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Estimating Snow Water Equivalent for a
Snow-Covered Ground Reflector using GPS
            Multipath Signals
              Dr. Mark Jacobson
               Mathematics Department
        1500 University Drive, Billings, MT 59101
             mjacobson@msubillings.edu
I. Introduction

 Proof-of-concept method for estimating snow
  water equivalent (SWE) at the GPS frequency of
  1.5 GHz
 SWE is the single most important parameter for
  hydrological studies because it represents the
  amount of water potentially available for runoff
 SWE estimations are used for the management of
  water supply and flood control systems
 The U.S. D.O.A. operates and manages the
  Snowpack Telemetry (SNOTEL) system, 730 sites
 GPS signals could provide a new and economical
  technique for estimating SWE
II. Theory
Relative received power at the antenna is

       rh  rv  exp(i )        2
                                                    4 (h  t ) sin 
P  1                                where,   
                2                                              0
h = height of antenna above conducting surface, m
     elevation angle, degrees

i  1
c  2.997925  108       m/s, the speed of light in a vacuum

f  1.57542  109        Hz

0  c / f  0.1902937 m, free-space wavelength

t   = snow layer thickness, m

   snow   s'  i s"               s'  1  2  d
 d  relative density of dry snow, g cm−3
For a single-layer of snow above a conducting
surface with horizontal polarization, x = h and
vertical polarization, x = v

     iZ x tan  1                  sin 
rx                        Zh 
     iZ x tan  1                  cos 2 



     2                    Zv 
                                  cos 2 
        t   cos 2 
                                  sin 
     0
III. Measurements and Computation
   March 31, 2007     T = -1.7 C, t = 7.6 cm,
   h = 45.1 cm, no snow density data



   III. Measurements and Computation
                     March 31, 2007
           T = -1.7 C, t = 7.6 cm, h = 45.1 cm
Equipment Setup for GPS Measurements
In order to utilize a Quasi-Newton Algorithm (QNA)
efficiently in finding estimates of snow depth and density, we
approximate the relative complex permittivity value of dry
snow as

 snow    i    1  2 d
               '
               s
                     "
                     s
                           '
                           s
                                                                             
                                                                                "
                                                                                s
                                                                                       '
                                                                                       s


                                  ������=������
                            1                                              2
SE ������, ������snow = ������������������                    ������ ������������ − ������ ������������ , ������, ������snow            n = 8,168
                         ������ − 2
                                  ������=1




From 45 input pairs, the smallest SE produced the following:

   t   = 6.8   cm                  d  0.30                                    s'  1.60
IV. Conclusions

 Theoretical results and GPS measurements
  are in good agreement using a nonlinear
  QNA
 Estimating SWE may be possible using a
  nonlinear least squares technique
 “Inferring Snow Water Equivalent for a
  Snow-Covered Ground Reflector Using GPS
  Multipath Signals”, Remote Sensing, Vol. 2,
  2426-2441, October 2010
V. Future Work
 Try a QNA for a snow layer above frozen
  soil
 Collect more in situ measurements of snow
  depth, snow density, and frozen soil
  permittivity
 Try other nonlinear least-squares
  algorithms: Levenbeg-Marquardt and
  Conjugate Gradient
 Incorporate 2 or more snow layers in the
  theoretical model
V. Future Work (continued)
 Incorporate the antenna pattern in the
  theoretical model
 Incorporate surface roughness of snow and
  frozen soil in the theoretical model
 Use a horizontally-mounted (zenith-pointing)
  GPS antenna
 Investigate this technique for GPS antennas
  housed on an aircraft or satellite
Acknowledgment
 Montana State University Billings
  – Dr. Tasneem Khaleel, Dean CAS
  – Dr. Maggie McBride, Math Dept.
  – RACE Grant
 Ron and Jeanne Jacobson, my parents
 Wade Dotson, Trimble Navigation
 C. McFarland and T. McFarland, land
  owners
 Anonymous reviewers of paper

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Jacobson_Mark_1041.pdf

  • 1. Estimating Snow Water Equivalent for a Snow-Covered Ground Reflector using GPS Multipath Signals Dr. Mark Jacobson Mathematics Department 1500 University Drive, Billings, MT 59101 mjacobson@msubillings.edu
  • 2. I. Introduction  Proof-of-concept method for estimating snow water equivalent (SWE) at the GPS frequency of 1.5 GHz  SWE is the single most important parameter for hydrological studies because it represents the amount of water potentially available for runoff  SWE estimations are used for the management of water supply and flood control systems  The U.S. D.O.A. operates and manages the Snowpack Telemetry (SNOTEL) system, 730 sites  GPS signals could provide a new and economical technique for estimating SWE
  • 4. Relative received power at the antenna is rh  rv  exp(i ) 2 4 (h  t ) sin  P  1 where,  2 0 h = height of antenna above conducting surface, m  elevation angle, degrees i  1 c  2.997925  108 m/s, the speed of light in a vacuum f  1.57542  109 Hz 0  c / f  0.1902937 m, free-space wavelength t = snow layer thickness, m    snow   s'  i s"  s'  1  2  d  d  relative density of dry snow, g cm−3
  • 5. For a single-layer of snow above a conducting surface with horizontal polarization, x = h and vertical polarization, x = v iZ x tan  1 sin  rx  Zh  iZ x tan  1   cos 2  2 Zv    cos 2   t   cos 2   sin  0
  • 6. III. Measurements and Computation March 31, 2007 T = -1.7 C, t = 7.6 cm, h = 45.1 cm, no snow density data III. Measurements and Computation March 31, 2007 T = -1.7 C, t = 7.6 cm, h = 45.1 cm
  • 7. Equipment Setup for GPS Measurements
  • 8. In order to utilize a Quasi-Newton Algorithm (QNA) efficiently in finding estimates of snow depth and density, we approximate the relative complex permittivity value of dry snow as  snow    i    1  2 d ' s " s ' s    " s ' s ������=������ 1 2 SE ������, ������snow = ������������������ ������ ������������ − ������ ������������ , ������, ������snow n = 8,168 ������ − 2 ������=1 From 45 input pairs, the smallest SE produced the following: t = 6.8 cm  d  0.30  s'  1.60
  • 9.
  • 10.
  • 11.
  • 12.
  • 13. IV. Conclusions  Theoretical results and GPS measurements are in good agreement using a nonlinear QNA  Estimating SWE may be possible using a nonlinear least squares technique  “Inferring Snow Water Equivalent for a Snow-Covered Ground Reflector Using GPS Multipath Signals”, Remote Sensing, Vol. 2, 2426-2441, October 2010
  • 14. V. Future Work  Try a QNA for a snow layer above frozen soil  Collect more in situ measurements of snow depth, snow density, and frozen soil permittivity  Try other nonlinear least-squares algorithms: Levenbeg-Marquardt and Conjugate Gradient  Incorporate 2 or more snow layers in the theoretical model
  • 15. V. Future Work (continued)  Incorporate the antenna pattern in the theoretical model  Incorporate surface roughness of snow and frozen soil in the theoretical model  Use a horizontally-mounted (zenith-pointing) GPS antenna  Investigate this technique for GPS antennas housed on an aircraft or satellite
  • 16. Acknowledgment  Montana State University Billings – Dr. Tasneem Khaleel, Dean CAS – Dr. Maggie McBride, Math Dept. – RACE Grant  Ron and Jeanne Jacobson, my parents  Wade Dotson, Trimble Navigation  C. McFarland and T. McFarland, land owners  Anonymous reviewers of paper