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7~ AD-763 9444 MTI (MOVING TARGET INDICTORS) TRACKING OF A REENTRY VEHICLE IN STRONG ATTACHED 'WAKE -I •M. Arm, et al Riverside Research Institute SIN .•_•_• •_Prepared for: . \White Sa~nds Missile Range 15 June 197,3 DISTRIBUTED BY: Nab"onl Technical Infomfi• Service .A U. S. DEPARTMENT Of COMMERCE 5285 Port Royal Road, Springfield Va. 22151 " I
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Page 1: SIN - DTIC · timirg diagram. Power divider PD2 drives the cancellation loop which introduces a 10,5 lisec delay and a loop gain of two. (The exact delay is adjusted ay the proper

7~

AD-763 9444

MTI (MOVING TARGET INDICTORS) TRACKINGOF A REENTRY VEHICLE IN STRONG ATTACHED'WAKE

-I •M. Arm, et al

Riverside Research Institute

SIN

.•_•_• •_Prepared for: .

• • \White Sa~nds Missile Range

• • 15 June 197,3

DISTRIBUTED BY:

Nab"onl Technical Infomfi• Service .AU. S. DEPARTMENT Of COMMERCE5285 Port Royal Road, Springfield Va. 22151

" I

Page 2: SIN - DTIC · timirg diagram. Power divider PD2 drives the cancellation loop which introduces a 10,5 lisec delay and a loop gain of two. (The exact delay is adjusted ay the proper

RIVERSIDE RESEARCH INSTITUTE

80 West End Avenue / New York, New York 10023 /1(212) 8-O-4000

,5 june 1973

TECHNICAL MEMORANDUM TM-64/241-4-60

MTI TRACKING OF A REENTRY VEHICLE

IN STRONG ATTACHED WA'(E

By

M. Arm and I. Wesssman

Prtpc-,'d for

Commanding Genera'

WIk,-te Sonds Mi;sile RangeNew Mexico

e8002

Contract No. DAAD07-72-C-0128

-•; ~~~~NAP-,r'4 .. A "LIC:.

C-DCI ,,,, II,

,1.7

16u'ill

+_3

++ D-A__________________________L +h z ->'+-+- . . ._L --.:---:- T U L-

Page 3: SIN - DTIC · timirg diagram. Power divider PD2 drives the cancellation loop which introduces a 10,5 lisec delay and a loop gain of two. (The exact delay is adjusted ay the proper

RIVERSIDE RESEARCH INSTITUTE

AUTHORI ZATI ON

This report describes research performed

at Riverside Research Institute and was pre-

pared by M. Arm and I. Weissman.

This research is supported by the Depart-

ment of the Army, White Sands Missile Range,

New Mexico, under Contract DA.AD07-72-C-0128.

Approved by:

N. B. MarileDirector.

Radar Division

.- 6 4 /, -4-60 1 -4----

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II ... RIVERSIDE RESEARCH INSTITbIE II. INTROIJCTIOUz

This memorandum presents data, o1g-ained by the AMRAD

2; radar at the White Sands Missile Range, which demonstrateSi the utility of _MTI clutter cancellation techniques for im-

proving the tracking of reentry vehicles in the presence

of strong wake echoes.SIf usprsewake returns within thetrcigae

of aBBMD radar could degrade the quality of metric data or

even steal the RV track, with ccitsequent detrimental effects

on the designation, discrimination and intercept functions.

MTI (moving target indicator) waveforms and processing tech-

niques provide an fficietit Ieans of wake suppression by

cancellation of echo Doppley components differing from that

of the RVM Other methods for eliminating or reducing the ef&* -fects of wake exist, including use of wideband tracking pulses,

coherent burst waveforms, or tracking using a long up-chirp

S-pulse, and these approaches may be advantageous under vari-

ous conditions. However, M.1i has the advantages of not re-

quiring particularly large pulse bandwidths, of not having

a long waveform duration more prone to ambiguous rangealecho interference, and of not being wasteful of radar energy

resources (as may be the case with a long pulse).

s As de:cribed in Ref. 1, MTI processing can be used to

suppress either the body echo or the wake echo within the

same range resolution cell. An application in which the wake

echoes are canceled in data processing in order to permit

nmeasurement of RV cross sections in strong wake is discussed

in Ref. 2. The data presented here are intended to demonstrate

S1 7--64/241-4-60 -1-

Page 5: SIN - DTIC · timirg diagram. Power divider PD2 drives the cancellation loop which introduces a 10,5 lisec delay and a loop gain of two. (The exact delay is adjusted ay the proper

RIVERSIDE RESEARCH INSTITUTE

the performance of a range tracker, using a real-time 3-pulse

canceler, which has recently been implemented in the AMRADradar. Section II, which follows, briefly describes the

principle and the expected performance using MTI processing.

Section III discusses the AMRAD data obtained during the

&. RANT-01 flight and analyzes the performance of the MTI tracker.

II. THEORY

The improvement of tracking performance in wake clutter

I• is accomplished by pulse cancellation techniques similar to

I those commonly employed in MTI radar. Several coherent pulses

are transmitted., as indicated in Fig. Ia. Upon reception,

the signals are processed by forming a weighted complex sum-

mation of the echoes corresponding to the individual pulses,

thereby synthesizing, in effect, a Doppler filter. Cancella-

tion can, for example, be achieved at a particular Doppler ve-

Slocity by forming the summation of echo voltages E:,E2 .... Em

for m equally-spaced pulses (of spacing TS) as follows:

E kE + k EC + kmE m "' (l\

where, for achieving a null at the Doppler velocity, Vnu 11'

the phase weighting T = 4VniT/A. is used (for radar wave-

4i length )), and the amplitude weights are chosen to satisfy

the condition k. k 0. The residual value of E then:j-i •

corresponds to the uncanceled components. The Doppler separa-

tion between peak -and null of the filter characteristics is

equal to W/(4TS) so that, at L-Band, spacings of between 8

and 12 ,Jsec would be typTical under ICBM conditions in order

to suppress the low-velocity wake components. As indicated

TM-64/241-4-60 -2-

-• L

Page 6: SIN - DTIC · timirg diagram. Power divider PD2 drives the cancellation loop which introduces a 10,5 lisec delay and a loop gain of two. (The exact delay is adjusted ay the proper

RIVERSIDE RESEARCH INSTITUE A

IT

I ~ timeI

*JCANCELLATION WAVEFORM

7j 7

0 [~ r

Sdp

-~05--~....*4*[0s

- m C---ii_ _ _ _ _

0pO :1Z

B;.i ASIN: WAVEF"OP. A-SO, CHARACTERISTICS-

T-64/241-.4-60

Page 7: SIN - DTIC · timirg diagram. Power divider PD2 drives the cancellation loop which introduces a 10,5 lisec delay and a loop gain of two. (The exact delay is adjusted ay the proper

RI VERSIDE RESEARCH INSTITUTE

in Fig. lb, the use of a simple two-pulse canceler (k 1,k 2= -1) results in a relatively sharp null in the Doppler

filter characteristic. For suppressing clutter echoes char-

acterized by a large Doppler spread E broader wake rejection -

characteristic may be required, such as that obtained by the 0th~ree-pu l.5e or four-pulse canceler. (For the cases shown,

a bnomalsequence of weighting coefficients was assigned;

in enealmore optimum filters can be synthesized, depene.-

.Ln ontheclutter echo spectra, by other cc. binations of

weihr- orby nonuniform pulse spacings.)

Figre2 gives the degree of wake RCS suppression (power

a1 wake r.m.s. Doppler spread, aV/V~. frm=2- - n4-pulse cancelers, and -for different a-mounts of misaligment be-

tween the null Dopple.,. and -the true mean wake Doppler. Xt is

see tht or n ~m.-.wake Doppler spread as large as 1-0 per-

cen o th bdyDoppler~ velocity, a 4plecanceler can

achevemor thn 3 dBof ,7ae sppresson orcases where

themea wke oplerhasber. ccratlypredicted. This

suppesson igue i no sevrel dci~aed venfor a meanwak~ Dople whch i unnow tothe extent; of 10 percent of

-th boy vlocty.Thee ol-clatonswer baedon the as-sizptonof Gu~sia wkeDoppler setu;actual spectra

havngdaifeentchrace istc esecall ot o te-ir ta-Us,car' substantially alter the~ser~ls-

Ncteý that, in practice, the actual azhievable wlake. sup-

pression. could be 'Limited, -by quanttizati-on coarseness it, analog-to-dig-ital. conversion (if a digital traýcker is iised), by

21nstabilities in the radar, or by spixrioais ampli-tude o~r phase

madialatiUon.

T14-64/241 -4-63 4

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RIVERSIDE RESEARCH MSONTE

"t -PUI,5E CANCELER-INOMIA,. WEIGHTING COEFFICIENTSGAUSS'AN WAKE SPECTRUM

-MEAN WAKE DOPPLERo'V: r.m.s. WAKE DOPPLER SPREAD

60 vpa• : v9: SODY DOPPLER

1 50

I m:4ý/V 9 :0

fe I*--.

Ft. AH VBVAWK 6 P0ESON!•

II

-20

gv o

0O 0.05 0.10 015 020

I *FI0.2 ACHIEVABLE WiAKEr SUPPRESSION

4 r-s4-64/241-4-:60 5

27

Page 9: SIN - DTIC · timirg diagram. Power divider PD2 drives the cancellation loop which introduces a 10,5 lisec delay and a loop gain of two. (The exact delay is adjusted ay the proper

PRIVEFISIDE RESEARCH INSTPIMIE

on the raw pulse echoes, both range and angle tracking can

Sbe improved. In most situations of interest in a terminal

defense geometry, the wake would introduce a negligible"amount of angle-tracking scintillation (glint) relative to A

the noise-determined monopu'-se error signals. However, the

vresence of uncanceled wake in the tracking range cell can

in fact limit t-he range tracking precision, as will be illus-

trated. When wake cancellation waveforms are employed, the

r.a.t.. 1'•nge tracking jitter for a steady (nonfluctuating)

reentry x..il cross section can be expressed as

K n ( /R;'S.D. (r) n g w :

b

where %, n and q. are the RCS values corresponding to

the body, integrated receiver noise, and wake clutter within

the body range resolution cell, respectively, B is the band-

width of the tracking pulse and K depends on the tracker Char-

acteristics (including the tracking loop dynamics and smoothing:

tracking PRF, leading edge threshold criteria, and detailed

tracking pulse shape). Tnis expression is only valid for suf-I ficiently large ratios of body to random-echo signals (qb /a

Rb/6w 3l1). Also, if signrificantly large body RCS fluctuations

are present the tracking quality can be affected. These latter

effects, as well as the effects of receiv-er noise, are not re-

duced by the cancellation process. (Techniques are available

for coping -with the effects of body RCS fluctuations.)

II . Br.SLTS-

The results presented here were obtained from data col-

lected on the RANT-01 payload (Athe-na 137) flown on 12 Jan--A

T?4-64/241-4-6 0 -6-

S-- -

Page 10: SIN - DTIC · timirg diagram. Power divider PD2 drives the cancellation loop which introduces a 10,5 lisec delay and a loop gain of two. (The exact delay is adjusted ay the proper

RIVERSIDE RESEARCH INSTITUTE

uary 1973 at the White Sands Missile Range, which was the firstflight test for which the AMRAD MTI tracker was operational.* A

In order to assess the effectiveness of the MT.L technique twoindependent range trackers were used at AMPAD to simultaneously

track the payload during reentry. The principal tzacker em- i

ployed a single pulse (3 Psec compressed to 0.1 p-sec). The

MTI tracker, which operated on the outout of a cancellation cir-cuit, used 3 pulses, each 0.1 P-sec wide,with a fixed spacing

4of 10.5 ;Lsec. Binominal amplitude weighting coefficients

(1,-2, 1) with no phase weighting (i = 0)were employed for thistest. Thus the transfer function null was at zero Doppler and,since the AMRAD frequency is 1300 MHz, the peak occurred at a

Doppler velocity of 5.5 km/sec.

A block diagram of the three-pulse cancellation circuitermployed is shown in Fig. 3. (A conventional analog design ap-

proach which would adequately demonstrate the tracking techniquewas selected.) The first loop provides the amplitude weighting

while the second loop provides the proper delay (and phase) to

form a null at the desired wake Doppler frequency. Two powerdividers (PD1 and PD.) and one gate (Gl) perform the amplitudeweighting function with coefficients k1 - 1, k 2 = -2, k3 = I.

Cable (0 ) cut to the proper length is used to maintain proper"1 • phase between the gated and ungated signal paths. The second

pulse of the received triplet is gated on by G1 as shown in the

timirg diagram. Power divider PD2 drives the cancellation loopwhich introduces a 10,5 lisec delay and a loop gain of two. (Theexact delay is adjusted ay the proper iezngth of cable 0,-N The

7-' output of the cancellation circuit feeds the MTI range trackerwhi-rh is gated on with the third pulse. In practice, this cir- A

cuit achieved a cancellation ratio (R') of about 30 dB.

-h* e PANRT-01 target was flown under the sponsorship of the V- -tUS. Air Force, SAMSO. AMRAD data are presented in Ref. 3.

rXRP/A1A46 -7-

Page 11: SIN - DTIC · timirg diagram. Power divider PD2 drives the cancellation loop which introduces a 10,5 lisec delay and a loop gain of two. (The exact delay is adjusted ay the proper

RIVERSIDE RESEARCH INSTITUTE

I I

MIDi

0li

al

z go-: - 0

c-i IN

SFIG., 3-PULSE ANALOG CANCELLATION CIRCUIT EMPLOYED AT AMRAD

-1-q-4-64/241-4-60 -8- A

Page 12: SIN - DTIC · timirg diagram. Power divider PD2 drives the cancellation loop which introduces a 10,5 lisec delay and a loop gain of two. (The exact delay is adjusted ay the proper

RIVERSIDE RESEARCH INSTITUTE

Both trackers operated in a leading edge mode at a wiuve-

form repetition rate of 50 Hz; the trackers were identical in

all other respects, including the tracking loop time constant

(approximately 0.1 sec).

N6 attempt was made to incorporate an MTI waveform for wake

suppression in the AMRAD angle tracker, which uses a 1.2-ýLsec

uncompressed- pulse. For "he RANT-01 flight, the slant range at

maximum waking was approximately 125 km and the radar aspect

angle was 20 deg. Thus, the angle subtended by the wake within

the angle tracking range cell was at most 0.5 mrad, which is not f N

significantly greater than the single-pulse angle tracking jitte.L..

due to noise alone. (In fact, the wake had no discernible effect

upon the angle tracking quality for this test. 3)

Fig. 4 shows the range vs. time history and the range trank-

ing residuals obtained during data processing for both the MTI

and single-pulse trackers over the interval (313 to 32 sec) forSwhich comparisons are meaningful. The residuals correspond to

the tracking fluctuations about a 2-sec running polynomial fit to

the range vs. time history. Fig. 5 shows the reentry body and

wake RCS in the body range cell, the wake mean Doppler and Doppic :

spread in the body range cell at various times,* and the sup-

pressed wake echo RCS calculated on the basis of both the ideal

cancellation ratio (as determined by: the wake Doppler moments)

and the actual cancellation ratio (29 d3) measured for the cir-

cuit employed. For reference purposes, the equivalent RCS acorresponding to the receiver noise is also shown.

The effects of wake upon the single-pulse range trackingcan be observed in Fig. 4, particularly when strong attached

* The body RCS and wa3ce RCS and Doppler measurements were ob-tained by burst waveform Doppler processing.

TM-64/241-4-SO -9-

.61I

Page 13: SIN - DTIC · timirg diagram. Power divider PD2 drives the cancellation loop which introduces a 10,5 lisec delay and a loop gain of two. (The exact delay is adjusted ay the proper

RIVERSIDE RESEARCH INSTIUTE]

Li NMI

so in

14 IK

1~L0A

zlnl~ OV

FIG.4AMRA RANE TRCKIN DATTM-64/41-4-0 -1)

Page 14: SIN - DTIC · timirg diagram. Power divider PD2 drives the cancellation loop which introduces a 10,5 lisec delay and a loop gain of two. (The exact delay is adjusted ay the proper

_______________________ - -u---

-- - - ----------- -- �--.---�---�---�-----F UVERSIDE RESEARCH ESTITUIE

-f ALTITUDE (ka�)

40 35 30 25 20 IS

24 -4

1 � 0.02C) A I WA�CE DOPPLER M0MEt�TS;

�c. 6V/VPEAK

0.005 -- K, i' 15�a.tsr SQOY RANGE CELL

0.002W �PEAK � . -�

4 ________________________

p0.001 I I I

01��� RCS� V�b(O.lsecAVERAGE)

. tI...

-�

a0I �!01'�

-- WAKE RCS. o�(0.�-sec AVERAGE IN15 mtsr BODY RANGE CELL)

ISmeter 301W RANGE CELLK q�/R (ft u TNEORETICAL WA�CE

** NOISE LEVEL-Mn TRACKER @�/R' IR"AC7UAL CANCELLATONa29dB)(3 Q.1-�&sec PULSES)

I

- - - - - - -

xx '1NOISE �c �x

�eoh LEVELSIt4GLE PULSE TRACKER0. (3ps.c-.0�p&.ec)

'UI ...7�I___________ j4 I I* 513 314 315 �'16 317 318 319 320 321 322 1 �

*1 - TIME (see)

A91 F�S. 5 AMRAD DATA RELEVANT TO MTI TRACKIZR PERFORMANCE FOR

RA#�'O� FLIGHT i<I !I�M- 64/241-4-60 1�

-- - - -. - - - -�

Page 15: SIN - DTIC · timirg diagram. Power divider PD2 drives the cancellation loop which introduces a 10,5 lisec delay and a loop gain of two. (The exact delay is adjusted ay the proper

RIVERSIL'E RESEARCH INSTITUTE

wake is present (317.5 to 319.5- sec). During the entire inter-

val the wake RCS exceeds the noise level and therefore contrib-

utes more to the -tracking jitte-r. tor the 14TI trackleT. the

* ~wake echo is suppressed to levels where it is negligible corn-

pared to the receiver noise, except in the interval 317.5 to

319.5 sec when-it somewh-at exceeds the noise (see Fig. 5).

during this latter interval. In any case, note the general irl-

provement in tracking performance obtained with the MIT tra-:ker.

More striking examples of the tracking improvement using

MItechiiiques have been obtained for more recent WSMR fli.31hts,

frwhich the alata are classified. Those interested in those AXrecent data are invited to contact M. Arm at i~he AMRAI) site forfurther details.

ACKNOWLEDGMENT

The authors acknowledge the Contzributions of D. Grieco and

~ I W. Edelson for helping to develop the M1TI technique for reentry

$measurement applications (Refs. 2 and 4), of K. Krabbe and 3. Harrell t 2

for implementing the circuitry, and of F. McIntyre for assistance

in the preparation of the RANT-Ol1 data.

REFERENCES

-f eissman, I,, "Low-A1*-itude Discrimination Waveforms (U%,,"in Proceedings of t.-: 1.97i le5w-Altitude Workshop, pulb-lished b~y River-side Resaarch Institute, 4., 5 M.arch 1971,ISSecret,/RD.

2. Edelson, W., "A Cancellation Technique for Processing RadarReentry M~easurements (u),, Riverside Research YnstLituteFI Report TM-45/186-4-10, 1 January 1973. $ecret/AD.

3. "Preliminaryv AMRAI) Data Report,, Ath-ena, Flight No. 137 I,H005OJ/RAIU-.01< Ri.verside Research Institute ReportPADR-2.5/241-4-l0, 9 February 1973, Uncl:-,ssified.

4. Weissman, 1. and Grieco, D., "A Low-Altitude Discrimina-

side Research institute, Technical Memorandum TM-33,/077-4-00, 30 June 1970, Secret.

jTM-64/241-4-60 -12-

- - -V-0


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