pdftexp | R Documentation |
This function computes the probability density of the Truncated Exponential distribution given parameters (\psi
and \alpha
) computed by partexp
. The parameter \psi
is the right truncation, and \alpha
is a scale parameter. The probability density function, letting \beta = 1/\alpha
to match nomenclature of Vogel and others (2008), is
f(x) = \frac{\beta\,\exp(-\beta{t})}{1 - \mathrm{exp}(-\beta\psi)}\mbox{,}
where x(x)
is the probability density for the quantile 0 \le x \le \psi
and \psi > 0
and \alpha > 0
. This distribution represents a nonstationary Poisson process.
The distribution is restricted to a narrow range of L-CV (\tau_2 = \lambda_2/\lambda_1
). If \tau_2 = 1/3
, the process represented is a stationary Poisson for which the probability density function is simply the uniform distribution and f(x) = 1/\psi
. If \tau_2 = 1/2
, then the distribution is represented as the usual exponential distribution with a location parameter of zero and a scale parameter 1/\beta
. Both of these limiting conditions are supported.
pdftexp(x, para)
x |
A real value vector. |
para |
The parameters from |
Probability density (F
) for x
.
W.H. Asquith
Vogel, R.M., Hosking, J.R.M., Elphick, C.S., Roberts, D.L., and Reed, J.M., 2008, Goodness of fit of probability distributions for sightings as species approach extinction: Bulletin of Mathematical Biology, DOI 10.1007/s11538-008-9377-3, 19 p.
cdftexp
, quatexp
, lmomtexp
, partexp
lmr <- vec2lmom(c(40,0.38), lscale=FALSE)
pdftexp(0.5,partexp(lmr))
## Not run:
F <- seq(0,1,by=0.001)
A <- partexp(vec2lmom(c(100, 1/2), lscale=FALSE))
x <- quatexp(F, A)
plot(x, pdftexp(x, A), pch=16, type='l')
by <- 0.01; lcvs <- c(1/3, seq(1/3+by, 1/2-by, by=by), 1/2)
reds <- (lcvs - 1/3)/max(lcvs - 1/3)
for(lcv in lcvs) {
A <- partexp(vec2lmom(c(100, lcv), lscale=FALSE))
x <- quatexp(F, A)
lines(x, pdftexp(x, A),
pch=16, col=rgb(reds[lcvs == lcv],0,0))
}
## End(Not run)
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