Multiple-target CW FM radar / [by] David B. Hoisington.

Survival, Water, Medical Field Manuals

Military Manuals

Hoisington, D. B. (David B.)

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LffiBART 

'■■-C'AUICAL  tePOK'f  SECTION 
i'^Jtt  ^°STGfiAOUArc  SCHOOl 
HQMESST,  CALIFOBNIA    93640 


NAVAL  POSTGRADUATE  SCHOOL 


// 


Monterey,  California 


MULTIPLE-TARGET  CW  FM  RADAR  ♦ 


David  B.  HOISINGTON 


June  1972 


Technical  Report^ for  Period  July  1971  -  June  1972 


Approved  for  public  release;  distribution  unlimited 


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NAVAL  POSTGRADUATE  SCHOOL 
Monterey,  California 


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The  work  reported  herein  was  supported  by  the  Naval  Postgraduate  School 
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MULTIPLE-TARGET  CW  FM  RADAR 


5.     TYPE   OF   REPORT   &   PERIOD   COVERED 

Technical  Report 
July  1971  -  June  1972 


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David  B.  HOISINGTON 


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Naval  Postgraduate  School 
Monterey,  CA  Code  52Hs 


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Naval  Postgraduate  School 
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15  June  1972 


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RADAR 
CW  radar 


20.     ABSTRACT  (Continue  on  reverse  aide  If  neceaaary  and  Identify  by  block  number) 


Development  of  a  multiple-target  CW  FM  radar  is  described.  This 
type  of  radar  has  advantages  over  pulse  radars  particularly  in  port- 
able, battery  operated  applications. 


DD     1  JAN  73     1473  EDITION  OF   1  NOV  65  IS  OBSOLETE 

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MULTIPLE-TARGET  CW  m  RADAR 

David  B.  Holsington 

Naval  Postgraduate  School 

Monterey,  California 


Abstract 


Development  of  a  multiple-target  CW  FM  radar  is  described.   This  type  of  radar 
has  advantages  over  pulse  radars  particularly  in  portable,  battery  operated 
applications. 


INTRODUCTION 

Althougli  multiple-target  CW  FM  radars  have  been 
suf;gested  [1],  little  application  of  FM  radar  in 
this  mode  of  operation  seems  to  have  been  made. 
Recent  advances  in  solid-state  technology  have 
made  availnble  devices  that  would  permit  the  con- 
struction of  a  multiple-target  FM  radar  that  would 
be  complctelv  solid  state  except  for  the  cathode- 
ray  tube  indicator,  and  perhaps  even  a  solid- 
state  replacement  for  the  cathode-ray  tube  will 
be  available  within  a  few  years. 

Tlie  most  obvious  application  for  a  radar  of  this 
type  would  be  in  situations  where  light  weight, 
low  power  consumption,  and  high  reliability  are 
of  paramount  importance.   Light  weight  indicates 
operation  at  9  Cllz  or  liigher  to  obtain  narrow  an- 
tenna beam  width  wilh  reasonable  antenna  size. 
It  will  be  shown  that  doppler  frequency  shifts 
can  be  of  acceptable  magnitude  at  9  GHz  for  sur- 
face targets.   Powers  in  the  order  of  1  watt  can 
be  obtained  at  9  (iHz  from  solid-state  devices, 
and  tin's  is  adequatt-  for  many  applications.   An 
experimental  program  has  been  initiated  to  demon- 
strate the  feasibiljl^  of  such  a  radar  suitable 
for  use  on  small  vi-ssi'Js  down  to  the  size  of 
motor  whale  boatP. 


THEORY  OF  OPERATION 

If  the  transmitted  frequency  of  a  CW  radar  is  swept 
linearly  with  time  as  shown  in  Figure  la,  the  re- 
ceived echos  from  fixed  targets  will  have  a  simi- 
lar pattern,  but  will  be  delayed  in  time  by  2  R/c 
where  R  is  the  target  range,  and  c  is  the  velocity 
of  propagation.   If  now  the  echo  frequency  is 
heterodyned  with  the  transmitted  signal  to  obtain 
the  beat  frequency,  f ,  ,  then 


=  2R  d f  ^  2RAf 
b   c   dt    c  T 


(1) 


where  Af  is  the  transmitter  frequency  excursion 
and  T  is  the  sweep  period.   Figure  1 -b  shows  that 
during  the  initial  portion  of  the  transmitter 
sweep,  echos  are  still  being  received  from  the  pre- 
vious sweep,  hence  the  beat  frequency  is  higher 
than  given  by  (1).   After  a  time  AT  corresponding 
to  targets  at  maximum  range  tlie  difference  fre- 
quencies associated  with  all  targets  are  as  given 
by  (1).   Tlie  receiver  is  gated  off  during  the 
initial  interval  to  prevent  the  passage  of  the 
incorrect  frequencies.   It  is  convenient  to  make 
the  duty  cycle,  (I  -A),  equal  to  1/2  so  that  the 
receiver  is  gated  on  for  n    time  i    equal  to  one 
half  of  the  sweep  period,  T. 

Figure  2  shows  the  boat  frfi|urncy  spectrum  due  to 
a  single  sweep  and  a  single  l.irgct.  Tlie  spectrum 
Is  rontiiuious  and  h.is  a  (sin  x)/x  envelope. 


Figure  1-a  Radio  frequencies  vs.  time 


Figure  1-b  Beat  frequencies  vs.  time 

To  separate  targets  at  different  ranges  one  or 
more  filters  may  be  used.   The  ideal  filter  for 
maximum  output  slgnal-to-noise  ratio  would  be 
matched  to  the  spectrum.   As  a  practical  matter 
the  filter  may  be  matched  as  nearly  as  possible 
to  the  central  lobe  of  the  spectrum.   The  filter 
6dB  (hall  amplitude)  bandwidth  is,  then,  1.2/t  or 
2.4/T.   This  filter  has  rise  and  decay  time  ■ 
approximately  equal  to  t,  hence  the  signal  due  to 
one  target  decays  during  the  receiver  dead  time 
clearing  the  filter  to  accept  another  target 
during  the  succeeding  on  time. 

Figure  3  is  a  simplified  block  diagram  of  the 
complete  system.   Received  echos  are  converted 
to  an  intermediate  frequency  for  good  noise  per- 
formance and  convenience  in  filtering.   The 
carrier  oscillator  is  linearly  swept  over  the 
frequency  band  Af.   A  portion  of  this  signal  is 
mixed  with  the  output  of  the  IF  oscillator  at  the 
frequency  (f.  -  f,  ) .   A  bandpass  filter  passes 
the  sum  frequency  (f   +  f.  -  f,  ) ,  to  the  receiver 
mixer.   The  other  input  to  this  mixer  is  from  the 
receiving  antenna.  T\\e    received  signal  at  fre- 
quency (f   -  f,  )  is  mixed  to  form  a  signal  at  the 
IF  frequency,  f    The  IF  filter  with  6dB  band- 
wldtli  f   =  1.2/i  passes  this  signal  to  the  gated 
amplifier,  detector  and  indicator. 

By  sloulv  v.iryinc,  the  frequency  of  the  IF  oscil- 
lator from  f   to  (f   -  2R    Af/rT),  i/icomine 
1       I      max  " 

>;l>'.nals  from  cich  range  intervnl  from  zero  to 


^^o  -  t> 


(f  +  -) 

O    T 


Figure  2.  Beat-frequency  spectrum  due  to  a 
swingle  sweep  and  a   single  target. 


CARRIES 
OSCILLATOR 

/^        TRANSMITTING 

<ft> 

?). 

<^ 

7-H                  AWTENNA 

BAKDPASS 
FILTER 

»              ^ 

IF 

OSCILLATOR 

'              ^ 

y 

./<:>^ 

/"        RECEIVING 

(f,  -.    f,     - 

vw^ 

(^  -  V 

V'              ANTENNA 

riLTEK 
RAMMIDTH    f 

-^ 

GATED 
AMPLIFIER 

t 

TO   DFTECTOR 
■*"       AND    INDICATOR 

Figure  3.   System  block  diagram 

maximum  range  are  successively  converted  to  the 
frequency  f.  and  are  thus  separated  to  yield  tar- 
get range  information.   The  oscilloscope  PPl  dis- 
play is  deflected  radially  in  synchronism  with  the 
IF  oscillator  frequency  sweep,  and  deflected  in 
azimuth  synchronously  with  the  antenna  sweep. 

The  range  discrimination  of  the  systems  can  be  de- 
termined from  equation  (1) .   Targets  of  equal 
strength  can  be  separately  detected  if  their  beat 
frequencies  are  separated  by  f,.   It  follows  then 
the  range  discrimination,  6R,  is  given  by 
cTff   1.2c 


6R  = 


2Af 


Af 


(2) 


Now  for  TAf>>l  it  can  be  shown  that  the  width  of 
the  transmitted  spectrum  at  half  amplitude  is 
Af[2].   It  is  not  surprising  that  for  equal  band- 
width, the  range  discrimination  of  tlie  CW  FM  radar 
Is  the  same  as  that  of  the  pulse  radar. 

The  radar  shown  in  Figure  3  lias  the  advantage  of 
simplicity,  but  Information  rate  is  limited  since 


only  one  range  interval  can  be  examined  at  a  time. 
Information  rate  could  be  increased  by  using  a 
multiplicity  of  filters.   It  is  significant  to  de- 
termine the  time  required  to  search  all  range  and 
azimuth  bins.   Assume  that  the  maximum  range  of 
interest  is  N  times  tlie  range  discrimination.   If 
successive  range  intervals  examined  are  separated 
by  6R,  and  1/T  range  are  intervals  examined  per 
second,  then  the  time  required  to  sweep  from  0  to 


maximum  range,  t  ,  is 


t   "  NT 
s 


(3) 


If  the  antenna  is  rotated  one  beam  width,  e„ ,  in 

D 

time  t  ,  then  the  search  tine  required  to  rotate 
s '  ^ 

the  antenna  through  360°  is 
360NT 


e 


B 


(4) 


where  9   is  in  degrees.   For  example,  if  N  is  200, 
B 

T  is  400  usee,  and  6   is  3",  then  t   is  9.6 
seconds.   This  time  is  increased  if  N  is  increased, 
or  If,  as  is  desirable,  some  overlap  is  permitted 
between  successive  range  intervals  examined.   The 
search  time  decreases  if  a  sector  less  than  360° 
is  scanned. 

The  doppler  shift  due  to  target  motion  is 

2v  f  /c  where  v  is  the  radial  component  of  ve- 
r  o  r 

locity.   If  v  is  20  yards/sec,  representing  a 
very  fast  surface  target,  and  f   is  9  GHz,  the 
doppler  shift  is  1100  hertz.  Typically  f j,  would 
be  in  the  order  of  5000  hertz  for  a  marine  navi- 
gation radar,  so  this  doppler  shift  represents  a 
range  error  less  than  one  fourth  of  the  range 
discrimination,  an  entirely  acceptable  error. 

COMPARISON  WITH  PULSE  RADAR 

Equation  (2)  shows  for  eqoal  transmitted  band- 
widths,  CW  FM  and  pulse  radars  have  virtually  the 
same  range  discrimination.   In  the  pulse  radar 
the  receiver  must  have  a  bandwidth  comparable  to 
the  transmitted  bandwidth.   The  CW  FM  radar,  on 
the  other  hand,  has  an  IF  bandwidth  equal  to 
f,,  a  small  fraction  of  the  transmitted  bandwidth. 
Required  gain  can  therefore  be  obtained  with  a 
relatively  small  nimber  of  stages.  Moreover,  the 


range  discrimination  may  be  cliangfd  simply  by 
changing  &f,  the  transmitter  fn-qui-ncy  deviation. 
To  change  range  discrimination  of  a  pulsi'  radar 
one  generally  changes  pulse  width,  receiver  band- 
width, and  the  pulse  repetition  frequency. 

It  can  be  shown  that  for  equal  useful  average 
povers  transmitted,  target  illumination  times, 
equal  receiver  noise  figures,  antenna  gains,  inte- 
gration efficiences,  integration  times,  and  opti- 
mized bandwidths,  pulse  and  CW  FM  radars  have  the 
same  maximum  range  on  a  given  target.   Here  the 
OiJ  FM  radar  has  a  3dB  disadvantage  if  the  receiver 
duty  cycle  is  50  percent.   Additional  loss  of  up 
to  3dB  may  occur  if  the  echo  spectrum  is  not  cen- 
tered in  the  IF  filter.   The  pulse  radar,  on  the 
other  hand,  has  a  7dB  loss  when  in  a  typical  case 
25  pulses  from  a  given  target  are  integrated  by 
means  of  a  cathode-ray  tube.   Typically,  then,  the 
range  performance  of  a  CW  FM  radar  equals  that  of 
a  comparable  pulse  radar  when  the  average  trans- 
mitted powers  are  the  same. 

The  pulse  radar  transmits  high  peak  power  in  short 
pulses  to  obtain  a  given  average  power.   High  volt- 
ages are  therefore  required  in  the  relatively 
complicated  modulator.   In  the  CW  FM  transmitter 
the  power  is  constant,  and  only  relatively  low 
voltages  are  required  in  the  transmitter.   Solid 
state  oscillators  now  available  can  furnish  the 
power  required  for  a  moderate  (10  mile)  range 
marine  navigational  radar  while  operating  from  the 
storage  battery  voltages  available  on  most  small 
craft.   A  high  degree  of  modulation  linearity  is 
required  in  the  CW  FM  transmitter,  but  the  re- 
quired linearity  is  not  necessarily  hard  to 
obtain  [3]. 

Pulse  radars  do  not  suffer  from  any  range  ambi- 
guity provided  echos  are  not  received  from  targets 
at  a  time  greater  than  the  pulse  repetition  period. 
CW  FM  radars  may  have  a  range  ambiguity  problem 
when  weak  target  returns  are  received  at  ranges 
somewhat  smaller  or  larger  than  the  return  from  a 
very  strong  target.   Figure  2  shows  the  IF  spec- 
trum of  a  given  target.   If  the  IF  filter  is  at  a 
frequency  2/t  higher  than  the  center  of  thla 


spectrum  in  an  effort  to  locate  a  target  at  a 
range  difforing  by  2r/Af,  the  filter  will  respond 
to  the  side  bands  of  the  strong-target  spectrum. 
The  filter  output  in  this  case  will  be  In  the 
order  of  26  dB  less  than  if  the  strong  target  re- 
turn were  centered  In  the  filter,  but  this 
spurious  response  could  make  it  difficult  to  de- 
tect the  return  from  a  navigational  buoy  with  a 
relatively  large  object  such  as  a  ship  nearby. 
This  range  ambiguity  can  be  reduced,  for  example, 
by  shaping  the  IF  spectrum  of  targets  to  reduce 
the  amplitude  of  the  side  bands.   This  could  be 
accomplished  by  modulating  the  receiver  gain 
before  the  IF  filter  with  a  smooth  weighting  func- 
tion rather  than  by  employing  square-wave  gating 
as  has  been  assumed.   Further  work  needs  to  be 
done  in  this  area. 

EXPERIMENTAL  PROGRAM 

As  the  first  step  in  demonstrating  the  feasibility 
of  a  solid-state  CW  FM  radar,  a  hybrid  unit  was 
constructed  from  laboratory  components.   The 
basic  systiiii  block  diagram  was  as  indicated  in 
Figure  3.   Operation  was  at  a  frequency  of  about 
9  GHz  with  a  power  output  of  2  watts.   The  trans- 
mitter frequency  deviation  could  be  set  at  any 
value  up  to  12  Mllz.   The  receiver  intermediate 
frequency  was  30  MHz,  and  the  IF  filter  was  a 
linear  phase  (Gaussian)  filter  with  a  6  dB  band- 
width of  5.1  kHz.   Receiver  noise  figure  was  13.8 
dB.   Circular  parabolic  reflectors  with  a  3  de- 
gree beam  width  were  used  for  both  transmitting 
and  receiving  antennas.   These  antennas  could  not 
conveniently  be  scanned,  so  a  type  A  (amplitude 
vs  range)  presentation  was  used. 

Figure  U   shows  a  typical  display  obtained  with 
the  antenna  oriented  as  shown  in  Figure  5. 
Figure  6  shows  a  high  resolution  display  obtained 
with  the  antenna  oriented  as  shown  in  Figure  7. 
Note  that  objects  separated  by  AO  yards  are  com- 
pletely resolved.   This  display  was  obtained  with 
a  Af  of  12  MHz  for  a  theoretical  range  resolution 
from  equation  (2)  of  33  yards. 


Figure  4.      Long-range  display 


3°  BEAMWIDTH 


STACK 

KMBY  TOWER 


POINT  CABRILLO 


4000  YDS 
POINT  ALONES 


PACIFIC 
OCEAN 


MONTEREY 


COAST  GUARD  PIER 
MONTEREY  WHARF 


SPANAGEL  HALL 


Figure   5.      Kadar   field  of   view    (long-range) 


Figure   6.      Short-range   display  of   campus 
BEAM  WIDTH 


INGERSOLL 


HALUGAN 


BULLARD 


ROOT 


j       343  YDS 
305YDS 


4- 


RADAR 


rj-  i 

i        ,     173YDS 
133YDS 


Li_L 


SPANAGEL  HALL 
Figure  7.   Radar  field  of  view  (short-range) 

CONCLUSIONS 

The  feasibility  of  a  CW  FM  radar  with  a  range 
resolution  of  about  30  yards  has  been  demonstra- 
ted.  It  remains  to  be  shown  that  such  a  radar 
can  be  built  with  all  solid-state  components  in  a 
small,  lightweight  package.   Development  of  the 
necessary  solid-state  circuitry  is  proceeding  as 
time  and  limited  funding  pemit. 


ACKN()WLtD(TMENT 

Appreciation  is  expressed  to  Lieutenant  Ronald  P. 
Lewis,  tISN ,  who  performed  much  of  the  experimental 
work  reported  in  this  paper  as  part  of  the  require- 
ments for  a  Master  of  Science  tliesis. 

REFERENCES 

1.  Luck,  D.  G.  C. ,  FM  Radar,  McGraw-Hill  Book 
Company,  Inc.,  New  York,  19A9 

2.  Berkowitz,  R.  S.,  Modern  Radar,  P.  225,  John 
Wiley  &  Sons,  Inc.,  New  York,  1965. 

3.  Lewis,  R.  P.,  A  Developmental  CW  FM  Multi- 
Target  Radar,  M.S.  Thesis,  Naval  Postgraduate 
School,  Monterey,  California,  1971. 


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