CWRL 172-O5

-= Aerena Re 'fseattch -Laboretoiries

A TABLE OF THE INVERSE SINE-AMPLITUDEFUNCTION IN THE COMPLEX DOMAIN

HENRY E. FETTJSJAMES C. CASLIN

APPLIED MA THEMA TICS RESEARCH LABDORA TORY

PROJECT~ NO. 7071

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Applied Mathematics Research Laboratory 2b GRUncasfP

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A Table of the Inverse Sine-Amplitude Function in the Complex Domain

4 OSC~RIPT VC NOTES (Type of raport end inclu.ivo dae*~):1~ ~ Scientific Final________________________5 AV THOtttII (Firfleano, middle Miniet, loset na.m)

Henry r. Fettis

6 EOT AE? TOTAL NO Or PAGES 7NOt EP

____ ___ __1971_ 180 I4toOTACT ON GRANT NO In-FElose Research 12a ORIGONATORt'S RtEPORT NUM09"(S)

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.1 SUPPLCMCNTAKY NOTTS 12 SPONSORING MILIT ARY ACTIVITY

Tech Other Aerospace Research Laboratories (LB)e Wright-Patterson AFT, Ohio 45433

.3 ABSTRACT

. Let z =sn(vi,k) be the Jacobian sine-amplitude function as defined, e.g. in [1].The tables list five-D values of the quantity w = u + iv where z is given by za + ib, for the following values

a 0(.1)1 h b 0(.l)la .9 (. 0 1) 1 b 0=.1

a

.1(.I~lb O(.l)l

The values of u and v are expressed as decimal portions of the quarter-periods Kand K' raspectively. The modulus is given in the form k = sin 0, irith 6

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I Elliptic funictionsConformal mapping

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lp ARL 72-0050

A TABLE OF THE INVERSE SINE-AMPLITUDE

FUNCTION IN THE COMPLEX DOMAIN

HENRY E. FETTIS

JAMES C. CASLIN

APPLIED MA THEMA TICS RESEA RCH LA BORA TOR Y

APRIL 1972

PROJECT 7071

Approved for public release; distribution unlimited.

AEROSPACE RESEARCH LABORATORIESAIR FORCE SYSTEMS COMMAND

UNITED STATES AIR FORCEWRIGHT-PAITERSON AIR FORCE BASE, OHIO

FOREhO)RD

The present tables were prepared by the Applied Mathematics Research

Laboratory of Aerospace Research Laboratories, under Project No. 7071.

The computations were initiated by Mr. Henry E. Fettis, and carried out

by Mr. Jamas C. Caslin on the CDC 6600 electronic digital computer.

ii

- - .---. - -'~ v -- -~=- I.3I~ I.A. 1IJII~. OJ

ABS~TRC

Let z sn(w,k) be the Jacobian sine-amplitude function as defined,

e.g. in [1). The tables list five-i) values of the quantity w =u + iv

where z is given by z = a + ib, for the follcating values

a 0(.1)1 b 0(.l)l

a =.9(.01)1 b =0(.l)l

a 0(.1)1 - 1(.1)1

~. 01(.01).l ;b =0(.l)l

1(.I~lb 0(.1)1

a 1.1. 0 1(.01)l

The values of u and v are expressed as decimal portions of the quarter-

periods K a~nd K' respectively. The modulus is given in the form k=

sin 0, withl 0 0(0 50(080

r/

TABLE OF ONETS

INTRODUC TION 1

UIE ADDITION FORMULA FOR THE INVERSE SINE-AMPLIiTUDE FUNCTION 1

REFERENCES 6

TABLES - u/K + iv/K'; u - iv = sn' (a ib)

1. a: 0- 1 ; b : 0- 1 7

2. a: .9 -1 ; b: 0 -1 28

3, a :0 -1 ; .01 - .1 491

4. a: 0 -1 ; :.1-1 70

5. 01 .1 b:0- 1 91a

6. 1 . b:0-1 112

7. 1: .01- .1 .01 - .1 133

1 18. a-: I I - 1 154

iv

I

IMTIODUCTIMN

I• The Jacobian elliptic functions with ccap!ex agnumwi- occur primarily

in 2r- l(ns of conforma mapping (see, e.g. 14]). Tabulated values of

.e,. "ns can be found in jLjI a7 - [3]. Frcquently it is desirous

to k ..,.; inverse function, for exavple, to find w if sn(w) is given.

This would require interpolation in two variables, which is both incoLr-i nient end inaccurate, particularly in sowe regions where a small change

in thr: argument results in a large change in the function. The Liarts in

(2] can be employed to obtain qualitatively correct values of the inverse

function, but to date no explicit tabulation is kncwn.

The present tables give values of the inverse sine-amplitude fimntion

w = u + iv for values of a and b which cover the entire first quadrant of

the a + ib plane. The quantities u and v are expressed in the form u/K

and v/Kt where K = K(k) and K' = K(k') are the coirplete elliptic integrals

with modulus k and k' = k, re-pectively. These quantities define

the quarter-periods of the corresponding elliptic functions.

THE ADDITION 0IMMUA FOR ThE INVERSE SINE-A4PLITUDE FUNCTION

j Since by definition

u + iv = sn-l(a + ib) F (%',k) (1)

Swhere

a b =sin(4) =sin(e + if), (2)

1

the aroblem of obtaining the I nverse sine-amplitude function is actually

equivalent to coinputi_% the elliptic integial with conplex amplitude.

_'Tis could 6- course be accaiplished directly either by series or reduc-

tion of imodulus. However, a singler rathod cMa be derived I v %sing the

addition fonrula fcr the anplitude function.

We have, considering first the case of real cirgument,

G , e am(,,•v) (3)

and by the addition formiula [1]

tan'O'= tn u dn v

(4)

tan 0 = tn v dn u

where the modulus of the elliptic functions is k.

Eliminating successively sn u and sn v between Eqs (4) we get

k2 cos22sn4u -[ + k2 (Sin28cos2 - Cos 2 Osin 2 )]sn 2u + sin2e = 0(5)

k2cos 28sn4v -[1 + k2 (cos n - sin2ecos 2 )]sn 2v sin

Solving gives

2 2 (- ieo~ 2 -

2 2 2+ k sinecos.) - k cos Osin - 1 k sinkosý) - cos2Osin 2snu ..

2k ccosO2(6)

sn v s 1 +l)k . -_ksico~ -_1-I o~i4 - k 2si 2ecos 2 ¢ !

2k

Making usa of Ea. 2 and the result

Cos0= --{/7 (lb)' -a 2+ /(1-b) -a).,

(7)

Cos 4 = k{,/(1 + a) -b 2+ /(1 - a)- b'),

Eqs. 6 may be written explicitly in terms of a and b.

In the case of coiplex argume~nt v is replaced by iv, by i4, and

b by ib. Thie first equation 6 beccomes

+2 _a) Z 2sa (,I sk) = ~(kb) 2

- 41 ka) + (b

______________(8)

/,2a 2 24 b 2

4 1, a) 2+ (kb) 2+ /(l ka) + (kb)

while the imaginary part is more easily calculated from the second Eq. 4,

after ustig the transformation -tn(iv,k) = sn(v,k')

sra(v,k') tahý(9)

X7 -2 sn 2u

With sn(u,k) amid sn(v,k') kcnown it is easy t'n find u and v by 1ee

conventional method of modulus reductio~n from the formu~lae

u mF(ct,k)

v =F($,kl)

where sin a sn u, sin sn v.

3

..-

In the case where b = 0, Eqs. 8 and 9 simplify to

sn(uk) - (I + ka)j- 1i1 ka2k 7co4sh

sn(v,k') = tanh 4 (10)

1 - k2 sn2 u

cosh k = i'[(I + a) + 1i - al]

If a < 1, the above equations give

¢=0

sn(u,k) = a (11)

sn(v,k) = 0

and

u + iv = F(sin- a,k). (12)

If a > 1 and ka > 1, we obtain

cosh 4 = a

tanh4, a 2 -1Ia

(13)

sn(u.k) =1/'.

sn(v,k') = 1,

4

Hence

u + iv Fisin-1 (1/ka),k] + iK(k). (14)

Finally if a > 1 and ka < I

cosh 4) a

sn(u,k) = 1 (15)

sn(v,kl) = /ak

and

-• a ' k2 (16)u + iv= K(eK) + iF( a 71/ak kk).

If ka 1, both Eqs. 14 and 16 give

u + iv = KCK) + AK' (k) (17)

-E 1

- I

REFENCES

(1] Byrd, P. F. and Friedman, M. D,, "Handbook of Elliptic Integrals

for Engineers and Physicists", Springer (1954, 1971).

[2] Fettis, Henry E. and Caslin, James C, "Elliptic Functions for Com-

plex Arguments", ARL TR 67-0001 (Jan 1967).

[3] Henderson, F. M., "Elliptic Functions with Ccmplex Agruments",

University of Midcigan Press (1960).

[4] Kober, H., 'Dictionary of Conformal Representations", Dover (19S2).

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