp = 23.33 and WAC Time = 314264519.932493
  
  WAC_UV_Offset68_-10C_319412928T_Dark.0005.cub
  WAC_UV_Offset68_-15C_319412928T_Dark.0005.cub
  WAC_UV_Offset68_-20C_311632116T_Dark.0005.cub
  WAC_UV_Offset68_-20C_319412928T_Dark.0005.cub
  WAC_UV_Offset68_-25C_319412928T_Dark.0005.cub
  WAC_UV_Offset68_-30C_311632116T_Dark.0005.cub
  
  becomes
  
  WAC_UV_Offset68_-25C_319412928T_Dark.0005.cub
  WAC_UV_Offset68_-20C_311632116T_Dark.0005.cub
  WAC_UV_Offset68_-20C_319412928T_Dark.0005.cub
  WAC_UV_Offset68_-30C_311632116T_Dark.0005.cub
  WAC_UV_Offset68_-15C_319412928T_Dark.0005.cub
  WAC_UV_Offset68_-10C_319412928T_Dark.0005.cub
  
• Take the 2 closest temperatures (-25C and -20C in the example).
• Select the closest time for each temperature.
  Example result:
  
  WAC_UV_Offset68_-25C_319412928T_Dark.0005.cub
  WAC_UV_Offset68_-20C_311632116T_Dark.0005.cub
  
• If only one temperature is available, the 2 times that are closest to the WAC time will be chosen. This will allow WACs to always be calibrated against something, instead of just failing.
  Example result:
  
  WAC_UV_Offset68_-20C_311632116T_Dark.0005.cub
  WAC_UV_Offset68_-20C_319412928T_Dark.0005.cub
  

Once the dark files are found, the correction is applied:

        output[pixel] -= (dark1[pixel] - dark2[pixel])/(dark1Temp - dark2Temp)*(frameTemp-dark2Temp) + dark2[pixel]
      

        dark1, dark2 = dark file cubes
        dark1Temp, dark2Temp = temperature of dark1 file and dark2 file
        frameTemp = (WAC EndTemperatureFpa - WAC BeginTemperatureFpa)/WAC NumFramelets * frame + WAC BeginTemperatureFpa
      

Flat-field Correction:

        output[pixel] /= flatfield[pixel]
      

Radiometric Correction:

      output[pixel] /= WAC ExposureDuration
      if radiometricType == iof
        output[pixel] *= solarDistance2 / iofResponsivity[band]
      else
        output[pixel] /= radianceResponsivity[band]
      

        solarDistance is distance from the Moon to the Sun
      

Special Pixel Mask:

      for each framelet in the output cube
        if specialPixelMask[pixel] is special
          outputFramelet[pixel] = specialPixelMask[pixel]
      

Temperature Correction:

        for each framlet in the output cube
          if output[pixel] is special- leave it alone
          else preform the correction
        

                inputPixel
            --------------------
             a*(frameTemp) + b

             Where:
               'a' and 'b' are band dependent constants, read in from a file.
             AND
               frameTemp = (WAC EndTemperatureFpa - WAC BeginTemperatureFpa)/WAC NumFramelets * frame + WAC BeginTemperatureFpa
      

The DN level in an uncalibrated image is the sum of the true signal from the scene, the bias, the dark current, and random noise in all 3 components. The random noise in the true signal and dark current is called shot noise and the random noise in the bias is called read noise. The true signal, bias, and dark current are defined as mean values so that if the random noise were averaged down to insignificance by taking a very large number of images and averaging them, the resulting image would be the true scene, bias, and dark current with no systematic error. That implies the statistical distribution of the random noise has an average of zero, and therefore the random noise has both positive and negative values, except for the trivial case of zero random noise.

The calibration equation is:

  reportedDN = ObservedDN - MeanBias - DarkCurrent 

   ObservedDN = TrueDN + E
   E is a randomly sampled value from (mu, sigma^2) and mu=0
   TrueDN is the signal that would be reported in an idealized case of an instrument with zero noise.

Let's look at the case of a calibrated image for which the true signal is zero, a dark image. In calibration the mean bias and dark current are subtracted. The random noise term is then randomly sampled from a known distribution with a mean of zero. Since the distribution has a mean of zero, values for the random noise can be positive or negative. Therefore, the addition of random noise to a pixel with true signal near zero can result in negative DN values.

Negative reported DNs are possible when E < -1 * TrueDN. These are pixels in a very dark image that happen to have a strongly negative random noise value.

Note: ObservedDN and TrueDN both must be greater than or equal to zero. For ObservedDN, it's because the hardware is not able to report negative DN values . For TrueDN, it's because radiance and reflectivity cannot be negative. The dimmest target is one that is completely dark, and for that target TrueDN = 0.

If run on a non-spiceinited cube, this program requires access to local mission-specific SPICE kernels, in order to find the distance between the sun and the target body. When run on a spiceinited cube, this can be determined using the camera model. Using a spiceinited cube as input has the advantage of not requiring that local mission-specific kernels be available. (See spiceinit web=true.)

Description

This is the non-calibrated, unprojected WAC cube

Description

This is the calibrated WAC cube

Description

Calibrate using a correction based off of a dark file. Please see the Dark Correction section at the beginning of this document for a detailed explanation of how the correction is applied

Description

Dark file used for calibration. The default is to use the dark file with the closest time and temperature to the WAC image being calibrated. See the Dark Correction section at the beginning of this document for a detailed explanation of how dark files are chosen.

Description

Calibrate using a flatfield file.

Description

Flatfield file used for calibration. The default is to use the system defined dark file with the highest version number.

Description

Perform a radiometric calibration on the input cub. This type of this correction is defined by the RadiometricType parameter.

Description

Calibrated output cube units. I/F or radiance.

Description

Radiometric constants file used for calibration. The default is to use the system defined file with the highest version.

Description

This option will apply a special pixel mask to the input cub. The default is to use the system defined mask file with the matching WAC mode and closest Temperature to the input cub. Please see the main documentation for a detailed description of the Special Pixel Mask correction.

Description

Description

Calibrate using temperature gain and offset. Please see this document, which outlines how the correction was derived.

Description

Temperature gain and offset file. The default is to use the system defined temperature gain and offset file with the highest version number.