Basic RADAR Principles Prof. Sandra Cruz-Pol, Ph.D. Electrical and Computer Engineering UPRM.
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Transcript of Basic RADAR Principles Prof. Sandra Cruz-Pol, Ph.D. Electrical and Computer Engineering UPRM.
Basic RADAR PrinciplesBasic RADAR Principles
Prof. Sandra Cruz-Pol, Ph.D.
Electrical and Computer Engineering UPRM
What is a Radar?radio detection and ranging
How does a radar work?
Microwaves = have air Microwaves = have air wavelengthswavelengths in the mm – cm scales in the mm – cm scales
with with frequenciesfrequencies in the Giga Hertz [GHz] range in the Giga Hertz [GHz] range
Light is an electromagnetic wave.
Radar Band
s
Electromagnetic Spectrum
Microwave Remote Sensing
• Percentage transmission thought the earth’s atmosphere, along the vertical direction, under clear sky conditions.
Cloud and Precipitation Remote Sensing
• Atmospheric gases absorption spectrum at the ground in various humidity conditions indicated by the specific humidity values.
Types of Doppler Radar• Continuous Wave (CW)
– Simple– No range information
• Frequency Modulated CW, (FMCW)– Fine range resolution– Artifacts from target motion
• Pulse Doppler– Range and Doppler– No artifacts (except when pulse compression used)
We will see that Radars work by…
Transmitting microwave pulses….
and measuring the …•Time delay (range)•Amplitude•Polarization•Frequency
… of the microwave echo in each range gate
hello
Compare to: Acoustic Echo-location
hello
Acoustic Echo-location
hello
distance
Acoustic Echo-location
Hi !!
Hi !!
time
t = 2 x range / speed of soundExample: range = 150 mSpeed of sound ≈ 340 meters/secondt = 2 X 150 / 340 ≈ 1 second
RADAR Echolocation(RADAR ~ RAdio Detection And Ranging)
“Microwave Echo-Location”
MicrowaveTransmitter
Receiver
Tx
Rx
Target Range
time
t = 2 x range / speed of lightmeasure t, then determine Range
Example: t = .001 secSpeed of light = c = 3x108 meters/secondRange = .001 x 3x108 / 2 = 150,000 m = 150 km
Tx
Rx
We will see that Radars work by…
Transmitting microwave pulses….
and measuring the …•Time delay (range)•Amplitude•Polarization•Frequency
… of the microwave echo in each range gate
Pulse Doppler Radar
22
Range sUnambiguou
maxScT
PRF
cR
Range Resolution
Top View: 2D
DCAS advantages• Elimination of multiple echoes
False Echo
Radar 2 (Area B)
Radar 1 (Area A)
A&B
Unambiguous range of 1
radar
•Example illustrates
DCAS method for identifying real targets and false
targets that are aliased in
range
DCAS advantages (cont)
• Resolution optimization
Radar 1
Has signal
Radar 2
Has signal
x ’y ’
New resolution:
RX
Target
Range gate
Beam
We will see that Radars work by…
Transmitting microwave pulses….
and measuring the …•Time delay (range)•Amplitude•Polarization•Frequency
… of the microwave echo in each range gate
Polarization
Describes the way the electric field of the wave moves through space as seen from behind along time.•V = vertical lineal•H = Horizontal lineal
Sizes for cloud and rain dropsSizes for cloud and rain drops
Raindrops symmetryRaindrops symmetry
Differential Reflectivity
Zdr
Polarimetric radars, also called dual-pol radars, transmit radio wave pulses that have both H and V orientations. [NOAA]
TropiNET radars are the first Polarimatric Doppler radars in PR.
28
Reflectivity Factor, Reflectivity Factor, ZZ
• Is defined as
so that
• And expressed in dBZ to cover a wider dynamic range of weather conditions.
dDDNZ )(D6 ZKwo
vc2
4
5
||
ZdBZ log10
36
1-
24
512
/mmmin expressed is
and cmin is where
||
10
Z
ZKwo
vc
WHAT VARIABLES ARE MEASURED w/ Dual-pol radar?
• Differential Reflectivity –ratio of the reflected H & V power returns. Indicator of drop shape & good estimate of average drop size.
• Linear Depolarization Ratio –ratio of a V power return from a H pulse or a H from V. indicator of regions where mixtures of precipitation types occur.
• Specific Differential Phase –returned phase difference between the H V pulses caused by the difference in the number of wave cycles (or wavelengths) along the propagation path for horizontal and vertically polarized waves. It’s a "propagation effect.” very good estimator of rain rate.
Benefits of polarimetric radarsMeteorologists:•can significantly improve the accuracy of the estimates of amounts of precipitation•can tell the difference between very heavy rain and hail, which will improve flash flood watches and warnings•can identify types of precipitation in winter weather forecasts, improving forecasts of liquid water equivalent or snow depth•is more accurate than conventional radar, saving the forecasters the step of having to verify radar data•can contribute to increased lead time in flash flood and winter weather hazard warnings.Hydrologists:•provides critical rainfall estimation information for stream flow forecasts and river flooding
Raindrop shapes
Average within sample volume
We will see that Radars work by…
Transmitting microwave pulses….
and measuring the …•Time delay (range)•Amplitude•Polarization•Frequency
… of the microwave echo in each range gate
Doppler Effect
Target Radial Velocity
Frequency ft
Frequency ft+ fd In Weather radars, the
Doppler frequency shift, is caused by the motion
of the cloud and precipitation particles
Target Radial Velocity
Frequency ft
Frequency ft+ fd
Zero Velocity for “Crossing Targets”
t
rd
vf
2
Frequency ft
Frequency ft+ fd
Doppler Frequency
0.1 mm/hr
1 mm/hr
15 mm/hr
100 mm/hr
>150 mm/hr
QPE – Quantitative Precipitation Estimation
Radar reflectivity (intensity)
Doppler effect: shows vortex
Cloud and Precipitation Remote Sensing
Type of data collected by the millimeter-wave radar.
• Observations were made through the melting region of a stratiform cloud previously named “bright band” because of a systematic maximum of echo intensity observed just below the 0º isotherm.
Source: Dr. Steve Sekelsky 2004
Melting Layer at Mayaguez-Jun2011 (data from Doppler Pol radar at CID UPRM)
43
Radar equation for MeteorologyRadar equation for Meteorology• For weather applications
• for a volume
2
43
22
4 e
R
GPP oot
r drR
o
epceg
22
2pcR
V
vpoot
rR
ecGPP
2
2222
432
Vv
44
Radar EquationRadar Equation
• For power distribution in the main lobe assumed to be Gaussian function.
22
2
22
2ln1024 RL
LcGPP vrpoooot
r
22
as here defined are losses catmospheriway - two theAndeL
lossesreceiver and
tyreflectiviradar
where,
r
v
L
45
Radar EquationRadar Equation222
22
2ln1024 RLL
cGPP v
recatm
pooootr
RLLc
GPP
atmrec
prad
orad
oodBo
dBt
dBr
log20)2ln1024log(10log20log10log10log10
log10)log(10)log(10)log(2022
RRPP dBcp
dBt
dBr log20log10log10
RcdB=radar constant (including atmospheric attenuation)
For calibrated target
References• The COMET project [http://www.comet.ucar.edu/]• NASA TRMM• NCAR (National Center for Atmospheric Research) - University
Corporation for Atmospheric Research (UCAR)• NOAA http://www.nssl.noaa.gov/research/radar/dualpol.php• NOAA Educational Page
[http://www.nssl.noaa.gov/edu/ideas/radar.html]• Dave McLaughlin Basics of Radars presentation• NWS [http://www.crh.noaa.gov/fsd/soo/doppler/doppler.htm]• http://www.radartutorial.eu/07.waves/wa04.en.html