bruce h. stanley, oct. 16, 2003 del. chapter of asa meeting: mgf and 1 st -order dissipation slide 1...
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Bruce H. Stanley, Oct. 16, 2003Del. Chapter of ASA Meeting: MGF and 1st-Order Dissipation Slide 1
The Moment Generating Function As A Useful Tool in Understanding Random Effects on First-Order Environmental
Dissipation Processes
Dr. Bruce H. StanleyDuPont Crop Protection
Stine-Haskell Research Center
Newark, Delaware
Bruce H. Stanley, Oct. 16, 2003Del. Chapter of ASA Meeting: MGF and 1st-Order Dissipation Slide 2
The Moment Generating Function As A Useful Tool in Understanding Random Effects on First-
Order Environmental Dissipation Processes
Abstract
Many physical and, thus, environmental processes follow first-order kinetics, where the rate of change of a substance is proportional to its concentration. The rate of change may be affected by a variety of factors, such as temperature or light intensity, that follow a probability distribution. The moment generating function provides a quick method to estimate the mean and variance of the process through time. This allows valuable insights for environmental risk assessment or process optimization.
Bruce H. Stanley, Oct. 16, 2003Del. Chapter of ASA Meeting: MGF and 1st-Order Dissipation Slide 3
Agenda• First-order (FO) dissipation
• The moment generating function (MGF)
• Relationship between FO dissipation and MGF
• Calculating the variance of dissipation
• Other “curvilinear” models
• Half-lives of the models
• References
• Conclusions
Bruce H. Stanley, Oct. 16, 2003Del. Chapter of ASA Meeting: MGF and 1st-Order Dissipation Slide 4
- First-Order Dissipation -
Bruce H. Stanley, Oct. 16, 2003Del. Chapter of ASA Meeting: MGF and 1st-Order Dissipation Slide 5
Model: First-Order Dissipation
tt Cr
dt
dC
trt eCC 0
r
t 21ln
21
trCCt 0lnln
Rate of change:
Model:
Transformation to linearity:
Constant half-life:
Bruce H. Stanley, Oct. 16, 2003Del. Chapter of ASA Meeting: MGF and 1st-Order Dissipation Slide 6
First-Order Dissipation
0.1
1
10
100
1000
0 50 100 150 200 250 300
Time (days)
Co
nce
ntr
atio
n (
pp
m)
Example: First-Order Dissipation
trCCt 0lnln
Bruce H. Stanley, Oct. 16, 2003Del. Chapter of ASA Meeting: MGF and 1st-Order Dissipation Slide 7
Some Processes that Follow First-Order Kinetics
• Radio-active decay
• Population decline (i. e., “death” processes)
• Compounded interest/depreciation
• Chemical decomposition
• Etc…
Bruce H. Stanley, Oct. 16, 2003Del. Chapter of ASA Meeting: MGF and 1st-Order Dissipation Slide 8
- The Moment Generating Function -
Bruce H. Stanley, Oct. 16, 2003Del. Chapter of ASA Meeting: MGF and 1st-Order Dissipation Slide 9
Definition: Moment Generating Function
teEtm r
n
t
n
n
Edt
tmdr
0
Bruce H. Stanley, Oct. 16, 2003Del. Chapter of ASA Meeting: MGF and 1st-Order Dissipation Slide 10
Example: Moment Generating Function
t
dxexeeEtm xtxtX 1
0
2
2
2
2
00
2
222
0
1
0
0
)1()var(
tt
X
tt
X
n
t
n
n
dt
tdm
dt
tmdXEX
tdt
tdm
Edt
tmdr
X ~ Gamma(,)
Bruce H. Stanley, Oct. 16, 2003Del. Chapter of ASA Meeting: MGF and 1st-Order Dissipation Slide 11
Relationship Between – First-Order Dissipation –
and the Moment Generating Function
Bruce H. Stanley, Oct. 16, 2003Del. Chapter of ASA Meeting: MGF and 1st-Order Dissipation Slide 12
Random First-Order Dissipation
tt eCC r
0
tt eECCE r0
where r ~ PDF
Constant
Bruce H. Stanley, Oct. 16, 2003Del. Chapter of ASA Meeting: MGF and 1st-Order Dissipation Slide 13
Conceptual Model:Distribution of Dissipation Rates
dCt4/dt = r4
.Ct4
dCt3/dt = r3
.Ct3
dCt2/dt = r2
.Ct2
dCt1/dt = r1
.Ct1
0
0.020.04
0.060.08
0.10.12
0.140.16
0.180.2
-10 -8 -6 -4 -2 0
r
f(r)
r < 0
Bruce H. Stanley, Oct. 16, 2003Del. Chapter of ASA Meeting: MGF and 1st-Order Dissipation Slide 14
Transformation of r or t?
00.020.040.060.080.10.120.140.160.180.2
-10 -8 -6 -4 -2 0
r
f(r)
00.020.040.060.080.1
0.120.140.160.180.2
0 2 4 6 8 10
x = -r
f(x)
r < 0 X = -r
r = -1.X
fr(r) = fX(-r)
E(rn) = (-1)n.E(Xn)
It’s easier to transform t, I.e., = -t
= -tso substitute
t = -And treat r’s as positive
when necessary
Bruce H. Stanley, Oct. 16, 2003Del. Chapter of ASA Meeting: MGF and 1st-Order Dissipation Slide 15
Typical Table of Distributions(Mood, Graybill & Boes. 1974. Intro. To the Theory of Stats., 3rd Ed. McGraw-Hill. 564 pp.)
Bruce H. Stanley, Oct. 16, 2003Del. Chapter of ASA Meeting: MGF and 1st-Order Dissipation Slide 16
Some Possible Dissipation Rate Distributions
• Uniform r ~ U(min, max)
• Normal r ~ N(r, 2 r)
• Lognormal r ~ LN(r= e+ 2/2, 2r = r
2.(e 2-1))
= ln[r /(1+ r2/2
r)],;
2 = ln[1+ (r2/2
r)]
• Gamma r ~ (r= /, 2r = /2)
= r2/2
r; = r/2r
(distribution used in Gustafson and Holden
1990)* Where r and 2
r are the expected value and variance of the untransformed rates, respectively.
Bruce H. Stanley, Oct. 16, 2003Del. Chapter of ASA Meeting: MGF and 1st-Order Dissipation Slide 17
Application to Dissipation Model: Uniform
tt eECCE r0
t
eeCCE
tt
tminmax
0
minmax
rr
rr
No need to make = -t substitution
Bruce H. Stanley, Oct. 16, 2003Del. Chapter of ASA Meeting: MGF and 1st-Order Dissipation Slide 18
Application to Dissipation Model: Normal
tt eECCE r0
20
22 tt
t
rr
eCCE
Note: Begins increasing at t = -r/r2, and becomes >C0 after t = -2.r/r
2.
No need to make = -t substitution
Bruce H. Stanley, Oct. 16, 2003Del. Chapter of ASA Meeting: MGF and 1st-Order Dissipation Slide 19
Application to Dissipation Model: Lognormal
Note: Same as normal on the log scale.
Bruce H. Stanley, Oct. 16, 2003Del. Chapter of ASA Meeting: MGF and 1st-Order Dissipation Slide 20
Application to Dissipation Model: Gamma(Gustafson and Holden (1990) Model)
tt eECCE r0
2
2
2
2
2
0
200
1r
r
r
r
t
C
tC
tCCE
r
r
rr
rt
Make = -t substitution
Bruce H. Stanley, Oct. 16, 2003Del. Chapter of ASA Meeting: MGF and 1st-Order Dissipation Slide 21
Distributed Loss Model
10.00
20.00
30.00
40.00
50.00
60.00
70.00
80.00
90.00
100.00
0 2 4 6 8 10
t
C(t
)
Bruce H. Stanley, Oct. 16, 2003Del. Chapter of ASA Meeting: MGF and 1st-Order Dissipation Slide 22
Key Paper: Gustafson & Holden (1990)
Bruce H. Stanley, Oct. 16, 2003Del. Chapter of ASA Meeting: MGF and 1st-Order Dissipation Slide 23
- Calculating the Variance -
Bruce H. Stanley, Oct. 16, 2003Del. Chapter of ASA Meeting: MGF and 1st-Order Dissipation Slide 24
Example: Variance for the Gamma Case
2
2
2
2 2
2220
2
20
2220
22
2
2
r
r
r
r
ttC
ttC
eEeECCECECVar
rr
r
rr
r
ttttt
rr
Make = -t substitution
Bruce H. Stanley, Oct. 16, 2003Del. Chapter of ASA Meeting: MGF and 1st-Order Dissipation Slide 25
- Random Initial Concentration -
Bruce H. Stanley, Oct. 16, 2003Del. Chapter of ASA Meeting: MGF and 1st-Order Dissipation Slide 26
Variable Initial Concentration:Product of Random Variables
0
220
2
000
200
2200
2
0
000
220
0
000
2
2
,
,2
,
CVareEeVarCE
eEeCECECE
eEeCECEeE
eEeCECEeCCov
eCCoveECECVareEeVarCECVar
eECE
eCCoveECEeCECE
tt
tt
ttt
ttt
ttttt
t
tttt
rr
rr
rrr
rrr
rrrr
r
rrr
Delta Method
Delta Method
Bruce H. Stanley, Oct. 16, 2003Del. Chapter of ASA Meeting: MGF and 1st-Order Dissipation Slide 27
- Other “Non-Linear” Models -
Bruce H. Stanley, Oct. 16, 2003Del. Chapter of ASA Meeting: MGF and 1st-Order Dissipation Slide 28
• Bi- (or multi-) first-order model ………..…...
• Non-linear functions of time, …………..…… e.g., t = degree days or cum. rainfall (Nigg et al. 1977)
• First-order with asymptote (Pree et al. 1976)..
• Two-compartment first-order………………..
• Distributed loss rate…………………….…… (Gustafson and Holden 1990)
• Power-rate model (Hamaker 1972)………..…
Other “Non-linear” Models ii tr
t eCC 0
t
ii dfactornDegradatiox0
_
ii xr
t eCC 0
ii tr
t eCCCC 0
tktkt eeC i 2
21
t
CCt
10
1
0
0
1 trC
CCt
Bruce H. Stanley, Oct. 16, 2003Del. Chapter of ASA Meeting: MGF and 1st-Order Dissipation Slide 29
First-order With Asymptote
10.00
100.00
0 2 4 6 8 10
t
C(t
)
Bruce H. Stanley, Oct. 16, 2003Del. Chapter of ASA Meeting: MGF and 1st-Order Dissipation Slide 30
Two Compartment Model
10.00
100.00
0 2 4 6 8 10
t
C(t
)
Bruce H. Stanley, Oct. 16, 2003Del. Chapter of ASA Meeting: MGF and 1st-Order Dissipation Slide 31
Distributed Loss Model
10.00
100.00
0 2 4 6 8 10
t
C(t
)
Bruce H. Stanley, Oct. 16, 2003Del. Chapter of ASA Meeting: MGF and 1st-Order Dissipation Slide 32
Power Rate Model
10.00
100.00
0 2 4 6 8 10
t
C(t
)
Bruce H. Stanley, Oct. 16, 2003Del. Chapter of ASA Meeting: MGF and 1st-Order Dissipation Slide 33
- Half-lives -
Bruce H. Stanley, Oct. 16, 2003Del. Chapter of ASA Meeting: MGF and 1st-Order Dissipation Slide 34
Half-lives for Various Models (p = 0.5)
• First-order*……………………….
• Multi-first-order*…………………
• First-order with asymptote ………
• Two-compartment first-order ……
• Distributed loss rate ……………..
• Power-rate model ……………….
* Can substitute cumulative environmental factor for time, i.e.,
r
pt p
ln
i
ijjj
i r
trp
tp
ln
t
dfactornDegradatiox0
_
r
CCCCp
t p
0
0ln
slow
pfast r
pt
r
p lnln
1
2
2r
r
ptr
rp
11
0
prC
t p
Bruce H. Stanley, Oct. 16, 2003Del. Chapter of ASA Meeting: MGF and 1st-Order Dissipation Slide 35
- References -
Bruce H. Stanley, Oct. 16, 2003Del. Chapter of ASA Meeting: MGF and 1st-Order Dissipation Slide 36
ReferencesDuffy, M. J., M. K. Hanafey, D. M. Linn, M. H. Russell and C. J. Peter. 1987. Predicting
sulfonylurea herbicide behavior under field conditions Proc. Brit. Crop Prot. Conf. – Weeds. 2: 541-547. [Application of 2-compartment first-order model]
Gustafson, D. I. And L. R. Holden. 1990. Nonlinear pesticide dissipation in Soil: a new model based upon spatial variability. Environ. Sci. Technol. 24 (7): 1032-1038. [Distributed rate model]
Hamaker, J. W. 1972. Decomposition: quantitative aspects. Pp. 253-340 In C. A. I. Goring and J. W. Hamaker (eds.) Organic Chemicals in the Soil Environment, Vol 1. Marcel Dekker, Inc., NY. [Power rate model]
Nigg, H. N., J. C. Allen, R. F. Brooks, G. J. Edwards, N. P. Thompson, R. W. King and A. H. Blagg. 1977. Dislodgeable residues of ethion in Florida citrus and relationships to weather variables. Arch. Environ. Contam. Toxicol. 6: 257-267. [First-order model with cumulative environmental variables]
Pree, D. J., K. P. Butler, E. R. Kimball and D. K. R. Stewart. 1976. Persistence of foliar residues of dimethoate and azinphosmethyl and their toxicity to the apple maggot. J. Econ. Entomol. 69: 473-478. [First-order model with non-zero asymptote]
Bruce H. Stanley, Oct. 16, 2003Del. Chapter of ASA Meeting: MGF and 1st-Order Dissipation Slide 37
Conclusions
• Moment-generating function is a quick way to
predict the effects of variability on dissipation
• Variability in dissipation rates can lead to “non-
linear” (on log scale) dissipation curves
• Half-lives are not constant when variability is
present
• A number of realistic mechanisms can lead to a
curvilinear dissipation curve (i.e., model is not
“diagnostic”)
Bruce H. Stanley, Oct. 16, 2003Del. Chapter of ASA Meeting: MGF and 1st-Order Dissipation Slide 38
Questions?
Bruce H. Stanley, Oct. 16, 2003Del. Chapter of ASA Meeting: MGF and 1st-Order Dissipation Slide 39
- Thank You! -