Radar Meteorology 2: Radar reflectivity and products
Notes of Fabry, F. (2018). Radar meteorology: principles and practice. Cambridge University Press. Ch. 3
The radar equation
Most precipitation targets are much smaller than the usual radar wavelength (Rayleigh scatterers). For such targets, we define $Z$ as the radar reflectivity factor per unit volume:
\[Z=\int _0^{\infty}N(D)D^6\mathrm{d}D\]Note that $Z$ is usually expressed in nonstandard units of $\mathrm{mm^6}/\mathrm{m^3}$
A convenient version of radar equation for radars with parabolic antennas is
\[P_\mathrm{r}=\frac{1.22^2\times 0.55^2\times 10^{-18}\pi^7c}{1024\ln2}\frac{P_\mathrm{t}\tau D_\mathrm{a}^2}{\lambda^4}\frac{T^2(0,r)}{r^2}\Vert K\Vert^2Z\]first term: constants
second term: radar parameters
third term: path
the rest: target properties
where $P_t$ is the power of the transmit pulse and $\tau$ its duration; $D_\mathrm{a}$ is the diameter of the antenna; $T$ is the transmittance of the atmosphere along the path between the radar at range 0 and the sampling volume at range $r$, and $\Vert K\Vert^2$ is the dielectric constant of the scatterers and is related to the complex index of refraction of the hydrometeor $n(\lambda)$ via
\[\Vert K\Vert^2=\left\Vert\frac{n^2(\lambda)-1}{n^2(\lambda)+2}\right\Vert^2\]The equivalent reflectivity factor
In most cases, we don’t know for certain about the nature of the targets ($\Vert K\Vert^2$?, Rayleigh scattering or not). Because of that, we define the equivalent factor $Z_\mathrm{e}$ such that
\[P_\mathrm{r}=\frac{1.22^2\times 0.55^2\times 10^{-18}\pi^7c}{1024\ln2}\frac{P_\mathrm{t}\tau D_\mathrm{a}^2}{\lambda^4}\frac{T^2(0,r)}{r^2}\Vert K_\mathrm{w}\Vert^2Z_\mathrm{e}\]with $\Vert K_\mathrm{w}\Vert^2$ being the dielectric constant of liquid water(0.93). Normally, it is the $Z_\mathrm{e}$ that is measured by the radar.
For convenience, we generally express reflectivity factors in units of decibels (dB) as
\[\mathrm{dB}Z=10\log _{10}Z\]| Targets type | $Z_\mathrm{e}$($\mathrm{dB}Z$) |
|---|---|
| Light drizzle; insects | 0 |
| Moderate drizzle; a few raindrops; light snow; migrating birds | 10 |
| Light rain or moderate snow; typical of widespread precipitation (1 mm/h) | 25 |
| moderate rain, strong for widespread precipitation (5 mm/h) | 35 |
| Heavy rain from a convective shower (20 mm/h) | 45 |
| Hail or very heavy rain, peak of thunderstorms | 55 |
| Moderate to severe hail | >60 |
Reflectivity factor and rain rate
reflectivity factor:
\[Z=\int _0^{\infty}N(D)D^6\mathrm{d}D\]rainfall rate:
\[R=\int _0^{\infty}N(D)D^3w_\mathrm{r}(D)\mathrm{d}D\]$w_\mathrm{r}(D)$: fall speed of a raindrop of diameter $D$.
There are no mathematical functions linking $Z$ and $R$. On average, however, DSD varies systematically with reflectivity and precipitation intensity. $Z$-$R$ relationships are derived based on that fact:
\[\begin{aligned} & Z=200R^{1.6}\qquad\mathrm{Marshall-Palmer\ 1950s} \\ & Z=300R^{1.5}\qquad\mathrm{Joss\ and\ Waldvogel\ 1970} \\ & Z=300R^{1.4}\qquad\mathrm{WSR-88D} \end{aligned}\]$Z$-$R$ relationships power laws of the form $Z=aR^b$ of which the coefficients $a$ and $b$ depend on the dynamics and microphysics processes controlling precipitation formation. Hence, it varies from one region to another.
Radar products
- Vertical cross sections
- Vertically integrated liquid (VIL)
- …