Definite Integrals for Expressing
Polynomials into Fourier Series
Bennosuke TANIMOTO*, Dr. Eng. & Dr. Sci.
(Received October 10, 196e)
Synopsis. This article gives several !<inds of definite integrals, which will be con-
venient to express polynornials into Fourier series. Examples are added for illustration.
We take the following polynomial of p:
w(p) =ae -= aip+a2p2+-・+arpr, (1)
which isdefined in the interval (O,1>; ao, ai,・・・, ar being constants independent
of p. This polynorrLial may be writteR in the form
cx) w(p) =Xcn sin nzp, (2) n--1
or in the form
co w(p) =co +Zcn cos nzp. (3) n==1
The present tables will provide a convenient means for expressing equation
(1) into equation (2) or (3).
For instance, we take simple beams such as given in Figs.ItN,4. Figs.1
and 2 are subjected to "continuous" loads throughout the whole interval (1,O),
and hence Tables ItN-II serve for such cases. Fig.3 is subjected to two kinds
of loads, which is connected at the midpoint of the beam; and hence Tables
III--VI serve for such a case. Fig.4 is subjected to a partial load in a certain
range of the beam; and hence Tables VIIA"XII serve for s・uch a case. Several
examples which follow will serve as illustration.
Example1 <Fig.l). By the elementary theory of banding of beam, the
defiection w at poiRt x of the simple beam subjected to uniform Ioad q is given
by the equation
:S Professor of Civil Engineerlng, Faculty of Engineering, Shinslva University, Nagano,
Japan.
No. 10 Definite Integrals for Expressing
q
x・tv
Polynomials into Fourier Series
'
q
tX+zva
Fig. 1.
aa 22
o
xtv a
Fig.' 3.
.-,gZ`,(:- 21
where El is the flexural rigldity, and is
the length of the beam. To get the
put
tlli.ilicnsinnarrX..24qEa`i(:
multiply by sin nanv dx,on both sides,
Putting
fi = p, du ==
a
we have
(Integration of left-haRd side) =: S," (.O,O.nt-,
qa` <Integration of right-hand side) == 24EI
qa4
24EI
and hence
qa4 .1 Cn =2 24EI
Fig. 2.
B
67
・-・- cr-
X4 2- "5 - a4
supposed
Fourier
and intecrrate
a dp,
:E] c2n sin ManX) sin fZaffX -- u:'- cn,
S,a (: - 2tts3 + tl:t`) sin '7.ZX dx
i aS (p - 2p3 + p`) sin nr,pdp, o
5o (s) - 2p3 n- R`) sin nffp dp.
x--" lv a Fig. 4.
to be a constant throughout
sine series for equation (4), we
,.es3 -i- 2111)・
. the result fromOto a,
(5)
In virtue of Table I, we have
1 - (n = 1, 3, 5, ・・・), 7Zr, S: p sin nrrp dp ...
I - - (n == 2, 4, 6, ・・・); nrr
l6 i ffT- <nx)3 <n "= 1, 3, 5, ・・・), So p3 sin nzp dp ..r
}6 - 5itirr + <nz>3 (n = 2, 4, 6, ・・・);
112 48 i n". - (nrr)3+ (n.>s (n=1, 3, 5, ・・`), Sop` sin nap dp ,.
112 rm' iiTT + (nrr>3 (n = 2, 4, 6, ・・・).
Substituting these values into equation (5), we get
11 48 ,-,.(1 -2+ 1)+ (..)3[(th 2) × (- 6) - 12} + <nn)s qaa
× (n -- 1, 3, 5, ・->,cft = 12E7 11 iit}T(- l+2- 1) -i- <n.)3[(m 2) ×6+ 12} (n = 2, 4, 6, ・・・>
qa` 48 4qa` 1 == 12EJ' (nn)5 =: nsEI'fiT, <7Z = 1, 3, 5, ・'・).
Hence the wanted series becomes
w == 2a4aiiii (: - 2IIiil + illf) =- 4.q,{ii .=i$, II,,,, ... .-i, sin n.rrX. (6)
It wili be seen that the Fourier coeflicient cn is in general given by the equa-
tion
i cn == 2S, w(p) sin nrrp dp. (7)
Example2 (Fig.2). The deflection w of the beam of Fig.2is given by
Ne.10 Deimite lntegrals for Expressing Polynomials into Fourier Series 69
w=36qo"S-I-(7Z-lolilP+3}?). <s)
Referring to Table I, we at once have
w"= ;gifli`i ;,l].-l.iMni,)""isin naTX. (g)
Computation work negessary for getting equation <9) is rnerely
(- 1)n+i;.(7 - 10 + 3) =: O, <- 1)n+i(n}),{(- 10) × (- 6) +3 × (- 20)} = O,
(- i)n+'(ni.), ×3× i2o ×2× 36qoaiiii == 3,qEa ・(- in),""i, == c.;
and this work is effected ethciently by using small pieces of paper of about 5 mm
× 15 mm size, on respective sheets of which the numerals 7, - 10, 3 are written.
Example3 (Fig.3). The defiection w for the beam indicated in Fig.3is
given by the equations
xx3 wi in- g6qo"iiil(25a-4oEr,+!62?) (o<x<ba), (lo)
w2 = g6qo"b(i " is: + 4olil, - i2ot;t3 + soir - i61ilP) '(ga <x< a). (m
In this case equation (7) becomes
' cn = 2S: w(p) sin nmp dp = 2Si"' zvi(p) sin nrrp dR + 2Sl w2(p) sin nzp dp.
For two integrals ef the right-hand side, reference may be made to Tables
III and V respective!y. In this way we get
ttl 8qa" (- 1) 2 Cn = T6EI' n6 <n == 1, 3, 5, ・..).
Thus we arrive at the wanted series
t(ww-rm1 w ;=: £,6qEai;.tll;l3,s.... (-ni6) 2 sin 7i:X. (i2)
ee
70 B. TANIMoTo Example 4. The present integral tables may be used for converting
Fourier .qeries into its poiynomial. As asimple example, we take the
slne serles
W(P) == .x#, 3, s,... (fe.1.,)s Sin n"P (O<P< 1),
and shall find its polynomial. Now from Table I, we can put
ZV (,o) =: cro + aip H- cv2R2 + cr3p3 + a4p4,
where ao, cri, ・・・, cr4 are constants to be determined. Referring to Table
1collecting same powers of we have <nz)r'
2cro -Y cr1 + cr2 + cr3 + cr4 == O, 4a2 - 6crs - 12a4 == O, l <n = 1, 3, 5, ・・・);
48a4 := i, t
6rmcr,crX12crcr2, 1-cro3, ww cra rO' l (n .. 2, 4, 6, ...);
from which
l 11 crO=O, cr1 nd- -g6, cr2=O, a3 =:-li{g, cra={}Tt・
Hence the wanted polynomial becomes
I W<P) == {}itr (p - 2p3 -F p`) (o < p< 1> .
This is the reverse of Example 1.
a
F
No. 10
glven
ourler
(13)
I, and
<14)
No. 10 Defuite Integrals for Expressing
ART. 1 L So pr sin nrcp ap
II. I:prcosnflpdR
IIL S,Sprsinnffpd,o
IV・ Io"'prcosnnpdp
V. Sib pr sin nnp dy
i VL Ss pr cos nmp dp
vll. !i pr sin nrrp dp
VIIL S,e pr cos nup dp
IX SI pr sin nrrp dp
' X' Se? Pr cos nTp dp
XL Si pr sin nffp dp
XII. Si pr cos nTp dp
Polynomials into
Contents
(r == O, i, 2, 3, ・・・;
Fourier Series
PAGE
71
72
73
75
77
79
81
82
83
84
85
87
n = l, 2, 3, ・・・)
71
72
i・ S
B. TANIMOTO
1
pr sin nrrp dp
o. -
No. 10
III
l/
I
Il
r
o
/tt
IiI..j
n
1, 3, 5,・-
2, 4, 6, ・・・
t ttt S] Rr sin nzp dp
ttttttt-ttttt"ttttt tt ... .t.
L
l..I
iiir.
r
E
n
o
iiji
i
-I
l
i
1, 3, 5, -・
tt2, 4, 6, ・・・
s1
pr sin nTp dpo
1
IlI
I
1
itII
2
1
nrc
1 m
l
E
1-- (- 1)n+1pm nrc
1, 3, 5, ・・・
2, 4, 6, ・・・
3
4
5
l
IrlII-
1
li
6
o,2,4,
2s
l 1, 3, 5, ・・・
2, 4, 6, ・・・
1, 3, 5, ・・・
2, 4, 6, ・・・
l, 3, 5, ・・・
2, 4, 6, ・・・
1, 3, 5, ・・・
2, 4, 6, ・・・
--------t---
1, 3, 5, ・・・
2, 4, 6, ・・・
1
nrr
4(nx)3
l
nz
1
nrr
6(nrc)3
1
-e + fzr,
6(nT)3
(- IYI+1[1
nn
(n6rr)3 ]
1
nrc
12 +(nrt)3
48
<?Zff)5
1-- + nrc
12
(nz)3
1
'nrr
20 +(nr, )3
l20
(nx)5
1
-- + 7Zrr .
20
(TZrc)3
120
(nT)5
: (- 1)n+1[ 120nT (nrr),3
+(i.2.0)s]
1nR
.
30
- -+ (M)3
360
(nrr)5
1 440(un
nx)7
1
-- + flZ
30
(nx)3
360
(lzx)5
----------------------------4-
(2s)![ (2s i. nrr - 1
+(2s - 2)! (nz)3
1(2s - 4)! (nrc)5
(- 1)s-i
-F -Y 2! (nre)2s-1
2(- 1)sO!..(er,)2s+i
]
(2s)!rt 1
- +- <2s)! nr,
1(2s - 2)! <nr,)3
1 <2s - 4>! (nff>5
(- 1)s-i
4! (nz)2s-3
+ ...
(nt 1)s
2! (nT)2s-i]
..l
No. 10 Definite Integrals for Expressing Polvnomials ',nto Fourier Series 73
r
1,
3,
5,
2s +l
n
1, 3, 5, ・・・
2, 4, 6, ・・・
si
pr sin nzp dp
(2s + 1)!(
(2s +
1
1>! nrc
(2s + 1)!(um (2s+
11ww le(2s - l)! (n}l5T' + '(2s - 3)! (nx)g
- ・・・ -F 3:, th;)),S,--i, + 1!((i,S,),i-.,]
ttt1
1)! nrr 11+ (2s - 1)! (nrt)3 - Zisrmrrm3')! (f・zrc)5
<- 1)S+i (- l)s + +・-+ i! (nz)2s+1 3! (nre)2s-1
]
II. s1o
pr cos nxp dp
r
o
2
4
5
6
n
1, 3, 5, ・・・
2, 4, 6, ・・・
1, 3, 5, ・・・
2, 4, 6, ・・・
1, 3, 5, ・・・
2, 4, 6, ・・・
1, 3, 5, ・・・
2, 4, 6, ・・・
1, 3, 5, ・・・
2, 4, 6, ・・・
ttt-------t----
s1 pr cos nnp dpe
o
o
2 (7Zrr)2
2(flrc)2 l
.
= (- 1)n 2(nrc>2
r
1
3
n
1, 3, 5, ・・・
2, 4, 6, ・・・
1, 3, 5, ・・・
2, 4, 6, ・・・
s1o
pr cos nrrp dp
2(nz)2
o
3 (nrr)2
3(12rr)2
12+ (71 r, )4
4 (OIT)2
4(nrr)2
24--F (nx)4
24
(nn)4
=: (- 1)n[ 4(7Zrr>2 ww
(:.4),]
5(nrr)2
60+ (nrc)4
240
(nrc)6
5(7ZZ)
60
2 (nn)4
l I
.-m. I i
6 (nrr)2
6(7zT)2
120+ (nrc)4120 +(nrr)4
720 (nx)6
720
(nre)6
E
": (- 1)n[ 6(7z r, )2
120 <fZr,)4
720
(7ZT)61'
i-----i--------i--------------------
74 B. TANIMOTO No. 10
i'
IIl,
Ill
r
j
o,2,4,
2s
1,
3,
5,
2s+1
71
1, 3, 5, ・・・
2, 4, 6, ・・・
1, 3, 5, ・・・
2, 4, 6, ・・・
sg
pr cos nrrp dp
<2s)! [-(2s :'
1
l) ! (nrc)2 11 (2s - 3)! (nr,)` (2s - 5>! (7zT)6
(- 1)s-i <- 1)s +・-+ + 1! (nrc) 3! (nn)2s-2
2s]
(2s)! [(2s - 1
i) ! (nrc)2
1(2s - 3)! (nrc)4 +
+
1<2s - 5>! <nz)6
(ww 1)s +3! <nx) 2s-2
(- 1)s+i
1! <nsc>2s]
(2s +1)! (- 1
(2s) ! (nrt)2
1+ (2s - 2)! <nrr)`
+・-+
1 (2s - 4)! (nn)6
2(- 1)s+i (- 1)s + O! (nr,)2s+22! (nr, )2s
]
(2s +1)! ( (2,) !1
(?Zz)z
1(2s - 2) ! (nrr)4
-ww ---
--F
+
1(2s - 4) ! (ni)6
(- 1)s+i (- 1)s + 2! (nrr)2s4! (nrr)2s-2
]
III. sg
pr sin nTp dp
r
o
1
2
n
1, 5, 9, ・・・
'2, 6, 10, ・・-
sJ,e
R" sin nrrp dp
E 1
nff
2
nrr
1, 5, 9, ・・・
tt2, 6, 10, ・・・
l
1.(nrr)2
I
2nT
1
2
'
'
5, 9, ・・・
lt tt
6, 10, ・・・
1(nrc)
th4nr,
nt 22 <nr,)3
4 (07r,)3
T
o
1
2
n
3, 7, ll, ・・・
'4, 8, 12, ・・・
3, 7, 11, ・・・
tt4, 8, 12, ・・・
3, 7, 11, ・・・
4, 8, 12, ・・・
s.1..
x
o
pr sin nffp dp
1
71r,
o
1<m)r
1
2zZrt
1<s・er,)2
1
4nrt
2<nr, )3 5
]]l
El
No. Ie Definite Integrals for Expressing Polynomials into Fourier Series 75
r
3
4
5
o,
2,
4,
2s
7・z
s/1'
p" sin n-p dp
1, 5, 9, ・・-
i
2, 6, 10, ・・・
1, 5, 9, ・-・
2, 6, IO, ・・+
1, 5, 9, ・・・
2, 6, 10, ・・・
34(nr,)2
6(71r,)4
um.irm
8nrc
12( nr, )2
3
(nr,)3
12-.umnvt..m
ml-(nrc)4
24
(VZrr)5
.116nT
3(71rr)3
48+ (nT>5
516(nrr>
15L' (nrt)4
120+ (71rr)6
l32nrr
5
2(nn)3
60+ (nrc)5
-------b!-------t------t------
r
3
4
5
---
n
3, 7, 11, ・・・
4, 8, 12, ・・・
3, 7, !1, ...
4, 8, 12, ・・・
3, 7, 11, ・・・
4, 8, 12, ・・・
------------
j// pr sin nnp .dp
E
1, 5, 9, ・・・
3, 7, ll, ・・・
]
2, 6, 10, ・・・
1,
.3,
5,
---
2s -- 1
4, 8, 12, -・・
l, 5, 9, ・・・
34<nrc)2
6+ (Tlx>4
1
-- + 8nn 3(flrr)3
1 2(nz)2
'
12(71rr)4
24+ (nrt)5
1 16fzT
3(7Zn)3
5- 16(nrt)2 +
15
(nrc)4
120
(7zx)6
132nn
5 2(nT>3
60
(nrr)5
--------t----------"----------
(2S) ! [ 22s-i (2s
+
- 1)! (nT)2 22s-3(2s - 3)! (nz)`
22s-s(2s ve1 s)! (nn)6 + ' J,' + 2(. -1! l7)iSrrM)ls + ,,(,iF,.lii.,]
(2S)!(ww 22s-i(2s 1 ÷ - 1)! (nn)2'
122s-5(2s - 5)! (nfl)6
122sm3(2s - 3)! (nz>`
(nv 1)s+・"+ + 2.1! (na)2s
o!((irrlil+i]
t
'i
(2s)! [ 122s <2s>! nrr
122sm2(2s - 2>! (nre>3
! -i- "' + ÷ 22s-4(2s - 4) ! (nrc)5
oZ`(7,.lli+'-i]
<2s)! [- 122s (2s)! nrc
+ 122s-2<2s - 2)! (nx)3
1 ÷"-+22s-4(2s - 4) ! (nT)5
22 ' 2 [/ inl.))S2,- "
(2s +1)![ 1
22s <2s)! (nrr)2
+
122s-2(2s - 2) ! (nz)`
1 +."+22s-4(2s - 4)! (nz)6
o!` (irt38--2]
s
I
II
j!t
'
1
Ii[lii
76 B. TANIMOTO No. 10
r
1,
3,
5,
2s+1
n
3, 7, 11, ・・・
2, 6, 10, ・・・
4, 8, 12, ・・・
.1.sg
pr sin nx,o dp
(2s + 1)! (- 122s <2s)! (nz)
i '2 ' 22s-2(2s - 2)! (nz)`
1 -F ・・・ +22s-4(2s - 4)! (nrr)6
(- l)s+i
O! (nT)2s+2]
(2s +1)! [ 1
22s+i(2s +
+
l1)! nrr 22s-i (2s - 1)! (nrc)3
1 ÷-・+ 22sut3(2s - 3)! (nx)5
(- 1>s
2・1! (nT)2s+1)J
(2s + 1)! [- 122s+1(2s +
1 +・1)! nrr 22s-i(2s - l>! (n-)3
1 (- 1)s+i +'"+22snt3(2s - 3>! (fzr,>5 2・1! (nx)2s+i]
IV. sgo
pr cos nnR dp
r
o
l
2
3
n
1, 5, 9, ・・・
2, 6, 10, ・・・
1, 5, 9, ・-・
2, 6, 10, ・・・
1, 5, 9, ・・.
2, 6, 10, ・・・
1, 5, 9, ・・・
2, 6, 10, ・・・
s"o
pr cos nrrp dp
1
nx
o
l2nr,
1(nrr)2
2
<nR)2
1
4nn
2(nrr)3
ww 1 (flrr)2
18nre
---{l----
(?Zn)3
6+ m.ttttttumtL t
<7Zz)4
3'
4(nrr)2
12
(nr, )4
r
o
1
2
3
n
3, 7, 11, ・・・
4, 8, 12, ・・・
3, 7, 11, ・.t
4, 8, 12, ・・・
3, 7, 11, ・・・
4, 8, 12, ・・・
3, 7, 11, ・・・
4, 8, 12, ・・・
ss'
pr cos nnp dp
l
nrr
o
1
2nz-1 (elff)2
o
1
4nrc
2+ (nrr)3
1
.(IZz)2
1
-- + 8nn
LT3...ve-
(1・trr)3
6'・- (?Zn)4
34(nT)2
No. 10 Definite Integrals for Expressing Polynomials into Fourier Series 77t/,・
fF
t r
4
o,2,4,
2s
1,
3,
5,
2s +1
n
1, 5, 9, ・・・
2, 6, 10, ・・・
i-----------
1, 5, 9, ・・・
3, 7, 11, ・・・
2, 6, 10, ・・・
4, 8, 12, ・:・
1, 5, 9, ・・・
3, 7, 11, ・・・
2, 6, 10, ・・-
s"o
pr cos nrrp dp
1
16nre
3-- + (7Zrr)3
24 -
(nff)5
12(nrr)2
12+ (nn>4
t--------------i-------l
T
4
1・Z
3, 7, ll, ・・・
4, 8, 12, ・・・
------------
s8'
pr cos mp dp
1
-÷ l6nrr 3-(71x>3
24
(nz>5
12(nit)2
12
(nx)4
-i-t-t--------i---------
(2s)![ 122s (2s)! nz
122s-2(2s - 2)! (nn)3
1 + 22sm4(2s - 4)! (nrr)5 + --- +
(rm 1)s
O! (nre)2s+1]
(2s)![um 122s (2s)! 7tz
1-iun 22s->(2s - 2)! (nT)3
1 22s-4(2s - 4)! (nrc)5 +".+
(- 1>s+i
O! (nrt)2s+1]
(2s)![- 11 + 22s-3<2s - 3)! (nrr)`22smi(2s - 1)! (nrc)2
1 - 22S'5(2s - 5)! (nrr)6 + ''' +
(- 1)s
2. 1 ! (nrr)2s]
(2s)! [ 122s-1(2s - 1) ! (nx)2
+
1 22sm3(2s - 3)! (nrr)`
122s-5' (2s - 5)! (nrc)6 +
ttt(2s ÷ 1)! [22,+i(2s e 1>! nr, -
1 + 22sne3(2s - 3)! (nrr)5
." +(- 1)s+i
2・1!(nz)
2s]
122smi (2s - 1)! (nT)3
<- 1)s+ '- rl- un + 2. 1 ! <nrr)2s.+1
(- 1)s+i
O! (nz)2s+2]
'(2s + 1)!C- 2,,+,(2s lli 1)! 7z.
1 22s'3(2s - 3)! (nx)5
+
+
122s"i(2s - O! (nrti'3
(- 1)s+i"' + + 2・1! (nn)2s +1
(- 1>S+i
O! <nr)2s+2]
(2s -F
t tti)! [- nEis<28!nv(nT)2 ÷ 22s:i(2g']l' '2)'! (iiT)`
1 22sww4(2s - 4)! (nr,)G ". +
(- 1)s +22・2!(nz)2s
2<- 1)s+i
O! (nr,)2s+2]
78 B. TANIMOTO No. 10
r
1,
3, 5,
2s+1
n
4, 8, i2, ・・・
s"o
pr cos nmp dp
(2s +i)! C 1 1
22s (2s>! <nn)2
+
22s-2<2s - 2)! (nr,)`
l ., m... +
<- 1)s+i
22sww4<2s - 4)! (nz>6l 22 . 2 ! (nrc)2s
]
v. s1gpr sin nap dp
r
o
1
2
3
4
11
1, 5, 9, ・・・
2, 6, IO, ・・・
1, 5, 9, ・-・
2, 6, 10, ・・・
1, 5, 9, ・・・
2, 6, 10, ・-・
1, 5, 9, ・・・
2, 6, IO, ・・・
1, 5, 9, ・・・
2, 6, 10, ・・・
s1Spr sin nxp dp
1
nn
2
nx
1
nz
1(nn)2
3
2nn
1
nz
l(nre)2
2(nT)3
5
4m1
nrc
4+ (nre)3 ' 34(nn)2
t tttttwwt.tt
6 (flz>3
6-1- - (OZT)4
9
--- + 8nfi
9(nft)3
1
nr,
12(nr, >2
12+ -- (7Zre)4
12 (71.rr)3
24" (7-lrr)5
17- -i- 16nr,
15
(fiZrt)3
48<fln)5
r
o
1
n
3, 7, ll, ・・・
4, 8, 12, ・・・
3, 7, 11, ・・・
4, 8, 12, ・・・
2
3
4
3, 7, 11, ・・・
4, 8, 12, ・・・
3, 7, 11, ・・・
4, 8, 12, ・・・
3, 7, ll, ・+・
4, 8, 12, ・・・
s1 pr sin nxp dp"
i
nn
o
1
-÷m 1(nrt)2
1
2nT
1
-+nrt (nn)2 <nr,)3
3
4nr,
1
nx
3+ 4(nrr)2
e h --m 6 (nz)3
6 (nr, )4
7
8nr,
3÷ (nz)3
1
-+TZrr
12(nx)2
12
(nrr)4
12 (nfl)3
24"- (nx)5
15
--- + 16nrr
9(7trc)3
No, 10 Defuiite Integrals for Expressing P61ynomials into F ourler Series 79
r
5
---
o,2,4,
2s
1,
3,
5,
2s -F 1
71
1, 5, 9, ・・・
2, 6, 10, ・・・
-------t--i-
1, 5, 9, ・・・
3, 7, 11, ・・・
2, 6, 10, ・・・
4, 8, 12, ・・・
1, 5, 9, ・-+
1
fndtT
+
Sl pr sin nrrR dp
- 5 16<nx)2
15 120-- + (nT)5(71re)4
20
(nx)3
120 (nz)6
33 45- 32nz + nv2'
(nz)3
180
(7zz)5
----i-------------------
pt
5
n
3, 7, 11, ・・・
4, 8, 12, ・・・
------------
Sl,,
1
iit}Ir,
pr sin nmp dp
5
-F - 16(nrr)2
15 120 +(7Zff)4 (7Zfl)5
20(?lrc)3
120÷ ------- (11r,)6.
31
32nz
35mi- umrmm" 2(nr, )3
60
(nff)5
------------------------
(2s)![
(2s)! nT 22s-i <2s -
1+ 22sm3(2s - 3)! (nrr)` +
11)! (nz)2 (2s - 2)! (nT)3
(2s - 4)! (nrr)5 22s-5 (2s - 5)! (nn)6
(- 1)s (- 1>s - --- + ---um,.wu..unne + O! (nz>2s+1 2・1! (nrr)2s
]
(2S)!( (2si nz ÷ 22s-i(2s -i
i 22s-3(2s - 3)! (nrc)`
11)! (nz)2 (2s - 2)! (nrr>3
+(2s - 4)! (nrr)5 22s-5(2s - 5)! (nrr)6
(- 1)s+i (um 1)s
-・-+ + O! (nrc)2s+1 2. 1! (nrr)2s]
(2S)! [' 22?2i2s+)!lnrr 22s-2 + 1÷ 22sm2(2s - 2)! (nx)3
22s-4 + 1
22s-4(2s - 4)! (nn)5"- +
2(- 1)s+i
O! (nrr)2s+1]
(2s)! [- 22s - 1 -+ 22s <2s)! nr,
ttttttttttttt
i)![ (2s -i- 1)!7zr, -
i22s-2(2s - 2)! <nn)"
22s-2 - 1
22sum2(2s - 2)! (nx)3
22s-4 " 1
22s-4(2s - 4)! (nr,)5 + tt ttt t t
(- 1)s(22 - 1)
22.2! (nr,)2s-1]
(2s +
---
22s(2s)! (nrr)2 (2s - 1)! (nrr)3
22s-4(2s - 4) ! (nrc)6 (2s - 3)! (nrr)5
(- 1)s+i (- 1)s - ''' + 1! (nrr)2s+1 + o! (nz)2sTt ]
80 B. TANIMOTO No. 10
r ff'
I
1,
3,
5,
2s+1
3, 7, ll, ・・・
2, 6, 10, ・・・
4, 8, 12, ・・・
Sl,.
pr sin nr,p dp
(2s + 1)!((2s + l + 1)! nx
1 22s-2(2s - 2) ! (nrt)`
122s (2s>! (nrr)2
1 <2s - 3) ! (nr, )5
m '" -i- 1!
1 (2s - 1)! (nn)3
1+ 22s-4(2s - 4)! (nz)6
(ww l)s (- 1)s +(nx)2s+1 O! (nz)2s-F2
]
(2s + l)!(- 22s+1+1 22s-1+1 + 22s-i(2s - 1)! (nz)322s+i(2s + 1)! nrr
22s-3 + 1 3(- 1)s+i
- +".+ (nz)5 22s-3<2s - 3)! 2・1! (nff)2s--1
)j
(2s + 1)![- 22s÷1-1 22s-1-1 + 22s-i(2s - 1)! (nT)322s--i(2s + 1)! nn
22s-3 - 1 - 22s-3(2s - 3)! (nz)5 + ''' +
<-2・1!
1)s-
(nn)2s+1)
Vi・ S 1
pr cos nmp dpl
r
o
l
2
3
11 sL
pr cos nTp dp
1, 5, 9, ・・・
2, 6, 10, ・・・
!, 5, 9, ・・・
2, 6, 10, ・・・
1, 5, 9, ・・・
2, 6, IO, ・・・
1, 5, 9, ・・・
1
nn
o
ll2nfl (nn)2
2(nrc)L)
1
4nn
2- ・+ (f'Zz>2
2(nrc)3
3ewt)2
138nrr (nrr)2 +
+
3 (nT)3
6(fZrr)4
r
o
1
2
3
o・f.
3, 7, 11, ・・・
4, 8, 12, ・・・
3, 7, 11, ・・・
4, 8, 12, -・・
3, 7, 11, ・・-
4, 8, 12, t・・
3, 7, 11, ・・・
s1
gpr cos nrcp dp
1
mo
i
2nrr
1(nrr>2
o
1
4nn
2(na)2
2(nrr>3
I(71T)2
l
8nn
3(nz>2
+
3(nz)3
6(nff>4
iE
Ne. Ie Definite Integrals for Expressing Polynomials into Fourier Series 81
Ii
I:l
i
r
3
4
o,
2,
4,
2s
1,
3,
5,
2s +1
n
2, 6, 10, ・・・
1s pr cos nr,p dpth
l
-15 - 12ww4(nrc>2 (nrr)4
1, 5, 9, ・・・
2, 6, 10, ・・・
------------
14l6nn (nx)2
24 + (?Zrc)4 e
3÷ (nT)3
24 (nT)5
9362(nrr)2 <nrt)4
---l---i---------------l
r
3
4
1・Z
4, 8, 12, ・・・
3, 7, ll, ・・・
4, 8, 12, ・・・
--------i---
Sl, pr cos nmp dp
94(nz)2
1, 5, 9, ・・・
3, 7, 11, ・・・
2, 6, 10, ・・・
4, 8, 12, ・-・
1, 5, 9, ・・・
16nn (nrt)2
24 ++ (7Zz)4
3(nT)3
24(nrr)5
7 122<n rr)2 <nT)`
------------------------
(2S) ! [- 22s <is>! flz
1+ (2s - 3)! (nrr)4
1(2s - 1)! <nn)2
122s-4(2s - 4)!
+"
1+ 22s-2(2s - 2)! (nz)3
1(nrc)5 (2s - 5)! (nn)6
<- 1)s (- 1)s+i' + 1! (flz)2S + O! (nn)2s+1 ]
(2s)![ 22s(2is)!nrr
i+ <2s - 3)! (nrr)4 +
l(2s - !)! <nn)2
122s-4(2s - 4)!
l 22sm2(2s - 2)! (nrc)3
1(nrc)5 (2s - 5)! (nT)6
(- 1)s (- 1)s." + + 1! (nT)2s O! (nT>2s+1
)(2s) ! [ 22,-?iS2-s i-+ 1
1)! (nT)2
+
22s-3 + 1
22sm3(2s - 3) ! (nrr)4
22s-5 + 1
22s-5(2s - 5)! (nT)6
3(- 1)s+i"' 't- 2.1! (nrt) 2s
](2s)!(2,,-,2(2 gi-im 1
1)! (nn)2
+
22s-3 . 1
22s-3(2s - 3)! (nz)`
22s-5 nv 1
22s-5 (2s - 5) -."+・ (nz)6
(- 1)s+i
2・1! (nn)2s]
(2s + 1)!C- 22s+i(2is + i)! nz m (2s>!i(n-)2
22s-i (2s - (7ZT>3 <2s - 2)! (nff>4 1)! 22S-3(2s - 3)! (nr,)5
rm..(2s:.Al.Iwgwn.I)s. t..'':2・i(i(,i)l2"Lli mF 6!um(,i.)ee,1 pt
82 B. TANIMOTO No. 10
i: 1'
1,
3,
5,
2s +1
7¢
3, 7, 11, ・・・
2, 6, 10, ・・・
4, 8, 12, ・・・
Il, pr cos nrrp dp
'
(2S + 1)! ( 22s÷i(2sl+ 1)! nr, - (2s)!i(nrr)2
(2s - 2)! (nz)4 22s-3(2s - 3)! (nr,)5 1)! (m)3 22s-i(2s -
- 1. m".+ (- 1)s + (- 1)s+1 (2s - 4)! (nr,)6 2ol! (nT)2s+1 O! (nrr)2s+2
]
(2s +l)! [ 22s 22s + 1
<2s)! (nz)2
+
22s-2 + 1
22s-2(2s - 2)! (nz)`
22s-4 + 1 m".÷22srm4(2s - 4>! (nn>6
2(- 1)s
O! (nrr)2s+2]
(2s +1)! ( 22s - 1
22s (2s)! (nn)2
+
22s-2 m 1
22s-2(2s - 2)! (nn)`
22sm4 ffm- l
22sm4(2s - 4)! (nz)6--- ÷
3(- os+i22.2! (nrr)2s
>j
vll. Si pr sin nxp dp
r
o
1
2
3
4
"
l, 2, 3, ・・・
si
pr sin nzp dp
1
nx(i - cos nrre)
1, 2, 3, ・・・
1, 2, 3, ・・・
1, 2, 3, ・・・
!, 2, 3, ・・・
------------
1
nrrg cos nr,e +
1 sin nz6(nn)2
l
7Zrr
g2 cos nr,g S- 2 S sin nr,6 -(m)
2(11re>3
(1 - cos nr,g")
1. pte3 nr,
cos nrre 3rr
1wu (nfl)2 g"2 sin nag" 6+ -------・ (TZrr)3
a cos nrr6 --6-L
(nrr)4Sln 7zrgr
1- -e4 i¢z
COS nzg" lhft 4(nrc)2
' '12g3 sin nrrg + --- g"2 cos nzg" (TZrr)3
24 . 24 - -- 6sin nzg + <nz)4 (nr, )5
(1 - cos nne)
---t-t---tt---------i---
l
I
No. 10 Definite Integrals for Expressjng Polvnomials into Fourier Series 83
r
o,2,4,
2s
i'
3,
5,
2s+1
n
1, 2, 3, ・・・
1, 2, 3, ・・・
Si pr sin nTp dp
<2s) ! [- e2s-1 sin nrrge2s cos ozrrg e2s-2 cos nz8 -+ + (2S)! 11T (2s - 1)! (nrc>2 (2s - 2) ! (nrr)3
e2s-3 sin nxg e2s-4 cos ntf e2sm5 sin nrre
± <2s- 3)! (nn)` (2s- 4)! (nrc)5 (2s - 5)! (nx)6
+ ... rrt- (- 1)swwie.e.in nftg"' ntiun (- 1)s(1 - cos nT6)
O! (nx) 2s +1 1! (nr,)2s]
(2s + 1)! [- e2s+i cos nr,g" 82S sin nTslt e2s-1 cos nrrg ----- -y + (2s)!(nT)2 <2s + 1)! i・zn (2s - D! (nz)3
62s-2 sin n-$-" 62s-3 cos nffse 62s-4 sin nr,e- -tvet-ummmttttttttttttt.ttt.t. ..L..t m ..u-ttttttttrmtt..-utt.tttttttumtt + ttttt tttwuvettttttrm"
(2s - 2)! (nrc,)4 (2s - 3)! (nn)5 (2s - 4)! (nT)6
tttt -F...+(wwi),Sti,20,2,nTe+L-,,,i,).'Xli.I},il.tttS]
VIII.Si pr cos nmp dp
:
r
o
n
1, 2, 3, ・・・
Si pr cos nzp dp
1.- sln nrrenff
1
2
3
4
1, 2, 3, ・・・
1, 2, 3, -・・
1, 2, 3, ・・・
1, 2, 3, ・`・
'" l l I
1
nrr6 sin nTe -
lr(n.)2 (1 H COs nffg")
1
rmg2
f・zff
sin nrrg- + sin nne 6 cos me -(IZn)2 (fZr,)3
1 A3---gnx
sin nffg-+ A--.e2cosnzg- -6-ssin me a- 6 ( 1 - cos fzTe) (nrr)2 (nrr>3 (nr, )4
1 fi4-gnr,
sin nze + 12 4 e2 sin nz8 g-3 cos nne - (nz)3(fZx>2
24 24 - (n.>4 g COS nrr6 + (n.), sin nrcc".
I------lp----------t-----
84 B. TANIMOTO No. 10
I
rl i
n
11LI
sj
pr cos nrcp dp
o,2,4,
IZs
r
f[
E
1,
3,
5,
2s +1
1, 2, 3, ・・・
1, 2, 3, ・・・
(2s)! [ e2s sin nr,g e2s-i cos nr,e e2s-2 sin nrrg"
+- (nz)2 (2s - 1)! (2s)!nr, (2s - 2) ! (ozrc)3
e2Sww3 cos nffg- g"2sm4 sin nffe e2s-5 cos nzg (Vzrr・,)4 (2s - 3>! (2s - 5)! (nT)6 <nrc)5 (2s - 4)!
(- 1)s sin nrr6 (- 1)snti gfi cos nzg -".+ + O! (nrc)2s+1 1! (nrr)2s
hj
(2s ÷1)!
cg,2i{, sX,",1".,6 + i2g,sgi,:'#'i-t,{ - ,gfiIS--iE?ge, n,.-.6,,
62s-3 sin nTsr"- e2s-4 cos nTg" e2s-2 cos nx.h"
(nz)s <nT>4 (2s - 4)! <nx>6 (2s - 2)! (2s - 3)!
(- 1)sg sin nzg" ( -- 1) s+i(1 - cos nffg)
-". -F + 1! (nr,)2s+1 O! (nrc>2s+2]
IX. svg
prsin nTp dp
r
o
1
2
3
4
17
1, 2, 3, -・・
1, 2, 3, ・・・
1, 2, 3, ・・・
1, 2, 3, ・・・
1, 2, 3, ・・・
sr.
pr sin nTp dp
1
7Zre
(cos nzg - cos nzrp)
1
nrc
(g cos nrr.i - rp cos nTv) -1 (nx>2
(sin nrcg" - sin nr, rp)
1. (g27ZT
cos nzg - q2 cos nap> 2(fZz)2
(g sin nrrg - q sin nTq)
2 - (n.)3 (COS nntsft - cos nzny)
1
nT(g3 cO.
3 (g2 sin nrre - v2 sin nrrrp)nrce - ny3 cos nrcrp) - <nz)2
<sin nxg - sin nrcrp) <g cos nscg - rp cos nrcrp) -V (nrr)4 (nrr)3
1
nrr .4(64 cos 7trrtt - rp4 cos nxrp) - <nrc)2 12 (62 cos fzze - v2 cos nzv) +'7Zr, >3
(g3 sin nrrg"' - rp3 sin nnrp>
24 (e sin nfl.lt - rp sin nnv)(7ZT)4
24 t- (n.>, (COS nrce - cos nTty)
:t
'
---.i...----.
f
i
l
Il
No. Ie Definite Integrals for Expressing Polynomi..Is into Fourier Series 85
r
o,2,4,-s-
2s
n
1, 2, 3, ・・・
!t
3,
5,
2s+1
1, 2, 3, ・・・
si
pr sin nnp dp
(2s)! [
+
- ---
e2s cos nrcg - v2s cos nffrp 62s-l
<2s)! nrc
st2s-2 cos fz.rcE rLrm!z12.i::2LCOS 7Zt.tq +
(2s - 2)! (nT)3
g"2s-4 cos nxe - rp2s-4 cosnzrp
sin ulg - rp2s-i sin nr, rp
+
<2s - l)! <nre)2
g2s-3sin nrre - n2s-3 sin fzrte
(2s - 3)! (nrr)4
g2s-5 sin nng" - )7L'S-5 sin p'zT)7
(2s - 4)! (varc)s
(- 1)s(e sin nffs" - rp sin nrtv)
+
(2s- 5)!(nz)6
(- !)s (cos nxe - cos nTv)
1! (nrc)2s O! (nn)2s+11
(2s + 1>! [ 82s+i cos nrcg - rp2s+i cos nzrp e2s sinnrrg" - rp2s sin nno
<2s + 1)! nrr
e2s-i cos nze - rp2smi cos nxrp
(2s - 1)! (nz)3
e2s-3 cos nreg" - lf2S-3cos nnn
+
(2s)!<nx)2
g2s-2 sin nTe - tr2s-2sin nrrry
+
-・- +
(2s - 3)! (nre>5
(- 1)s (4 cos nzg- - v cos nxrp)
+
(2s - 2>! (nr,)`
g"2s-4 sin nz.lt - rp2Sm4 sin nnv
(2s - 4)! <nfl)6
(- 1)s+i(sin nrcg - sin nzs)
1! (nrc)2s+1 O! (nn)2s+2 ]
x. S:pr cos nTp dp
r
o
i
2
3
n
1, 2, 3, ・・・
1, 2, 3, ・・・
1, 2, 3, ・・・
1, 2, 3, ・・・
sne
pr cos nrcp dp
1
nz<sin nrca - sin nxn)
1
nn(6 sin nz8 - v sin nrcn> -1
<nz)2 (cos nrrG - cos nTrp)
1- -(42 nn
sin naf - rp2 sin nT?) -2 (nz)
, (g cos nTe - ny cos nap)
2 (sin nxe - sin nTv) + (nrr)3
+
!.-(63 sin nzg - u3 siB nnrp) -nn
6. inr,)3 (e Sln fZZts-" - ty sin nrrp>
3 (62(fZff)2
6+ (IZT)4
cos nne - ?2 cos nzv)
(cos nrc r/ - cos nrcrp)
86 B. TANIMOTO No. 10
I.1
r
Il
I.
7Z
4i'
ll・
[ii
I
l -・
l, 2, 3, ・・・
sl
pr cos nrcp dR
o,2,4,
2s
1,
3,
5,
2s+1
1Mn-t(g4
+ 12- <nr, >3
sin nr,g" - if sinnrcry) -
(g"2 sin nr,g" - rp2 sinnn7)
4 , (g3 cos nrr6 - ty3 cos nscv)(nT)
24+ (n.,)4(e COS IZree - rp cosnrcny)
24 ma (n.)s(Sin na4 - sin nTrp)
l-t ny ----l--t---------i---
1, 2, 3, ・・・
1, 2, 3, ・・・
(2s)! [- e2s sin nr.g - ny2S sm ngrp g2s-i cos nzg' - v2s-i cos nop
+
+ ... +
62s-2 sin nr, t'-'
<2s)! nrr
m ry2s-2 sin nzu
(2s -- 2)! (n r, )3
e2s-4 sin nr, gi - ry2S-4 sin nxv
+
(2s - 1)l (nT)2
g2s-3 cos nr, g' - rp2s-3 cos nzrp
(2s - 3)! (nrc)4
g2s-5 cos nxg - o2snt5 cosnxrp
(2s -- 4)! (nT)5
<- 1)s <g" cos nne - v coS nrcv)
+
(2s - 5)! <m)6
<- 1)s+i (sin nffg - sin nff1)
1! (nrr)2s O! (nz)2s+1]
(2s + 1)! [- gfi2s+i sin nr,ein
rp2s+1 sin nffrp e2s cos nffg" - rp2S cos nrcv
+
-l- ."
e2s-i sin nrtg"
(2s + 1)! nrc
ww rp2s-1sinnzty
+
(2s)! (nr, )2
e2s-2 cos nr,g - v2s-2 cos nrrrp
(2s -
e2s-3 sin n"gn'
1)! <nr,)3
rm .ry2s-3 sin nnq
<2s - 2)! (nrr)`
62s-4 cos nr,tf - rp2s-4 cos nz?
+
(2s - 3)! (nz)5
(- 1)s+i(5sinnne - 9 Sln 11T, rp>
+
(2s - 4)! (nx)6
(- 1)s+i<cosnrrgrv' -
1 ! (nrc)2s+1 O! (nre)2s+2
cos nffrp>]i
Xi・ S1
v
pr sin nnp dp
r
e
1
n
1, 3, 5, ・・・
2, 4, 6, -・・
s1
v
pr sin nr, ,D dp
1
-(cos nrrn ÷ 1)nx
1
-(cos nRij - 1)?1rc
I
l, 3, 5, ・・・1
-・(lf cos nr, ij
7'Zr,
1.{- 1) - Slll <nrr・,)2f7ff K・'
No, 10 Definite Integrals for Expressing Polynomials into Fourier Series 87
r
1
2
3
4
---
o,2,4,---
2s
n
2, 4, 6, ・:・
1, 3, 5, ・・・
2, 4, 6, ・・・
1, 3, 5, ・・・
2, 4, 6, ・・・
1, 3, 5, ・・・
2, 4, 6, ・・・
1, 3, 5, ・・・
2, 4, 6, ・・・
'
Sl pr sin nrcp dp
1
nrc
(rp cos nTty - 1) -1 (Olrr)2
sm nffo
Hl,-
nrr
(v2 cos nrr? 2+ }> ww (n.)2V Sin n-u -
2
(nrc),(cos nTq + O
1
nrr
(rp2 cos nrcrp me 2.1) - (n.),q sm nzq2
(ilT>,(Cosnrcny - 1)
1
nrc
(o3 cos nn? +
i'
321) - (nz)2ny sln nzn6
(nrc)3(i7 COS TZrr;7 + 1)
6 + (f7fl)4
sln nrcrp
1
nn<q3 cos nzty - 1)- 32(fZrc)2? sln nmp
6
<nx)3(v cos nr,rp - 1)
6 + (nz)g
sln nrcrp
1
nz(?4 cos nnv +
1) - (.4.)2rp3
12sin nrrq - (nT),(o2 cos nzq + 1)
24 24+ (n.,)4rp Sln nrcrp + (n.,)s(COS nrrrp + 1)
1
nrc
(rp4cos nrcrp - 1) -4
(nrr)2rp 123 sin nr,n - (n.),<v2 cos nnrp - 1)
24 . 24+ (n.)4V SM 7Znrp + (n.),(Cos nnq - 1)
---t-----------------4--
(2s)! [v2s cos nrrrp + 1 (2s>! nn
rp2s-3 sin nrcv
+ <2s - 3)! (n->`
-- -y
rp2s-i sin nrrrp ry2s'2 cos nrcrp + 1
(2s - 1)! (nn>2 <2s - 2)! (nrr)3
+ q2s-4cosnnty + l - rp2Sm5 sinnrcrp
(2s - 5)! (nz)6 (2s - 4) ! <nz)5
(- li!s(rpns.i)n,,nnv+ (- 1)8[C?7:.?,re,O+,+ 1)]
(2s)! [rp2s cos nflv -1 rp2smi sin nrcrp rp2s-2 cos }・tzq -1 (2s)! nz (2s - 1)! <nrr)2 (2s - 2)! (nr, >3 ,
+ (2rp,2Srm-3 s3iln! :i.T.ry), + viSi,`so2):z(q..->,i - <2v,2S-rm5sii!n(L,;,L?,
- ... + (- ii)l (n・./i):,nffrp ÷ (- igS!((c.o.s);z,rc.n, -- i))
i/
88 B. TANIMOTO No. 10
r
1,
3,
5,
2s+1
n
1, 3, 5, ・・・
2, 4, 6, ・・・
s1 pr sin m,p d,ov
(2s + 1)!
+
rp2s+l cos nr,o +c (2s {- 1)l nn
rp2s-2 sin nrrrp
(2s - 2)! (nrr)4
(- +
1 rp2s sin nr,7
(2s)! <nrr)2
+ rp2s-3 cos nz7 +.
<nrr)o (2s - 3)!
1)s(rp cos nrrv + 1)
1 ! (nr,)2s-1
q2s-i cos nr,rp + 1
<2s - 1>! (nz>3
1 o2S-4 sin nx? (2s - 4)! (nrc)6
(- 1)s+l sinnT7+ O! (nz)2s+2
)
i'
i
(2s ÷
1>! [v2s-}-(12csoi? zre)l i.,., 1
rp2s-2 sin nrrty
+ (2s - 2)! (nz)"
(- +
v2s sin nrrrp
(2s)! (nrr)2
rp2s-3 cos nffrp -
+ (2s - 3)! (nrt)51)s (o cos nzrp - 1)
!! (nn>2s+1
n2swwi cos nmp - 1
(2s - 1)! (nrr)3
1 T2s'4 sin nzrp
(2s - 4>! (nz)6
÷ (- &IS,;,ks,ie.#r・rp]
EI
XII. s1v
pr cos nnp dp
r
o
1
2
3
n
1, 3, 5, ・・・
2, 4, 6, ・・・
1, 3, 5, ・・・
2, 4, 6, ・・ ny
1, 3, 5, ・・・
2, 4, 6, ・・・
1, 3, 5, ・・・
N
s1 pr cos nzp dpn
1.- - sm nzrp nz
1.- - sln nzny nrr
1.- -v sln nrco - nT
l(nff>
,(COs nnlj + 1)
1.' ----n sln nrc? - nT
1(nT)
,(Cos nnrp - 1)
12-npm.q sln nzrp
2- (n.)2(rp COS nffrp + 1) + 2.
(nz)3Sln nfl7
1 2ww - v nT
sln nffrp 2(nx)
2<ty COS fZTrp - 2.1> + (n.,)3Slnnfllf
1.' iit}lnrp3 Sin nffv - 3(nrc
>2(vL' cos nrerp + 1) 6.+ (nrt)3rp Sln fZTo
6 -iM <n.,>4(COS nTty -}- 1>
No. 10 Definite Integrals for Expressing Polynomials into Fourier Series 89
r
3
4
--t
o,2,4,
2s
1,
3,
5,
2s+1
fl
2, 4, 6, ...
s)
pr cos nrrp dp
1ww pmV3 nr,
sln nrrq 3Ozrc)
2(rp2 cos nTv -
1, 3, 5, ・・・
i 1
nrc
rp4 sin nzn4
2(v3 cos nzo +(nrr)
24 4(rp Cos nrrrp +(nrr)
6.1) ÷ v sm nrcn <nz)3
6 (cos nrc? - 1) + (nrr)4
tt
2, 4, 6, ・・・
------------
1, 3, 5, ・・}
+
l) --
1> -
12 o. o- sm nzv(nrr>3
24 . sln nxn(nrc)5
1.- -o4 sin mrp nrc
4
(m)
12,(v3 cos nrcrp - 1) -- (n.),q2
24 + (n.)4(q COS nrco - O
sln nrrrp
24 ve <nz)sSinnrcrp
--!-----t------------i--
(2s)! [- o2s sin nrrrp rp2s-i cos nnrp +1
+rp2s-2 sin nzrp
+
(2s)! nff
rp2s-3 cos "r, rp +1
(2s - 1)! (nn)2
rp2s-4 sin nno
(2s - 2)! (nrc)3
o2srm5 cos nmp + 1
(2s - 3)!
+・-+
(nT)4
(-
(2s - 4)! (nz)5
1)s(ty cos nzry + 1)
+
(2s - 5)! (nn)6
(- 1)s+i sin nrrrp
1 ! <nre)2s O! <nx)2s+1]
2, 4, 6, ・・・
1, 3, 5, ・・・
(2s)! [-
+
ny2s sin nTo q2smi cos nTq - 1 +(2s - 1)! (nff>2
1 rp2sm4 sin nrrry
rp2s-2 sin nrcrp
(2s)! nz
lj2s-3 cos nnrp -
(2s - 2)! (nn)3
ry2s-5 cos nzv - 1
(2s - 3)!
+."+
(nrr)` (2s - 4)! (nx)5
(- 1)s (q cos nzrp - 1)--
<2s- 5)! (nn)6
(de 1)s+isin n rtv
1! (nz)2s O! (nn)2s+1]
(2s + 1)![- v2s+i sin nTo rp2s cos nr;ry + 1-y
ty2s-1 sin nnv
+
(2s + 1)! nrr
rp2s-2 cos nr, ty + i
(2s>1 (nre>2
ty2s-3 sin nrcrp
(2s - O! (nrr)3
ty2s-4 cos nffrp + 1
(2s - 2)! (nz)`
(- +."+
(2s - 3)!
1>s+i rp sin nrr4
1 ! (fzz)2s+l
<71z)5
(-+
(2s - 4)! (nrr>6
1)oS i (ln/L?2S,IZI7 -i" 1]
90
ili"l
i' '''"'
Definite Integrals for Expressing Polynomials into Fourier Series No. 10
n
IItIt
s1
pr cos naR dpv
i
I,
3,
5,
2s+1
l
2, 4, 6, ・・・
(2s +
+
i)!(mu nyimiigi,gi?,IZ?,th " .kS ;o,;."z.z,fi+ ,g,2ili ?,i?,;z,;;,?,
g2s-2 cos nr,ry -1 ep2spm3sin 7zr,v ty2s-4 cos nrq-1
<2s - 2)! (nff)" (2s - 3)! (nn)5 (2s-4)! (?zfl>6
+ ・・・ + (thi/)i;i)rp,,/r,n nnv + (- 1>so+.!i(;c.o>s,,7{n,,o- 1> ]l}