InfoDotInc / archive systemEstablished online record · rebuilding deliberately
InfoDotInc

Technical documents, historic paths, and source-backed reference material.

Archive / Airship Aerodynamics Technical Manual / Airship Aerodynamics Technical Manual: Complete Handbook

Complete Handbook

Complete Handbook — Part 1

TM 1-320 (1941)

TECHNI CAL MANUAL }

No. 1-820

*TM 1-320

WAR DEPARTMENT ,

W ASHlNGTON, Pebr·um·y 11, 1941.

AIRSHIP AERODYNAMICS

Prepar ed under direction of

Chief of the Air Corps

SroriON I. General. Paragraph

Definition of aerodynamic s__________________ 1

Purpose and scope__________________________ 2

Importance --- - ------ ---------------------- 3

Glossary of terms__ ________________________ 4

Types of airships---- ------ - -------- -------- 5

Aerodynamic forces_________________________ 6

ll. Resistance .

Fluid resi&ance____________________________ 7

Shape coefficients ___________________________ 8

Coefficient of skin friction_ __________________ 9

Resista nce of streamlined body------ --- ----- 10

Prismatic coefficient----------- ---- --------- 11

Index of form efficiency____________________ 12

lllust rative resistance problem_______________ 13

Scale effect-------- ----- ------- --- ---- - ---- 14

Resistance of completely rigged airship ______ 15

Deceleration test -------- - ------ ------- ----- 16

III. P ower requirements.

Power require d to overcome airship resistance_ 17

Results of vari ous speed t rials_______________ 18

Burgess form ula for horsepower------ --- ---- 19

Speed developed by given horsepower________ 20

Summary---------------------- -""'--------- - - 21

IV. Stability.

Variation of pressure distribution on airship

hull--------- ---------- ------------------ 22

Specific stability and center of grav ity of air-

shiP----- ------------------ ---- ------ - --- 23

Center of buoyancy________________________ 24

Descrip tion of major axis of airship__________ 25

T ypes of stab ility_ _________________________ 26

Forces and moment s acting on airship________ 9/l

Dampi ng moment----- --- ------------------ 28

Longi tudina l stabilitY--------- ------- ------ 29

Directiona l stability_________ _______________ 30

Latera l sta bility- ------- --------- --- --- --- -- 31

SummarY--------- -- ---- - ------ ------------ 32

*Thia m anual supersedes or:a ll'lG-290 , November 16, 1929.

285746°--41 1

TM: 1-320

SECTION

AIR CORPS

V. Control. Paragraph

<Jenera! types______________________________ 33

Directional__ ______________________________ 34

Altitude-------- -------------------- - ------ 35

Re 36 verse ___________________________________ _

Applica tion of dynamic control to operation of

. h' airs Ips _________________________________ _

VI. Aerodynam ic stress.

Assumption as to conditior1 of maximum stress_

Transverse forces acting on airship flying at

constant angle of pitch __________________ _

Transverse forces acting on airship in steady

turn_____________________________________ 40

Force s caused by gusts______________________ 41

Empirical formulas for max imum aerodynamic

bending moment on hull and for forces on

tail surfaces----- ·------------------------ 42

Method of calculating shear and ben_ding mo-

ment on hulL ___ . _________________ ;________ 43

Conclusion____ _____________________________ 44

SE<:mON I

<JENERAL

Paragraph

Definition of aerodynamics-- - ~ ------ --- --- --- -- - ---- -- --- ----------- -- -- 1

Purpose and scope---- - --- ---- --- ------- - ---·-- ------ --- ------------ ---- -- 2

Importance-- --------------~--------------- -- ----- - ---- - ---- - ------ ----- 3

Glossary of terms -------- ----- -------- ----- --- - ------ -------- ----- - - ---- 4

Types of airships_ ·----- ---- ------------ - ------------ - ----- ----- ------- -- 5

Aerodynamic forces ------ --------- --- ------------- - ---- - --- --- -------- - - 6 .

1. Definition of aerodynamics.-Aer odynamics is that branch

of dynamics which treats of the motion of air and other gaseous

fluids, and of the forces on solids in motion relative to such fluids.

2. Purpose and scope. - This manual is designed as a text for the·

instru ction of airship student pilots and as a reference text for th~

rated pilot. A ccordingly the subject has been so approached as to ·

give the knowledge of aerodynamics essential to the operation of air­

ships . Intricate formulas involving higher mathematics, although

valuable to the designer, are of secondary importance to the pilot.

Such formulas therefore have been omitted and the entire subject so

treated as to bring . out basic principles and their application to lighter

than air aircraft operation.

AffiSHIP AERODYNAMICS

TM 1-320

3. Importance.-Ai rships are controlled in two ways, stati<-ally

a.nd dynami cally. The former method is discussed in TM 1-325 and

will be mentioned but incidentally in this manual. Because of the

existence of stat ic means of control, the study of aerodynamics may"

appear of minor importance to the operation of airships . This is

untrue . Stabili ty and contr ol are constantly effected by a combina­

tion of static and dynamic forces. To insure safet y of the airshi p

and to preclude possibility of exposing it to dang erous conditiOJ:!.S, the

pilot must be aware of existing dynamic for ces and their effects on

the airship itself and on its flight path. F requently airships, due tJ

unavoidable causes such as leakage of gas or accumulation of mois­

ture, have become statically uncontrollable but have been sayed by the

intelligent application of dynamic means of control.

4. Glossary of t erm s.-During recent years many terms have

been introduced into the English language covering vari ous aspects of

aeronau tical science. Report No. 240, Nationa l Advi sory Commit­

tee for Aeronautics, defines the meaning of the most common of these

expressions, from which most of the following definitions have been

abstr acted :

.A.erodynamics.-Branch of dynamics which treats of the motion of

air and other gaseous fluids and of the forces acting on solids in

motion relative to such fluids .

.A.eronautics.-Science and art pertaining to the flight of aircr aft .

.A.ero3tat.-Ge neric term for aircraft whose support ·is chiefly due to

buoyancy derived from . aerostatic forces. The immer sed body

consists of one or more bags, cells, or other containers filled with

a gas which is lighter than air.

Airfoil.- Any surface designed to be projected through the air in

order to produce a useful dynamic reaction .

Airfoil section (or profile) .- Cross section of an airfoil made by a

plane parallel to a specified reference plane . A line perpendic ular

to this plane is called the axis of the airfoil.

Air scoop.-Projecting scoop which uses the wind or slipst ream to

maintain air pressure in the interior of the ball<:met of an aerostat.

Airship .-Aerostat provided with a propelling . system and with

means of contro lling the dire ction of motion. W hen its power

plant is not operating it acts like a free balloon.

Nonrigid .-Air ship whose form is maintained by the inte rnal

pressure in the gas bags and ballonets (fig. 1) .

Rigid.-Airsh ip whose form is maintained by a rigid structure

(fig. 3).

TM 1-320

4 AIR CORPS

Se1nirigid.- Airship whose form is maintained by means of a

rigid or jointed keel in conjun ction with internal pressure in

the gas containers and ballonets (fig. 2).

The term "airship" is sometimes incorrectly appli ed to

heavier than air aircraft either in full or as "ship ." This is a

slang use of the word and should be avoided.

Air speed'.-Speed of an aircraft relative to the air. Its symbol

is V.

Angle, critical.-An gle of attack at which the flow about an airfoil

changes abruptly with corresponding abrupt changes in lift and

drag.

Angle, elevator.-Angular displacement of elevator from neutr al

position. It is positive when trailing edge of the elevator is below

neutra l position.

Angle of attack.-Acute angle bet-.veen the . chord of an airfoil and

its direction of motion relative to the air. (This definition may

be extended to other bodies than airfoils.) Its symbol is a.

Angl e of pitch .-Acute angle between two planes defined as follows:

One plane includes lateral axis of the aircraft and direct ion of

the relat ive wind; the other plane includes lateral axis and longi­

tudinal axis. (In normal flight the angle of pitch is the angle

between longitudinal axis and direction of relative wind.) This

angle is denoted by 0 and is positive when nose of the aircraft has

•

nsen .

Angle of roll, or angle of bank.- Acute angle through which aircra ft

must be rotated about its longitudinal axis in order to bring its

lateral axis into a horizontal plane. This angl e is denoted by

<I> and is positive when the left wing is higher than the right.

Angle of yaw.-Acute angle between dire ction of relati ve wind and

plane of symmetr y of an aircraft . This angle is denoted by 'II

and is positive when the aircraft has turned to the right.

Angle, propeller blad'e.-Actual angle between chord of propeller

section and plane perpendi cular to axis of rotation of propeller.

Usually caUed "blade angle."

Angle, rudder.-Ac ute angle between rudder and plane of symmetry

of the aircraft. It is positive when trailing edge has moved to

the left with reference to normal position of pilot.

Angle, zero lift;.-Angle of attack of an airfoil when its lift is zero.

Aspect rati o of propeller blade.- Half the ratio of propeller diameter

to maximum blade width .

Awes of aircraft.- Three fixed lines of refer ence, usually centroidal

and mutually perpendicular. The longitudinal axis in the plane

AIRSHIP AERODYNAMICS

TM 1-320

of symmetry, usually parallel to axis of the propeller, is called

the longitudinal axis; the axis perpendicular to this in the plane

of symmetry is called the normal axis; and the third axis perpen ­

dicular to the other two is called the lateral axis. In mathe ­

matical discussions, the first of these axes, drawn from front to

rear , is called the X axis; the second, drawn upward, the Z axis;

and the third, running from right to left, the Y axis.

Ballast.-Any substance, usually sand or water, carried in a balloon

or airship and intended to be thrown out, if necessary, for the pur­

pose of redu cing load carried and thus altering aerostatic rela­

tions.

Ballonet.- Compartment of variable volume constructed of fabric

or partitioned otf within the interior of a balloon or airship. It is

usually partially inflated with air under control of valves from a

blower or from an air scoop. By blowing in or letting out air,

it serves to compensate for changes of volume in gas contained in

the envelope and to mainta in gas pressure, thus preventing defor­

mati on or structura l failure. By means of two or niore ballonets,

often used in nonrigid airships, the trim can also be controlled.

The ballonet should not be confused with gas cell.

Blade back.-Si<le of propeller blade which corresponds to upper

surface of an airfoil.

Blade face.-Surface of propeller blade which corresponds to lower

surface of an airfoil. Sometimes called "thrust face" or "driving

face."

Blade width ratio.-Ratio of developed width of propeller blade at

any point to circumferen ce of ·a circle whose radius is the distance

of that point from the propeller axis.

Bow stiffener.- Rigid member attached to bow of nonrigid or semi­

rigid envelope to reinforce it against pressure caused by motion

of the airship. Sometimes called "nose stiffener" or "nose batten."

Buoyancy.-Upw ard air force on aerostat which is derived from

aerostatic conditions . It is equal to weight of air displaced.

Buoyancy, center of (aerostat).-Center of gravity of volume of

contained gas.

Oamber.-Rise in curve of an airfoil section from its chord, usually

expressed as ratio of departure of the curve from the chord to the

length of the chord. "Upper camber" refers to the upper surface

of an airfoi l and "lower camber" to the lower surface; "mean

camber" is the mean of these two.

Capacity.- Volume of the gas-containing portion of an aerostat.

Oar.- That portion of an airship intended to carry power unit or units,

TM 1-320

4 AIR CORPS

personnel, cargo, or equipment. It may be suspended from the buoy­

ant portion or it may be built close up against it. It is not to be

applied to parts of the keel of a rigid or semirigid airship which

have been fitted for the purposes mentioned .

Oeiling, static.-A ltitude in stand ard atmosphere at which an aerostat

is in static equilibrium a.fter removal of all dischargeable weights.

Oenter of presswre coetflaient.- Ratio of distance of center of pressure

from leading edge to chord length.

Oenter of pressure of cd1•foil section.-Point in chord of airfoil sec­

tion, prolonged if necessary, which is at the intersection of the

chord and the line of action of the resultant air force. Abbreviation

is C. P.

Ohord (of airfoi l section) .-Line of straightedge brought into con­

tact with lower surface of the section at two points; in the case of

an airfoil having double convex camber, the straight line joining

the leading and trailing edges. (These edges may be defined for this

pur pose as the two points in the section w~ich are farthest apart.)

The line joining leading and trailing edges should be used also in

those cases in which lower surface is convex except for a short flat

portion. The method used for determining the chord should always

be explicitly stated for those sections concerning which ambiguity

seems likely to arise.

Ohord length .-Length of pro jection of airfoil section on its chord.

Its symbol is c.

Oont1•ols.-General term appli ed to means provided to enable the pilot

to control speed, direction of flight, altitud e, and power of aircraft .

D1•ag.-C omponent parallel to relative wind of tota l air force on

aircraft or airfoil. Its symbol is D.

Dynamic (or impact) pressure.-Product 1;2pV 2 , where p is density

and V is relative speed of the air. It is the quantity measured by

most air speed instrum ents. Its symbol is q.

:Elervator.-Movable auxiliary airfoil, function of which is to impr ess

pitching moment on the aircraft. The elevator is usually hinged to

the stabilizer .

Envelope.-Outer covering of aerostat, usually of fabric. It may or

may not be also the gas container. It may be divided by dia­

phragms into separa te gas compartment s or cells, and it may also

contain internal air cells or ballonets.

F light path.-Path of center of gravity of aircraft with reference to

the earth.

H orsepower of engine, ma.:vim-wm.-Maximum horsepower engine can

develop.

AIRSHIP AERODYNAMICS

TM 1-320

Horsepowe'l' of engine, rated.-Average horsepower developed by an

engine of a given type in passing the standard 50-hour endurance

test.

Hull (airship) .-Main structure of a rigid airship consist ing of a

covered elongated framewor k w hich incloses gas cells and supports

cars and equipment. May also be applied to complete buoyant unit

of any aerostat. In this latter sense sometim es called "gas bag."

lndraft (inflow) .-Flow of air from in front of propeJler into blades.

K eel (airship) .-Assembly of members at bottom of hull of semi­

rigid or rigid airship which provides special strength to resist hog­

ging and sagging and also serves to distribute effect of concent rated .

loads along the hull. It may be a simple Gall's chain as in some

semirigids, or a very extensive structure inclosing the corridor as

in most rigids.

Leading edge .-Foremo st edge of airfoil or propeller blade. Also

called "entering edge."

Lift.-That component of tot al air force on aircraft or airfoil which

is perpendicular to relative wind and in plane of symmetry. It

must be specified whethe r this applies to complete aircra ft or to

parts thereof. In the case of an airship this is often called

"dynamic lift." Its symbol is L.

Lift , gross (air ship) .-Lift obtaine d f rom volume of buoyant gas

equal to nominal gas capacity of the a;ircraft. Obtained by multi­

plying nominal gas capacity by lift per unit volume of gas used for

inflation.

Lift, static ( aerostat) .-Re sultant upward force on an aerostat at

rest obtained by multiplying actual volume of the air displaced by

density of the air and subtracting weight of contained gas. (The

volume of the air displaced multiplied by the differen ce of density

of the air u.nd the contained gas.)

Load:

Dead.-Structure, power plant, and fixed equipment of an air·

craft. Included in this fixed equipment are water in radiator

and cooling system, all essential instruments and furni shings,

fixed electric wiring for lighting, heating, etc. In the case of

the aerostat the amount of ballast which must be carried to

assist in making a safe landing must also be included.

Full.-W eight empty plus useful load. Also called "gross

weight."

Pay.-Tha.t part of useful load from which reven ue is derived.

namely, passengers and freight.

TM 1-320

4 AIR CORPS

U seful .-Crew and passengers, oil and fuel, ballast other than

emergency, ordnance, and portable equipment .

Nose heavy.-Condition of an airship which when at rest in still air

trims with its axis inclined down by the bow. The term "bow

heavy" is preferred to "nose heavy" in describing airships.

Oscillation, stable.-Oscillation whose amplitude does not increase.

Oscillation, ~tnstable .-Osc illation whose amplitude incres.ses con­

tinuously until an attitude is reached from which there is no

tendency to return toward the origina l attitude, the motion becom- .

ing a steady divergence.

P erform ance CM'I'CUJteristics (air ship) .-In general:

Maximum speed at various altitudes.

Maximum altitude attainable with definite weight relations and

ballonet volume (if fitted).

Endurance at full and half power.

Static ceiling.

Dynamic lift under specified conditions.

Pitch of propeller :

Etfective.-Distance which aircraft advances along its flight

path for one revolution of propeller. Its symbol is pa.

Geomet ,rical.-Distan ce which an element of a propeller would

advance in one revolution if it were moving along a helix of

slope equal to its blade ang le.

Mean geometrical.- Mean of the geometrical pitche s of the sev­

eral elements. I ts symbol is p0 •

Standa rd.-Geometrical pitch taken at two-thirds of thE' radius.

Also called "nominal pitch." Its symbol is Ps·

Ze1'0 th?'U8t.- Distance which propeller would have to advance

in one revolution in order that there might be no thrust. Also

called "experimental mean pitch." Its symbol is pv.

Zero torque.-Distance which propeller would have to advance in

one revolution in order that the torque might be zero. I ts

symbol is Pa·

Pitch mtio .-Ratio of the pitch (geometrical unless otherwi se stated)

to the diam eter pj D.

Pitch speed.- Product of mean geometrical pitch by number of revo­

lution s of propelle r in unit time, that is, the speed aircraft would

make if there were no slip.

Propeller area, proje~ted.-Total area in the plane perpendicu lar to:

propeller shaf t swept by propeller, except portion covered by the

boss and that swept by root of the blade. This portion is usually

taken as extending 0.2 of maximum radius from axis of the shaft.

Original source PDFPublished from pages 1–9 of the recorded source chapter.
Open source PDF ↗