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An Introduction to Geostatistics Presented to Math 216, Spring, 2012 Chris Vanags, Ph.D. Associate Director, Vanderbilt Center for Science Outreach Instructor, School for Science and Math at Vanderbilt
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Page 1: An Introduction to Geostatistics Presented to Math 216, Spring, 2012 Chris Vanags, Ph.D. Associate Director, Vanderbilt Center for Science Outreach Instructor,

An Introduction to Geostatistics

Presented to Math 216, Spring, 2012

Chris Vanags, Ph.D.Associate Director, Vanderbilt Center for Science Outreach

Instructor, School for Science and Math at Vanderbilt

Page 2: An Introduction to Geostatistics Presented to Math 216, Spring, 2012 Chris Vanags, Ph.D. Associate Director, Vanderbilt Center for Science Outreach Instructor,

A brief experiment . . .

Is it hot it here?

Page 3: An Introduction to Geostatistics Presented to Math 216, Spring, 2012 Chris Vanags, Ph.D. Associate Director, Vanderbilt Center for Science Outreach Instructor,

Follow up from assigned reading

“Analyzing the Consequences of Chernobyl Using GIS and Spatial Statistics”

Page 4: An Introduction to Geostatistics Presented to Math 216, Spring, 2012 Chris Vanags, Ph.D. Associate Director, Vanderbilt Center for Science Outreach Instructor,

Relative to your other course readings was this article. . .

1. Inappropriately simple

2. Easier to understand

3. On par with the level of difficulty

4. More difficult to understand

5. Inappropriately complex

Page 5: An Introduction to Geostatistics Presented to Math 216, Spring, 2012 Chris Vanags, Ph.D. Associate Director, Vanderbilt Center for Science Outreach Instructor,

●Did you feel that this article was appropriately informative?

1. The article did not contain enough detail to be interesting

2. The article captured my attention, but was not sufficiently detailed for my level of understanding

3. The article was well matched to the course requirements and my level of understanding

4. The article captured my attention, but was overly detailed for my level of understanding

Page 6: An Introduction to Geostatistics Presented to Math 216, Spring, 2012 Chris Vanags, Ph.D. Associate Director, Vanderbilt Center for Science Outreach Instructor,

I found this article to be relevant to what we are studying in this class.

1. Strongly Agree

2. Agree

3. Disagree

4. Strongly Disagree

Page 7: An Introduction to Geostatistics Presented to Math 216, Spring, 2012 Chris Vanags, Ph.D. Associate Director, Vanderbilt Center for Science Outreach Instructor,

Based on the reading, I can see using geostatistcal tools in the future

Stro

ngly Agree

Agree

Disa

gree

Stro

ngly Disa

gree

25% 25%25%25%1. Strongly Agree

2. Agree

3. Disagree

4. Strongly Disagree

Page 8: An Introduction to Geostatistics Presented to Math 216, Spring, 2012 Chris Vanags, Ph.D. Associate Director, Vanderbilt Center for Science Outreach Instructor,

Why am I here?

“How do geostatistics differ from "normal" statistics in terms of determining the probability of given events assuming they have these large, vaguely defined sample sizes?”

Page 9: An Introduction to Geostatistics Presented to Math 216, Spring, 2012 Chris Vanags, Ph.D. Associate Director, Vanderbilt Center for Science Outreach Instructor,

A brief history of geostatistics

● $962Billion Global mining industry

Georges Matheron (1930 – 2000)Gold deposits in Witwaterstand, SA

Page 10: An Introduction to Geostatistics Presented to Math 216, Spring, 2012 Chris Vanags, Ph.D. Associate Director, Vanderbilt Center for Science Outreach Instructor,

Fundamental concepts: interpolation models

● Nearest neighbor (right)– Exact values

● Inverse-distance weighting– Interpolation based on

distance from known values

● Trend analysis– Interpolation based on

distance and variation

Nearest neighbor approximationFrom: Wikipedia Commons

Page 11: An Introduction to Geostatistics Presented to Math 216, Spring, 2012 Chris Vanags, Ph.D. Associate Director, Vanderbilt Center for Science Outreach Instructor,

Fundamental concepts: the (semi)variogram

● Change in distance vs. change in property

● Used to weight estimates of variation between known points

● Key terms:– Nugget– Range– Sill

Semivariogram of topsoil clay content vs. lag distanceFrom: USGS

Page 12: An Introduction to Geostatistics Presented to Math 216, Spring, 2012 Chris Vanags, Ph.D. Associate Director, Vanderbilt Center for Science Outreach Instructor,

Fundamental concepts: Kriging

● Interpolation based on the modeled semivariogram

● Provides estimates of properties AND estimates of uncertainty of the prediction (right)

● Multi-dimensional● Computationally

expensive

Page 13: An Introduction to Geostatistics Presented to Math 216, Spring, 2012 Chris Vanags, Ph.D. Associate Director, Vanderbilt Center for Science Outreach Instructor,

Fundamental concepts: covariability● “Using information that

is easy to obtain to predict information that is difficult to obtain”

● Trend Kriging● Regression Kriging● Co-Kriging

Page 14: An Introduction to Geostatistics Presented to Math 216, Spring, 2012 Chris Vanags, Ph.D. Associate Director, Vanderbilt Center for Science Outreach Instructor,

Where to go from here. . . ?

● Indicator kriging (right)

● Stochastic modeling (below)

Page 15: An Introduction to Geostatistics Presented to Math 216, Spring, 2012 Chris Vanags, Ph.D. Associate Director, Vanderbilt Center for Science Outreach Instructor,

Geostatistics in practice:“Predicting the field-scale hydrological impacts of shallow palæochannels in the semi-arid landscape of Northern New South Wales, Australia “

Chris Vanags

Page 16: An Introduction to Geostatistics Presented to Math 216, Spring, 2012 Chris Vanags, Ph.D. Associate Director, Vanderbilt Center for Science Outreach Instructor,

Background“Expansion of flood irrigation in the Lower Macquarie Valley of New South Wales, Australia has been suggested as a major cause of increased groundwater recharge”

- Willis et al, 1997

www.boreline.co.uk

Page 17: An Introduction to Geostatistics Presented to Math 216, Spring, 2012 Chris Vanags, Ph.D. Associate Director, Vanderbilt Center for Science Outreach Instructor,

“The areas exhibiting the largest probability of excessive DD correspond to permeable soil types associated with a prior stream channel.”

Background

From: Stannard and Kelly (1977)

- Triantafilis et al, 2003

Page 18: An Introduction to Geostatistics Presented to Math 216, Spring, 2012 Chris Vanags, Ph.D. Associate Director, Vanderbilt Center for Science Outreach Instructor,

Water BudgetFlow (m3/day) from:

palaeochannel (2)

to water table (4)

Background

Layers 1-5 Layers 6-1011

1 12

2

3 4

y = 8.9302x + 1.1831

R2 = 0.9896

0

5

10

15

20

25

0 0.5 1 1.5 2 2.5

Channel Ksat multiplier

“a two fold increase in the contrast in saturated conductivity between channel sediments and those surrounding the channel increases the predicted deep drainage by 64% in our Modflow simulation”-Vanags and Vervoort, 2004

Page 19: An Introduction to Geostatistics Presented to Math 216, Spring, 2012 Chris Vanags, Ph.D. Associate Director, Vanderbilt Center for Science Outreach Instructor,

Study siteMoree, NSW

Page 20: An Introduction to Geostatistics Presented to Math 216, Spring, 2012 Chris Vanags, Ph.D. Associate Director, Vanderbilt Center for Science Outreach Instructor,

MethodsDirect

Observation

HydrologicalProperties

ConceptualModel

AncillaryData

GroundwaterFlow

Prediction

Page 21: An Introduction to Geostatistics Presented to Math 216, Spring, 2012 Chris Vanags, Ph.D. Associate Director, Vanderbilt Center for Science Outreach Instructor,

Groundwater response to irrigation

Perched watertable during irrigation events

Immediate response to irrigation events

Source of perched water?

769300 769400 769500 769600 769700 7698006751700

6751800

6751900

6752000

6752100

6752200

1 2,38

5,6,749

11,12

21,22

Irrigation canalCarroll Creek

-9

-8

-7

-6

-5

-4

-3

25/10/2005 19/11/2005 14/12/2005 8/01/2006 2/02/2006 27/02/2006

Date

wat

erle

vel

in m

be

low

th

e s

urf

ace

A: well 2 (9m) below PC B: well 3 (5m) inside PC C: well 4 (9m) outside PC

A

B

C

Page 22: An Introduction to Geostatistics Presented to Math 216, Spring, 2012 Chris Vanags, Ph.D. Associate Director, Vanderbilt Center for Science Outreach Instructor,

Ancillary information“… the high costs and intrinsic features of invasive sampling techniques such as drilling and cone penetrometer technologies limit their use to a finite number of sampling locations and do not allow complete coverage of the area under consideration”

-Borchers et al 1997

Page 23: An Introduction to Geostatistics Presented to Math 216, Spring, 2012 Chris Vanags, Ph.D. Associate Director, Vanderbilt Center for Science Outreach Instructor,

EM 31

DGPS height-adjustable stabiliser

Easting

Sou

thin

g

769400 769600 769800

6751500

6751700

6751900

6752100

6752300

Quad-bike EM survey

Clear delineation of channel inside paddock

No delineation outside paddock

Strongly related to soil wetness

Distance (m)

Var

ianc

e

inside paddock

outside paddock

combined

outside paddock

inside paddock

combined

3 people hours = 2,700 data points

Page 24: An Introduction to Geostatistics Presented to Math 216, Spring, 2012 Chris Vanags, Ph.D. Associate Director, Vanderbilt Center for Science Outreach Instructor,

EM Survey: Depth sounding

Tx Rxseparation

½ separation

TxTx RxRxseparation

½ separation

Bi var i at e Fi t of 2 By ydi st Xval ue=2

Sm oot hing Spline Fit , lam bda=0. 1 I D==" EM 31_0_H"

Sm oot hing Spline Fit , lam bda=0. 1 I D==" EM 31_0_V"

Sm oot hing Spline Fit , lam bda=0. 1 I D==" EM 31_1. 5_H"

Sm oot hing Spline Fit , lam bda=0. 1 I D==" EM 31_1. 5_v "

Sm oot hing Spline Fit , lam bda=0. 1 I D==" EM 31_1_H"

Sm oot hing Spline Fit , lam bda=0. 1 I D==" EM 31_1_V"

Sm oot hing Spline Fit , lam bda=0. 1 I D==" EM 34_10"

Sm oot hing Spline Fit , lam bda=0. 1 I D==" EM 34_20"

Sm oot hing Spline Fit , lam bda=0. 1 I D==" EM 38_H"

Sm oot hing Spline Fit , lam bda=0. 1 I D==" EM 38_V"

40

50

60

70

80

90

100

110

120

130

140

2

0 10 20 30 40 50 60 70 80 90 100

ydis t

Bi var i at e Fi t of 1 By ydi st Xval ue=2

Sm oot hing Spline Fit , lam bda=0. 1 I D==" EM 31_0_H"

Sm oot hing Spline Fit , lam bda=0. 1 I D==" EM 31_0_V"

Sm oot hing Spline Fit , lam bda=0. 1 I D==" EM 31_1. 5_H"

Sm oot hing Spline Fit , lam bda=0. 1 I D==" EM 31_1. 5_v "

Sm oot hing Spline Fit , lam bda=0. 1 I D==" EM 31_1_H"

Sm oot hing Spline Fit , lam bda=0. 1 I D==" EM 31_1_V"

Sm oot hing Spline Fit , lam bda=0. 1 I D==" EM 34_10"

Sm oot hing Spline Fit , lam bda=0. 1 I D==" EM 34_20"

Sm oot hing Spline Fit , lam bda=0. 1 I D==" EM 38_H"

Sm oot hing Spline Fit , lam bda=0. 1 I D==" EM 38_V"

40

50

60

70

80

90

100

110

120

130

140

1

0 10 20 30 40 50 60 70 80 90 100

ydis t

1m Rx Tx

Bi var i at e Fi t of 2 By ydi st Xval ue=2

Sm oot hing Spline Fit , lam bda=0. 1 I D==" EM 31_0_H"

Sm oot hing Spline Fit , lam bda=0. 1 I D==" EM 31_0_V"

Sm oot hing Spline Fit , lam bda=0. 1 I D==" EM 31_1. 5_H"

Sm oot hing Spline Fit , lam bda=0. 1 I D==" EM 31_1. 5_v "

Sm oot hing Spline Fit , lam bda=0. 1 I D==" EM 31_1_H"

Sm oot hing Spline Fit , lam bda=0. 1 I D==" EM 31_1_V"

Sm oot hing Spline Fit , lam bda=0. 1 I D==" EM 34_10"

Sm oot hing Spline Fit , lam bda=0. 1 I D==" EM 34_20"

Sm oot hing Spline Fit , lam bda=0. 1 I D==" EM 38_H"

Sm oot hing Spline Fit , lam bda=0. 1 I D==" EM 38_V"

40

50

60

70

80

90

100

110

120

130

140

2

0 10 20 30 40 50 60 70 80 90 100

ydis t

Bi var i at e Fi t of 1 By ydi st Xval ue=2

Sm oot hing Spline Fit , lam bda=0. 1 I D==" EM 31_0_H"

Sm oot hing Spline Fit , lam bda=0. 1 I D==" EM 31_0_V"

Sm oot hing Spline Fit , lam bda=0. 1 I D==" EM 31_1. 5_H"

Sm oot hing Spline Fit , lam bda=0. 1 I D==" EM 31_1. 5_v "

Sm oot hing Spline Fit , lam bda=0. 1 I D==" EM 31_1_H"

Sm oot hing Spline Fit , lam bda=0. 1 I D==" EM 31_1_V"

Sm oot hing Spline Fit , lam bda=0. 1 I D==" EM 34_10"

Sm oot hing Spline Fit , lam bda=0. 1 I D==" EM 34_20"

Sm oot hing Spline Fit , lam bda=0. 1 I D==" EM 38_H"

Sm oot hing Spline Fit , lam bda=0. 1 I D==" EM 38_V"

40

50

60

70

80

90

100

110

120

130

140

1

0 10 20 30 40 50 60 70 80 90 100

ydis t

Bi var i at e Fi t of 2 By ydi st Xval ue=2

Sm oot hing Spline Fit , lam bda=0. 1 I D==" EM 31_0_H"

Sm oot hing Spline Fit , lam bda=0. 1 I D==" EM 31_0_V"

Sm oot hing Spline Fit , lam bda=0. 1 I D==" EM 31_1. 5_H"

Sm oot hing Spline Fit , lam bda=0. 1 I D==" EM 31_1. 5_v "

Sm oot hing Spline Fit , lam bda=0. 1 I D==" EM 31_1_H"

Sm oot hing Spline Fit , lam bda=0. 1 I D==" EM 31_1_V"

Sm oot hing Spline Fit , lam bda=0. 1 I D==" EM 34_10"

Sm oot hing Spline Fit , lam bda=0. 1 I D==" EM 34_20"

Sm oot hing Spline Fit , lam bda=0. 1 I D==" EM 38_H"

Sm oot hing Spline Fit , lam bda=0. 1 I D==" EM 38_V"

40

50

60

70

80

90

100

110

120

130

140

2

0 10 20 30 40 50 60 70 80 90 100

ydis t

Bi var i at e Fi t of 1 By ydi st Xval ue=2

Sm oot hing Spline Fit , lam bda=0. 1 I D==" EM 31_0_H"

Sm oot hing Spline Fit , lam bda=0. 1 I D==" EM 31_0_V"

Sm oot hing Spline Fit , lam bda=0. 1 I D==" EM 31_1. 5_H"

Sm oot hing Spline Fit , lam bda=0. 1 I D==" EM 31_1. 5_v "

Sm oot hing Spline Fit , lam bda=0. 1 I D==" EM 31_1_H"

Sm oot hing Spline Fit , lam bda=0. 1 I D==" EM 31_1_V"

Sm oot hing Spline Fit , lam bda=0. 1 I D==" EM 34_10"

Sm oot hing Spline Fit , lam bda=0. 1 I D==" EM 34_20"

Sm oot hing Spline Fit , lam bda=0. 1 I D==" EM 38_H"

Sm oot hing Spline Fit , lam bda=0. 1 I D==" EM 38_V"

40

50

60

70

80

90

100

110

120

130

140

1

0 10 20 30 40 50 60 70 80 90 100

ydis t

480 people hours = 1000 data points

Page 25: An Introduction to Geostatistics Presented to Math 216, Spring, 2012 Chris Vanags, Ph.D. Associate Director, Vanderbilt Center for Science Outreach Instructor,

1

8

Inverted conductivity profiles

McNeill Discontinuous profiles Channel not delineated

Tikhonov 0th order Laterally smooth profiles Large range in predictions

Tikhonov 1st order Smooth profiles Channel delineated

Tikhonov 2nd order Smooth profiles Channel delineated

McNeill Tikh 0

Tikh 1 Tikh 2

Distance along transect (m)

De

pth

(m

be

low

su

rfa

ce

)

Page 26: An Introduction to Geostatistics Presented to Math 216, Spring, 2012 Chris Vanags, Ph.D. Associate Director, Vanderbilt Center for Science Outreach Instructor,

EM results: significant relation with clay content

McNeill

poor correlation with clay content

Tikhonov 0th order

best correlation, high RMSE

Tikhonov 1st order

significant correlation

Tikhonov 2nd order

significant correlation, lowest RMSE

Tikh 2r2=0.19RMSE = 19

Tikh 0r2=0.40RMSE = 42

Clay (g/g)

McNeillr2=0.06RMSE = 77

EC

(m

S/m

)

Tikh 1r2=0.20RMSE = 23

Page 27: An Introduction to Geostatistics Presented to Math 216, Spring, 2012 Chris Vanags, Ph.D. Associate Director, Vanderbilt Center for Science Outreach Instructor,

Groundwater flow through palæochannel

heavyclays

coarsesand andgravel

finesand

partic le s ize c lusters a long channel

S outhing

de

pth

be

low

su

rfa

ce (

m)

-15

-10

-5

6751800 6751900 6752000 6752100

1

2

3

coarse gravel (Narrabri Formation)

palæochannel

reduced clays

permanent water table (1-2 m annual variation)

deep drainage

lateralflow

De

pth

(m

be

low

su

rfa

ce

)

Page 28: An Introduction to Geostatistics Presented to Math 216, Spring, 2012 Chris Vanags, Ph.D. Associate Director, Vanderbilt Center for Science Outreach Instructor,

Direct characterization

Identify important units

Measure hydrologic properties

Assign reference Ksat values for geologic facies

discontinuous predictions, assumed homogeneity within structure

Page 29: An Introduction to Geostatistics Presented to Math 216, Spring, 2012 Chris Vanags, Ph.D. Associate Director, Vanderbilt Center for Science Outreach Instructor,

Testing the scaling methods with 3D regression kriging

Use trend from ancillary data to weight direct observations

Assumptions: Direct observations

are related to ancillary data

Weighting is based on regression analysis

2.5m 1.5m 0.5m

6.5m 5.5m 4.5m 3.5m

10.5m 9.5m 8.5m 7.5m

Page 30: An Introduction to Geostatistics Presented to Math 216, Spring, 2012 Chris Vanags, Ph.D. Associate Director, Vanderbilt Center for Science Outreach Instructor,

Improved groundwater model

2D laterally-continuous Ksat from EM data X 20 layers

Simulated input from irrigation channel and deep drainage

Limited temporal prediction (single event)

Page 31: An Introduction to Geostatistics Presented to Math 216, Spring, 2012 Chris Vanags, Ph.D. Associate Director, Vanderbilt Center for Science Outreach Instructor,

MODFLOW Simulations

Ksat predictions from 2D EM surveys

Continuous Ksat in slice (projected in 3 dimensions)

Ksat = Kref x λ

Top boundary input

Inversion method accounted for 33% of predicted deep drainage

Tikhonov2m depth

McNeill2m depth

Page 32: An Introduction to Geostatistics Presented to Math 216, Spring, 2012 Chris Vanags, Ph.D. Associate Director, Vanderbilt Center for Science Outreach Instructor,

Conclusions

High variability of Ksat within palæochannel

2 orders of magnitude within channel

3 orders between palæochannel and surrounding sediments

Is direct characterization possible for a landscape scale effort?

Palæochannel associated with deep drainage AND lateral flow

In presence of irrigation channel: lateral flow >> deep drainage

31 Ml water lost during a single year of irrigation on one site.

where is this water headed?

what is the water quality?

Page 33: An Introduction to Geostatistics Presented to Math 216, Spring, 2012 Chris Vanags, Ph.D. Associate Director, Vanderbilt Center for Science Outreach Instructor,

Future research

Continue groundwater monitoring Calibrate groundwater model

Improve Ksat predictions

Incorporate measured data i.e. Kriging with trend

Incorporate uncertainty from ptf and scaling Generate stochastic groundwater model

Translate to landscape scale Use prediction method for larger data set


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