temporalBehaviour {StormR} | R Documentation |
Computing wind behaviour time series and summary statistics at given point locations
Description
The temporalBehaviour()
function allows computing wind speed and direction
for a given location or set of locations along the lifespan of a tropical cyclone.
It also allows to compute three associated summary statistics.
Usage
temporalBehaviour(
sts,
points,
product = "TS",
windThreshold = NULL,
method = "Willoughby",
asymmetry = "Chen",
empiricalRMW = FALSE,
tempRes = 60,
verbose = 1
)
Arguments
sts |
|
points |
data.frame. Consisting of two columns names as "x" (for the longitude) and "y" (for the latitude), providing the coordinates in decimal degrees of the point locations. Row names can also be provided to named the locations. |
product |
character. Desired output statistics:
|
windThreshold |
numeric vector. Minimal wind threshold(s) (in |
method |
character. Model used to compute wind speed and direction. Three different models are implemented:
|
asymmetry |
character. If
|
empiricalRMW |
logical. Whether (TRUE) or not (FALSE) to compute
the radius of maximum wind ( |
tempRes |
numeric. Temporal resolution (min). Can be |
verbose |
numeric. Information displayed. Can be:
|
Details
Storm track data sets, such as those extracted from IBRTrACKS (Knapp et
al., 2010), usually provide observation at a 3- or 6-hours temporal
resolution. In the temporalBehaviour() function, linear interpolations are
used to reach the temporal resolution specified in the tempRes
argument
(default value = 60 min).
The Holland (1980) model, widely used in the literature, is based on the 'gradient wind balance in mature tropical cyclones. The wind speed distribution is computed from the circular air pressure field, which can be derived from the central and environmental pressure and the radius of maximum winds.
v_r = \sqrt{\frac{b}{\rho} \times \left(\frac{R_m}{r}\right)^b \times (p_{oci} - p_c)
\times e^{-\left(\frac{R_m}{r}\right)^b} + \left(\frac{r \times f}{2}\right)^2} -
\left(\frac{r \times f}{2}\right)
with,
b = \frac{\rho \times e \times v_m^2}{p_{oci} - p_c}
f = 2 \times 7.29 \times 10^{-5} \sin(\phi)
where, v_r
is the tangential wind speed (in m.s^{-1}
),
b
is the shape parameter,
\rho
is the air density set to 1.15 kg.m^{-3}
,
e
being the base of natural logarithms (~2.718282),
v_m
the maximum sustained wind speed (in m.s^{-1}
),
p_{oci}
is the pressure at outermost closed isobar of the storm (in Pa
),
p_c
is the pressure at the centre of the storm (in Pa
),
r
is the distance to the eye of the storm (in km
),
R_m
is the radius of maximum sustained wind speed (in km
),
f
is the Coriolis force (in N.kg^{-1}
, and
\phi
being the latitude).
The Willoughby et al. (2006) model is an empirical model fitted to aircraft observations. The model considers two regions: inside the eye and at external radii, for which the wind formulations use different exponents to better match observations. In this model, the wind speed increases as a power function of the radius inside the eye and decays exponentially outside the eye after a smooth polynomial transition across the eyewall.
\left\{\begin{aligned}
v_r &= v_m \times \left(\frac{r}{R_m}\right)^{n} \quad if \quad r < R_m \\
v_r &= v_m \times \left((1-A) \times e^{-\frac{|r-R_m|}{X1}} +
A \times e^{-\frac{|r-R_m|}{X2}}\right) \quad if \quad r \geq R_m \\
\end{aligned}
\right.
with,
n = 2.1340 + 0.0077 \times v_m - 0.4522 \times \ln(R_m) - 0.0038 \times |\phi|
X1 = 287.6 - 1.942 \times v_m + 7.799 \times \ln(R_m) + 1.819 \times |\phi|
A = 0.5913 + 0.0029 \times v_m - 0.1361 \times \ln(R_m) - 0.0042 \times |\phi|
and A\ge0
where, v_r
is the tangential wind speed (in m.s^{-1}
),
v_m
is the maximum sustained wind speed (in m.s^{-1}
),
r
is the distance to the eye of the storm (in km
),
R_m
is the radius of maximum sustained wind speed (in km
),
\phi
is the latitude of the centre of the storm,
X2 = 25
.
Asymmetry can be added to Holland (1980) and Willoughby et al. (2006) wind fields as follows,
\vec{V} = \vec{V_c} + C \times \vec{V_t}
where, \vec{V}
is the combined asymmetric wind field,
\vec{V_c}
is symmetric wind field,
\vec{V_t}
is the translation speed of the storm, and
C
is function of r
, the distance to the eye of the storm (in km
).
Two formulations of C proposed by Miyazaki et al. (1962) and Chen (1994) are implemented.
Miyazaki et al. (1962)
C = e^{(-\frac{r}{500} \times \pi)}
Chen (1994)
C = \frac{3 \times R_m^{\frac{3}{2}} \times
r^{\frac{3}{2}}}{R_m^3 + r^3 +R_m^{\frac{3}{2}} \times r^{\frac{3}{2}}}
where, R_m
is the radius of maximum sustained wind speed (in km
)
The Boose et al. (2004) model, or “HURRECON” model, is a modification of the Holland (1980) model. In addition to adding asymmetry, this model treats of water and land differently, using different surface friction coefficient for each.
v_r = F\left(v_m - S \times (1 - \sin(T)) \times \frac{v_h}{2} \right)
\times \sqrt{\left(\frac{R_m}{r}\right)^b \times e^{1 - \left(\frac{R_m}{r}\right)^b}}
with,
b = \frac{\rho \times e \times v_m^2}{p_{oci} - p_c}
where, v_r
is the tangential wind speed (in m.s^{-1}
),
F
is a scaling parameter for friction (1.0
in water, 0.8
in land),
v_m
is the maximum sustained wind speed (in m.s^{-1}
),
S
is a scaling parameter for asymmetry (usually set to 1
),
T
is the oriented angle (clockwise/counter clockwise in Northern/Southern Hemisphere) between
the forward trajectory of the storm and a radial line from the eye of the storm to point $r$
v_h
is the storm velocity (in m.s^{-1}
),
R_m
is the radius of maximum sustained wind speed (in km
),
r
is the distance to the eye of the storm (in km
),
b
is the shape parameter,
\rho = 1.15
is the air density (in kg.m^{-3}
),
p_{oci}
is the pressure at outermost closed isobar of the storm (in Pa
), and
p_c
is the pressure at the centre of the storm (pressure
in Pa
).
Value
For each storm and each point location, the temporalBehaviour()
function returns
a data.frame. The data frames are organised into named lists. Depending on the product
argument
different data.frame are returned:
if
product == "TS"
, the function returns a data.frame with one row for each observation (or interpolated observation) and four columns for wind speed (inm.s^{-1}
), wind direction (in degree), the observation number, and the ISO time of observations,if
product == "PDI"
, the function returns a data.frame with one row for each point location and one column for the PDI,if
product == "Exposure"
, the function returns a data.frame with one row for the duration of exposure to winds above each wind speed threshold defined by thewindThreshold
argument and one column for each point location.
References
Boose, E. R., Serrano, M. I., & Foster, D. R. (2004). Landscape and regional impacts of hurricanes in Puerto Rico. Ecological Monographs, 74(2), Article 2. https://doi.org/10.1890/02-4057
Chen, K.-M. (1994). A computation method for typhoon wind field. Tropic Oceanology, 13(2), 41–48.
Holland, G. J. (1980). An Analytic Model of the Wind and Pressure Profiles in Hurricanes. Monthly Weather Review, 108(8), 1212–1218. https://doi.org/10.1175/1520-0493(1980)108<1212:AAMOTW>2.0.CO;2
Knapp, K. R., Kruk, M. C., Levinson, D. H., Diamond, H. J., & Neumann, C. J. (2010). The International Best Track Archive for Climate Stewardship (IBTrACS). Bulletin of the American Meteorological Society, 91(3), Article 3. https://doi.org/10.1175/2009bams2755.1
Miyazaki, M., Ueno, T., & Unoki, S. (1962). The theoretical investigations of typhoon surges along the Japanese coast (II). Oceanographical Magazine, 13(2), 103–117.
Willoughby, H. E., Darling, R. W. R., & Rahn, M. E. (2006). Parametric Representation of the Primary Hurricane Vortex. Part II: A New Family of Sectionally Continuous Profiles. Monthly Weather Review, 134(4), 1102–1120. https://doi.org/10.1175/MWR3106.1
Examples
# Creating a stormsDataset
sds <- defStormsDataset()
# Geting storm track data for tropical cyclone Pam (2015) near Vanuatu
pam <- defStormsList(sds = sds, loi = "Vanuatu", names = "PAM")
pts <- data.frame(x = c(168.5, 168), y = c(-17.9, -16.3))
row.names(pts) <- c("point_1", "point_2")
# Computing time series of wind speed and direction for Pam
# over points 1 and 2 defined above
ts.pam <- temporalBehaviour(pam, points = pts)
# Computing PDI for Pam over points 1 and 2 defined above
pdi.pam <- temporalBehaviour(pam, points = pts, product = "PDI")
# Computing the duration of exposure to wind speeds above the thresholds
# used by the Saffir-Simpson hurricane wind scale for Pam
# over points 1 and 2 defined above
exp.pam <- temporalBehaviour(pam, points = pts, product = "Exposure")