predADTS2 | R Documentation |
Predicts the occurrence times using the accumulated days transferred to a standardized temperature (ADTS) method based on observed or predicted minimum and maximum daily air temperatures (Konno and Sugihara, 1986; Aono, 1993; Shi et al., 2017a, b).
predADTS2(S, Ea, AADTS, Year2, DOY, Tmin, Tmax, DOY.ul = 120)
S |
the starting date for thermal accumulation (in day-of-year) |
Ea |
the activation free energy (in kcal |
AADTS |
the expected annual accumulated days transferred to a standardized temperature |
Year2 |
the vector of the years recording the climate data for predicting the occurrence times |
DOY |
the vector of the dates (in day-of-year) for which climate data exist |
Tmin |
the minimum daily air temperature data (in |
Tmax |
the maximum daily air temperature data (in |
DOY.ul |
the upper limit of |
Organisms exhibiting phenological events in early spring often experience several cold days
during their development. In this case, Arrhenius' equation (Shi et al., 2017a, b,
and references therein) has been recommended to describe the effect of the absolute temperature
(T
in Kelvin [K]) on the developmental rate (r
):
r = \mathrm{exp}\left(B - \frac{E_{a}}{R\,T}\right),
where E_{a}
represents the activation free energy (in kcal \cdot
mol{}^{-1}
);
R
is the universal gas constant (= 1.987 cal \cdot
mol{}^{-1}
\cdot
K{}^{-1}
);
B
is a constant. To maintain consistence between the units used for E_{a}
and R
, we need to
re-assign R
to be 1.987\times {10}^{-3}
, making its unit 1.987\times {10}^{-3}
kcal \cdot
mol{}^{-1}
\cdot
K{}^{-1}
in the above formula.
\qquad
According to the definition of the developmental rate (r
),
it is the developmental progress per unit time (e.g., per day, per hour),
which equals the reciprocal of the developmental duration D
, i.e., r = 1/D
. Let T_{s}
represent the standard temperature (in K), and r_{s}
represent the developmental rate at T_{s}
.
Let r_{j}
represent the developmental rate at T_{j}
, an arbitrary
temperature (in K). It is apparent that D_{s}r_{s} = D_{j}r_{j} = 1
. It follows that
\frac{D_{s}}{D_{j}} = \frac{r_{j}}{r_{s}} =
\mathrm{exp}\left[\frac{E_{a}\left(T_{j}-T_{s}\right)}{R\,T_{j}\,T_{s}}\right],
where D_{s}/D_{j}
is referred to as the number of days transferred to a standardized temperature
(DTS) (Konno and Sugihara, 1986; Aono, 1993).
\qquad
In the accumulated days transferred to a standardized temperature (ADTS) method,
the annual accumulated days transferred to a standardized temperature (AADTS) is assumed to be a constant.
Let \mathrm{AADTS}_{i}
denote the AADTS of the i
th year, which equals
\mathrm{AADTS}_{i} = \sum_{j=S}^{E_{i}}\sum_{w=1}^{24}\left\{\frac{1}{24}\,\mathrm{exp}\left[\frac{E_{a}\left(T_{ijw}-T_{s}\right)}{R\,T_{ijw}\,T_{s}}\right]\right\},
where E_{i}
represents the ending date (in day-of-year), i.e., the occurrence time of a pariticular
phenological event in the i
th year, and T_{ijw}
represents the estimated mean hourly temperature of
the w
th hour of the j
th day of the i
th year (in K). This packages takes the method proposed by
Zohner et al. (2020) to estimate the mean hourly temperature (T_{w}
) for each of 24 hours:
T_{w} = \frac{T_{\mathrm{max}} - T_{\mathrm{min}}}{2}\, \mathrm{sin}\left(\frac{w\pi}{12}-
\frac{\pi}{2}\right)+\frac{T_{\mathrm{max}} + T_{\mathrm{min}}}{2},
where w
represents the w
th hour of a day, and T_{\mathrm{min}}
and T_{\mathrm{max}}
represent the minimum and maximum temperatures of the day, respectively.
\qquad
In theory, \mathrm{AADTS}_{i} = \mathrm{AADTS}
,
i.e., the AADTS values of different years are a constant. However, in practice, there is
a certain deviation of \mathrm{AADTS}_{i}
from \mathrm{AADTS}
that is estimated by \overline{\mathrm{AADTS}}
(i.e., the mean of the \mathrm{AADTS}_{i}
values). The following approach
is used to determine the predicted occurrence time.
When \sum_{j=S}^{F}\sum_{w=1}^{24}\left\{\frac{1}{24}\,\mathrm{exp}\left[\frac{E_{a}\left(T_{ijw}-T_{s}\right)}
{R\,T_{ijw}\,T_{s}}\right]\right\} = \overline{\mathrm{AADTS}}
(where F \geq S
), it follows that F
is
the predicted occurrence time; when \sum_{j=S}^{F}\sum_{w=1}^{24}\left\{\frac{1}{24}\,\mathrm{exp}\left[
\frac{E_{a}\left(T_{ijw}-T_{s}\right)}{R\,T_{ijw}\,T_{s}}\right]\right\} < \overline{\mathrm{AADTS}}
and
\sum_{j=S}^{F+1}\sum_{w=1}^{24}\left\{\frac{1}{24}\,\mathrm{exp}\left[\frac{E_{a}\left(T_{ijw}-T_{s}\right)}
{R\,T_{ijw}\,T_{s}}\right]\right\} > \overline{\mathrm{AADTS}}
, the trapezoid method (Ring and Harris, 1983)
is used to determine the predicted occurrence time.
Year |
the years with climate data |
Time.pred |
the predicted occurrence times (day-of-year) in different years |
The entire minimum and maximum daily temperature data set for the spring of each year should be provided.
It should be noted that the unit of Tmin
and Tmax
in Arguments is {}^{\circ}
C, not K.
Peijian Shi pjshi@njfu.edu.cn, Zhenghong Chen chenzh64@126.com, Jing Tan jmjwyb@163.com, Brady K. Quinn Brady.Quinn@dfo-mpo.gc.ca.
Aono, Y. (1993) Climatological studies on blooming of cherry tree (Prunus yedoensis) by means
of DTS method. Bulletin of the University of Osaka Prefecture. Ser. B, Agriculture and life sciences
45, 155-
192 (in Japanese with English abstract).
Konno, T., Sugihara, S. (1986) Temperature index for characterizing biological activity in soil and
its application to decomposition of soil organic matter. Bulletin of National Institute for
Agro-Environmental Sciences 1, 51-
68 (in Japanese with English abstract).
Ring, D.R., Harris, M.K. (1983) Predicting pecan nut casebearer (Lepidoptera: Pyralidae) activity
at College Station, Texas. Environmental Entomology 12, 482-
486. \Sexpr[results=rd]{tools:::Rd_expr_doi("10.1093/ee/12.2.482")}
Shi, P., Chen, Z., Reddy, G.V.P., Hui, C., Huang, J., Xiao, M. (2017a) Timing of cherry tree blooming:
Contrasting effects of rising winter low temperatures and early spring temperatures.
Agricultural and Forest Meteorology 240-
241, 78-
89. \Sexpr[results=rd]{tools:::Rd_expr_doi("10.1016/j.agrformet.2017.04.001")}
Shi, P., Fan, M., Reddy, G.V.P. (2017b) Comparison of thermal performance equations in describing
temperature-dependent developmental rates of insects: (III) Phenological applications.
Annals of the Entomological Society of America 110, 558-
564. \Sexpr[results=rd]{tools:::Rd_expr_doi("10.1093/aesa/sax063")}
Zohner, C.M., Mo, L., Sebald, V., Renner, S.S. (2020) Leaf-out in northern ecotypes of wide-ranging
trees requires less spring warming, enhancing the risk of spring frost damage at cold limits.
Global Ecology and Biogeography 29, 1056-
1072. \Sexpr[results=rd]{tools:::Rd_expr_doi("10.1111/geb.13088")}
ADTS2
data(apricotFFD)
data(BJDAT)
X1 <- apricotFFD
X2 <- BJDAT
Year1.val <- X1$Year
Time.val <- X1$Time
Year2.val <- X2$Year
DOY.val <- X2$DOY
Tmin.val <- X2$MinDT
Tmax.val <- X2$MaxD
DOY.ul.val <- 120
S.val <- 46
Ea.val <- 22.3
AADTS.val <- 4.911035
cand.res4 <- predADTS2( S = S.val, Ea = Ea.val, AADTS = AADTS.val,
Year2 = Year2.val, DOY = DOY.val, Tmin = Tmin.val,
Tmax = Tmax.val, DOY.ul = DOY.ul.val )
cand.res4
ind3 <- cand.res4$Year %in% intersect(cand.res4$Year, Year1.val)
ind4 <- Year1.val %in% intersect(cand.res4$Year, Year1.val)
RMSE2 <- sqrt( sum((Time.val[ind4]-cand.res4$Time.pred[ind3])^2) / length(Time.val[ind4]) )
RMSE2
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