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Activation of new aaa units - Air Defense Artillery

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19.J8 DETERMINATION OF FIRING ERRORS FOR HEAVY AAA 31<br />

c:-- ALL COURSES ARE PAftALLEL TO THE INOOM'". COURSE AND DISTAIfT<br />

_ . __ .J fftOM THE I"-COMINe COURSE: A PREOETERMINED DISTANCE<br />

~J:<br />

"l-<br />

:-<br />

-<br />

~<br />

DEAD AREA<br />

INCOMING COURSE .PASSES DIRECTLY OVER FIRING BATTERY)<br />

Figure 2-Courses used to obtain the data for changes in<br />

minimum range.<br />

considered have a 360 degree field <strong>of</strong> fire, and their accuracy<br />

is not affected by the azimuth <strong>of</strong> the target, it was<br />

~ecessaryto study only one area <strong>of</strong> the sky with respect to<br />

field<strong>of</strong> fire. Figure 2 shows the courses which were used to<br />

obtain the data for changes in minimum range. The first<br />

courseat each altitude was Hown directly over the batterv<br />

giving the data on incoming targets. Succeeding course's<br />

at each altitude were Ho\vnparallel to the first course and<br />

at various minimum ranges. On each <strong>of</strong> the courses shown,<br />

data were taken with each type <strong>of</strong> fire control, radar and<br />

\'isual. Since the type fire control which a potential enemy<br />

might use wo -generally be unknown, the values obtained<br />

b averaging the results <strong>of</strong> the two groups were<br />

considered <strong>of</strong> more value than either group considered<br />

alone. The effects <strong>of</strong> changes in target speed were determined<br />

by a combination <strong>of</strong> experiments on a limited<br />

scale and application <strong>of</strong> the results obtained to all other<br />

points for which experimental data with respect to target<br />

speedwere not obtained. The requirement that an average<br />

battery conduct the experiment caused some difficulty.<br />

However, with normal turnover <strong>of</strong> personnel and replacement<br />

by relatively inexperienced personnel, the possibility<br />

<strong>of</strong> the battery becoming too highly trained to be considered<br />

a\'eragewas overcome.<br />

Data were taken on both firing and sim'ulated firing<br />

courses. Simulated firing courses were necessary due to<br />

safetyrequirements and the huge ammunition requirements<br />

<strong>of</strong> an "all firing" problem. Errors <strong>of</strong> simulated firing data<br />

Wereobtained by a comparison <strong>of</strong> true firing data vl.'ithfiring<br />

data furnished by the director. True data for this compari-<br />

SOnwere obtained by an electronic ballistic computer using<br />

target present position data determined by phototheodolite<br />

~ethods. The ballistic computer solves for future position<br />

In terms <strong>of</strong> quadrant elevation and azimuth, and prints errorsbased<br />

on the comparison with director data. ;'\0 data<br />

on fuze errors \"ere compiled at this time, since the study<br />

Wasmade assuming ~'ariabletime fuze conditions. Only<br />

prediction errors could be determined by simulated firing.<br />

:\ctual firinu \vas done with 11ledul1lical,ime fzced ammu--<br />

• _ D<br />

Ultlon,and bursts \\-ere then moved by computation to detennine<br />

the points at \vhich bursts would ha\-e occurred if<br />

variable time fuzes had been used. The points so computed<br />

were used to establish errors in azimuth and quadrant elevation.<br />

The difference between actual firing errors and simulated<br />

firing ermrs is an increment <strong>of</strong> error due to ballistic<br />

conditions and materiel and personnel errors. Considerations<br />

which affect the size <strong>of</strong> this increment are (1) Parallax,<br />

(2) Dither, (3) Additional Computer Circuit errors,<br />

(4) Density and Muzzle Velocity Computer Correction<br />

errors, (5) Firing table errors, (6) a group <strong>of</strong> other sources<br />

<strong>of</strong> small errors which do not individually affect the result<br />

but which collectively may be significant. It is a popular<br />

misconception that the firing errors listed in the firing<br />

tables are the only ones which should be expected when<br />

firing at aerial targets. The firing tables list firing errors for<br />

static problems only. The errors determined by this study<br />

are for dynamic problems. This difference, or increment,<br />

was obtained theoretically and added to the simulated firing<br />

errors. The summation <strong>of</strong> simulated firing errors and the<br />

computed increment was then checked against firing errors<br />

obtained in actual firings. Agreement between the summation<br />

and actual firing errors indicated that use <strong>of</strong> the summation<br />

in lieu <strong>of</strong> actual firing errors was permissible. This<br />

use <strong>of</strong> a measured prediction error plus a computed firing<br />

increment error is further supported by a comparison <strong>of</strong> the<br />

size <strong>of</strong> the two components. The comparison shows that<br />

prediction error makes up the major portion <strong>of</strong> the whole<br />

firing error. /<br />

Simulated firing has the distinct advantage over actual<br />

firing in that data are furnished every second instead <strong>of</strong> only<br />

when bursts occur. This materially decreases the number<br />

Figure 3-An example <strong>of</strong> total errors with the erroneous center<br />

<strong>of</strong> impact errors resulting from using a block size too<br />

small to include a complete cycle.<br />

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