RADAR
EQUATION
Dr.
Brad Muller
RADAR is an acronym that stands for
"RAdio Detection And Ranging." This is an active remote
sensing technique because it involves a transmitter sending out pulses of
electromagnetic radiation, then measuring the amount of power reflected
(scattered) back to the radar antenna. This process can be quantified in
the Radar Equation.
The Radar Equation is given as
follows:

where
pt= power transmitted by radar (watts)
pr=
power received back by radar (watts)
g = gain of the antenna (ratio of
power on the beam axis to power from an isotropic [i.e., radiating equally in
all directions] antenna at the same point); it is a measure of how
focused the radar beam is.
q = horizontal beamwidth (radians)
f = vertical beamwidth (radians)
h = pulselength (m)
|K|2 = dielectric constant for hydrometeors; usually taken as
0.93 for liquid water, 0.197 for ice. (Note that for an equivalent mass of
frozen precipitation, much less power is returned from the ice than from liquid
precipitation; thus snow with the same water content is less reflective than
rain). For this reason, NEXRAD’s clear
air mode rather than precipitation mode is sometimes used to monitor snow
situations because of its greater sensitivity).
l
= loss factor for attenuation of radar beam, varies between 0 and 1, usually
near 1. Since the attenuation of the beam is often unknown, it is often
ignored.
l =wavelength
of radar pulse (m)
r = range or distance to the target
(i.e., the distance to an area of precipitation that reflects the originally
transmitted pulse back to the radar).
z = radar reflectivity factor (mm6/m3)
and can be expressed as

where D is the drop
diameter and the summation is over the total number of drops (of varying
sizes) within a unit volume within the beam; in the equation it gets
multiplied by the radar volume [defined by the beam width, height, pulse length
and distance from the radar]

Therefore z is a function of the
diameters and number of drops in unit volume, i.e., the drop size
distribution.
Note that z is an
inherent property of the drop size distribution sampled and is not radar-dependent.
In other words, it is a property of the precipitation characteristics
within a given storm, and whatever drop sizes happen to be in that storm, and
has nothing to do with the radar.
[Note: The radar equation can also
be written in this slightly different form

where h, the pulse length in
distance units, is replaced by c, the speed of electromagnetic radiation, and
t, the pulse duration.]
However, the drop size distribution
in the measured volume is unknown. Therefore, we calculate the radar
reflectivity factor, z, from the return power, pr, by solving the
above equation for z:


We can combine the known
(radar-specific) variables like beamwidth, gain etc., the numerical values, and
the assumed values (|K|2 is assumed as the liquid water value, 0.93,
since we don’t know a priori what the
precipitation type is, even though it may actually be snow or hail, and l is usually assumed to be 1) in the
above equation into a single known constant, c1, to arrive at the
simplified expression:
z = c1 pr r2
Thus, given a specific radar and
configuration, the only real variables in this problem are the amount of power
returned, pr, and the range, r, to the echoes, which are both
measured by the radar based on the elapsed time since the pulse was sent out.
Because the radar reflectivity
factor spans a huge range of magnitudes (from 0.001 mm6/m3 for
fog, to 36,000,000
mm6/m3 for softball-sized
hail, it is usually expressed in decibels (dB) of reflectivity or dBZ
as follows:
Z = 10log10(z / 1 mm6/m3)
[Note: be sure to distinguish
between capital Z and lower case z here!]
The logarithmic transformation here
is used to compress the large range of magnitudes into a more comprehensible
scale of values. Logarithms are actually just exponents, so the "log10 of z" is just the exponent that 10
would be raised to, to obtain a value of z.
The following table shows
interrelationships between z, Z, exponents, logs, and the decibel
scale:
|
z |
10x
= z |
x
= log10 z |
Z |
|
0.001 |
10-3
|
-3 |
-30 |
|
0.01 |
10-2
|
-2 |
-20 |
|
0.1 |
10-1
|
-1 |
-10 |
|
1 |
100
|
0 |
0 |
|
10 |
101
|
1 |
10 |
|
100 |
102
|
2 |
20 |
|
1,000 |
103
|
3 |
30 |
|
10,000 |
104
|
4 |
40 |
|
100,000 |
105
|
5 |
50 |
|
1,000,000 |
106
|
6 |
60 |
|
10,000,000 |
107
|
7 |
70 |
Color-filled contours of 22 levels of reflectivity, Z,
are what is plotted on NEXRAD radar data displays.
Prior to NEXRAD, reflectivity from the WSR-57’s or WSR74’s was plotted as 6
levels of reflectivity called VIP (Video Integrator Processor) levels. NEXRAD data plotted as VIP levels can be
found on an Aviation Digital Data Service radar page showing radar
coded messages .
Rain
rates from Reflectivity
Rain rates can be calculated from
radar reflectivity data if we assume that we know the drop size distribution
within a volume of air measured by the radar.
So-called z-R relationships relate the radar reflectivity factor, z (mm6/m3),
to the rain rate, R (mm/hr) based on different assumed drop sizes for
different kinds of storms, and are of the form
![]()
where A and b are
empirically-derived constants. Over the
years, many z-R relations have been obtained by researchers. A few z-R relations recommended by the Radar
Operations Center are listed in this table borrowed from
https://www.ou.edu/radar/z_r_relationships.pdf
|
Relationship |
Optimum for: |
Also recommended for: |
|
Marshall-Palmer |
General stratiform precipitation |
|
|
(z = 200R1.6) |
|
|
|
East-Cool Stratiform |
Winter stratiform precipitation - |
Orographic rain -East |
|
(z = 130R2.0) |
east of continental divide |
|
|
West-Cool Stratiform |
Winter stratiform precipitation - |
Orographic rain -West |
|
(z = 75R2.0) |
west of continental divide |
|
|
WSR-88D Convective |
Summer deep convection |
Other non-tropical |
|
(z = 300R1.4) |
|
convection |
|
Rosenfeld Tropical |
Tropical convective systems |
|
|
(z = 250R1.2) |
|
|
Note that this form of the z-R
relation is not useful for calculating the rain rate—we must
solve the equation for R and convert from radar reflectivity factor, z, to
reflectivity, Z, then we can plug in
the reflectivity measured by the radar.
The result for a Marshall-Palmer
drop size distribution is:
R
= C 10(0.0625 Z)
where R is rain rate in mm/hr, C = 0.036 mm/hr, and Z is the
reflectivity in dBZ.
Example:
For a reflectivity of 39 dBZ, the rain rate is
RR
= 0.036 x 10(0.0625 x 39)
=
9.86 mm/hr x (1 cm/10 mm) x (1 in/2.54 cm)
=
0.39 inches/hour