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"lfk f; \"A Lt. - Airborne Systems

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'"<br />

Axial Force Coefficient<br />

I t is customary to use the term "tangential" with<br />

reference to vectors tangent to the flight path , the<br />

rm " axial' is used instead when defining components<br />

of fmce and mo:ion applied along the major<br />

longitUdinal axis or axis of symmetry at :he decelerator<br />

The axial force equals the decelerator drag coefficient<br />

at angle of attack O. The axial force coefficient,<br />

CA' presented in Figure 6.28 are calculated<br />

from tes1 data<br />

AlqS<br />

obtai1ed on model wind<br />

6.<br />

tunnel tests<br />

(Ref. 3891. The axial force coefficient is calculated<br />

as follows<br />

CA F<br />

The speed for these tests was 1. Axial force<br />

data for tests 391 with sirrilar canopy designs 131 M =<br />

and are shovvn in FigJre 6.29.<br />

Parachute Cluster Drag Coefficient<br />

The cluster dl'ag coefficien: COC 's less than<br />

of the individual parachutes, the ratio COe/CO be.<br />

ing inversely proportional to tr,e number of para-<br />

ChJleS as sl10wn in Figure 6. 30. While differences in<br />

rate 01 descent account for some difference in CDC'<br />

the data spread is too large to be the resuit of this<br />

factor alone 1te divergent trends suggest 1'18 pres.<br />

ence also of differences in both parachute and cluster<br />

riggin ) geometry not evident in the source informJticn.<br />

ThE' effactive rigging leng:h used for referen::e pur.<br />

poses, and sometimes in cluster design, is based on<br />

the cqllivalent single pa" achute length ratio<br />

0. In terms of the nomi1el diameter of the incivid.<br />

ual canopies of the cluster th is converts to<br />

o =(nc) 6where<br />

/ c is the combi ned lengtns of suspension I incs<br />

and cluster risers to the riser confluence, and<br />

the number of canop es in the cluster. The following<br />

numerical '/a,ucs are obteined:<br />

TABLE 6.3 EFFECTIVE RIGGING LENGTH FOA<br />

CLUSTERED PARACHUTES<br />

CID<br />

141<br />

For practical reasons, shorter rigging lengths 31'e used<br />

in airdrop cluster of G- A, 100 ft and G- 12D,<br />

64 ft parachutes: (See Table 6.4)<br />

Emrir:cal data from differen sources on the norrral.<br />

ized drag coefficients of clustered parachutes are plotted<br />

in Fi gure 6.30. The relat:ve riggi ng lengths of the<br />

individual parachutes and of the clusters are indicated<br />

where known,<br />

264<br />

TABLE 6. EFFECTIVE RIGGING LENGTH FOR<br />

CLUSTERED G- 11A AND G- 12D<br />

PARACHUTES<br />

11A<br />

12D<br />

1.2 1.4 1.6 1.8<br />

1.1 1.1<br />

it will be seen that ,n steady descent the individJal<br />

canopies stand apart. as in F:gure 6. 31. They 0150<br />

:end to wander about, constrained somewhat by the<br />

number in the cluster. Apparently the fl owfield has a<br />

radial component away from the sys1em axis in addition<br />

to the familiar oatte n of flow about each can,::py,<br />

which would tend to hold them apart, but this is<br />

not strong enough to prevent the caropies frcm occasionally<br />

conlac:iny each other lightly, Thus, on the<br />

average it would appear that the mean relative flow at<br />

each canopy has an angle of attack of roughly a'"<br />

de'grees , provided the canopy is not gllding 390 . Sil'<br />

the clus1er as a w'lole does not glide , the only way<br />

the member canopies might glide is to move away<br />

from the system axis and stand at an al1gle of attack<br />

to the relative flow. This behavior would result in<br />

some flattening of the outer or leecin\) edges of the<br />

canooies and so would be visi:;le in fi, m records.<br />

That suer evidence has not been observed tends to<br />

support the idea t"1at on the average degrees,<br />

and random shifting of the aerodynamic force vec10rs<br />

driven by vortex shedding, causes the canopies to<br />

wander, possibly seeking a stab,e angle of attack.<br />

TI11S rei:scning justifies :he proposition that the cluster<br />

drag coe'fficient may be rej:resented as<br />

CD COo COS tpc 6-<br />

where rPc is the irnegrated average angle of the cluster<br />

risers from the system axis, The implicit assumptions<br />

'1ere are t.18t there is l1ut nutual interference<br />

and the dynamic pressure 1elt bV ea:h canopy is equal<br />

to Q8' i.e.. th€ sarna as its equilibrium dyna11: c pres.<br />

sure descending alone at the system rate of descent.<br />

The angle<br />

is mainly a function of<br />

.:c<br />

and has<br />

its m nimum value when all the canopies of the cluster<br />

are in contact with each other " as some rave been<br />

rigged on occasion with tangent points on the skirt<br />

bcund togetner. Then presumably CDC would be a<br />

maximum ard the assllmption of n::Jn-inte'ference<br />

may be tested by comparative evaluation.

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