THE DEVELOPIflENT AND EVALUATION OF THE TMB KNOTAETER TYPE 205A
by
Leo F0 Fehiner
and Thomas GibbonsRESEARCH AND DEVELOPZENT REPORT
January 1956
: Report 1026 I Labv.
ScheepsbouwkundeTechnische Hogeschool
Delfi
NAVY DEPARTMENT
THE DAVID W. TAYLOR MODEL BASIN
TI
PEVLQP!1
AI1D EVALUATION OP TIiQTMETERTYPE2O5A
by
Leo F. Fehiner
and
Thomas Gibbons
ii
TABLE OF CONTENTS
LIST OF ILLUSTRATIONS iii
Kfiotmeter Installation, Matntenance and Adjustments
REPERENCES 12 INITIAL DISTRIBUTION. . ABSTRACT INTRODUCTION DETAILS OF DESIGN 3' 1 2 .Body 2 Wing 2 Tall Surfaces k Tow Point 6 Impeller . . . 6 INSTRUMENTATION 6 Transducer . 6 Speed Indicator . 7 EVALUATION TESTS . Basin Tests 7 Sea Trials 7' ACKNOWLEDGMENTS . . 7 APPENDIX 8
iii
LIST OF ILJUSThATIONS
Figure 1 Towed Body for the T Knotmeter
Type
205A. 15Figure 2 Schematic Diagram of the Body for the T .. 16
Knotmeter Type 205A.
Figure
3 Cable Tension at the Body as aFiinction of 17Towing. Speed. .
Figure k Depth Of T Knotmeter as a Function of Spied 18
and Scope of Cable. :
Figure 5 Assembly Drawing of Towed Body0 19
Figure 6 TMB Knotmeter Type 205A Instrumentation Cabinets 20
Figure 7 Block Diagram TMB Knotmeter Type 205A. 21
Figure 8 Circuit DiaErarn TNB Knotrneter Tje 05A. 22
THE DEVELOPMENT AND EVALUATION OF THE TMB KNOTMETER TYPE 205A
by
Leo F. Fehlner and ThomaB Gibbons
ABSTRACT
The design and evaluation of an instrument to measure the speed of a ship relative to the undisturbed water is
pre-sented. This device consists of a towed body and associated
instrumentation and is known as TMB Knotmeter Type 205A. The
knotmeter towed satisfactorily in the "high-speed" basin at
speeds up to 30 knots. Although 15 knots was the top speed
attained at sea due to limitations on other towing gear, it is not anticipated that difficulty would be encountered in
reaching higher speeds. The body was launched and retrieved
from the side and stern of the towing vessel with no difficulty.
INTRODUCTION
As a result of previous sea trials aboard naval surface ships, it became evident that the previous methods of measuring
and Indicating ship speed were inadequate. A specially
de-'signed towed body and its associate electronic equipment, known as the TMB Knotmeter Type 205A, was therefore developed and
constructed. This knotmeter was designed to be towed from a ship
at speeds up to 30 knots and at depths of approximately 100
feet so that it would tow out of the pressure field of the
tow-ing shi,p. The knotmeter indicates the speed of the ship, in
knots, relative to the undisturbed water. Also, it was
de-signed small enough for two men to launch arid retrieve at. speeds of 3 to 6 knots.
2
This report presents an account of the design procedure and the results of evaluation tests of the TNB Knotineter Type
205A. Additional data are provided for installation,
main-tenance and adjustments of the knotmeterand associated
equip-ment.
DAILS OF DESIGN
BODY
To provide an adequate streamline housingfor the pulse
generator and magnetic pickup, a body of. revolution with a fineness
ratio of 5 was selected. A photograph of the body is shown
in Figure 1. The body is composed of several sections,
consist-ing.of a 2-tL. ellipsoidal nose, a cylindrical center body and a conical tail section. The housing and its components were made of brass to prevent sea-water corrosion.
WING
From the results of cable calculations based upon the
tables given in Reference 1, it was determined that the
knot-meter body would have to produce a total downward force of 900
pounds at 30 knots. The weight of the body and its internal
parts were expected to be approximately 100 pounds in water,
leaving 800 pounds to be supplied by a depressing wing.
The lift force developed by a wing can be expressed as
2,3
'L= PU?SWCL (1
(b/2)2) (1]
where
p is the fluid mass density,
U is the towing velocity, .
S is the projodted area of the wing,
CL Is the lift coefficient,
23
References are listed on page3
is the span of the wing as shown in Figure 2,
R is the effective radius of the body (equal to
'D/2), and
.Ii
K21 isa factor which approximately
ac-L (b/2)2 J counts for the wing-body interterece,
By substituting in. Equation [1] for the wing span In terms
or the wing-aspect ratio, it follows that the wing area Is
L
pU2C a.
where
a is the wing aspect ratio,
b2
If the values,. CL = 0.11., U = 50.7 feet/second (30 knots), R = 0.25 feet,
a =k,
L =800 pounds, and 2 slugs/cubic footare substituted in Equation [2] the area of the wing, &,, is
o.8M. square feet.'
k
The lift coefficient of a wing of finite aspect ratio
can be expressed according to lifting-line theor72 as
a
2fllsina
L
a+x
where
a
is the angle of attack of the wing,
K
is correction factor to the section l2ft
curve slope of 2fl .whioh. accounts for the
section thickness (K = 0.9').
Assuming a lift coefficient of 0.11, an aspect. ratio of 11, and
that for small angles. sin' a is equa.l to a In radtans, EqVtion
[3] gives the required wing angle
t attack
5.85.8 degreea.
TAIL URFACESUsing the approximate method described in Reference 2,
the hydrodynamic moment produced by the, tail surta.ce
can be
written, as
MT = SlpU
a
211K sin a
[k]
The Mtlnk or ide1 xflometit4prodtced ....the'.body is
MB = '
(K-
K1) *pU2 Sin2a
[5]
where
18
the volume of body.Equating Equations (k]. and
(5]
for equilibrium and assumingfor small angles sina is equal to a in radians,the total tail area, 5T for the case where the tail surfaces are 25 degrees with respect to the body axis is
is the moment produced by tail surfaces,
MB is the moment produced by the body,
ST is the total area of tail surtaces,
2T is the distance from center of pressure of tail surface to center-of-pressure of body
and tail surfaces combined,
aT
(K2 - K1)
is the aspect ratiO of tail surfaces based on total area and equal to _b!,
isthe virtual..masa:..tactor, and
(K2
-l.k2rli
aK
(6]
where l.k is a fáctbr to allow fo the.k5...degree
orientation of the tail surfaces For an e]Upàoid of
fineneRs ratio
5,
the vIrtual- mass factor (K2 - K1)equals0.836. 5
Assuming
=
0.75
feet= 0.296 cubic feet
aT = 1L0 .
then from Equation [6.] the required tail area, 3T' is 0.12. square feet.
No correction was made to the lift to account for the
sweep backof the tail surfaces. The tail surfaces were swept back to protect the impeller when the body
i8
on the deck andto allow sea weed to slide off the surfaces. There was no
correction made to the Munk or ideal moment to account for viscous effects as shown in Reference
7.
TOW POINT
To facilitate handling of the body in air and to orient
the housing advantageously for its entry into the water, the body should hang horizontally from its tow cable in the air.
The center of buoyancy was selected as the towpoint and the body ballasted so that its center of gravity was located below
the towpoint and on a vertical line containing the towpoint
and quarter chord of the wing. Experience obtained in towing
previous towed housings indicates that it is necessax9 to
provide a rigid towstaff to avoid chafing of the cable cr cable
fairing at the intersection of cable and body2. The towstaff
was extended out of the body approximately 6 inches when ver-tical, as shown in
Figur9111..
For spee4s up to 30 knots the towstaff was given freedom to pivot forward about 15 degrees.IMPELLER
A three-bladed impeller was designed, which rotates at
approximately
66I
revolutions per minute per knot. This im-peller drives the transducer which is used to generate pulses. The blades of the impeller, as shown in Figure 2, are swept back 15 degrees to prevent sea weed from gathering on them.INSTRUMENTATION
6
TRANSDUCER
The transducer consists
spaced iron slugs around it. disk past an. electromagnetic
and carried up the tow cable
of a brass disk, with 90 equally-The impeller wheel drives the
pickup and pulses are generated
SPEED INDICATOR
From the electromagnetic pickup, the speed indicating
8ystem counts and di'splays the pulses on a Berkley Counter. These pulses are prodticed at a rate of 200 per, second per
knot, Therefore, counting for 1/2 second, a speed of 10
knots produces 1000 pulses on the Berkley Counters and with. proper placement of the decimal, the resulting reading 18 10'
knots. This calibration is the same over the speed range
since the impeller RPM varies linearly with speed.
EVALUATION TESTS BASIN TESTS
The knotmeter towed satisfactorily:at.speedsup to 30
knots in the "high-speed" basin. The instrumentation was
calibrated with the high-speed towing carriage.. 'The
variation of the àabie tension at the.bddy with' spëéd. ..s
presented in Figure
3.
SEA TRIALS
The TMB knotmeter was used sucessful].y on sea trials.
Over a period of approximately four months at sea, minor troubles were discovered and corrected such as, excessive
cable vibration at the towstaff, bearing failure and'
cor-rosion of tow cable. A variation in the indicated readings
due to pitching and rolling of the ship was noted. ' This may
be minimized by increasing the uunting period' and indicating
the average speed over a' longer time interval, Although,
15 knots was the top speed attained at sea 'due 'to limitations
on other towing gear, it is not anticipated that difficulty would be encountered In reaching higher speeds. The body was launched an4 retrieved from the side aüd stern of the' towing vessel with no difficulty.
.ACIQ0WLEDGMTS
The design and development of the'electronic instrumenta-tion was carried out by Mr. J, F. Hunt with the assistance of
Mr. G. N. Metsel, '
8
APPDIX
Knotmeter Installaticn, Maintenance and Adjustment From the results of previous sea trials, it appears that the location of the knotmeter launching site on the deck of the
ship need not be restricted. It is recommended, however, that
the location of the launching site be such that the ship
motion is a minimum. The ithotmeter cable used in all sea
trials was a l-H-0, 0.185-inch diameter stainless steel
cable, number 18 AWG conductor, Kel-F insulation, manufactured
by American Steel and Wire Company.
Figure k, presents the variation of the towing depth of. the knotmeter as a function of speed and scope of tow cable.
Greater.towing depths may be obtained by installing a cable
fairing on the tow cable. These towing depths may be
calcu-lated u8ing the procedure of Reference 1.
The special instructions for connecting the tow cable to the towataff are given in Figure 5 which also shows the assembly of transducer, magnetic pickup, impeller, and
bear-ings. The modification made to the .towstaff to reduce the
effect of vibration, is also shown in Figure 5. This
con-sists of the addition of a six-inch section of rubber fairing whose shape is given in Reference .6. This rubber fairing
substantially reduces the ef1fect of cable vibrations at the towataff and prolongs the life of the tow cable.
The instrumentation is housed in a cabinet, as shown in
Figure
6.
This cabinet may be located in some convenientplac and connected to a standard 115 volts 60 cpa a-c source.
The lead from the cabinet is plugged Into the connect3r from the tow cable and the operation is automatic when the power
is turned on. The followIng figures show the electronic
instrumentation; Figure 7-block diagram, Figure 8-circuit
diagram, Figure 9-power supply. A parts list of the
instru-mentation and power supply' are included0 Additional
infor-mation on the design and construction of the electronic instrumentation may be obtained from the preliminary report by Mr. HDBOO. Davis, entitled "The Circuitry of An Aecurate High Resolution Knotmeter TMB Type 205", October
195k.
9
TABLE 1
Parts List for TMB Knotmeter Type 205A
InstrumentationRi
3M R31100 K
R61k.7K
R2 150 Ohm R322k K
R62 20 M R3 1470 K R33 214 K R63 147 K27 'X
R31433 K
R614200 K
R5180 K
R3550 K Precision
.R65 147 K R6 150 Ohm R36 50 K Potentiometer R66 147 K R715 K
R3750 K
Precision R67270 K
R8 .5M R3822 K
R68270 K
R9150 Ohm
R3922 K
R69100 K
RiO5 K
Rk0 2 M R7012 K
Ru27 K
Mi
1.8 K
R71100 K
R12 147 KM2
18 K
R72 1 M R13 150 Ohm R143 210K R73220 K
Rik
150 Ohm
R1414270 K
R71410 K
Rik
.5M R145390 K
R75,5 M
ni6
2 M n14650 K
Potentiometer R76 147 K R1722 K
Rk7 147 K R77100 K
22 K
nk8
147 K R7810 K Pot.
R191.8 K
R1#9 14.7 K R79500 Ohm
R2018
K R50390 K
R80220 K
R21270K
R5].50
K Potentiometer R81120 K
R22270 K
R52 5M R8227 K
R23100 K
R53 147K R8310 K
R2k100 K
R514 147 K R814150 Ohm 10 W
R2520 K
R55 14,7 K C2.1 pit
R2625 K lOW R56
50 K
Potentiometer C320
D R27 R5.7390 K
014.01 pe
I28
100. K R58 10 M 140 pipit R2951K
R59 14 K C6.01 pf
R30.5 M
'R60
47 .K.5 pf
c8 C9
do
100 141f 100 )1f 20 !4FD Cli .01 if C12 C138
i'
Clk Picked to set Oscillator Frequency C15.05
)lf SilverMica
ci6
.1
.ifCii
.1 pif.
ci8 .01 if'C19
C2040 ppf
C2140 pjif
C22.0011.5 uf
C23 14Qijif
C2kO3 p
C2515 zf
C26150 ,if
C2750 if
C2850 pif
C2901 if.
C30100 ;ipf
C31 25 .1f C32 .01 pf C33.01 if
V-k
581k
v-S
581k
v-6
5814 10 TABLE 2 (Qon1.) V-T5963
v-k
V-3 5727 V-9*5814
V-].O 6Au6 v-il 6Au6 V-125814
V-6
V-135963
58lk
Crystal Diode D-1 N63t-2
.1N63 D-3 1N63 SI-DPST 52-DPSTV-5
TP-1
TP-2
TP-3 TP-kTP-5
TP-.6I-1
H-]. H-2 H-3 8 Pinconnector for D.C,VO B18
Pinconnectorfor D.C.VC, B1
8 Pinconnectorfor DSC.V. B1
Banana Jacks Banana JacksBanana
Jacks Banana Jacks Banana Jacks Banana: Jacks Even Pilot Light NEON 6w 110 V 6w 110 V 6w. 110 V AN3102-16S-5P V-2 :AN3O5_2O_16P V-3 PtflConnector for D.CSV. B1v-i
5814
Connectors. V-2 .581k V-3581k
R1
12K
10 Watts R2 100 K 1 Watt. R3.k7X
iWatt
RLI 180 K 1 Watt R582K
lWatt
R6500
K 1 watt R7 10 K I Watt. R8 kO K 1 Watt R9 10 K 10 WattsRiO 1 Meg. 1 Watt Ru 1 Meg. .1 Wat;t R12 100 K .1 Watt R13 100 K . 1 Watt Capacitors ci k !IFD 600
VD.C.
C2 k MFD 600 V.D. C,. 03 k )IFD600
V0D.C.ck
.1 MFD kOO V.DOC. C5 8 NPD LI.50V.D.C,c6
8
Dk50 v0n.00
Transformers
T1. Chicago .PV 200 R2 21FQ8 fil. .1 Amp. 11 TABLE 2Knotmeter Type 205A Power Supply
Re si store Iiduc tore
Li
8Hen'y 150 Ma.
L2 8,Hez'y 150 Ma. .L38Heiary kOMa.
ValTe8 vi.5'L.
.V2.66&
V3 6Au6 )4. . 0A2 V5 0A2v6
6x
Miscellaneous
SWIS,PJ.T.
Fuse
3 Amp,
12
REFERENCES
Pode, Leonard, "Tables for Computing the Equilibrium COn-figuration of Flexible Cable in a Ur.Uorm Stream",. TLVIB
Report
687,
March1951.
Fehiner, Leo F, "The Hydrodynamic 'Properties
Of the
Air-Towed Sonar Housing". CONPID1TIAL Report -76 April.
1911.8..
Joers, J. E. "The Development of the Air 'rowed Scanning
Sonar Housing". T CONFIDENTIAL Report 0-351, July
1951.
Munk1 Max, "The Aerodynamic Forces on Airship Hulls", NACA
TR 15k, 1923.
Lamb, H., "Hydrodynamics", Sixth Edition,
Dover
Publications,New York,
19k5, page
155.Drawing E-929-lO.
Johnson, J. L. "The Static Stability
:oerivat5.esof a
Series of Related Bodies of Revolution , 'iB CONFIDENTIAL1
13
INITIAL DISTRIBUTION
Copies
11 Chief, Bureau of Ships, Technical LI-.
brary (Code 312) for distributIon:
5 -
Technical IIbrary1 - Technical Assistant to Chief o the
Bureau (Code 106)
Chief, Bureau of Aeronautio8 (Aeronautics and Hydrodynamics) Washington, D. C.
Naval Research Establisbinent
Halifax, Nova Scotia
Attn: Mr. Michael Eames
1 Commander, Portsmouth Nàv1 Shipyard
Portsmouth, New Hampshire
.1 Commanding Officer, Surface Anti-Submarire
Development Detachment, Key Florida
1 Commanding Officer and Director .IJ. S. Navy
Mine Defense Laboratory, Panama City, Florida
2 Commanding Offiôer and Director, U. S. Navy Underwater Sound Laboratory, Fort Trumbell,
ew London, ConnectIcut
1 - Attn: Mr. Don Nicols
1 Commander, Naval Ordnance
]Aboratory
White Oak, Silver Spring,
Maryland
2 Commander, CharlestQn Naval Shipyard Charleston, SQJ1
OaróUna
1 - Attn: E. D. Bigger8taff
1 Conunandng. 0ffieer and Director
U. S. Nva1 Electronics Iaxatory,
San Diego, Califez'nia
1 Commander, Naval Or4nanCe Ltet Station,
continued: Copies
1 Director, Bureau of tanda±"ds,
Washington
16, D. C.
Director, Naval Research Laboratory, Washington 25, D. C.
Mr. L. Fehiner, John Hopkins, Applied
Physics Laboratory, Silver Spring,
Maryland
Commanding Officer and Director, Engineering Experiment Station,
Annapolis, Maryland
Director, Georgia Institute of Technology,
680 Cherry Street, Atlanta, Georgia
1 - Attn: Mr. Ward Sachs
Commander, Noi'Thli..N4ya1 Shipyard,.
Norfolk, Virginia
British Joint Services Mission (Navy stáf)
P. 0. Box 165,
Benjamin Franklin Station,Washington, D. C0
Naval Member
Canadian Joint Staff
2450
Maa3achn5étt Avenue, Washington, D0 C 1 1 29
35
I I - L
400
100 80 40 20
A
Its
15 Its
25 Its
30 Its
20 Its
Scope. of Cable in feet.
Figure 4.-Depth of TMB Knotmeter as a Function of Speed and Scope of Cable
£ iGI%C-2TAP A%% oN 346C, A SNowI% %N PC '-S ft%-4 T #S5'r.Tq TPPP"6 L%OJ ONPC%4 H6fl %L PC %-4 0%N..' ro RodS .%DS 4-SEE SuB-flCM&y OF FAIRINO E-959-I I. Gl.N I'Ft -
-i1
0 lP1iI
M. VENT HOtES LOCATE AS cHowNOil YCATICAL S
/.
j
Figure 5-Assembly Drawlng.of Towed Body
005- SAAi C.A.wkAC
NOTE.
riMs s,ioww 450.?T or PoSrTi.,il
(TO HE SC Al TA wING.)
GMv_wA_ 4O -I- MOUSiM, WIR8. ROiM y .4MTt
PC i-i ow o,i i -2%_NiM IIIbWIOiJL wiw ow vi
MOV CU%_.
3- CLAAH T%wN%o viiwos , ow
WDqOcNLoiMtc ACID.
4.-T%bI W1iM5j5 WITh PUH TIN (pwo-r,.., lA-*CI$(.
CA%, FiMOM r1w. VHI%%C.VI W5.LT8 Al LID 2)
3-DiMiM iOII.D wi INTO 6OC.IItT,
WHIC.14 AN %%S% T0 350p
I -POU,i ISoCcvrM&5. ct to % rI*UL.I.. WIlbH 2CIN.
Si.. VO7 3WJ3TVi $'( VowOly 1W' L%.C.TIHIC. CKSi%. CI.WT53I.pou
A1
1 t4T$ MdØ%.
3oIAE5Aj$f5-AIAP11tNL CDNNSCTOJI. CLCTRIC PRObOcflLAB. IMC. 45 6% tAVtW$IiIH MW. - CiMII!.4a 41 IlL.
MU5T BE TRIMMED ZERO IN WATER
LLECTRICAL CONNEc .TO iM
KEYS I8OAIINJIT
II AND MM.D5. WAI !.
LOCATE A1 ASSEMBLY
PROOp G.Y CO 23$
CL 4 FIT IN NI.
Sit 5LI?O RSSWJLY
c-rn-s
46 S4GSWW 2VD 7 4WXCZ. A:I IP
NP21..5].22
11-5-53
MPi3P4ET%C PICK UP
(4)
0Sc
(2)
WAVE SHAPER(3)
DOUBLER a' GATE(5)
SCALER+500
Figure 7 Block Diagram TMB Knotmeter Type 205A
COUNTERS
(9)
IMPULSE GENERATOR N) H(6).
GATE CONTROLC)
AUTO RESET(8)
BLANKUI
O5CILLATOI
SIGNAL S GNAL WAVE
AMPLIFIER AMP IFIER SHAPER
OSCILLATOR TANK OVEN I 4110 4140 IWpIfl. yO 8c.A&i l__F1L_. FAN MOTOR
WAVE AD,JUST IST ADJUST 2-ND ADJUST 3RD GATE
SHAPER SC.IG SCALER SC.IO SCALER 5C. SCALER CONTROL.
WE
+ 300
+
RESET DECIMAL COUNTING UNITS
LB-V AC ALL. FILAMENTS 22, RIS .5M N SF1114 MUL METAl.
m.Trn
HI HZ 143'I
I'
-I 4-S V AC - DECIMAL. COUNTING UNITS FiLAMENTS-BLANKINGFigure 8-Circuit Diagram TMB Knotmeter Type 205A
(ID VAC TO COO. DECiMAl. COISIrING UNITS 1.1040!. NOTE PRECISION RESISTORO.
ALL VOLTAGE MEASURED WIN- H.P UCOEL. 4108 -VLM
WITH SI IN lEST-POSITION.
ENCIRCLED N" REFER TO BLOCK N" OF'DLOCI( 8(!AIA
-KNOTMETE,R TYPE 2054 NAVY DEPARTMENT MECNGTCII,O. 229 SMElT I CF
-3A FUSE
swi
AC. INPUTfl.
CHICAGC I C. pv200T2
2 I FO 8 I AMP23
63-v L3 20052 BR845.VI
5V4 G TNAD 6040 CL ThJAD 604Q C3, RI 12K ISOy
° S 6X5R7
Figure 9-Power Supply Diagram TMB Knotmeter Type 205A
0
-+300 R 10 114 4O0V UNREGULATED C.0
0
E [DRAWN CHECKED& REVIEWED.L -150POWER SUPPLY
FOR USE WITH